Log-distance path loss model: Difference between revisions
m →Mathematical formulation: Fix grammar. |
The '''log-distance path loss model''' is a radio propagation model that predicts the path loss a signal encounters inside a building or densely populated areas over long distance. |
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The '''log-distance path loss model''' is a [[radio propagation model]] that predicts the [[path loss]] a [[Wiktionary:signal|signal]] encounters inside a building or densely populated areas over distance. |
The '''log-distance path loss model''' is a [[radio propagation model]] that predicts the [[path loss]] a [[Wiktionary:signal|signal]] encounters inside a building or densely populated areas over long distance. While the log-distance model is suitable for longer distances, the short-distance path loss model is often used for indoor environments or very short outdoor distances. It's simpler and assumes a more direct line-of-sight propagation. |
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==Mathematical formulation== |
== Mathematical formulation == |
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=== |
=== Model === |
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[[File:Slow fading Log-distance.png|thumb|Log-distance path loss model]] |
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Log-distance path loss model is formally expressed as: |
Log-distance path loss model is formally expressed as: |
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where |
where |
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* <math display=inline>L_\text{Tx}=10\log_{10}\frac{P_\text{Tx}}{\mathrm{1~mW}} \mathrm{~dBm}</math> is the transmitted power [[Level (logarithmic quantity)|level]], and <math>P_\text{Tx}</math> is the transmitted power. |
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* <math> |
* <math display=inline>L_\text{Rx}=10\log_{10}\frac{P_\text{Rx}}{\mathrm{1~mW}} \mathrm{~dBm}</math> is the received power level where <math>{P_\text{Rx}}</math> is the received power. |
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* <math>L_0</math> is the [[path loss]] in decibels (dB) at the reference distance <math>d_0</math>. This is based on either close-in measurements or calculated based on a free space assumption with the Friis [[free-space path loss]] model.<ref name="gau">{{Cite web|url=https://www.gaussianwaves.com/2013/09/log-distance-path-loss-or-log-normal-shadowing-model/|title = Log Distance Path Loss or Log Normal Shadowing Model|date = 30 September 2013}}</ref> |
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* <math>P_{Rx_{dBm}}=10\log_{10}\frac{P_{Rx}}{1mW}</math> is the received power in dBm where <math>{P_{Rx}}</math> is the received power in watts. |
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* <math>PL_0</math> is the [[path loss]] in decibels (dB) at the reference distance <math>d_0</math> calculated using the Friis [[free-space path loss]] model. |
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* <math>{d}</math> is the length of the path. |
* <math>{d}</math> is the length of the path. |
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* <math>{d_0}</math> is the reference distance, usually 1 |
* <math>{d_0}</math> is the reference distance, usually 1 km (or 1 mile) for a large cell and 1 m to 10 m for a microcell.<ref name="gau"/> |
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* <math>\gamma</math> is the [[path loss]] exponent. |
* <math>\gamma</math> is the [[path loss]] exponent. |
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* <math> |
* <math>X_\text{g}</math> is a [[normal random variable|normal (Gaussian) random variable]] with zero [[mean]], reflecting the attenuation (in decibels) caused by [[flat fading]]{{Citation needed|date=October 2011}}. In the case of no fading, this variable is 0. In the case of only [[shadow fading]] or [[slow fading]], this random variable may have [[Gaussian distribution]] with <math>\sigma</math> [[standard deviation]] in decibels, resulting in a [[log-normal distribution]] of the received power in watts. In the case of only fast fading caused by multipath propagation, the corresponding fluctuation of the signal envelope in volts may be modelled as a random variable with [[Rayleigh distribution]] or [[Ricean distribution]]<ref>{{cite book|title=Handbook of Propagation Effects for Vehicular and Personal Mobile Satellite Systems|author=Julius Goldhirsh|author2=Wolfhard J. Vogel |url=http://vancouver.chapters.comsoc.org/files/2016/05/handbook.pdf|chapter=11.4}}</ref> (and thus the corresponding power gain <math display=inline>F_\text{g}=10^{-X_\text{g}/10}</math> may be modelled as a random variable with [[exponential distribution]]). |
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===Corresponding non-logarithmic model=== |
=== Corresponding non-logarithmic model === |
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This corresponds to the following non-logarithmic gain model: |
This corresponds to the following non-logarithmic gain model: |
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where |
where |
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<math display=inline>c_0={d_0^{\gamma}}10^{-L_0/10}</math> is the average multiplicative gain at the reference distance <math>d_0</math> from the transmitter. This gain depends on factors such as [[carrier frequency]], antenna heights and antenna gain, for example due to directional antennas; and <math display=inline>F_\text{g}=10^{-X_\text{g}/10}</math> is a [[stochastic process]] that reflects [[flat fading]]. In case of only slow fading (shadowing), it may have [[log-normal]] distribution with parameter <math>\sigma</math> dB. In case of only [[fast fading]] due to [[multipath propagation]], its amplitude may have [[Rayleigh distribution]] or [[Ricean distribution]]. This can be convenient, because power is proportional to the square of amplitude. Squaring a Rayleigh-distributed random variable produces an [[Exponential distribution |exponentially distributed]] random variable. In many cases, exponential distributions are computationally convenient and allow direct closed-form calculations in many more situations than a Rayleigh (or even a Gaussian). |
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<math>c_0\;=\;{d_0^{\gamma}}10^{\frac{-PL_0}{10}}</math> is the average multiplicative gain at the reference distance <math>d_0</math> from the transmitter. This gain depends on factors such as [[carrier frequency]], antenna heights and antenna gain, for example due to directional antennas; and |
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<math>F_g\;=\;10^{\frac{-X_g}{10}}</math> is a [[stochastic process]] that reflects [[flat fading]]. In case of only slow fading (shadowing), it may have [[log-normal]] distribution with parameter <math>\sigma\;</math> dB. In case of only [[fast fading]] due to [[multipath propagation]], its amplitude may have [[Rayleigh distribution]] or [[Ricean distribution]]. |
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Empirical measurements of coefficients <math>\gamma</math> and <math>\sigma</math> in dB have shown the following values for a number of indoor wave propagation cases.<ref name = "Ref 1">''Wireless communications principles and practices'', T. S. Rappaport, 2002, Prentice-Hall</ref> |
Empirical measurements of coefficients <math>\gamma</math> and <math>\sigma</math> in dB have shown the following values for a number of indoor wave propagation cases.<ref name = "Ref 1">''Wireless communications principles and practices'', T. S. Rappaport, 2002, Prentice-Hall</ref> |
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{| class="wikitable" |
{| class="wikitable" |
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! Building |
! Building type !! Frequency of transmission !! <math>\gamma</math> !! <math>\sigma</math> [dB] |
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| Vacuum, infinite space || || 2.0 || 0 |
| Vacuum, infinite space || || 2.0 || 0 |
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| Commercial || 60 GHz || 1.7 || 7.9 |
| Commercial || 60 GHz || 1.7 || 7.9 |
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|} |
|} |
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''' |
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==See also== |
== See also == |
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*[[ITU model for indoor attenuation]] |
* [[ITU model for indoor attenuation]] |
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*[[Radio propagation model]] |
* [[Radio propagation model]] |
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*[[Young model]] |
* [[Young model]] |
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* [[Path loss]] |
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{{reflist}} |
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* {{cite book |last1=Seybold |first1=John S. |title=Introduction to RF Propagation |date=2005 |publisher=Wiley-Interscience |location=Hoboken, N.J. |isbn=9780471655961}} |
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<references/> |
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* {{cite book |last1=Rappaport |first1=Theodore S. |title=Wireless Communications: Principles and Practice |date=2002 |publisher=Prentice Hall PTR |location=Upper Saddle River, N.J. |isbn=9780130995728 |edition=2nd}} |
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{{Radio frequency propagation models}} |
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* ''Introduction to RF propagation'', John S. Seybold, 2005, Wiley. |
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* ''Wireless communications principles and practices'', T. S. Rappaport, 2002, Prentice-Hall. |
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[[Category:Radio frequency propagation]] |
[[Category:Radio frequency propagation model]] |
Latest revision as of 22:49, 6 November 2024
The log-distance path loss model is a radio propagation model that predicts the path loss a signal encounters inside a building or densely populated areas over long distance. While the log-distance model is suitable for longer distances, the short-distance path loss model is often used for indoor environments or very short outdoor distances. It's simpler and assumes a more direct line-of-sight propagation.
Mathematical formulation
[edit]Model
[edit]Log-distance path loss model is formally expressed as:
where
- is the total path loss in decibels (dB).
- is the transmitted power level, and is the transmitted power.
- is the received power level where is the received power.
- is the path loss in decibels (dB) at the reference distance . This is based on either close-in measurements or calculated based on a free space assumption with the Friis free-space path loss model.[1]
- is the length of the path.
- is the reference distance, usually 1 km (or 1 mile) for a large cell and 1 m to 10 m for a microcell.[1]
- is the path loss exponent.
- is a normal (Gaussian) random variable with zero mean, reflecting the attenuation (in decibels) caused by flat fading[citation needed]. In the case of no fading, this variable is 0. In the case of only shadow fading or slow fading, this random variable may have Gaussian distribution with standard deviation in decibels, resulting in a log-normal distribution of the received power in watts. In the case of only fast fading caused by multipath propagation, the corresponding fluctuation of the signal envelope in volts may be modelled as a random variable with Rayleigh distribution or Ricean distribution[2] (and thus the corresponding power gain may be modelled as a random variable with exponential distribution).
Corresponding non-logarithmic model
[edit]This corresponds to the following non-logarithmic gain model:
where is the average multiplicative gain at the reference distance from the transmitter. This gain depends on factors such as carrier frequency, antenna heights and antenna gain, for example due to directional antennas; and is a stochastic process that reflects flat fading. In case of only slow fading (shadowing), it may have log-normal distribution with parameter dB. In case of only fast fading due to multipath propagation, its amplitude may have Rayleigh distribution or Ricean distribution. This can be convenient, because power is proportional to the square of amplitude. Squaring a Rayleigh-distributed random variable produces an exponentially distributed random variable. In many cases, exponential distributions are computationally convenient and allow direct closed-form calculations in many more situations than a Rayleigh (or even a Gaussian).
Empirical coefficient values for indoor propagation
[edit]Empirical measurements of coefficients and in dB have shown the following values for a number of indoor wave propagation cases.[3]
Building type | Frequency of transmission | [dB] | |
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Vacuum, infinite space | 2.0 | 0 | |
Retail store | 914 MHz | 2.2 | 8.7 |
Grocery store | 914 MHz | 1.8 | 5.2 |
Office with hard partition | 1.5 GHz | 3.0 | 7 |
Office with soft partition | 900 MHz | 2.4 | 9.6 |
Office with soft partition | 1.9 GHz | 2.6 | 14.1 |
Textile or chemical | 1.3 GHz | 2.0 | 3.0 |
Textile or chemical | 4 GHz | 2.1 | 7.0, 9.7 |
Office | 60 GHz | 2.2 | 3.92 |
Commercial | 60 GHz | 1.7 | 7.9 |
See also
[edit]References
[edit]- ^ a b "Log Distance Path Loss or Log Normal Shadowing Model". 30 September 2013.
- ^ Julius Goldhirsh; Wolfhard J. Vogel. "11.4". Handbook of Propagation Effects for Vehicular and Personal Mobile Satellite Systems (PDF).
- ^ Wireless communications principles and practices, T. S. Rappaport, 2002, Prentice-Hall
Further reading
[edit]- Seybold, John S. (2005). Introduction to RF Propagation. Hoboken, N.J.: Wiley-Interscience. ISBN 9780471655961.
- Rappaport, Theodore S. (2002). Wireless Communications: Principles and Practice (2nd ed.). Upper Saddle River, N.J.: Prentice Hall PTR. ISBN 9780130995728.