Variance: Difference between revisions
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{{Short description|Statistical measure of how far values spread from their average}} |
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{{About|the mathematical concept|other uses|Variance (disambiguation)}} |
{{About|the mathematical concept|other uses|Variance (disambiguation)}} |
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[[File:Comparison standard deviations.svg|thumb|400px|right|Example of samples from two populations with the same mean but different variances. The red population has mean 100 and variance 100 (SD=10) while the blue population has mean 100 and variance 2500 (SD=50) where SD stands for Standard Deviation.]] |
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In [[probability theory]] and [[statistics]], the '''variance''' is a measure of how far a set of numbers is spread out. It is one of several descriptors of a [[probability distribution]], describing how far the numbers lie from the [[mean]] (expected value). In particular, the variance is one of the [[Moment (mathematics)|moments]] of a distribution. In that context, it forms part of a systematic approach to distinguishing between probability distributions. While other such approaches have been developed, those based on [[Moment (mathematics)|moments]] are advantageous in terms of mathematical and computational simplicity. |
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In [[probability theory]] and [[statistics]], '''variance''' is the [[expected value]] of the [[Squared deviations from the mean|squared deviation from the mean]] of a [[random variable]]. The [[standard deviation]] (SD) is obtained as the square root of the variance. Variance is a measure of [[statistical dispersion|dispersion]], meaning it is a measure of how far a set of numbers is spread out from their average value. It is the second [[central moment]] of a [[Probability distribution|distribution]], and the [[covariance]] of the random variable with itself, and it is often represented by <math>\sigma^2</math>, <math>s^2</math>, <math>\operatorname{Var}(X)</math>, <math>V(X)</math>, or <math>\mathbb{V}(X)</math>.<ref>{{cite book |last1=Wasserman |first1=Larry |title=All of Statistics: a concise course in statistical inference |date=2005 |publisher=Springer texts in statistics |isbn=978-1-4419-2322-6 |page=51}}</ref> |
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The variance is a [[population parameter|parameter]] describing in part either the actual probability distribution of an observed population of numbers, or the theoretical probability distribution of a sample (a not-fully-observed population) of numbers. In the latter case a sample of data from such a distribution can be used to construct an estimate of its variance: in the simplest cases this estimate can be the sample variance. |
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An advantage of variance as a measure of dispersion is that it is more amenable to algebraic manipulation than other measures of dispersion such as the [[Average absolute deviation|expected absolute deviation]]; for example, the variance of a sum of uncorrelated random variables is equal to the sum of their variances. A disadvantage of the variance for practical applications is that, unlike the standard deviation, its units differ from the random variable, which is why the standard deviation is more commonly reported as a measure of dispersion once the calculation is finished. Another disadvantage is that the variance is not finite for many distributions. |
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There are two distinct concepts that are both called "variance". One, as discussed above, is part of a theoretical [[probability distribution]] and is defined by an equation. The other variance is a characteristic of a set of observations. When variance is calculated from observations, those observations are typically measured from a real-world system. If all possible observations of the system are present, then the calculated variance is called the population variance. Normally, however, only a subset is available, and the variance calculated from this is called the sample variance. The variance calculated from a sample is considered an estimate of the full population variance. There are multiple ways to calculate an estimate of the population variance, as discussed in the section below. |
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The two kinds of variance are closely related. To see how, consider that a theoretical probability distribution can be used as a generator of hypothetical observations. If an infinite number of observations are generated using a distribution, then the sample variance calculated from that infinite set will match the value calculated using the distribution's equation for variance. Variance has a central role in statistics, where some ideas that use it include [[descriptive statistics]], [[statistical inference]], [[hypothesis testing]], [[goodness of fit]], and [[Monte Carlo method|Monte Carlo sampling]]. |
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{{TOC limit}} |
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[[File:variance_visualisation.svg|thumb|Geometric visualisation of the variance of an arbitrary distribution (2, 4, 4, 4, 5, 5, 7, 9): {{ordered list |
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|A frequency distribution is constructed. |
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|The centroid of the distribution gives its mean. |
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|A square with sides equal to the difference of each value from the mean is formed for each value. |
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|Arranging the squares into a rectangle with one side equal to the number of values, ''n'', results in the other side being the distribution's variance, ''σ''<sup>2</sup>. |
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}}]] |
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==Definition== |
==Definition== |
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The variance of a random variable |
The variance of a random variable <math>X</math> is the [[expected value]] of the [[Squared deviations from the mean|squared deviation from the mean]] of <math>X</math>, <math>\mu = \operatorname{E}[X]</math>: |
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: <math> \operatorname{Var}(X) = \operatorname{E}\left[(X - \mu)^2 \right]. </math> |
: <math> \operatorname{Var}(X) = \operatorname{E}\left[(X - \mu)^2 \right]. </math> |
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This definition encompasses random variables that are [[discrete random variable|discrete]], [[continuous random variable|continuous]], [[Cantor distribution|neither]], or mixed. The variance can also be thought of as the [[covariance]] of a random variable with itself: |
This definition encompasses random variables that are generated by processes that are [[discrete random variable|discrete]], [[continuous random variable|continuous]], [[Cantor distribution|neither]], or mixed. The variance can also be thought of as the [[covariance]] of a random variable with itself: |
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: <math>\operatorname{Var}(X) = \operatorname{Cov}(X, X).</math> |
: <math>\operatorname{Var}(X) = \operatorname{Cov}(X, X).</math> |
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The variance is also equivalent to the second [[cumulant]] of |
The variance is also equivalent to the second [[cumulant]] of a probability distribution that generates <math>X</math>. The variance is typically designated as <math>\operatorname{Var}(X)</math>, or sometimes as <math>V(X)</math> or <math>\mathbb{V}(X)</math>, or symbolically as <math>\sigma^2_X</math> or simply <math>\sigma^2</math> (pronounced "[[sigma]] squared"). The expression for the variance can be expanded as follows: |
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:<math>\begin{align} |
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:<math>\operatorname{Var}(X)= \operatorname{E}\left[X^2 - 2X\operatorname{E}[X] + (\operatorname{E}[X])^2\right] = \operatorname{E}\left[X^2\right] - 2\operatorname{E}[X]\operatorname{E}[X] + (\operatorname{E}[X])^2 = \operatorname{E}\left[X^2 \right] - (\operatorname{E}[X])^2</math> |
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\operatorname{Var}(X) &= \operatorname{E}\left[(X - \operatorname{E}[X])^2\right] \\[4pt] |
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&= \operatorname{E}\left[X^2 - 2X\operatorname{E}[X] + \operatorname{E}[X]^2\right] \\[4pt] |
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&= \operatorname{E}\left[X^2\right] - 2\operatorname{E}[X]\operatorname{E}[X] + \operatorname{E}[X]^2 \\[4pt] |
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&= \operatorname{E}\left[X^2\right] - 2\operatorname{E}[X]^2 + \operatorname{E}[X]^2 \\[4pt] |
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&= \operatorname{E}\left[X^2 \right] - \operatorname{E}[X]^2 |
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\end{align}</math> |
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In other words, the variance of {{mvar|X}} is equal to the mean of the square of {{mvar|X}} minus the square of the mean of {{mvar|X}}. This equation should not be used for computations using [[floating point arithmetic]], because it suffers from [[catastrophic cancellation]] if the two components of the equation are similar in magnitude. For other numerically stable alternatives, see [[algorithms for calculating variance]]. |
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A mnemonic for the above expression is "mean of square minus square of mean". |
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=== |
===Discrete random variable=== |
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If the random variable |
If the generator of random variable <math>X</math> is [[Discrete probability distribution|discrete]] with [[probability mass function]] <math>x_1 \mapsto p_1, x_2 \mapsto p_2, \ldots, x_n \mapsto p_n</math>, then |
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:<math>\operatorname{Var}(X) = |
:<math>\operatorname{Var}(X) = \sum_{i=1}^n p_i\cdot(x_i - \mu)^2,</math> |
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where <math>\mu</math> is the expected value, |
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:<math>\mu = \int x \, f(x) \, dx\, </math> |
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and where the integrals are [[definite integral]]s taken for ''x'' ranging over the range of ''X''. |
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where <math>\mu</math> is the expected value. That is, |
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If a continuous distribution does not have an expected value, as is the case for the [[Cauchy distribution]], it does not have a variance either. Many other distributions for which the expected value does exist also do not have a finite variance because the integral in the variance definition diverges. An example is a [[Pareto distribution]] whose [[Pareto index|index]] ''k'' satisfies {{nowrap|1 < ''k'' ≤ 2}}. |
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:<math>\mu = \sum_{i=1}^n p_i x_i .</math> |
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===Discrete random variable=== |
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(When such a discrete [[weighted variance]] is specified by weights whose sum is not 1, then one divides by the sum of the weights.) |
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If the random variable ''X'' is [[Discrete probability distribution|discrete]] with [[probability mass function]] ''x''<sub>1</sub> ↦ ''p''<sub>1</sub>, ..., ''x''<sub>''n''</sub> ↦ ''p''<sub>''n''</sub>, then |
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The variance of a collection of <math>n</math> equally likely values can be written as |
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:<math>\operatorname{Var}(X) = \sum_{i=1}^n p_i\cdot(x_i - \mu)^2 = \sum_{i=1}^n (p_i\cdot x_i^2) - \mu^2</math> |
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where <math>\mu</math> is the expected value, i.e. |
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:<math>\mu = \sum_{i=1}^n p_i\cdot x_i </math> . |
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:<math> \operatorname{Var}(X) = \frac{1}{n} \sum_{i=1}^n (x_i - \mu)^2 </math> |
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(When such a discrete [[weighted variance]] is specified by weights whose sum is not 1, then one divides by the sum of the weights.) |
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where <math>\mu</math> is the average value. That is, |
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The variance of a set of ''n'' equally likely values can be written as |
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:<math> \operatorname{Var}(X) = \frac{1}{n} \sum_{i=1}^n (x_i - \mu)^2. </math> |
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:<math>\mu = \frac{1}{n}\sum_{i=1}^n x_i .</math> |
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The variance of a set of ''n'' equally likely values can be equivalently expressed, without directly referring to the mean, in terms of squared deviations of all points from each other: |
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:<math> \operatorname{Var}(X) = \frac{1}{n^2} \sum_{i=1}^n \sum_{j=1}^n \frac{1}{2}(x_i - x_j)^2. </math> |
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The variance of a set of <math>n</math> equally likely values can be equivalently expressed, without directly referring to the mean, in terms of squared deviations of all pairwise squared distances of points from each other:<ref>{{cite conference|author=Yuli Zhang |author2=Huaiyu Wu |author3=Lei Cheng |date=June 2012|title=Some new deformation formulas about variance and covariance|conference=Proceedings of 4th International Conference on Modelling, Identification and Control(ICMIC2012)|pages=987–992}}</ref> |
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==Examples== |
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:<math> \operatorname{Var}(X) = \frac{1}{n^2} \sum_{i=1}^n \sum_{j=1}^n \frac{1}{2}(x_i - x_j)^2 = \frac{1}{n^2}\sum_i \sum_{j>i} (x_i-x_j)^2. </math> |
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===Normal distribution=== |
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The [[normal distribution]] with parameters μ and σ is a continuous distribution whose [[probability density function]] is given by: |
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:<math> |
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f(x) = \frac{1}{\sqrt{2\pi \sigma^2}} e^{ -\frac{(x-\mu)^2}{2\sigma^2} }. |
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</math> |
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It has mean μ and variance equal to: |
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:<math> |
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\operatorname{Var}(X) = \int_{-\infty}^\infty \frac{(x - \mu)^2}{\sqrt{2\pi \sigma^2}} e^{ -\frac{(x-\mu)^2}{2\sigma^2} } \, dx = \sigma^2. |
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</math> |
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The role of the normal distribution in the [[central limit theorem]] is in part responsible for the prevalence of the variance in probability and statistics. |
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===Absolutely continuous random variable=== |
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If the random variable <math>X</math> has a [[probability density function]] <math>f(x)</math>, and <math>F(x)</math> is the corresponding [[cumulative distribution function]], then |
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===Exponential distribution=== |
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The [[exponential distribution]] with parameter λ is a continuous distribution whose support is the semi-infinite interval [0,∞). Its [[probability density function]] is given by: |
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:<math> |
:<math>\begin{align} |
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\operatorname{Var}(X) = \sigma^2 &= \int_{\R} (x-\mu)^2 f(x) \, dx \\[4pt] |
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&= \int_{\R} x^2f(x)\,dx -2\mu\int_{\R} xf(x)\,dx + \mu^2\int_{\R} f(x)\,dx \\[4pt] |
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&= \int_{\R} x^2 \,dF(x) - 2 \mu \int_{\R} x \,dF(x) + \mu^2 \int_{\R} \,dF(x) \\[4pt] |
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&= \int_{\R} x^2 \,dF(x) - 2 \mu \cdot \mu + \mu^2 \cdot 1 \\[4pt] |
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&= \int_{\R} x^2 \,dF(x) - \mu^2, |
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\end{align}</math> |
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or equivalently, |
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and it has expected value μ = λ<sup>−1</sup>. The variance is equal to: |
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:<math> |
:<math>\operatorname{Var}(X) = \int_{\R} x^2 f(x) \,dx - \mu^2 ,</math> |
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where <math>\mu</math> is the expected value of <math>X</math> given by |
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So for an exponentially distributed random variable σ<sup>2</sup> = μ<sup>2</sup>. |
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:<math>\mu = \int_{\R} x f(x) \, dx = \int_{\R} x \, d F(x). </math> |
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In these formulas, the integrals with respect to <math>dx</math> and <math>dF(x)</math> |
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===Poisson distribution=== |
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are [[Lebesgue integral|Lebesgue]] and [[Lebesgue–Stieltjes integration|Lebesgue–Stieltjes]] integrals, respectively. |
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The [[Poisson distribution]] with parameter λ is a discrete distribution for ''k'' = 0, 1, 2, ... Its [[probability mass function]] is given by: |
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If the function <math>x^2f(x)</math> is [[Riemann-integrable]] on every finite interval <math>[a,b]\subset\R,</math> then |
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:<math>p(k) = \frac{\lambda^k}{k!} e^{-\lambda},</math> |
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:<math>\operatorname{Var}(X) = \int^{+\infty}_{-\infty} x^2 f(x) \, dx - \mu^2, </math> |
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and it has expected value μ = λ. The variance is equal to: |
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where the integral is an [[improper Riemann integral]]. |
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:<math> \operatorname{Var}(X) = \sum_{k=1}^{n} \frac{\lambda^k}{k!} e^{-\lambda k} (k-\lambda)^2 = \lambda,</math> |
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==Examples== |
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So for a Poisson-distributed random variable σ<sup>2</sup> = μ. |
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=== |
===Exponential distribution=== |
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The [[ |
The [[exponential distribution]] with parameter {{mvar|λ}} is a continuous distribution whose [[probability density function]] is given by |
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:<math> |
:<math>f(x) = \lambda e^{-\lambda x}</math> |
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on the interval {{math|[0, ∞)}}. Its mean can be shown to be |
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and it has expected value μ = ''np''. The variance is equal to: |
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:<math> |
:<math>\operatorname{E}[X] = \int_0^\infty x \lambda e^{-\lambda x} \, dx = \frac{1}{\lambda}.</math> |
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====Coin toss==== |
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The binomial distribution with ''p'' = 0.5 describes the probability of getting ''k'' heads in ''n'' tosses. Thus the expected value of the number of heads is ''n''/2, and the variance is ''n''/4. |
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Using [[integration by parts]] and making use of the expected value already calculated, we have: |
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===Fair die<!--Singular: die; plural: dice. Don't change-->=== |
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:<math>\begin{align} |
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A six-sided [[dice|fair die]] can be modelled with a discrete random variable with outcomes 1 through 6, each with equal probability <math>\textstyle\frac{1}{6}</math>. The expected value is (1 + 2 + 3 + 4 + 5 + 6)/6 = 3.5. Therefore the variance can be computed to be: |
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\operatorname{E}\left[X^2\right] &= \int_0^\infty x^2 \lambda e^{-\lambda x} \, dx \\ |
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&= \left[ -x^2 e^{-\lambda x} \right]_0^\infty + \int_0^\infty 2xe^{-\lambda x} \,dx \\ |
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&= 0 + \frac{2}{\lambda}\operatorname{E}[X] \\ |
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&= \frac{2}{\lambda^2}. |
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\end{align}</math> |
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Thus, the variance of {{mvar|X}} is given by |
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:<math> |
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:<math>\operatorname{Var}(X) = \operatorname{E}\left[X^2\right] - \operatorname{E}[X]^2 = \frac{2}{\lambda^2} - \left(\frac{1}{\lambda}\right)^2 = \frac{1}{\lambda^2}.</math> |
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\begin{align} |
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\sum_{i=1}^6 \tfrac{1}{6}(i - 3.5)^2 = \tfrac{1}{6}\sum_{i=1}^6 (i - 3.5)^2 & = \tfrac{1}{6}\left((-2.5)^2{+}(-1.5)^2{+}(-0.5)^2{+}0.5^2{+}1.5^2{+}2.5^2\right) \\ |
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& = \tfrac{1}{6} \cdot 17.50 = \tfrac{35}{12} \approx 2.92. |
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\end{align} |
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</math> |
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===Fair dice<!--Singular: die; plural: dice. Don't change-->=== |
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The general formula for the variance of the outcome ''X'' of a die of n sides is: |
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A fair [[dice|six-sided dice]] can be modeled as a discrete random variable, {{mvar|X}}, with outcomes 1 through 6, each with equal probability 1/6. The expected value of {{mvar|X}} is <math>(1 + 2 + 3 + 4 + 5 + 6)/6 = 7/2.</math> Therefore, the variance of {{mvar|X}} is |
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:<math> |
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\begin{align} |
:<math>\begin{align} |
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\operatorname{Var}(X) &= \sum_{i=1}^6 \frac{1}{6}\left(i - \frac{7}{2}\right)^2 \\[5pt] |
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\sigma^2=E(X^2)-(E(X))^2 |
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&=\frac{1}{ |
&= \frac{1}{6}\left((-5/2)^2 + (-3/2)^2 + (-1/2)^2 + (1/2)^2 + (3/2)^2 + (5/2)^2\right) \\[5pt] |
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&= \frac{35}{12} \approx 2.92. |
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&=\tfrac 16 (n+1)(2n+1) - \tfrac 14 (n+1)^2\\ |
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\end{align}</math> |
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&=\frac{ n^2-1 }{12}. |
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\end{align} |
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The general formula for the variance of the outcome, {{mvar|X}}, of an {{nowrap|{{mvar|n}}-sided}} die is |
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</math> |
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:<math>\begin{align} |
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\operatorname{Var}(X) &= \operatorname{E}\left(X^2\right) - (\operatorname{E}(X))^2 \\[5pt] |
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&= \frac{1}{n}\sum_{i=1}^n i^2 - \left(\frac{1}{n}\sum_{i=1}^n i\right)^2 \\[5pt] |
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&= \frac{(n + 1)(2n + 1)}{6} - \left(\frac{n + 1}{2}\right)^2 \\[4pt] |
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&= \frac{n^2 - 1}{12}. |
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\end{align}</math> |
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=== Commonly used probability distributions === |
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The following table lists the variance for some commonly used probability distributions. |
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{| class="wikitable" |
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|- |
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! Name of the probability distribution |
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! Probability distribution function |
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! Mean |
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! Variance |
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|- |
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| [[Binomial distribution]] |
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| <math>\Pr\,(X=k) = \binom{n}{k}p^k(1 - p)^{n-k}</math> |
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| <math>np</math> |
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! <math>np(1 - p)</math> |
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|- |
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| [[Geometric distribution]] |
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| <math>\Pr\,(X=k) = (1 - p)^{k-1}p</math> |
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| <math>\frac{1}{p}</math> |
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! <math>\frac{(1 - p)}{p^2}</math> |
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|- |
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| [[Normal distribution]] |
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| <math>f\left(x \mid \mu, \sigma^2\right) = \frac{1}{\sqrt{2\pi\sigma^2}} e^{-\frac{(x - \mu)^2}{2\sigma^2}}</math> |
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| <math>\mu</math> |
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! <math>\sigma^2</math> |
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|- |
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| [[Uniform distribution (continuous)]] |
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| <math>f(x \mid a, b) = \begin{cases} |
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\frac{1}{b - a} & \text{for } a \le x \le b, \\[3pt] |
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0 & \text{for } x < a \text{ or } x > b |
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\end{cases}</math> |
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| <math>\frac{a + b}{2}</math> |
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! <math>\frac{(b - a)^2}{12}</math> |
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|- |
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| [[Exponential distribution]] |
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| <math>f(x \mid \lambda) = \lambda e^{-\lambda x}</math> |
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| <math>\frac{1}{\lambda}</math> |
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! <math>\frac{1}{\lambda^2}</math> |
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|- |
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| [[Poisson distribution]] |
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| <math>f(k \mid \lambda) = \frac{e^{-\lambda}\lambda^{k}}{k!}</math> |
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| <math>\lambda </math> |
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! <math>\lambda </math> |
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|} |
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==Properties== |
==Properties== |
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===Basic properties=== |
===Basic properties=== |
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Variance is non-negative because the squares are positive or zero |
Variance is non-negative because the squares are positive or zero: |
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:<math>\operatorname{Var}(X)\ge 0.</math> |
:<math>\operatorname{Var}(X)\ge 0.</math> |
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The variance of a constant |
The variance of a constant is zero. |
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:<math>\operatorname{Var}(a) = 0.</math> |
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Conversely, if the variance of a random variable is 0, then it is [[almost surely]] a constant. That is, it always has the same value: |
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:<math>\operatorname{Var}(X)= 0 \iff \exists a : P(X=a) = 1.</math> |
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===Issues of finiteness=== |
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If a distribution does not have a finite expected value, as is the case for the [[Cauchy distribution]], then the variance cannot be finite either. However, some distributions may not have a finite variance, despite their expected value being finite. An example is a [[Pareto distribution]] whose [[Pareto index|index]] <math>k</math> satisfies <math>1 < k \leq 2.</math> |
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===Decomposition=== |
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The general formula for variance decomposition or the [[law of total variance]] is: If <math>X</math> and <math>Y</math> are two random variables, and the variance of <math>X</math> exists, then |
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:<math>\operatorname{Var}[X]=\operatorname{E}(\operatorname{Var}[X\mid Y])+\operatorname{Var}(\operatorname{E}[X\mid Y]).</math> |
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The [[conditional expectation]] <math>\operatorname E(X\mid Y)</math> of <math>X</math> given <math>Y</math>, and the [[conditional variance]] <math>\operatorname{Var}(X\mid Y)</math> may be understood as follows. Given any particular value ''y'' of the random variable ''Y'', there is a conditional expectation <math>\operatorname E(X\mid Y=y)</math> given the event ''Y'' = ''y''. This quantity depends on the particular value ''y''; it is a function <math> g(y) = \operatorname E(X\mid Y=y)</math>. That same function evaluated at the random variable ''Y'' is the conditional expectation <math>\operatorname E(X\mid Y) = g(Y).</math> |
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In particular, if <math>Y</math> is a discrete random variable assuming possible values <math>y_1, y_2, y_3 \ldots</math> with corresponding probabilities <math>p_1, p_2, p_3 \ldots, </math>, then in the formula for total variance, the first term on the right-hand side becomes |
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:<math>\operatorname{E}(\operatorname{Var}[X \mid Y]) = \sum_i p_i \sigma^2_i,</math> |
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where <math>\sigma^2_i = \operatorname{Var}[X \mid Y = y_i]</math>. Similarly, the second term on the right-hand side becomes |
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:<math>\operatorname{Var}(\operatorname{E}[X \mid Y]) = \sum_i p_i \mu_i^2 - \left(\sum_i p_i \mu_i\right)^2 = \sum_i p_i \mu_i^2 - \mu^2,</math> |
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where <math>\mu_i = \operatorname{E}[X \mid Y = y_i]</math> and <math>\mu = \sum_i p_i \mu_i</math>. Thus the total variance is given by |
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:<math>\operatorname{Var}[X] = \sum_i p_i \sigma^2_i + \left( \sum_i p_i \mu_i^2 - \mu^2 \right).</math> |
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A similar formula is applied in [[analysis of variance]], where the corresponding formula is |
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:<math>\mathit{MS}_\text{total} = \mathit{MS}_\text{between} + \mathit{MS}_\text{within};</math> |
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here <math>\mathit{MS}</math> refers to the Mean of the Squares. In [[linear regression]] analysis the corresponding formula is |
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:<math>\mathit{MS}_\text{total} = \mathit{MS}_\text{regression} + \mathit{MS}_\text{residual}.</math> |
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This can also be derived from the additivity of variances, since the total (observed) score is the sum of the predicted score and the error score, where the latter two are uncorrelated. |
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Similar decompositions are possible for the sum of squared deviations (sum of squares, <math>\mathit{SS}</math>): |
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:<math>\mathit{SS}_\text{total} = \mathit{SS}_\text{between} + \mathit{SS}_\text{within},</math> |
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:<math>\mathit{SS}_\text{total} = \mathit{SS}_\text{regression} + \mathit{SS}_\text{residual}.</math> |
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===Calculation from the CDF=== |
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The population variance for a non-negative random variable can be expressed in terms of the [[cumulative distribution function]] ''F'' using |
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:<math>2\int_0^\infty u(1 - F(u))\,du - \left(\int_0^\infty (1 - F(u))\,du\right)^2.</math> |
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This expression can be used to calculate the variance in situations where the CDF, but not the [[probability density function|density]], can be conveniently expressed. |
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===Characteristic property=== |
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The second [[moment (mathematics)|moment]] of a random variable attains the minimum value when taken around the first moment (i.e., mean) of the random variable, i.e. <math>\mathrm{argmin}_m\,\mathrm{E}\left(\left(X - m\right)^2\right) = \mathrm{E}(X)</math>. Conversely, if a continuous function <math>\varphi</math> satisfies <math>\mathrm{argmin}_m\,\mathrm{E}(\varphi(X - m)) = \mathrm{E}(X)</math> for all random variables ''X'', then it is necessarily of the form <math>\varphi(x) = a x^2 + b</math>, where {{nowrap|''a'' > 0}}. This also holds in the multidimensional case.<ref>{{Cite journal | last1 = Kagan | first1 = A. | last2 = Shepp | first2 = L. A. | doi = 10.1016/S0167-7152(98)00041-8 | title = Why the variance? | journal = Statistics & Probability Letters | volume = 38 | issue = 4 | pages = 329–333 | year = 1998 }}</ref> |
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===Units of measurement=== |
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Unlike the [[Average absolute deviation|expected absolute deviation]], the variance of a variable has units that are the square of the units of the variable itself. For example, a variable measured in meters will have a variance measured in meters squared. For this reason, describing data sets via their [[standard deviation]] or [[root mean square deviation]] is often preferred over using the variance. In the dice example the standard deviation is {{math|{{sqrt|2.9}} ≈ 1.7}}, slightly larger than the expected absolute deviation of 1.5. |
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The standard deviation and the expected absolute deviation can both be used as an indicator of the "spread" of a distribution. The standard deviation is more amenable to algebraic manipulation than the expected absolute deviation, and, together with variance and its generalization [[covariance]], is used frequently in theoretical statistics; however the expected absolute deviation tends to be more [[Robust statistics|robust]] as it is less sensitive to [[outlier]]s arising from [[measurement error|measurement anomalies]] or an unduly [[heavy-tailed distribution]]. |
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==Propagation== |
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:<math>P(X=a) = 1\Leftrightarrow \operatorname{Var}(X)= 0.</math> |
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===Addition and multiplication by a constant=== |
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Variance is [[Invariant (mathematics)|invariant]] with respect to changes in a [[location parameter]]. That is, if a constant is added to all values of the variable, the variance is unchanged. |
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Variance is [[Invariant (mathematics)|invariant]] with respect to changes in a [[location parameter]]. That is, if a constant is added to all values of the variable, the variance is unchanged: |
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:<math>\operatorname{Var}(X+a)=\operatorname{Var}(X).</math> |
:<math>\operatorname{Var}(X+a)=\operatorname{Var}(X).</math> |
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If all values are scaled by a constant, the variance is scaled by the square of that constant |
If all values are scaled by a constant, the variance is scaled by the square of that constant: |
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:<math>\operatorname{Var}(aX)=a^2\operatorname{Var}(X).</math> |
:<math>\operatorname{Var}(aX)=a^2\operatorname{Var}(X).</math> |
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The variance of a sum of two random variables is given by |
The variance of a sum of two random variables is given by |
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:<math>\operatorname{Var}(aX+bY)=a^2\operatorname{Var}(X)+b^2\operatorname{Var}(Y)+2ab\, \operatorname{Cov}(X,Y) |
:<math>\operatorname{Var}(aX + bY)=a^2\operatorname{Var}(X)+b^2\operatorname{Var}(Y)+2ab\, \operatorname{Cov}(X,Y)</math> |
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:<math>\operatorname{Var}( |
:<math>\operatorname{Var}(aX - bY)=a^2\operatorname{Var}(X)+b^2\operatorname{Var}(Y)-2ab\, \operatorname{Cov}(X,Y)</math> |
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where <math>\operatorname{Cov}(X,Y)</math> is the [[covariance]]. |
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In general we have for the sum of <math>N</math> random variables <math>\{X_1,\dots,X_N\}</math>: |
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:<math>\operatorname{Var}\left(\sum_{i=1}^N X_i\right)=\sum_{i,j=1}^N\operatorname{Cov}(X_i,X_j)=\sum_{i=1}^N\operatorname{Var}(X_i)+\sum_{i\ne j}\operatorname{Cov}(X_i,X_j).</math> |
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=== Linear combinations === |
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In general, for the sum of <math>N</math> random variables <math>\{X_1,\dots,X_N\}</math>, the variance becomes: |
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:<math>\operatorname{Var}\left(\sum_{i=1}^N X_i\right)=\sum_{i,j=1}^N\operatorname{Cov}(X_i,X_j)=\sum_{i=1}^N\operatorname{Var}(X_i)+ \sum_{i\ne j}\operatorname{Cov}(X_i,X_j),</math> |
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see also general [[Bienaymé's identity]]. |
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These results lead to the variance of a [[linear combination]] as: |
These results lead to the variance of a [[linear combination]] as: |
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Line 134: | Line 259: | ||
:<math> |
:<math> |
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\begin{align} |
\begin{align} |
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\operatorname{Var}\left( \sum_{i=1}^ |
\operatorname{Var}\left( \sum_{i=1}^N a_iX_i\right) &=\sum_{i,j=1}^{N} a_ia_j\operatorname{Cov}(X_i,X_j) \\ |
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&=\sum_{i=1}^ |
&=\sum_{i=1}^N a_i^2\operatorname{Var}(X_i)+\sum_{i\not=j}a_ia_j\operatorname{Cov}(X_i,X_j)\\ |
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& =\sum_{i=1}^ |
& =\sum_{i=1}^N a_i^2\operatorname{Var}(X_i)+2\sum_{1\le i<j\le N}a_ia_j\operatorname{Cov}(X_i,X_j). |
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\end{align} |
\end{align} |
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</math> |
</math> |
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Line 142: | Line 267: | ||
If the random variables <math>X_1,\dots,X_N</math> are such that |
If the random variables <math>X_1,\dots,X_N</math> are such that |
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:<math>\operatorname{Cov}(X_i,X_j)=0\ ,\ \forall\ (i\ne j) ,</math> |
:<math>\operatorname{Cov}(X_i,X_j)=0\ ,\ \forall\ (i\ne j) ,</math> |
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they are said to be [[Covariance#Definition| |
then they are said to be [[Covariance#Definition|uncorrelated]]. It follows immediately from the expression given earlier that if the random variables <math>X_1,\dots,X_N</math> are uncorrelated, then the variance of their sum is equal to the sum of their variances, or, expressed symbolically: |
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:<math>\operatorname{Var}\left(\sum_{i=1}^N X_i\right)=\sum_{i=1}^N\operatorname{Var}(X_i).</math> |
:<math>\operatorname{Var}\left(\sum_{i=1}^N X_i\right)=\sum_{i=1}^N\operatorname{Var}(X_i).</math> |
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Since |
Since independent random variables are always uncorrelated (see {{Section link|Covariance|Uncorrelatedness and independence}}), the equation above holds in particular when the random variables <math>X_1,\dots,X_n</math> are independent. Thus, independence is sufficient but not necessary for the variance of the sum to equal the sum of the variances. |
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====Matrix notation for the variance of a linear combination==== |
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===Sum of uncorrelated variables (Bienaymé formula)=== |
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{{see also|Sum of normally distributed random variables}} |
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One reason for the use of the variance in preference to other measures of dispersion is that the variance of the sum (or the difference) of [[uncorrelated]] random variables is the sum of their variances: |
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Define <math>X</math> as a column vector of <math>n</math> random variables <math>X_1, \ldots,X_n</math>, and <math>c</math> as a column vector of <math>n</math> scalars <math>c_1, \ldots,c_n</math>. Therefore, <math>c^\mathsf{T} X</math> is a [[linear combination]] of these random variables, where <math>c^\mathsf{T}</math> denotes the [[transpose]] of <math>c</math>. Also let <math>\Sigma</math> be the [[covariance matrix]] of <math>X</math>. The variance of <math>c^\mathsf{T}X</math> is then given by:<ref>{{Cite book | last1=Johnson | first1=Richard | last2=Wichern | first2=Dean | year=2001 | title=Applied Multivariate Statistical Analysis | url=https://archive.org/details/appliedmultivari00john_130 | url-access=limited | publisher=Prentice Hall | page=[https://archive.org/details/appliedmultivari00john_130/page/n96 76] | isbn=0-13-187715-1 }}</ref> |
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:<math>\operatorname{Var}\Big(\sum_{i=1}^n X_i\Big) = \sum_{i=1}^n \operatorname{Var}(X_i).</math> |
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:<math>\operatorname{Var}\left(c^\mathsf{T} X\right) = c^\mathsf{T} \Sigma c .</math> |
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This statement is called the [[Irénée-Jules Bienaymé|Bienaymé]] formula.<ref>[[Michel Loeve|Loeve, M.]] (1977) "Probability Theory", ''Graduate Texts in Mathematics'', Volume 45, 4th edition, Springer-Verlag, p. 12.</ref> and was discovered in 1853.{{citation needed|date=February 2013}} It is often made with the stronger condition that the variables are [[statistical independence|independent]], but uncorrelatedness suffices. So if all the variables have the same variance σ<sup>2</sup>, then, since division by ''n'' is a linear transformation, this formula immediately implies that the variance of their mean is |
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This implies that the variance of the mean can be written as (with a column vector of ones) |
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:<math>\operatorname{Var}\left(\overline{X}\right) = \operatorname{Var}\left(\frac {1} {n}\sum_{i=1}^n X_i\right) = \frac {1} {n^2}\sum_{i=1}^n \operatorname{Var}\left(X_i\right) = \frac {\sigma^2} {n}.</math> |
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:<math>\operatorname{Var}\left(\bar{x}\right) = \operatorname{Var}\left(\frac{1}{n} 1'X\right) = \frac{1}{n^2} 1'\Sigma 1.</math> |
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That is, the variance of the mean decreases when ''n'' increases. This formula for the variance of the mean is used in the definition of the [[standard error (statistics)|standard error]] of the sample mean, which is used in the [[central limit theorem]]. |
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=== |
===Sum of variables=== |
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====Sum of uncorrelated variables==== |
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If two variables X and Y are [[Independence (probability theory)|independent]], the variance of their product is given by<ref>[[Leo Goodman|Goodman, Leo A.]], "On the exact variance of products," ''[[Journal of the American Statistical Association]]'', December 1960, 708–713.</ref><ref>Goodman, Leo A., "The variance of the product of K random variables," ''Journal of the American Statistical Association'', March 1962, 54ff.</ref> |
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{{main article|Bienaymé's identity}} |
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{{see also|Sum of normally distributed random variables}} |
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One reason for the use of the variance in preference to other measures of dispersion is that the variance of the sum (or the difference) of [[uncorrelated]] random variables is the sum of their variances: |
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:<math>\operatorname{Var}( |
:<math>\operatorname{Var}\left(\sum_{i=1}^n X_i\right) = \sum_{i=1}^n \operatorname{Var}(X_i).</math> |
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This statement is called the [[Irénée-Jules Bienaymé|Bienaymé]] formula<ref>[[Michel Loève|Loève, M.]] (1977) "Probability Theory", ''Graduate Texts in Mathematics'', Volume 45, 4th edition, Springer-Verlag, p. 12.</ref> and was discovered in 1853.<ref>[[Irénée-Jules Bienaymé|Bienaymé, I.-J.]] (1853) "Considérations à l'appui de la découverte de Laplace sur la loi de probabilité dans la méthode des moindres carrés", ''Comptes rendus de l'Académie des sciences Paris'', 37, p. 309–317; digital copy available [http://visualiseur.bnf.fr/CadresFenetre?O=NUMM-2994&I=313]</ref><ref>[[Irénée-Jules Bienaymé|Bienaymé, I.-J.]] (1867) "Considérations à l'appui de la découverte de Laplace sur la loi de probabilité dans la méthode des moindres carrés", ''Journal de Mathématiques Pures et Appliquées, Série 2'', Tome 12, p. 158–167; digital copy available [http://gallica.bnf.fr/ark:/12148/bpt6k16411c/f166.image.n19][http://sites.mathdoc.fr/JMPA/PDF/JMPA_1867_2_12_A10_0.pdf]</ref> It is often made with the stronger condition that the variables are [[statistical independence|independent]], but being uncorrelated suffices. So if all the variables have the same variance σ<sup>2</sup>, then, since division by ''n'' is a linear transformation, this formula immediately implies that the variance of their mean is |
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===Sum of correlated variables=== |
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:<math> |
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In general, if the variables are [[correlated]], then the variance of their sum is the sum of their [[covariance]]s: |
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\operatorname{Var}\left(\overline{X}\right) = \operatorname{Var}\left(\frac{1}{n} \sum_{i=1}^n X_i\right) = |
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\frac{1}{n^2}\sum_{i=1}^n \operatorname{Var}\left(X_i\right) = |
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\frac{1}{n^2}n\sigma^2 = |
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\frac{\sigma^2}{n}. |
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</math> |
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That is, the variance of the mean decreases when ''n'' increases. This formula for the variance of the mean is used in the definition of the [[standard error (statistics)|standard error]] of the sample mean, which is used in the [[central limit theorem]]. |
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:<math>\operatorname{Var}\left(\sum_{i=1}^n X_i\right) = \sum_{i=1}^n \sum_{j=1}^n \operatorname{Cov}(X_i, X_j).</math> |
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To prove the initial statement, it suffices to show that |
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(Note: This by definition includes the variance of each variable, since Cov(''X''<sub>''i''</sub>,''X''<sub>''i''</sub>) = Var(''X''<sub>''i''</sub>).) |
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:<math>\operatorname{Var}(X + Y) = \operatorname{Var}(X) + \operatorname{Var}(Y).</math> |
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Here Cov is the covariance, which is zero for independent random variables (if it exists). The formula states that the variance of a sum is equal to the sum of all elements in the covariance matrix of the components. This formula is used in the theory of [[Cronbach's alpha]] in [[classical test theory]]. |
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The general result then follows by induction. Starting with the definition, |
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So if the variables have equal variance ''σ''<sup>2</sup> and the average correlation of distinct variables is ''ρ'', then the variance of their mean is |
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:<math>\begin{align} |
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:<math>\operatorname{Var}(\overline{X}) = \frac {\sigma^2} {n} + \frac {n-1} {n} \rho \sigma^2.</math> |
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\operatorname{Var}(X + Y) &= \operatorname{E}\left[(X + Y)^2\right] - (\operatorname{E}[X + Y])^2 \\[5pt] |
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&= \operatorname{E}\left[X^2 + 2XY + Y^2\right] - (\operatorname{E}[X] + \operatorname{E}[Y])^2. |
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\end{align}</math> |
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Using the linearity of the [[Expectation Operator|expectation operator]] and the assumption of independence (or uncorrelatedness) of ''X'' and ''Y'', this further simplifies as follows: |
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This implies that the variance of the mean increases with the average of the correlations. Moreover, if the variables have unit variance, for example if they are standardized, then this simplifies to |
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:<math>\begin{align} |
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:<math>\operatorname{Var}(\overline{X}) = \frac {1} {n} + \frac {n-1} {n} \rho.</math> |
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\operatorname{Var}(X + Y) &= \operatorname{E}\left[X^2\right] + 2\operatorname{E}[XY] + \operatorname{E}\left[Y^2\right] - \left(\operatorname{E}[X]^2 + 2\operatorname{E}[X]\operatorname{E}[Y] + \operatorname{E}[Y]^2\right) \\[5pt] |
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&= \operatorname{E}\left[X^2\right] + \operatorname{E}\left[Y^2\right] - \operatorname{E}[X]^2 - \operatorname{E}[Y]^2 \\[5pt] |
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&= \operatorname{Var}(X) + \operatorname{Var}(Y). |
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\end{align}</math> |
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====Sum of correlated variables==== |
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This formula is used in the [[Spearman–Brown prediction formula]] of classical test theory. This converges to ''ρ'' if ''n'' goes to infinity, provided that the average correlation remains constant or converges too. So for the variance of the mean of standardized variables with equal correlations or converging average correlation we have |
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=====Sum of correlated variables with fixed sample size===== |
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:<math> \lim_{n \to \infty} \operatorname{Var}(\overline{X}) = \rho.</math> |
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{{main article|Bienaymé's identity}} |
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In general, the variance of the sum of {{math|n}} variables is the sum of their [[covariance]]s: |
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:<math>\operatorname{Var}\left(\sum_{i=1}^n X_i\right) = \sum_{i=1}^n \sum_{j=1}^n \operatorname{Cov}\left(X_i, X_j\right) = \sum_{i=1}^n \operatorname{Var}\left(X_i\right) + 2\sum_{1\le i<j\le n}\operatorname{Cov}\left(X_i, X_j\right).</math> |
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Therefore, the variance of the mean of a large number of standardized variables is approximately equal to their average correlation. This makes clear that the sample mean of correlated variables does generally not converge to the population mean, even though the [[Law of large numbers]] states that the sample mean will converge for independent variables. |
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(Note: The second equality comes from the fact that {{math|Cov(''X''<sub>''i''</sub>,''X''<sub>''i''</sub>) {{=}} Var(''X''<sub>''i''</sub>)}}.) |
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===Weighted sum of variables=== |
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Here, <math>\operatorname{Cov}(\cdot,\cdot)</math> is the [[covariance]], which is zero for independent random variables (if it exists). The formula states that the variance of a sum is equal to the sum of all elements in the covariance matrix of the components. The next expression states equivalently that the variance of the sum is the sum of the diagonal of covariance matrix plus two times the sum of its upper triangular elements (or its lower triangular elements); this emphasizes that the covariance matrix is symmetric. This formula is used in the theory of [[Cronbach's alpha]] in [[classical test theory]]. |
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The scaling property and the Bienaymé formula, along with this property from the [[covariance]] page: Cov(''aX'', ''bY'') = ''ab'' Cov(''X'', ''Y'') jointly imply that |
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So, if the variables have equal variance ''σ''<sup>2</sup> and the average [[correlation]] of distinct variables is ''ρ'', then the variance of their mean is |
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:<math>\operatorname{Var}(aX+bY) =a^2 \operatorname{Var}(X) + b^2 \operatorname{Var}(Y) + 2ab\, \operatorname{Cov}(X, Y).</math> |
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:<math>\operatorname{Var}\left(\overline{X}\right) = \frac{\sigma^2}{n} + \frac{n - 1}{n}\rho\sigma^2.</math> |
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This implies that in a weighted sum of variables, the variable with the largest weight will have a disproportionally large weight in the variance of the total. For example, if ''X'' and ''Y'' are uncorrelated and the weight of ''X'' is two times the weight of ''Y'', then the weight of the variance of ''X'' will be four times the weight of the variance of ''Y''. |
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This implies that the variance of the mean increases with the average of the correlations. In other words, additional correlated observations are not as effective as additional independent observations at reducing the [[standard error|uncertainty of the mean]]. Moreover, if the variables have unit variance, for example if they are standardized, then this simplifies to |
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The expression above can be extended to a weighted sum of multiple variables: |
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:<math>\operatorname{Var}\left(\ |
:<math>\operatorname{Var}\left(\overline{X}\right) = \frac{1}{n} + \frac{n - 1}{n}\rho.</math> |
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This formula is used in the [[Spearman–Brown prediction formula]] of classical test theory. This converges to ''ρ'' if ''n'' goes to infinity, provided that the average correlation remains constant or converges too. So for the variance of the mean of standardized variables with equal correlations or converging average correlation we have |
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===Decomposition=== |
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:<math>\lim_{n \to \infty} \operatorname{Var}\left(\overline{X}\right) = \rho.</math> |
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The general formula for variance decomposition or the [[law of total variance]] is: If <math>X</math> and <math>Y</math> are two random variables and the variance of <math>X</math> exists, then |
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Therefore, the variance of the mean of a large number of standardized variables is approximately equal to their average correlation. This makes clear that the sample mean of correlated variables does not generally converge to the population mean, even though the [[law of large numbers]] states that the sample mean will converge for independent variables. |
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:<math>\operatorname{Var}(X) = \operatorname{Var}(\operatorname{E}(X|Y))+ \operatorname{E}(\operatorname{Var}(X|Y)).</math> |
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=====Sum of uncorrelated variables with random sample size===== |
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Here, <math>\operatorname E(X|Y)</math> is the [[conditional expectation]] of <math>X</math> given <math>Y</math>, and <math>\operatorname{Var}(X|Y)</math> is the [[conditional variance]] of <math>X</math> given <math>Y</math>. (A more intuitive explanation is that given a particular value of <math>Y</math>, then <math>X</math> follows a distribution with mean <math>\operatorname E(X|Y)</math> and variance <math>\operatorname{Var}(X|Y)</math>. The above formula tells how to find <math>\operatorname{Var}(X)</math> based on the distributions of these two quantities when <math>Y</math> is allowed to vary.) This formula is often applied in [[analysis of variance]], where the corresponding formula is |
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There are cases when a sample is taken without knowing, in advance, how many observations will be acceptable according to some criterion. In such cases, the sample size {{math|N}} is a random variable whose variation adds to the variation of {{math|X}}, such that, |
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: <math>\operatorname{Var}\left(\sum_{i=1}^{N}X_i\right)=\operatorname{E}\left[N\right]\operatorname{Var}(X)+\operatorname{Var}(N)(\operatorname{E}\left[X\right])^2</math><ref>Cornell, J R, and Benjamin, C A, ''Probability, Statistics, and Decisions for Civil Engineers,'' McGraw-Hill, NY, 1970, pp.178-9.</ref> |
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which follows from the [[law of total variance]]. |
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If {{math|N}} has a [[Poisson distribution]], then <math>\operatorname{E}[N]=\operatorname{Var}(N)</math> with estimator {{math|n}} = {{math|N}}. So, the estimator of <math>\operatorname{Var}\left(\sum_{i=1}^{n}X_i\right)</math> becomes <math>n{S_x}^2+n\bar{X}^2</math>, giving <math>\operatorname{SE}(\bar{X})=\sqrt{\frac{{S_x}^2+\bar{X}^2}{n}}</math> |
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:<math>\mathit{MS}_\mathrm{Total} = \mathit{MS}_\mathrm{Between} + \mathit{MS}_\mathrm{Within};</math> |
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(see [[Standard error#Standard_error_of_the_sample_mean|standard error of the sample mean]]). |
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here <math>\mathit{MS}</math> refers to the Mean of the Squares. It is also used in [[linear regression]] analysis, where the corresponding formula is |
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====Weighted sum of variables==== |
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:<math>\mathit{MS}_\mathrm{Total} = \mathit{MS}_\mathrm{Regression} + \mathit{MS}_\mathrm{Residual}.</math> |
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{{see also|Weighted arithmetic mean#Variance{{!}}Variance of a weighted arithmetic mean}} |
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{{distinguish|Weighted variance}} |
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The scaling property and the Bienaymé formula, along with the property of the [[covariance]] {{math|Cov(''aX'', ''bY'') {{=}} ''ab'' Cov(''X'', ''Y'')}} jointly imply that |
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This can also be derived from the additivity of variances, since the total (observed) score is the sum of the predicted score and the error score, where the latter two are uncorrelated. |
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:<math>\operatorname{Var}(aX \pm bY) =a^2 \operatorname{Var}(X) + b^2 \operatorname{Var}(Y) \pm 2ab\, \operatorname{Cov}(X, Y).</math> |
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Similar decompositions are possible for the sum of squared deviations (sum of squares, <math>\mathit{SS}</math>): |
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:<math>\mathit{SS}_\mathrm{Total} = \mathit{SS}_\mathrm{Between} + \mathit{SS}_\mathrm{Within},</math> |
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:<math>\mathit{SS}_\mathrm{Total} = \mathit{SS}_\mathrm{Regression} + \mathit{SS}_\mathrm{Residual}.</math> |
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This implies that in a weighted sum of variables, the variable with the largest weight will have a disproportionally large weight in the variance of the total. For example, if ''X'' and ''Y'' are uncorrelated and the weight of ''X'' is two times the weight of ''Y'', then the weight of the variance of ''X'' will be four times the weight of the variance of ''Y''. |
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===Formulae for the variance=== |
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{{Main|algebraic formula for the variance}} |
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A formula often used for deriving the variance of a theoretical distribution is as follows: |
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The expression above can be extended to a weighted sum of multiple variables: |
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:<math> \operatorname{Var}(X) =\operatorname{E}(X^2) - (\operatorname{E}(X))^2. </math> |
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:<math>\operatorname{Var}\left(\sum_{i}^n a_iX_i\right) = \sum_{i=1}^na_i^2 \operatorname{Var}(X_i) + 2\sum_{1\le i}\sum_{<j\le n}a_ia_j\operatorname{Cov}(X_i,X_j)</math> |
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This will be useful when it is possible to derive formulae for the expected value and for the expected value of the square. |
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===Product of variables=== |
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This formula is also sometimes used in connection with the sample variance. While useful for hand calculations, it is not advised for computer calculations as it suffers from [[catastrophic cancellation]] if the two components of the equation are similar in magnitude and floating point arithmetic is used.{{citation needed|date=February 2013}} This is discussed below. |
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====Product of independent variables==== |
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===Calculation from the CDF=== |
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If two variables X and Y are [[Independence (probability theory)|independent]], the variance of their product is given by<ref>{{Cite journal |last=Goodman |first=Leo A. |author-link=Leo Goodman |date=December 1960 |title=On the Exact Variance of Products |journal=Journal of the American Statistical Association |volume=55 |issue=292 |pages=708–713 |doi=10.2307/2281592 |jstor=2281592}}</ref> |
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The population variance for a non-negative random variable can be expressed in terms of the [[cumulative distribution function]] ''F'' using |
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:<math>\operatorname{Var}(XY) = [\operatorname{E}(X)]^2 \operatorname{Var}(Y) + [\operatorname{E}(Y)]^2 \operatorname{Var}(X) + \operatorname{Var}(X)\operatorname{Var}(Y).</math> |
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Equivalently, using the basic properties of expectation, it is given by |
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:<math> |
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2\int_0^\infty uH(u)\,du - \Big(\int_0^\infty H(u)\,du\Big)^2. |
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</math> |
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:<math>\operatorname{Var}(XY) = \operatorname{E}\left(X^2\right) \operatorname{E}\left(Y^2\right) - [\operatorname{E}(X)]^2 [\operatorname{E}(Y)]^2.</math> |
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where ''H''(''u'') = 1 − ''F''(''u'') is the right tail function. This expression can be used to calculate the variance in situations where the CDF, but not the [[probability density function|density]], can be conveniently expressed. |
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====Product of statistically dependent variables==== |
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===Characteristic property=== |
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The second [[moment (mathematics)|moment]] of a random variable attains the minimum value when taken around the first moment (i.e., mean) of the random variable, i.e. <math>\mathrm{argmin}_m\,\mathrm{E}((X - m)^2) = \mathrm{E}(X)\,</math>. Conversely, if a continuous function <math>\varphi</math> satisfies <math>\mathrm{argmin}_m\,\mathrm{E}(\varphi(X - m)) = \mathrm{E}(X)\,</math> for all random variables ''X'', then it is necessarily of the form <math>\varphi(x) = a x^2 + b</math>, where {{nowrap|''a'' > 0}}. This also holds in the multidimensional case.<ref>{{cite doi|10.1016/S0167-7152(98)00041-8}}</ref> |
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===Matrix notation for the variance of a linear combination=== |
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Let's define <math>X</math> as a column vector of n random variables <math>X_1, ...,X_n</math>, and c as a column vector of N scalars <math>c_1, ...,c_n</math>. Therefore <math>c^T X</math> is a [[linear combination]] of these random variables, where <math>c^T</math> denotes the [[transpose]] of vector <math>c</math>. Let also be <math>\Sigma</math> the variance-covariance matrix of the vector X. The variance of <math>c^TX</math> is given by:<ref>{{Cite book | last1=Johnson | first1=Richard | last2=Wichern | first2=Dean | year=2001 | title=Applied Multivariate Statistical Analysis | publisher=Prentice Hall | page=76 | isbn=0-13-187715-1 | postscript=<!-- Bot inserted parameter. Either remove it; or change its value to "." for the cite to end in a ".", as necessary. -->{{inconsistent citations}} }}</ref> |
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:<math>\operatorname{Var}(c^T X) = c^T \Sigma c .</math> |
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===Units of measurement=== |
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Unlike expected absolute deviation, the variance of a variable has units that are the square of the units of the variable itself. For example, a variable measured in inches will have a variance measured in square inches. For this reason, describing data sets via their [[standard deviation]] or [[root mean square deviation]] is often preferred over using the variance. In the dice example the standard deviation is √2.9 ≈ 1.7, slightly larger than the expected absolute deviation of 1.5. |
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The standard deviation and the expected absolute deviation can both be used as an indicator of the "spread" of a distribution. The standard deviation is more amenable to algebraic manipulation than the expected absolute deviation, and, together with variance and its generalization [[covariance]], is used frequently in theoretical statistics; however the expected absolute deviation tends to be more [[Robust statistics|robust]] as it is less sensitive to [[outlier]]s arising from [[measurement error|measurement anomalies]] or an unduly [[heavy-tailed distribution]]. |
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In general, if two variables are statistically dependent, then the variance of their product is given by: |
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:<math>\begin{align} |
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\operatorname{Var}(XY) |
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={} &\operatorname{E}\left[X^2 Y^2\right] - [\operatorname{E}(XY)]^2 \\[5pt] |
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={} &\operatorname{Cov}\left(X^2, Y^2\right) + \operatorname{E}(X^2)\operatorname{E}\left(Y^2\right) - [\operatorname{E}(XY)]^2 \\[5pt] |
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={} &\operatorname{Cov}\left(X^2, Y^2\right) + \left(\operatorname{Var}(X) + [\operatorname{E}(X)]^2\right)\left(\operatorname{Var}(Y) + [\operatorname{E}(Y)]^2\right) \\[5pt] |
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&- [\operatorname{Cov}(X, Y) + \operatorname{E}(X)\operatorname{E}(Y)]^2 |
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\end{align}</math> |
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===Arbitrary functions=== |
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{{main|Uncertainty propagation}} |
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==Approximating the variance of a function== |
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The [[delta method]] uses second-order [[Taylor expansion]]s to approximate the variance of a function of one or more random variables: see [[Taylor expansions for the moments of functions of random variables]]. For example, the approximate variance of a function of one variable is given by |
The [[delta method]] uses second-order [[Taylor expansion]]s to approximate the variance of a function of one or more random variables: see [[Taylor expansions for the moments of functions of random variables]]. For example, the approximate variance of a function of one variable is given by |
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:<math>\operatorname{Var}\left[f(X)\right] \approx \left(f'(\operatorname{E}\left[X\right])\right)^2\operatorname{Var}\left[X\right]</math> |
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provided that ''f'' is twice differentiable and that the mean and variance of ''X'' are finite. |
provided that ''f'' is twice differentiable and that the mean and variance of ''X'' are finite. |
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==Population variance and sample variance== |
==Population variance and sample variance== |
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{{anchor|Estimation |
{{anchor|Estimation}} |
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{{see also|Unbiased estimation of standard deviation}} |
{{see also|Unbiased estimation of standard deviation}} |
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Real-world observations such as the measurements of yesterday's rain throughout the day typically cannot be complete sets of all possible observations that could be made. As such, the variance calculated from the finite set will in general not match the variance that would have been calculated from the full population of possible observations. This means that one [[Estimation theory|estimates]] the mean and variance from a limited set of observations by using an [[estimator]] equation. The estimator is a function of the [[Sample (statistics)|sample]] of ''n'' [[observations]] drawn without observational bias from the whole [[Statistical population|population]] of potential observations. In this example, the sample would be the set of actual measurements of yesterday's rainfall from available rain gauges within the geography of interest. |
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{{move section portions|Unbiased estimation of standard deviation|date=April 2013}} |
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The simplest estimators for population mean and population variance are simply the mean and variance of the sample, the '''sample mean''' and '''(uncorrected) sample variance''' – these are [[consistent estimator]]s (they converge to the value of the whole population as the number of samples increases) but can be improved. Most simply, the sample variance is computed as the sum of [[squared deviations]] about the (sample) mean, divided by ''n'' as the number of samples''.'' However, using values other than ''n'' improves the estimator in various ways. Four common values for the denominator are ''n,'' ''n'' − 1, ''n'' + 1, and ''n'' − 1.5: ''n'' is the simplest (the variance of the sample), ''n'' − 1 eliminates bias,<ref name=bessel /> ''n'' + 1 minimizes [[mean squared error]] for the normal distribution,<ref name=Kourouklis/> and ''n'' − 1.5 mostly eliminates bias in [[unbiased estimation of standard deviation]] for the normal distribution.<ref>{{cite journal | last = Brugger | first = R. M. | year = 1969 | title = A Note on Unbiased Estimation of the Standard Deviation | journal = The American Statistician | volume = 23 | issue = 4 | pages = 32 | doi = 10.1080/00031305.1969.1048186| doi-broken-date = 16 December 2024 }}</ref> |
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Real-world distributions such as the distribution of yesterday's rain throughout the day are typically not fully known, unlike the behavior of perfect dice or an ideal distribution such as the [[normal distribution]], because it is impractical to account for every raindrop. Instead one [[Estimation theory|estimates]] the mean and variance of the whole distribution as the computed mean and variance of a [[Sample (statistics)|sample]] of ''n'' [[observations]] drawn suitably randomly from the whole [[sample space]], in this example the set of all measurements of yesterday's rainfall in all available rain gauges. |
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Firstly, if the true population mean is unknown, then the sample variance (which uses the sample mean in place of the true mean) is a [[biased estimator]]: it underestimates the variance by a factor of (''n'' − 1) / ''n''; correcting this factor, resulting in the sum of squared deviations about the sample mean divided by ''n'' -1 instead of ''n'', is called ''[[Bessel's correction]]''.<ref name=bessel>{{cite book |
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This method of estimation is close to optimal, with the caveat that it underestimates the variance by a factor of (''n'' − 1) / ''n''. (For example, when ''n'' = 1 the variance of a single observation is obviously zero regardless of the true variance). This gives a [[Unbiased estimation of standard deviation|bias]] which should be corrected for when ''n'' is small by multiplying by ''n'' / (''n'' − 1). If the mean is determined in some other way than from the same samples used to estimate the variance then this bias does not arise and the variance can safely be estimated as that of the samples. |
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| last = Reichmann |
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| first = W. J. |
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| title = Use and Abuse of Statistics |
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| publisher = Methuen |
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| year = 1961 |
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| edition = Reprinted 1964–1970 by Pelican |
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| location = London |
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| chapter = Appendix 8 |
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}}</ref> The resulting estimator is unbiased and is called the '''(corrected) sample variance''' or '''unbiased sample variance'''. If the mean is determined in some other way than from the same samples used to estimate the variance, then this bias does not arise, and the variance can safely be estimated as that of the samples about the (independently known) mean. |
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Secondly, the sample variance does not generally minimize [[mean squared error]] between sample variance and population variance. Correcting for bias often makes this worse: one can always choose a scale factor that performs better than the corrected sample variance, though the optimal scale factor depends on the [[excess kurtosis]] of the population (see [[Mean squared error#Variance|mean squared error: variance]]) and introduces bias. This always consists of scaling down the unbiased estimator (dividing by a number larger than ''n'' − 1) and is a simple example of a [[shrinkage estimator]]: one "shrinks" the unbiased estimator towards zero. For the normal distribution, dividing by ''n'' + 1 (instead of ''n'' − 1 or ''n'') minimizes mean squared error.<ref name=Kourouklis>{{Cite journal |last=Kourouklis |first=Stavros |date=2012 |title=A New Estimator of the Variance Based on Minimizing Mean Squared Error |url=https://www.jstor.org/stable/23339501 |journal=The American Statistician |volume=66 |issue=4 |pages=234–236 |doi=10.1080/00031305.2012.735209 |jstor=23339501 |issn=0003-1305}}</ref> The resulting estimator is biased, however, and is known as the '''biased sample variation'''. |
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===Population variance=== |
===Population variance=== |
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In general, the '''''population variance''''' of a ''finite'' [[statistical population|population]] of size ''N'' with values ''x''<sub>''i''</sub> is given by |
In general, the '''''population variance''''' of a ''finite'' [[statistical population|population]] of size ''N'' with values ''x''<sub>''i''</sub> is given by<math display="block">\begin{align} |
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\sigma^2 &= \frac{1}{N} \sum_{i=1}^N \left(x_i - \mu\right)^2 = \frac{1}{N} \sum_{i=1}^N \left(x_i^2 - 2\mu x_i + \mu^2 \right) \\[5pt] |
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&= \left(\frac 1N \sum_{i=1}^N x_i^2\right) - 2\mu \left(\frac{1}{N} \sum_{i=1}^N x_i\right) + \mu^2 \\[5pt] |
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&= \operatorname{E}[x_i^2] - \mu^2 |
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\end{align}</math>where the population mean is <math display="inline">\mu = \operatorname{E}[x_i] = \frac 1N \sum_{i=1}^N x_i </math> and <math display="inline">\operatorname{E}[x_i^2] = \left(\frac{1}{N} \sum_{i=1}^N x_i^2\right) </math>, where <math display="inline">\operatorname{E} </math> is the [[Expected value|expectation value]] operator. |
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The population variance can also be computed using<ref>{{cite conference|author=Yuli Zhang |author2=Huaiyu Wu |author3=Lei Cheng |date=June 2012|title=Some new deformation formulas about variance and covariance|conference=Proceedings of 4th International Conference on Modelling, Identification and Control(ICMIC2012)|pages=987–992}}</ref> |
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:<math> \sigma^2 = \frac 1N \sum_{i=1}^N \left(x_i - \mu \right)^2 = \left(\frac 1N \sum_{i=1}^N x_i^2\right) - \mu^2 </math> |
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:<math>\sigma^2 = \frac {1} {N^2}\sum_{i<j}\left( x_i-x_j \right)^2 = \frac{1}{2N^2} \sum_{i, j=1}^N\left( x_i-x_j \right)^2.</math> |
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where |
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(The right side has duplicate terms in the sum while the middle side has only unique terms to sum.) This is true because<math display="block"> \begin{align} |
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: <math> \mu = \frac 1N \sum_{i=1}^N x_i </math> |
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&\frac{1}{2N^2} \sum_{i, j=1}^N\left( x_i - x_j \right)^2 \\[5pt] |
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={} &\frac{1}{2N^2} \sum_{i, j=1}^N\left( x_i^2 - 2x_i x_j + x_j^2 \right) \\[5pt] |
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is the population mean. The population variance therefore is the variance of the underlying probability distribution. In this sense, the concept of population can be extended to continuous random variables with infinite populations. |
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={} &\frac{1}{2N} \sum_{j=1}^N\left(\frac{1}{N} \sum_{i=1}^N x_i^2\right) - \left(\frac{1}{N} \sum_{i=1}^N x_i\right)\left(\frac{1}{N} \sum_{j=1}^N x_j\right) + \frac{1}{2N} \sum_{i=1}^N\left(\frac{1}{N} \sum_{j=1}^N x_j^2\right) \\[5pt] |
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={} &\frac{1}{2} \left( \sigma^2 + \mu^2 \right) - \mu^2 + \frac{1}{2} \left( \sigma^2 + \mu^2 \right) \\[5pt] |
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={} &\sigma^2. |
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\end{align}</math>The population variance matches the variance of the generating probability distribution. In this sense, the concept of population can be extended to continuous random variables with infinite populations. |
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===Sample variance=== |
===Sample variance=== |
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{{see also|Sample standard deviation}} |
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In many practical situations, the true variance of a population is not known ''a priori'' and must be computed somehow. When dealing with extremely large populations, it is not possible to count every object in the population, so the computation must be performed on a [[sample (statistics)|sample]] of the population.<ref>Navidi, William (2006) ''Statistics for Engineers and Scientists'', McGraw-Hill, pg 14.</ref> Sample variance can also be applied to the estimation of the variance of a continuous distribution from a sample of that distribution. |
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===={{visible anchor|Biased sample variance}}==== |
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We take a [[statistical sample|sample with replacement]] of ''n'' values ''y''<sub>1</sub>, ..., ''y''<sub>''n''</sub> from the population, where ''n'' < ''N'', and estimate the variance on the basis of this sample.<ref>Montgomery, D. C. and Runger, G. C. (1994) ''Applied statistics and probability for engineers'', page 201. John Wiley & Sons New York</ref> Directly taking the variance of the sample gives: |
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In many practical situations, the true variance of a population is not known ''a priori'' and must be computed somehow. When dealing with extremely large populations, it is not possible to count every object in the population, so the computation must be performed on a [[sample (statistics)|sample]] of the population.<ref>Navidi, William (2006) ''Statistics for Engineers and Scientists'', McGraw-Hill, p. 14.</ref> This is generally referred to as '''sample variance''' or '''empirical variance'''. Sample variance can also be applied to the estimation of the variance of a continuous distribution from a sample of that distribution. |
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We take a [[statistical sample|sample with replacement]] of ''n'' values ''Y''<sub>1</sub>, ..., ''Y''<sub>''n''</sub> from the population of size <math display="inline">N </math>, where ''n'' < ''N'', and estimate the variance on the basis of this sample.<ref>Montgomery, D. C. and Runger, G. C. (1994) ''Applied statistics and probability for engineers'', page 201. John Wiley & Sons New York</ref> Directly taking the variance of the sample data gives the average of the [[squared deviations]]: |
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:<math>\sigma_y^2 = \frac 1n \sum_{i=1}^n \left(y_i - \overline{y} \right)^2 </math> |
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:<math>\tilde{S}_Y^2 = |
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Here, <math>\overline{y}</math> denotes the [[sample mean]]: |
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\frac{1}{n} \sum_{i=1}^n \left(Y_i - \overline{Y}\right)^2 = \left(\frac 1n \sum_{i=1}^n Y_i^2\right) - \overline{Y}^2 = |
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\frac{1}{n^2} \sum_{i,j\,:\,i<j}\left(Y_i - Y_j\right)^2. |
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</math><ref>{{cite conference|author=Yuli Zhang |author2=Huaiyu Wu |author3=Lei Cheng |date=June 2012|title=Some new deformation formulas about variance and covariance|conference=Proceedings of 4th International Conference on Modelling, Identification and Control(ICMIC2012)|pages=987–992}}</ref> |
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(See the section [[Variance#Population variance|Population variance]] for the derivation of this formula.) Here, <math>\overline{Y}</math> denotes the [[sample mean]]: |
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Since the ''y''<sub>''i''</sub> are selected randomly, both <math>\scriptstyle\overline{y}</math> and <math>\scriptstyle\sigma_y^2</math> are random variables. Their expected values can be evaluated by summing over the ensemble of all possible samples {''y''<sub>''i''</sub>} from the population. For <math>\scriptstyle\sigma_y^2</math> this gives: |
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:<math>\overline{Y} = \frac{1}{n} \sum_{i=1}^n Y_i .</math> |
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:<math> |
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\begin{align} |
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E[\sigma_y^2] |
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& = E\left[ \frac 1n \sum_{i=1}^n \left(y_i - \frac 1n \sum_{j=1}^n y_j \right)^2 \right] \\ |
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& = \frac 1n \sum_{i=1}^n E\left[ y_i^2 - \frac 2n y_i \sum_{j=1}^n y_j + \frac{1}{n^2} \sum_{j=1}^n y_j \sum_{k=1}^n y_k \right] \\ |
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& = \frac 1n \sum_{i=1}^n \left[ \frac{n-2}{n} E[y_i^2] - \frac 2n \sum_{j \neq i} E[y_i y_j] + \frac{1}{n^2} \sum_{j=1}^n \sum_{k \neq j} E[y_j y_k] +\frac{1}{n^2} \sum_{j=1}^n E[y_j^2] \right] \\ |
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& = \frac 1n \sum_{i=1}^n \left[ \frac{n-2}{n} (\sigma^2+\mu^2) - \frac 2n (n-1) \mu^2 + \frac{1}{n^2} n (n-1) \mu^2 + \frac 1n (\sigma^2+\mu^2) \right] \\ |
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& = \frac{n-1}{n} \sigma^2. |
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\end{align} |
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</math> |
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Since the ''Y''<sub>''i''</sub> are selected randomly, both <math>\overline{Y}</math> and <math>\tilde{S}_Y^2</math> are [[Random variable|random variables]]. Their expected values can be evaluated by averaging over the ensemble of all possible samples {''Y''<sub>''i''</sub>} of size ''n'' from the population. For <math>\tilde{S}_Y^2</math> this gives: |
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Hence <math>\scriptstyle\sigma_y^2</math> gives an estimate of the population variance that is biased by a factor of (''n''-1)/''n''. For this reason, <math>\scriptstyle\sigma_y^2</math> is referred to as the ''biased sample variance''. Correcting for this bias yields the ''unbiased sample variance'': |
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:<math>\begin{align} |
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\operatorname{E}[\tilde{S}_Y^2] |
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&= \operatorname{E}\left[ \frac{1}{n} \sum_{i=1}^n \left(Y_i - \frac{1}{n} \sum_{j=1}^n Y_j \right)^2 \right] \\[5pt] |
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&= \frac 1n \sum_{i=1}^n \operatorname{E}\left[ Y_i^2 - \frac{2}{n} Y_i \sum_{j=1}^n Y_j + \frac{1}{n^2} \sum_{j=1}^n Y_j \sum_{k=1}^n Y_k \right] \\[5pt] |
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&= \frac 1n \sum_{i=1}^n \left( \operatorname{E}\left[Y_i^2\right] - \frac{2}{n} \left( \sum_{j \neq i} \operatorname{E}\left[Y_i Y_j\right] + \operatorname{E}\left[Y_i^2\right] \right) + \frac{1}{n^2} \sum_{j=1}^n \sum_{k \neq j}^n \operatorname{E}\left[Y_j Y_k\right] +\frac{1}{n^2} \sum_{j=1}^n \operatorname{E}\left[Y_j^2\right] \right) \\[5pt] |
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&= \frac 1n \sum_{i=1}^n \left( \frac{n - 2}{n} \operatorname{E}\left[Y_i^2\right] - \frac{2}{n} \sum_{j \neq i} \operatorname{E}\left[Y_i Y_j\right] + \frac{1}{n^2} \sum_{j=1}^n \sum_{k \neq j}^n \operatorname{E}\left[Y_j Y_k\right] +\frac{1}{n^2} \sum_{j=1}^n \operatorname{E}\left[Y_j^2\right] \right) \\[5pt] |
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&= \frac 1n \sum_{i=1}^n \left[ \frac{n - 2}{n} \left(\sigma^2 + \mu^2\right) - \frac{2}{n} (n - 1)\mu^2 + \frac{1}{n^2} n(n - 1)\mu^2 + \frac{1}{n} \left(\sigma^2 + \mu^2\right) \right] \\[5pt] |
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&= \frac{n - 1}{n} \sigma^2. |
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\end{align}</math> |
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Here <math display="inline">\sigma^2 = \operatorname{E}[Y_i^2] - \mu^2 </math> derived in the section [[Variance#Population variance|Population variance]] and <math display="inline">\operatorname{E}[Y_i Y_j] = \operatorname{E}[Y_i] \operatorname{E}[Y_j] = \mu^2</math> due to independency of <math display="inline">Y_i</math> and <math display="inline">Y_j</math> are used. |
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Hence <math display="inline">\tilde{S}_Y^2</math> gives an estimate of the population variance that is biased by a factor of <math display="inline">\frac{n - 1}{n}</math> as the expectation value of <math display="inline">\tilde{S}_Y^2</math> is smaller than the population variance (true variance) by that factor. For this reason, <math display="inline">\tilde{S}_Y^2</math> is referred to as the ''biased sample variance''. |
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===={{visible anchor|Unbiased sample variance}}==== |
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Correcting for this bias yields the ''unbiased sample variance'', denoted <math>S^2</math>: |
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:<math>S^2 = \frac{n}{n - 1} \tilde{S}_Y^2 = \frac{n}{n - 1} \left[ \frac{1}{n} \sum_{i=1}^n \left(Y_i - \overline{Y}\right)^2 \right] = \frac{1}{n - 1} \sum_{i=1}^n \left(Y_i - \overline{Y} \right)^2</math> |
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:<math>s^2 = \frac{1}{n-1} \sum_{i=1}^n \left(y_i - \overline{y} \right)^2 </math> |
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Either estimator may be simply referred to as the ''sample variance'' when the version can be determined by context. The same proof is also applicable for samples taken from a continuous probability distribution. |
Either estimator may be simply referred to as the ''sample variance'' when the version can be determined by context. The same proof is also applicable for samples taken from a continuous probability distribution. |
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The unbiased sample variance is a [[U-statistic]] for the function ''ƒ''(''y''<sub>1</sub>, ''y''<sub>2</sub>) = (''y''<sub>1</sub> − ''y''<sub>2</sub>)<sup>2</sup>/2, meaning that it is obtained by averaging a 2-sample statistic over 2-element subsets of the population. |
The unbiased sample variance is a [[U-statistic]] for the function ''ƒ''(''y''<sub>1</sub>, ''y''<sub>2</sub>) = (''y''<sub>1</sub> − ''y''<sub>2</sub>)<sup>2</sup>/2, meaning that it is obtained by averaging a 2-sample statistic over 2-element subsets of the population. |
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===== Example ===== |
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===Distribution of the sample variance=== |
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For a set of numbers {10, 15, 30, 45, 57, 52 63, 72, 81, 93, 102, 105}, if this set is the whole data population for some measurement, then variance is the population variance 932.743 as the sum of the squared deviations about the mean of this set, divided by 12 as the number of the set members. If the set is a sample from the whole population, then the unbiased sample variance can be calculated as 1017.538 that is the sum of the squared deviations about the mean of the sample, divided by 11 instead of 12. A function VAR.S in [[Microsoft Excel]] gives the unbiased sample variance while VAR.P is for population variance. |
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====Distribution of the sample variance==== |
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Being a function of [[random variable]]s, the sample variance is itself a random variable, and it is natural to study its distribution. In the case that ''y''<sub>''i''</sub> are independent observations from a [[normal distribution]], [[Cochran's theorem]] shows that ''s''<sup>2</sup> follows a scaled [[chi-squared distribution]]:<ref>Knight K. (2000), ''Mathematical Statistics'', Chapman and Hall, New York. (proposition 2.11)</ref> |
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Being a function of [[random variable]]s, the sample variance is itself a random variable, and it is natural to study its distribution. In the case that ''Y''<sub>''i''</sub> are independent observations from a [[normal distribution]], [[Cochran's theorem]] shows that the [[Variance#Unbiased sample variance|unbiased sample variance]] ''S''<sup>2</sup> follows a scaled [[chi-squared distribution]] (see also: [[chi-squared distribution#Asymptotic properties|asymptotic properties]] and an [[Chi-squared distribution#Cochran's_theorem|elementary proof]]):<ref>Knight K. (2000), ''Mathematical Statistics'', Chapman and Hall, New York. (proposition 2.11)</ref> |
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:<math> |
:<math> |
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(n-1)\frac{ |
(n - 1)\frac{S^2}{\sigma^2}\sim\chi^2_{n-1} |
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</math> |
</math> |
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As a direct consequence, it follows that |
where ''σ''<sup>2</sup> is the [[Variance#Population variance|population variance]]. As a direct consequence, it follows that |
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:<math> |
:<math> |
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\operatorname{E}( |
\operatorname{E}\left(S^2\right) = \operatorname{E}\left(\frac{\sigma^2}{n - 1} \chi^2_{n-1}\right) = \sigma^2 , |
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</math> |
</math> |
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and<ref>Casella and Berger (2002) ''Statistical Inference'', Example 7.3.3, p. 331 {{full|date=March 2013}}</ref> |
and<ref>Casella and Berger (2002) ''Statistical Inference'', Example 7.3.3, p. 331 {{full citation needed|date=March 2013}}</ref> |
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: |
:<math> |
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\operatorname{Var}[ |
\operatorname{Var}\left[S^2\right] = \operatorname{Var}\left(\frac{\sigma^2}{n - 1} \chi^2_{n-1}\right) = \frac{\sigma^4}{(n - 1)^2}\operatorname{Var}\left(\chi^2_{n-1}\right) = \frac{2\sigma^4}{n - 1}. |
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</math> |
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If |
If ''Y''<sub>''i''</sub> are independent and identically distributed, but not necessarily normally distributed, then<ref>Mood, A. M., Graybill, F. A., and Boes, D.C. (1974) ''Introduction to the Theory of Statistics'', 3rd Edition, McGraw-Hill, New York, p. 229</ref> |
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:<math> |
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\operatorname{E}\left[S^2\right] = \sigma^2, \quad |
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\operatorname{Var}\left[S^2\right] = \frac{\sigma^4}{n} \left(\kappa - 1 + \frac{2}{n - 1} \right) = \frac{1}{n} \left(\mu_4 - \frac{n - 3}{n - 1}\sigma^4\right), |
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</math> |
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where ''κ'' is the [[kurtosis]] of the distribution and ''μ''<sub>4</sub> is the fourth [[central moment]]. |
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: <math> |
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\operatorname{E}[s^2] = \sigma^2, \quad |
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\operatorname{Var}[s^2] = \sigma^4 \left (\frac{2}{n-1} + \frac{\kappa}{n} \right) = \frac{1}{n} \left(\mu_4 - \frac{n-3}{n-1}\sigma^4\right), |
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</math> |
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where ''κ'' is the [[excess kurtosis]] of the distribution and ''μ<sub>4</sub>'' is the fourth [[moment about the mean]]. |
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If the conditions of the [[law of large numbers]] hold for the squared observations, ''S''<sup>2</sup> is a [[consistent estimator]] of ''σ''<sup>2</sup>. One can see indeed that the variance of the estimator tends asymptotically to zero. An asymptotically equivalent formula was given in Kenney and Keeping (1951:164), Rose and Smith (2002:264), and Weisstein (n.d.).<ref>{{cite book |last1=Kenney |first1=John F. |last2=Keeping |first2=E.S. |date=1951 |title=Mathematics of Statistics. Part Two. |edition=2nd |publisher=D. Van Nostrand Company, Inc. |location=Princeton, New Jersey |url=http://krishikosh.egranth.ac.in/bitstream/1/2025521/1/G2257.pdf |via=KrishiKosh |url-status=dead |archive-url=https://web.archive.org/web/20181117022434/http://krishikosh.egranth.ac.in/bitstream/1/2025521/1/G2257.pdf |archive-date= Nov 17, 2018 }}</ref><ref>Rose, Colin; Smith, Murray D. (2002). "[http://www.mathstatica.com/book/Mathematical_Statistics_with_Mathematica.pdf Mathematical Statistics with Mathematica]". Springer-Verlag, New York.</ref><ref>Weisstein, Eric W. "[http://mathworld.wolfram.com/SampleVarianceDistribution.html Sample Variance Distribution]". MathWorld Wolfram.</ref> |
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If the conditions of the [[law of large numbers]] hold for the squared observations, ''s''<sup>2</sup> is a [[consistent estimator]] of ''σ''<sup>2</sup>.{{Citation needed|date=April 2012}}. One can see indeed that the variance of the estimator tends asymptotically to zero. |
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===Samuelson's inequality=== |
====Samuelson's inequality==== |
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[[Samuelson's inequality]] is a result that states bounds on the values that individual observations in a sample can take, given that the sample mean and (biased) variance have been calculated.<ref>Samuelson |
[[Samuelson's inequality]] is a result that states bounds on the values that individual observations in a sample can take, given that the sample mean and (biased) variance have been calculated.<ref>{{cite journal |last=Samuelson |first=Paul |title=How Deviant Can You Be? |journal=[[Journal of the American Statistical Association]] |volume=63 |issue=324 |year=1968 |pages=1522–1525 |jstor=2285901 |doi=10.1080/01621459.1968.10480944}}</ref> Values must lie within the limits <math>\bar y \pm \sigma_Y (n-1)^{1/2}.</math> |
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===Relations with the harmonic and arithmetic means=== |
===Relations with the harmonic and arithmetic means=== |
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It has been shown<ref> |
It has been shown<ref>{{cite journal |first=A. McD. |last=Mercer |title=Bounds for A–G, A–H, G–H, and a family of inequalities of Ky Fan's type, using a general method |journal=J. Math. Anal. Appl. |volume=243 |issue=1 |pages=163–173 |year=2000 |doi=10.1006/jmaa.1999.6688 |doi-access=free }}</ref> that for a sample {''y''<sub>''i''</sub>} of positive real numbers, |
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: <math> \sigma_y^2 \le 2y_{max} (A - H) </math> |
: <math> \sigma_y^2 \le 2y_{\max} (A - H), </math> |
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where ''y''<sub> |
where ''y''<sub>max</sub> is the maximum of the sample, ''A'' is the arithmetic mean, ''H'' is the [[harmonic mean]] of the sample and <math>\sigma_y^2</math> is the (biased) variance of the sample. |
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This bound has been improved |
This bound has been improved, and it is known that variance is bounded by |
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: <math> \sigma_y^2 \le \frac{ |
: <math> \sigma_y^2 \le \frac{y_{\max} (A - H)(y_\max - A)}{y_\max - H}, </math> |
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: <math> \sigma_y^2 \ge \frac{ |
: <math> \sigma_y^2 \ge \frac{y_{\min} (A - H)(A - y_\min)}{H - y_\min}, </math> |
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where ''y''<sub> |
where ''y''<sub>min</sub> is the minimum of the sample.<ref name=Sharma2008>{{cite journal |first=R. |last=Sharma |title= Some more inequalities for arithmetic mean, harmonic mean and variance|journal= Journal of Mathematical Inequalities|volume=2 |issue=1 |pages=109–114 |year=2008 |doi=10.7153/jmi-02-11|citeseerx=10.1.1.551.9397 }}</ref> |
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==Tests of equality of variances== |
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==Generalizations== |
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The [[F-test of equality of variances]] and the [[chi square test]]s are adequate when the sample is normally distributed. Non-normality makes testing for the equality of two or more variances more difficult. |
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If <math>X</math> is a [[vector space|vector]]-valued random variable, with values in <math>\mathbb{R}^n</math>, and thought of as a column vector, then the natural generalization of variance is <math>\operatorname{E}((X - \mu)(X - \mu)^{\operatorname{T}})</math>, where <math>\mu = \operatorname{E}(X)</math> and <math>X^{\operatorname{T}}</math> is the transpose of <math>X</math>, and so is a row vector. This variance is a [[positive definite matrix|positive semi-definite square matrix]], commonly referred to as the [[covariance matrix]]. |
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Several non parametric tests have been proposed: these include the Barton–David–Ansari–Freund–Siegel–Tukey test, the [[Capon test]], [[Mood test]], the [[Klotz test]] and the [[Sukhatme test]]. The Sukhatme test applies to two variances and requires that both [[median]]s be known and equal to zero. The Mood, Klotz, Capon and Barton–David–Ansari–Freund–Siegel–Tukey tests also apply to two variances. They allow the median to be unknown but do require that the two medians are equal. |
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If <math>X</math> is a [[complex number|complex]]-valued random variable, with values in <math>\mathbb{C}</math>, then its variance is <math>\operatorname{E}((X - \mu)(X - \mu)^{\dagger})</math>, where <math>X^{\dagger}</math> is the [[conjugate transpose]] of <math>X</math>. This variance is also a positive semi-definite square matrix. |
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The [[Lehmann test]] is a parametric test of two variances. Of this test there are several variants known. Other tests of the equality of variances include the [[Box test]], the [[Box–Anderson test]] and the [[Moses test]]. |
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==Tests of equality of variances== |
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Resampling methods, which include the [[Bootstrapping (statistics)|bootstrap]] and the [[Resampling (statistics)|jackknife]], may be used to test the equality of variances. |
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Testing for the equality of two or more variances is difficult. The [[F test]] and [[chi square test]]s are both sensitive to non normality and are not recommended for this purpose. |
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==Moment of inertia== |
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Several non parametric tests have been proposed: these include the Barton-David-Ansari-Fruend-Siegel-Tukey test, the [[Capon test]], [[Mood test]], the [[Klotz test]] and the [[Sukhatme test]]. The Sukhatme test applies to two variances and requires that both [[median]]s be known and equal to zero. The Mood, Klotz, Capon and Barton-David-Ansari-Fruend-Siegel-Tukey tests also apply to two variances. They allow the median to be unknown but do require that the two medians are equal. |
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{{see also|Moment (physics)#Examples}} |
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The variance of a probability distribution is analogous to the [[moment of inertia]] in [[classical mechanics]] of a corresponding mass distribution along a line, with respect to rotation about its center of mass.<ref name=pearson>{{Cite web |last=Magnello |first=M. Eileen |title=Karl Pearson and the Origins of Modern Statistics: An Elastician becomes a Statistician | url=https://rutherfordjournal.org/article010107.html |website=The Rutherford Journal}}</ref> It is because of this analogy that such things as the variance are called ''[[moment (mathematics)|moment]]s'' of [[probability distribution]]s.<ref name=pearson/> The covariance matrix is related to the [[moment of inertia tensor]] for multivariate distributions. The moment of inertia of a cloud of ''n'' points with a covariance matrix of <math>\Sigma</math> is given by{{Citation needed|date=February 2012}} |
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:<math>I = n\left(\mathbf{1}_{3\times 3} \operatorname{tr}(\Sigma) - \Sigma\right).</math> |
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This difference between moment of inertia in physics and in statistics is clear for points that are gathered along a line. Suppose many points are close to the ''x'' axis and distributed along it. The covariance matrix might look like |
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:<math>\Sigma = \begin{bmatrix}10 & 0 & 0 \\ 0 & 0.1 & 0 \\ 0 & 0 & 0.1\end{bmatrix}.</math> |
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That is, there is the most variance in the ''x'' direction. Physicists would consider this to have a low moment ''about'' the ''x'' axis so the moment-of-inertia tensor is |
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:<math>I = n\begin{bmatrix}0.2 & 0 & 0 \\ 0 & 10.1 & 0 \\ 0 & 0 & 10.1\end{bmatrix}.</math> |
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==Semivariance== |
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The ''semivariance'' is calculated in the same manner as the variance but only those observations that fall below the mean are included in the calculation:<math display="block">\text{Semivariance} = {1\over{n}}\sum_{i:x_{i} < \mu}(x_{i}-\mu)^{2}</math>It is also described as a specific measure in different fields of application. For skewed distributions, the semivariance can provide additional information that a variance does not.<ref>{{Cite web|url=https://famafrench.dimensional.com/questions-answers/qa-semi-variance-a-better-risk-measure.aspx|title=Q&A: Semi-Variance: A Better Risk Measure?|last1=Fama|first1=Eugene F.|last2=French|first2=Kenneth R.|date=2010-04-21|website=Fama/French Forum}}</ref> |
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The [[Lehman test]] is a parametric test of two variances. Of this test there are several variants known. Other tests of the equality of variances include the [[Box test]], the [[Box-Anderson test]] and the [[Moses test]]. |
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For inequalities associated with the semivariance, see {{Section link|Chebyshev's inequality|Semivariances}}. |
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Resampling methods, which include the [[bootstrap]] and the [[Resampling (statistics)|jackknife]], may be used to test the equality of variances. |
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== |
==Etymology== |
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The term ''variance'' was first introduced by [[Ronald Fisher]] in his 1918 paper ''[[The Correlation Between Relatives on the Supposition of Mendelian Inheritance]]'':<ref>[[Ronald Fisher]] (1918) [http://digital.library.adelaide.edu.au/dspace/bitstream/2440/15097/1/9.pdf The correlation between relatives on the supposition of Mendelian Inheritance]</ref> |
The term ''variance'' was first introduced by [[Ronald Fisher]] in his 1918 paper ''[[The Correlation Between Relatives on the Supposition of Mendelian Inheritance]]'':<ref>[[Ronald Fisher]] (1918) [http://digital.library.adelaide.edu.au/dspace/bitstream/2440/15097/1/9.pdf The correlation between relatives on the supposition of Mendelian Inheritance]</ref> |
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<blockquote>The great body of available statistics show us that the deviations of a [[biometry|human measurement]] from its mean follow very closely the [[Normal distribution|Normal Law of Errors]], and, therefore, that the variability may be uniformly measured by the [[standard deviation]] corresponding to the [[square root]] of the [[mean square error]]. When there are two independent causes of variability capable of producing in an otherwise uniform population distributions with standard deviations <math>\ |
<blockquote>The great body of available statistics show us that the deviations of a [[biometry|human measurement]] from its mean follow very closely the [[Normal distribution|Normal Law of Errors]], and, therefore, that the variability may be uniformly measured by the [[standard deviation]] corresponding to the [[square root]] of the [[mean square error]]. When there are two independent causes of variability capable of producing in an otherwise uniform population distributions with standard deviations <math>\sigma_1</math> and <math>\sigma_2</math>, it is found that the distribution, when both causes act together, has a standard deviation <math>\sqrt{\sigma_1^2 + \sigma_2^2}</math>. It is therefore desirable in analysing the causes of variability to deal with the square of the standard deviation as the measure of variability. We shall term this quantity the Variance...</blockquote> |
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==Generalizations== |
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==Moment of inertia== |
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The variance of a probability distribution is analogous to the [[moment of inertia]] in [[classical mechanics]] of a corresponding mass distribution along a line, with respect to rotation about its center of mass.{{Citation needed|date=February 2012}} It is because of this analogy that such things as the variance are called ''[[moment (mathematics)|moment]]s'' of [[probability distribution]]s.{{Citation needed|date=February 2012}} The covariance matrix is related to the [[moment of inertia tensor]] for multivariate distributions. The moment of inertia of a cloud of ''n'' points with a covariance matrix of <math>\Sigma</math> is given by{{Citation needed|date=February 2012}} |
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===For complex variables=== |
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:<math>I=n (\mathbf{1}_{3\times 3} \operatorname{tr}(\Sigma) - \Sigma).</math> |
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If <math>x</math> is a scalar [[complex number|complex]]-valued random variable, with values in <math>\mathbb{C},</math> then its variance is <math>\operatorname{E}\left[(x - \mu)(x - \mu)^*\right],</math> where <math>x^*</math> is the [[complex conjugate]] of <math>x.</math> This variance is a real scalar. |
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This difference between moment of inertia in physics and in statistics is clear for points that are gathered along a line. Suppose many points are close to the ''x'' axis and distributed along it. The covariance matrix might look like |
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:<math>\Sigma=\begin{bmatrix}10 & 0 & 0\\0 & 0.1 & 0 \\ 0 & 0 & 0.1\end{bmatrix}.</math> |
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===For vector-valued random variables=== |
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That is, there is the most variance in the ''x'' direction. However, physicists would consider this to have a low moment ''about'' the ''x'' axis so the moment-of-inertia tensor is |
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:<math>I=n\begin{bmatrix}0.2 & 0 & 0\\0 & 10.1 & 0 \\ 0 & 0 & 10.1\end{bmatrix}.</math> |
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====As a matrix==== |
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If <math>X</math> is a [[vector space|vector]]-valued random variable, with values in <math>\mathbb{R}^n,</math> and thought of as a column vector, then a natural generalization of variance is <math>\operatorname{E}\left[(X - \mu)(X - \mu)^{\operatorname{T}}\right],</math> where <math>\mu = \operatorname{E}(X)</math> and <math>X^{\operatorname{T}}</math> is the transpose of <math>X,</math> and so is a row vector. The result is a [[positive definite matrix|positive semi-definite square matrix]], commonly referred to as the [[variance-covariance matrix]] (or simply as the ''covariance matrix''). |
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If <math>X</math> is a vector- and complex-valued random variable, with values in <math>\mathbb{C}^n,</math> then the [[Covariance matrix#Complex random vectors|covariance matrix is]] <math>\operatorname{E}\left[(X - \mu)(X - \mu)^\dagger\right],</math> where <math>X^\dagger</math> is the [[conjugate transpose]] of <math>X.</math>{{Citation needed|date=September 2016}} This matrix is also positive semi-definite and square. |
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====As a scalar==== |
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Another generalization of variance for vector-valued random variables <math>X</math>, which results in a scalar value rather than in a matrix, is the [[generalized variance]] <math>\det(C)</math>, the [[determinant]] of the covariance matrix. The generalized variance can be shown to be related to the multidimensional scatter of points around their mean.<ref>{{cite book |last1=Kocherlakota |first1=S. |title=Encyclopedia of Statistical Sciences |last2=Kocherlakota |first2=K. |chapter=Generalized Variance |publisher=Wiley Online Library |doi=10.1002/0471667196.ess0869 |year=2004 |isbn=0-471-66719-6 }}</ref> |
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A different generalization is obtained by considering the equation for the scalar variance, <math> \operatorname{Var}(X) = \operatorname{E}\left[(X - \mu)^2 \right] </math>, and reinterpreting <math>(X - \mu)^2</math> as the squared [[Euclidean distance]] between the random variable and its mean, or, simply as the scalar product of the vector <math>X - \mu</math> with itself. This results in <math>\operatorname{E}\left[(X - \mu)^{\operatorname{T}}(X - \mu)\right] = \operatorname{tr}(C),</math> which is the [[Trace (linear algebra)|trace]] of the covariance matrix. |
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==See also== |
==See also== |
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{{Portal| |
{{Portal|Mathematics}} |
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{{Wiktionary|variance}} |
{{Wiktionary|variance}} |
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*[[Bhatia–Davis inequality]] |
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<div style="-moz-column-count:2; column-count:2;"> |
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* [[Coefficient of variation]] |
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* [[Algorithms for calculating variance]] |
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* [[Homoscedasticity]] |
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* [[Average absolute deviation]] |
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* [[Least-squares spectral analysis]] for computing a [[frequency spectrum]] with spectral magnitudes in % of variance or in [[Decibel|dB]] |
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* [[Bhatia–Davis inequality]] |
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* [[Modern portfolio theory]] |
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* [[Common-method variance]] |
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* [[Popoviciu's inequality on variances]] |
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* [[Statistical dispersion|Measures for statistical dispersion]] |
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* [[Variance-stabilizing transformation]] |
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=== Types of variance === |
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* [[Correlation]] |
* [[Correlation]] |
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* [[Covariance]] |
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* [[Chebyshev's inequality]] |
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* [[Distance variance]] |
* [[Distance variance]] |
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* [[Estimation of covariance matrices]] |
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* [[Explained variance]] |
* [[Explained variance]] |
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* [[Homoscedasticity]] |
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* [[Mean absolute error]] |
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* [[Mean difference]] |
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* [[Mean preserving spread]] |
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* [[Pooled variance]] |
* [[Pooled variance]] |
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* [[Pseudo-variance]] |
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* [[Popoviciu's inequality on variances]] |
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* [[Qualitative variation]] |
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* [[Sample mean and covariance]] |
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* [[Semivariance]] |
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* [[Skewness]] |
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* [[Taylor's law]] |
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* [[Weighted mean#Weighted sample variance|Weighted sample variance]] |
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</div> |
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== |
== References == |
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{{Reflist |
{{Reflist}} |
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{{-}} |
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{{Theory of probability distributions}} |
{{Theory of probability distributions}} |
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{{Statistics|descriptive|state=collapsed}} |
{{Statistics|descriptive|state=collapsed}} |
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{{Authority control}} |
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[[Category:Theory of probability distributions]] |
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[[Category:Moment (mathematics)]] |
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[[Category:Statistical deviation and dispersion]] |
[[Category:Statistical deviation and dispersion]] |
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[[Category:Articles containing proofs]] |
[[Category:Articles containing proofs]] |
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[[Category:Data analysis]] |
Latest revision as of 10:32, 23 December 2024
In probability theory and statistics, variance is the expected value of the squared deviation from the mean of a random variable. The standard deviation (SD) is obtained as the square root of the variance. Variance is a measure of dispersion, meaning it is a measure of how far a set of numbers is spread out from their average value. It is the second central moment of a distribution, and the covariance of the random variable with itself, and it is often represented by , , , , or .[1]
An advantage of variance as a measure of dispersion is that it is more amenable to algebraic manipulation than other measures of dispersion such as the expected absolute deviation; for example, the variance of a sum of uncorrelated random variables is equal to the sum of their variances. A disadvantage of the variance for practical applications is that, unlike the standard deviation, its units differ from the random variable, which is why the standard deviation is more commonly reported as a measure of dispersion once the calculation is finished. Another disadvantage is that the variance is not finite for many distributions.
There are two distinct concepts that are both called "variance". One, as discussed above, is part of a theoretical probability distribution and is defined by an equation. The other variance is a characteristic of a set of observations. When variance is calculated from observations, those observations are typically measured from a real-world system. If all possible observations of the system are present, then the calculated variance is called the population variance. Normally, however, only a subset is available, and the variance calculated from this is called the sample variance. The variance calculated from a sample is considered an estimate of the full population variance. There are multiple ways to calculate an estimate of the population variance, as discussed in the section below.
The two kinds of variance are closely related. To see how, consider that a theoretical probability distribution can be used as a generator of hypothetical observations. If an infinite number of observations are generated using a distribution, then the sample variance calculated from that infinite set will match the value calculated using the distribution's equation for variance. Variance has a central role in statistics, where some ideas that use it include descriptive statistics, statistical inference, hypothesis testing, goodness of fit, and Monte Carlo sampling.
Definition
[edit]The variance of a random variable is the expected value of the squared deviation from the mean of , :
This definition encompasses random variables that are generated by processes that are discrete, continuous, neither, or mixed. The variance can also be thought of as the covariance of a random variable with itself:
The variance is also equivalent to the second cumulant of a probability distribution that generates . The variance is typically designated as , or sometimes as or , or symbolically as or simply (pronounced "sigma squared"). The expression for the variance can be expanded as follows:
In other words, the variance of X is equal to the mean of the square of X minus the square of the mean of X. This equation should not be used for computations using floating point arithmetic, because it suffers from catastrophic cancellation if the two components of the equation are similar in magnitude. For other numerically stable alternatives, see algorithms for calculating variance.
Discrete random variable
[edit]If the generator of random variable is discrete with probability mass function , then
where is the expected value. That is,
(When such a discrete weighted variance is specified by weights whose sum is not 1, then one divides by the sum of the weights.)
The variance of a collection of equally likely values can be written as
where is the average value. That is,
The variance of a set of equally likely values can be equivalently expressed, without directly referring to the mean, in terms of squared deviations of all pairwise squared distances of points from each other:[2]
Absolutely continuous random variable
[edit]If the random variable has a probability density function , and is the corresponding cumulative distribution function, then
or equivalently,
where is the expected value of given by
In these formulas, the integrals with respect to and are Lebesgue and Lebesgue–Stieltjes integrals, respectively.
If the function is Riemann-integrable on every finite interval then
where the integral is an improper Riemann integral.
Examples
[edit]Exponential distribution
[edit]The exponential distribution with parameter λ is a continuous distribution whose probability density function is given by
on the interval [0, ∞). Its mean can be shown to be
Using integration by parts and making use of the expected value already calculated, we have:
Thus, the variance of X is given by
Fair dice
[edit]A fair six-sided dice can be modeled as a discrete random variable, X, with outcomes 1 through 6, each with equal probability 1/6. The expected value of X is Therefore, the variance of X is
The general formula for the variance of the outcome, X, of an n-sided die is
Commonly used probability distributions
[edit]The following table lists the variance for some commonly used probability distributions.
Name of the probability distribution | Probability distribution function | Mean | Variance |
---|---|---|---|
Binomial distribution | |||
Geometric distribution | |||
Normal distribution | |||
Uniform distribution (continuous) | |||
Exponential distribution | |||
Poisson distribution |
Properties
[edit]Basic properties
[edit]Variance is non-negative because the squares are positive or zero:
The variance of a constant is zero.
Conversely, if the variance of a random variable is 0, then it is almost surely a constant. That is, it always has the same value:
Issues of finiteness
[edit]If a distribution does not have a finite expected value, as is the case for the Cauchy distribution, then the variance cannot be finite either. However, some distributions may not have a finite variance, despite their expected value being finite. An example is a Pareto distribution whose index satisfies
Decomposition
[edit]The general formula for variance decomposition or the law of total variance is: If and are two random variables, and the variance of exists, then
The conditional expectation of given , and the conditional variance may be understood as follows. Given any particular value y of the random variable Y, there is a conditional expectation given the event Y = y. This quantity depends on the particular value y; it is a function . That same function evaluated at the random variable Y is the conditional expectation
In particular, if is a discrete random variable assuming possible values with corresponding probabilities , then in the formula for total variance, the first term on the right-hand side becomes
where . Similarly, the second term on the right-hand side becomes
where and . Thus the total variance is given by
A similar formula is applied in analysis of variance, where the corresponding formula is
here refers to the Mean of the Squares. In linear regression analysis the corresponding formula is
This can also be derived from the additivity of variances, since the total (observed) score is the sum of the predicted score and the error score, where the latter two are uncorrelated.
Similar decompositions are possible for the sum of squared deviations (sum of squares, ):
Calculation from the CDF
[edit]The population variance for a non-negative random variable can be expressed in terms of the cumulative distribution function F using
This expression can be used to calculate the variance in situations where the CDF, but not the density, can be conveniently expressed.
Characteristic property
[edit]The second moment of a random variable attains the minimum value when taken around the first moment (i.e., mean) of the random variable, i.e. . Conversely, if a continuous function satisfies for all random variables X, then it is necessarily of the form , where a > 0. This also holds in the multidimensional case.[3]
Units of measurement
[edit]Unlike the expected absolute deviation, the variance of a variable has units that are the square of the units of the variable itself. For example, a variable measured in meters will have a variance measured in meters squared. For this reason, describing data sets via their standard deviation or root mean square deviation is often preferred over using the variance. In the dice example the standard deviation is √2.9 ≈ 1.7, slightly larger than the expected absolute deviation of 1.5.
The standard deviation and the expected absolute deviation can both be used as an indicator of the "spread" of a distribution. The standard deviation is more amenable to algebraic manipulation than the expected absolute deviation, and, together with variance and its generalization covariance, is used frequently in theoretical statistics; however the expected absolute deviation tends to be more robust as it is less sensitive to outliers arising from measurement anomalies or an unduly heavy-tailed distribution.
Propagation
[edit]Addition and multiplication by a constant
[edit]Variance is invariant with respect to changes in a location parameter. That is, if a constant is added to all values of the variable, the variance is unchanged:
If all values are scaled by a constant, the variance is scaled by the square of that constant:
The variance of a sum of two random variables is given by
where is the covariance.
Linear combinations
[edit]In general, for the sum of random variables , the variance becomes:
see also general Bienaymé's identity.
These results lead to the variance of a linear combination as:
If the random variables are such that
then they are said to be uncorrelated. It follows immediately from the expression given earlier that if the random variables are uncorrelated, then the variance of their sum is equal to the sum of their variances, or, expressed symbolically:
Since independent random variables are always uncorrelated (see Covariance § Uncorrelatedness and independence), the equation above holds in particular when the random variables are independent. Thus, independence is sufficient but not necessary for the variance of the sum to equal the sum of the variances.
Matrix notation for the variance of a linear combination
[edit]Define as a column vector of random variables , and as a column vector of scalars . Therefore, is a linear combination of these random variables, where denotes the transpose of . Also let be the covariance matrix of . The variance of is then given by:[4]
This implies that the variance of the mean can be written as (with a column vector of ones)
Sum of variables
[edit]Sum of uncorrelated variables
[edit]One reason for the use of the variance in preference to other measures of dispersion is that the variance of the sum (or the difference) of uncorrelated random variables is the sum of their variances:
This statement is called the Bienaymé formula[5] and was discovered in 1853.[6][7] It is often made with the stronger condition that the variables are independent, but being uncorrelated suffices. So if all the variables have the same variance σ2, then, since division by n is a linear transformation, this formula immediately implies that the variance of their mean is
That is, the variance of the mean decreases when n increases. This formula for the variance of the mean is used in the definition of the standard error of the sample mean, which is used in the central limit theorem.
To prove the initial statement, it suffices to show that
The general result then follows by induction. Starting with the definition,
Using the linearity of the expectation operator and the assumption of independence (or uncorrelatedness) of X and Y, this further simplifies as follows:
Sum of correlated variables
[edit]Sum of correlated variables with fixed sample size
[edit]In general, the variance of the sum of n variables is the sum of their covariances:
(Note: The second equality comes from the fact that Cov(Xi,Xi) = Var(Xi).)
Here, is the covariance, which is zero for independent random variables (if it exists). The formula states that the variance of a sum is equal to the sum of all elements in the covariance matrix of the components. The next expression states equivalently that the variance of the sum is the sum of the diagonal of covariance matrix plus two times the sum of its upper triangular elements (or its lower triangular elements); this emphasizes that the covariance matrix is symmetric. This formula is used in the theory of Cronbach's alpha in classical test theory.
So, if the variables have equal variance σ2 and the average correlation of distinct variables is ρ, then the variance of their mean is
This implies that the variance of the mean increases with the average of the correlations. In other words, additional correlated observations are not as effective as additional independent observations at reducing the uncertainty of the mean. Moreover, if the variables have unit variance, for example if they are standardized, then this simplifies to
This formula is used in the Spearman–Brown prediction formula of classical test theory. This converges to ρ if n goes to infinity, provided that the average correlation remains constant or converges too. So for the variance of the mean of standardized variables with equal correlations or converging average correlation we have
Therefore, the variance of the mean of a large number of standardized variables is approximately equal to their average correlation. This makes clear that the sample mean of correlated variables does not generally converge to the population mean, even though the law of large numbers states that the sample mean will converge for independent variables.
Sum of uncorrelated variables with random sample size
[edit]There are cases when a sample is taken without knowing, in advance, how many observations will be acceptable according to some criterion. In such cases, the sample size N is a random variable whose variation adds to the variation of X, such that,
which follows from the law of total variance.
If N has a Poisson distribution, then with estimator n = N. So, the estimator of becomes , giving (see standard error of the sample mean).
Weighted sum of variables
[edit]The scaling property and the Bienaymé formula, along with the property of the covariance Cov(aX, bY) = ab Cov(X, Y) jointly imply that
This implies that in a weighted sum of variables, the variable with the largest weight will have a disproportionally large weight in the variance of the total. For example, if X and Y are uncorrelated and the weight of X is two times the weight of Y, then the weight of the variance of X will be four times the weight of the variance of Y.
The expression above can be extended to a weighted sum of multiple variables:
Product of variables
[edit]Product of independent variables
[edit]If two variables X and Y are independent, the variance of their product is given by[9]
Equivalently, using the basic properties of expectation, it is given by
Product of statistically dependent variables
[edit]In general, if two variables are statistically dependent, then the variance of their product is given by:
Arbitrary functions
[edit]The delta method uses second-order Taylor expansions to approximate the variance of a function of one or more random variables: see Taylor expansions for the moments of functions of random variables. For example, the approximate variance of a function of one variable is given by
provided that f is twice differentiable and that the mean and variance of X are finite.
Population variance and sample variance
[edit]
Real-world observations such as the measurements of yesterday's rain throughout the day typically cannot be complete sets of all possible observations that could be made. As such, the variance calculated from the finite set will in general not match the variance that would have been calculated from the full population of possible observations. This means that one estimates the mean and variance from a limited set of observations by using an estimator equation. The estimator is a function of the sample of n observations drawn without observational bias from the whole population of potential observations. In this example, the sample would be the set of actual measurements of yesterday's rainfall from available rain gauges within the geography of interest.
The simplest estimators for population mean and population variance are simply the mean and variance of the sample, the sample mean and (uncorrected) sample variance – these are consistent estimators (they converge to the value of the whole population as the number of samples increases) but can be improved. Most simply, the sample variance is computed as the sum of squared deviations about the (sample) mean, divided by n as the number of samples. However, using values other than n improves the estimator in various ways. Four common values for the denominator are n, n − 1, n + 1, and n − 1.5: n is the simplest (the variance of the sample), n − 1 eliminates bias,[10] n + 1 minimizes mean squared error for the normal distribution,[11] and n − 1.5 mostly eliminates bias in unbiased estimation of standard deviation for the normal distribution.[12]
Firstly, if the true population mean is unknown, then the sample variance (which uses the sample mean in place of the true mean) is a biased estimator: it underestimates the variance by a factor of (n − 1) / n; correcting this factor, resulting in the sum of squared deviations about the sample mean divided by n -1 instead of n, is called Bessel's correction.[10] The resulting estimator is unbiased and is called the (corrected) sample variance or unbiased sample variance. If the mean is determined in some other way than from the same samples used to estimate the variance, then this bias does not arise, and the variance can safely be estimated as that of the samples about the (independently known) mean.
Secondly, the sample variance does not generally minimize mean squared error between sample variance and population variance. Correcting for bias often makes this worse: one can always choose a scale factor that performs better than the corrected sample variance, though the optimal scale factor depends on the excess kurtosis of the population (see mean squared error: variance) and introduces bias. This always consists of scaling down the unbiased estimator (dividing by a number larger than n − 1) and is a simple example of a shrinkage estimator: one "shrinks" the unbiased estimator towards zero. For the normal distribution, dividing by n + 1 (instead of n − 1 or n) minimizes mean squared error.[11] The resulting estimator is biased, however, and is known as the biased sample variation.
Population variance
[edit]In general, the population variance of a finite population of size N with values xi is given bywhere the population mean is and , where is the expectation value operator.
The population variance can also be computed using[13]
(The right side has duplicate terms in the sum while the middle side has only unique terms to sum.) This is true becauseThe population variance matches the variance of the generating probability distribution. In this sense, the concept of population can be extended to continuous random variables with infinite populations.
Sample variance
[edit]Biased sample variance
[edit]In many practical situations, the true variance of a population is not known a priori and must be computed somehow. When dealing with extremely large populations, it is not possible to count every object in the population, so the computation must be performed on a sample of the population.[14] This is generally referred to as sample variance or empirical variance. Sample variance can also be applied to the estimation of the variance of a continuous distribution from a sample of that distribution.
We take a sample with replacement of n values Y1, ..., Yn from the population of size , where n < N, and estimate the variance on the basis of this sample.[15] Directly taking the variance of the sample data gives the average of the squared deviations:
(See the section Population variance for the derivation of this formula.) Here, denotes the sample mean:
Since the Yi are selected randomly, both and are random variables. Their expected values can be evaluated by averaging over the ensemble of all possible samples {Yi} of size n from the population. For this gives:
Here derived in the section Population variance and due to independency of and are used.
Hence gives an estimate of the population variance that is biased by a factor of as the expectation value of is smaller than the population variance (true variance) by that factor. For this reason, is referred to as the biased sample variance.
Unbiased sample variance
[edit]Correcting for this bias yields the unbiased sample variance, denoted :
Either estimator may be simply referred to as the sample variance when the version can be determined by context. The same proof is also applicable for samples taken from a continuous probability distribution.
The use of the term n − 1 is called Bessel's correction, and it is also used in sample covariance and the sample standard deviation (the square root of variance). The square root is a concave function and thus introduces negative bias (by Jensen's inequality), which depends on the distribution, and thus the corrected sample standard deviation (using Bessel's correction) is biased. The unbiased estimation of standard deviation is a technically involved problem, though for the normal distribution using the term n − 1.5 yields an almost unbiased estimator.
The unbiased sample variance is a U-statistic for the function ƒ(y1, y2) = (y1 − y2)2/2, meaning that it is obtained by averaging a 2-sample statistic over 2-element subsets of the population.
Example
[edit]For a set of numbers {10, 15, 30, 45, 57, 52 63, 72, 81, 93, 102, 105}, if this set is the whole data population for some measurement, then variance is the population variance 932.743 as the sum of the squared deviations about the mean of this set, divided by 12 as the number of the set members. If the set is a sample from the whole population, then the unbiased sample variance can be calculated as 1017.538 that is the sum of the squared deviations about the mean of the sample, divided by 11 instead of 12. A function VAR.S in Microsoft Excel gives the unbiased sample variance while VAR.P is for population variance.
Distribution of the sample variance
[edit]Being a function of random variables, the sample variance is itself a random variable, and it is natural to study its distribution. In the case that Yi are independent observations from a normal distribution, Cochran's theorem shows that the unbiased sample variance S2 follows a scaled chi-squared distribution (see also: asymptotic properties and an elementary proof):[17]
where σ2 is the population variance. As a direct consequence, it follows that
and[18]
If Yi are independent and identically distributed, but not necessarily normally distributed, then[19]
where κ is the kurtosis of the distribution and μ4 is the fourth central moment.
If the conditions of the law of large numbers hold for the squared observations, S2 is a consistent estimator of σ2. One can see indeed that the variance of the estimator tends asymptotically to zero. An asymptotically equivalent formula was given in Kenney and Keeping (1951:164), Rose and Smith (2002:264), and Weisstein (n.d.).[20][21][22]
Samuelson's inequality
[edit]Samuelson's inequality is a result that states bounds on the values that individual observations in a sample can take, given that the sample mean and (biased) variance have been calculated.[23] Values must lie within the limits
Relations with the harmonic and arithmetic means
[edit]It has been shown[24] that for a sample {yi} of positive real numbers,
where ymax is the maximum of the sample, A is the arithmetic mean, H is the harmonic mean of the sample and is the (biased) variance of the sample.
This bound has been improved, and it is known that variance is bounded by
where ymin is the minimum of the sample.[25]
Tests of equality of variances
[edit]The F-test of equality of variances and the chi square tests are adequate when the sample is normally distributed. Non-normality makes testing for the equality of two or more variances more difficult.
Several non parametric tests have been proposed: these include the Barton–David–Ansari–Freund–Siegel–Tukey test, the Capon test, Mood test, the Klotz test and the Sukhatme test. The Sukhatme test applies to two variances and requires that both medians be known and equal to zero. The Mood, Klotz, Capon and Barton–David–Ansari–Freund–Siegel–Tukey tests also apply to two variances. They allow the median to be unknown but do require that the two medians are equal.
The Lehmann test is a parametric test of two variances. Of this test there are several variants known. Other tests of the equality of variances include the Box test, the Box–Anderson test and the Moses test.
Resampling methods, which include the bootstrap and the jackknife, may be used to test the equality of variances.
Moment of inertia
[edit]The variance of a probability distribution is analogous to the moment of inertia in classical mechanics of a corresponding mass distribution along a line, with respect to rotation about its center of mass.[26] It is because of this analogy that such things as the variance are called moments of probability distributions.[26] The covariance matrix is related to the moment of inertia tensor for multivariate distributions. The moment of inertia of a cloud of n points with a covariance matrix of is given by[citation needed]
This difference between moment of inertia in physics and in statistics is clear for points that are gathered along a line. Suppose many points are close to the x axis and distributed along it. The covariance matrix might look like
That is, there is the most variance in the x direction. Physicists would consider this to have a low moment about the x axis so the moment-of-inertia tensor is
Semivariance
[edit]The semivariance is calculated in the same manner as the variance but only those observations that fall below the mean are included in the calculation:It is also described as a specific measure in different fields of application. For skewed distributions, the semivariance can provide additional information that a variance does not.[27]
For inequalities associated with the semivariance, see Chebyshev's inequality § Semivariances.
Etymology
[edit]The term variance was first introduced by Ronald Fisher in his 1918 paper The Correlation Between Relatives on the Supposition of Mendelian Inheritance:[28]
The great body of available statistics show us that the deviations of a human measurement from its mean follow very closely the Normal Law of Errors, and, therefore, that the variability may be uniformly measured by the standard deviation corresponding to the square root of the mean square error. When there are two independent causes of variability capable of producing in an otherwise uniform population distributions with standard deviations and , it is found that the distribution, when both causes act together, has a standard deviation . It is therefore desirable in analysing the causes of variability to deal with the square of the standard deviation as the measure of variability. We shall term this quantity the Variance...
Generalizations
[edit]For complex variables
[edit]If is a scalar complex-valued random variable, with values in then its variance is where is the complex conjugate of This variance is a real scalar.
For vector-valued random variables
[edit]As a matrix
[edit]If is a vector-valued random variable, with values in and thought of as a column vector, then a natural generalization of variance is where and is the transpose of and so is a row vector. The result is a positive semi-definite square matrix, commonly referred to as the variance-covariance matrix (or simply as the covariance matrix).
If is a vector- and complex-valued random variable, with values in then the covariance matrix is where is the conjugate transpose of [citation needed] This matrix is also positive semi-definite and square.
As a scalar
[edit]Another generalization of variance for vector-valued random variables , which results in a scalar value rather than in a matrix, is the generalized variance , the determinant of the covariance matrix. The generalized variance can be shown to be related to the multidimensional scatter of points around their mean.[29]
A different generalization is obtained by considering the equation for the scalar variance, , and reinterpreting as the squared Euclidean distance between the random variable and its mean, or, simply as the scalar product of the vector with itself. This results in which is the trace of the covariance matrix.
See also
[edit]- Bhatia–Davis inequality
- Coefficient of variation
- Homoscedasticity
- Least-squares spectral analysis for computing a frequency spectrum with spectral magnitudes in % of variance or in dB
- Modern portfolio theory
- Popoviciu's inequality on variances
- Measures for statistical dispersion
- Variance-stabilizing transformation
Types of variance
[edit]References
[edit]- ^ Wasserman, Larry (2005). All of Statistics: a concise course in statistical inference. Springer texts in statistics. p. 51. ISBN 978-1-4419-2322-6.
- ^ Yuli Zhang; Huaiyu Wu; Lei Cheng (June 2012). Some new deformation formulas about variance and covariance. Proceedings of 4th International Conference on Modelling, Identification and Control(ICMIC2012). pp. 987–992.
- ^ Kagan, A.; Shepp, L. A. (1998). "Why the variance?". Statistics & Probability Letters. 38 (4): 329–333. doi:10.1016/S0167-7152(98)00041-8.
- ^ Johnson, Richard; Wichern, Dean (2001). Applied Multivariate Statistical Analysis. Prentice Hall. p. 76. ISBN 0-13-187715-1.
- ^ Loève, M. (1977) "Probability Theory", Graduate Texts in Mathematics, Volume 45, 4th edition, Springer-Verlag, p. 12.
- ^ Bienaymé, I.-J. (1853) "Considérations à l'appui de la découverte de Laplace sur la loi de probabilité dans la méthode des moindres carrés", Comptes rendus de l'Académie des sciences Paris, 37, p. 309–317; digital copy available [1]
- ^ Bienaymé, I.-J. (1867) "Considérations à l'appui de la découverte de Laplace sur la loi de probabilité dans la méthode des moindres carrés", Journal de Mathématiques Pures et Appliquées, Série 2, Tome 12, p. 158–167; digital copy available [2][3]
- ^ Cornell, J R, and Benjamin, C A, Probability, Statistics, and Decisions for Civil Engineers, McGraw-Hill, NY, 1970, pp.178-9.
- ^ Goodman, Leo A. (December 1960). "On the Exact Variance of Products". Journal of the American Statistical Association. 55 (292): 708–713. doi:10.2307/2281592. JSTOR 2281592.
- ^ a b Reichmann, W. J. (1961). "Appendix 8". Use and Abuse of Statistics (Reprinted 1964–1970 by Pelican ed.). London: Methuen.
- ^ a b Kourouklis, Stavros (2012). "A New Estimator of the Variance Based on Minimizing Mean Squared Error". The American Statistician. 66 (4): 234–236. doi:10.1080/00031305.2012.735209. ISSN 0003-1305. JSTOR 23339501.
- ^ Brugger, R. M. (1969). "A Note on Unbiased Estimation of the Standard Deviation". The American Statistician. 23 (4): 32. doi:10.1080/00031305.1969.1048186 (inactive 16 December 2024).
{{cite journal}}
: CS1 maint: DOI inactive as of December 2024 (link) - ^ Yuli Zhang; Huaiyu Wu; Lei Cheng (June 2012). Some new deformation formulas about variance and covariance. Proceedings of 4th International Conference on Modelling, Identification and Control(ICMIC2012). pp. 987–992.
- ^ Navidi, William (2006) Statistics for Engineers and Scientists, McGraw-Hill, p. 14.
- ^ Montgomery, D. C. and Runger, G. C. (1994) Applied statistics and probability for engineers, page 201. John Wiley & Sons New York
- ^ Yuli Zhang; Huaiyu Wu; Lei Cheng (June 2012). Some new deformation formulas about variance and covariance. Proceedings of 4th International Conference on Modelling, Identification and Control(ICMIC2012). pp. 987–992.
- ^ Knight K. (2000), Mathematical Statistics, Chapman and Hall, New York. (proposition 2.11)
- ^ Casella and Berger (2002) Statistical Inference, Example 7.3.3, p. 331 [full citation needed]
- ^ Mood, A. M., Graybill, F. A., and Boes, D.C. (1974) Introduction to the Theory of Statistics, 3rd Edition, McGraw-Hill, New York, p. 229
- ^ Kenney, John F.; Keeping, E.S. (1951). Mathematics of Statistics. Part Two (PDF) (2nd ed.). Princeton, New Jersey: D. Van Nostrand Company, Inc. Archived from the original (PDF) on Nov 17, 2018 – via KrishiKosh.
- ^ Rose, Colin; Smith, Murray D. (2002). "Mathematical Statistics with Mathematica". Springer-Verlag, New York.
- ^ Weisstein, Eric W. "Sample Variance Distribution". MathWorld Wolfram.
- ^ Samuelson, Paul (1968). "How Deviant Can You Be?". Journal of the American Statistical Association. 63 (324): 1522–1525. doi:10.1080/01621459.1968.10480944. JSTOR 2285901.
- ^ Mercer, A. McD. (2000). "Bounds for A–G, A–H, G–H, and a family of inequalities of Ky Fan's type, using a general method". J. Math. Anal. Appl. 243 (1): 163–173. doi:10.1006/jmaa.1999.6688.
- ^ Sharma, R. (2008). "Some more inequalities for arithmetic mean, harmonic mean and variance". Journal of Mathematical Inequalities. 2 (1): 109–114. CiteSeerX 10.1.1.551.9397. doi:10.7153/jmi-02-11.
- ^ a b Magnello, M. Eileen. "Karl Pearson and the Origins of Modern Statistics: An Elastician becomes a Statistician". The Rutherford Journal.
- ^ Fama, Eugene F.; French, Kenneth R. (2010-04-21). "Q&A: Semi-Variance: A Better Risk Measure?". Fama/French Forum.
- ^ Ronald Fisher (1918) The correlation between relatives on the supposition of Mendelian Inheritance
- ^ Kocherlakota, S.; Kocherlakota, K. (2004). "Generalized Variance". Encyclopedia of Statistical Sciences. Wiley Online Library. doi:10.1002/0471667196.ess0869. ISBN 0-471-66719-6.