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See also: +"...,same identity taking 𝛼=2^{-𝑛} x on Morrie's law" (added clarification)((Viète)sin(x)=2ⁿsin2⁻ⁿx∏ⁿᵢ₌₁ cos2⁻ⁱx=2ⁿsinα∏ⁿᵢ₌₁ cos2ⁿ⁻ⁱα =2ⁿsinα∏ⁿ⁻¹ₖ₌₀cos2ᵏα=sin(2ⁿα)(Morrie)))
 
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{{short description|For angles in degrees, cos(20)*cos(40)*cos(80) equals 1/8}}
'''Morrie's law''' is a name, that occasionally is used for the [[trigonometric identity]]
'''Morrie's law''' is a special [[trigonometric identity]]. Its name is due to the physicist [[Richard Feynman]], who used to refer to the identity under that name. Feynman picked that name because he learned it during his childhood from a boy with the name Morrie Jacobs and afterwards remembered it for all of his life.<ref>W. A. Beyer, J. D. Louck, and [[Doron Zeilberger|D. Zeilberger]], ''A Generalization of a Curiosity that Feynman Remembered All His Life'', Math. Mag. 69, 43–44, 1996. ([https://www.jstor.org/stable/2691393 JSTOR])</ref>


== Identity and generalisation==
:<math> \cos(20^\circ) \cdot \cos(40^\circ) \cdot \cos(80^\circ)=\frac{1}{8}.</math>


:<math> \cos(20^\circ) \cdot \cos(40^\circ) \cdot \cos(80^\circ) = \frac{1}{8}.</math>
It is a special case of the more general identity


It is a [[special case]] of the more general identity
:<math> 2^n \cdot \prod_{k=0}^{n-1} \cos(2^k \alpha)=\frac{\sin(2^n \alpha)}{\sin(\alpha)}</math>


:<math> 2^n \cdot \prod_{k=0}^{n-1} \cos(2^k \alpha) = \frac{\sin(2^n \alpha)}{\sin(\alpha)}</math>
with ''n'' = 3 and &alpha; = 20&deg;. The name is due to the physicist [[Richard Feynman]], who used to refer to the identity under that name. Feynman picked that name, because he learned it during his childhood from a boy with the name Morrie Jacobs and afterwards remembered it for all of his life.


with ''n'' = 3 and α = 20° and the fact that

:<math> \frac{\sin(160^\circ)}{\sin(20^\circ)} = \frac{\sin(180^\circ-20^\circ)}{\sin(20^\circ)} = 1,</math>

since

:<math> \sin(180^\circ-x) = \sin(x).</math>

== Similar identities ==
A similar identity for the sine function also holds:
A similar identity for the sine function also holds:
:<math> \sin(20^\circ) \cdot \sin(40^\circ) \cdot \sin(80^\circ)=\frac{\sqrt 3\ }{8}.</math>


:<math> \sin(20^\circ) \cdot \sin(40^\circ) \cdot \sin(80^\circ) = \frac{\sqrt 3}{8}.</math>
Moreover, dividing each of these identities by the other, the following two identities are evident:

:<math> \tan(20^\circ) \cdot \tan(40^\circ) \cdot \tan(80^\circ)={\sqrt 3\ }=tan(60^\circ).</math>
Moreover, dividing the second identity by the first, the following identity is evident:
:<math> \cot(20^\circ) \cdot \cot(40^\circ) \cdot \cot(80^\circ)=\frac{1}{\sqrt 3\}.</math>

:<math> \tan(20^\circ) \cdot \tan(40^\circ) \cdot \tan(80^\circ) = \sqrt 3 = \tan(60^\circ).</math>

==Proof==
=== Geometric proof of Morrie's law ===
[[File:Morries law geometric proof.svg|thumb|upright=1.5|Regular nonagon <math>ABCDEFGHI</math> with <math>O</math> being the center of its [[circumcircle]]. Computing of the angles:<br/><math>\begin{align} 40^\circ&=\frac{360^\circ}{9} \\70^\circ&=\frac{180^\circ-40^\circ}{2}\\ \alpha&=180^\circ-90^\circ-70^\circ =20^\circ \\ \beta&=180^\circ -90^\circ-(70^\circ-\alpha)=40^\circ \\ \gamma&=140^\circ -\beta -\alpha=80^\circ \end{align}</math>]]
Consider a regular [[nonagon]] <math>ABCDEFGHI</math> with side length <math>1</math> and let <math>M</math> be the midpoint of <math>AB</math>, <math>L</math> the midpoint <math>BF</math> and <math>J</math> the midpoint of <math>BD</math>. The inner angles of the nonagon equal <math>140^\circ</math> and furthermore <math>\gamma=\angle FBM=80^\circ</math>, <math>\beta=\angle DBF=40^\circ</math> and <math>\alpha=\angle CBD=20^\circ</math> (see graphic). Applying the [[Trigonometric_functions#Right-angled_triangle_definitions|cosinus definition]] in the [[right angle triangle]]s <math>\triangle BFM</math>, <math>\triangle BDL</math> and <math>\triangle BCJ</math> then yields the proof for Morrie's law:<ref> Samuel G. Moreno, Esther M. García-Caballero: "'A Geometric Proof of Morrie's Law". In: ''American Mathematical Monthly'', vol. 122, no. 2 (February 2015), p. 168 ([https://www.jstor.org/stable/10.4169/amer.math.monthly.122.02.168 JSTOR])</ref>

:<math>\begin{align}
1&=|AB|\\
&=2\cdot|MB|\\
&=2\cdot|BF|\cdot\cos(\gamma)\\
&=2^2|BL|\cos(\gamma)\\
&=2^2\cdot|BD|\cdot\cos(\gamma)\cdot\cos(\beta)\\
&=2^3\cdot|BJ|\cdot\cos(\gamma)\cdot\cos(\beta) \\
&=2^3\cdot|BC|\cdot\cos(\gamma)\cdot\cos(\beta)\cdot\cos(\alpha) \\
&=2^3\cdot 1 \cdot\cos(\gamma)\cdot\cos(\beta)\cdot\cos(\alpha) \\
&=8\cdot\cos(80^\circ)\cdot\cos(40^\circ)\cdot\cos(20^\circ)
\end{align}</math>

=== Algebraic proof of the generalised identity ===
Recall the double angle formula for the sine function

:<math> \sin(2 \alpha) = 2 \sin(\alpha) \cos(\alpha). </math>

Solve for <math> \cos(\alpha) </math>

:<math> \cos(\alpha)=\frac{\sin(2 \alpha)}{2 \sin(\alpha)}. </math>

It follows that:

:<math>
\begin{align}
\cos(2 \alpha) & = \frac{\sin(4 \alpha)}{2 \sin(2 \alpha)} \\[6pt]
\cos(4 \alpha) & = \frac{\sin(8 \alpha)}{2 \sin(4 \alpha)} \\
& \,\,\,\vdots \\
\cos\left(2^{n-1} \alpha\right)
& = \frac{\sin\left(2^n \alpha\right)}{2 \sin\left(2^{n-1} \alpha\right)}.
\end{align}
</math>

Multiplying all of these expressions together yields:

:<math>
\cos(\alpha) \cos(2 \alpha) \cos(4 \alpha) \cdots \cos\left(2^{n-1} \alpha\right) =
\frac{\sin(2 \alpha)}{2 \sin(\alpha)} \cdot
\frac{\sin(4 \alpha)}{2 \sin(2 \alpha)} \cdot
\frac{\sin(8 \alpha)}{2 \sin(4 \alpha)} \cdots
\frac{\sin\left(2^n \alpha\right)}{2 \sin\left(2^{n-1} \alpha\right)}.
</math>

The intermediate numerators and denominators cancel leaving only the first denominator, a power of 2 and the final numerator. Note that there are ''n'' terms in both sides of the expression. Thus,

:<math> \prod_{k=0}^{n-1} \cos\left(2^k \alpha\right) = \frac{\sin\left(2^n \alpha\right)}{2^n \sin(\alpha)}, </math>

which is equivalent to the generalization of Morrie's law.

== See also ==

* [[Viète's formula]], same identity taking <math>\alpha=2^{-n} x</math> on Morrie's law
* [[List of trigonometric identities]]


==References==
==References==
<References/>
* W.A. Beyer, J.D. Louck, and D. Zeilberger, ''A Generalization of a Curiosity that Feynman Remembered All His Life'', Math. Mag. 69, 43-44, 1996.

== Further reading ==
* Glen Van Brummelen: ''Trigonometry: A Very Short Introduction''. Oxford University Press, 2020, {{ISBN|9780192545466}}, pp. 79–83
* Ernest C. Anderson: ''Morrie's Law and Experimental Mathematics''. In: ''Journal of recreational mathematics'', 1998


==External links==
==External links==
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[[Category:Mathematical identities]]
[[Category:Mathematical identities]]
[[Category:Trigonometry]]
[[Category:Trigonometry]]
[[Category:Articles containing proofs]]

Latest revision as of 13:45, 29 July 2024

Morrie's law is a special trigonometric identity. Its name is due to the physicist Richard Feynman, who used to refer to the identity under that name. Feynman picked that name because he learned it during his childhood from a boy with the name Morrie Jacobs and afterwards remembered it for all of his life.[1]

Identity and generalisation

[edit]

It is a special case of the more general identity

with n = 3 and α = 20° and the fact that

since

Similar identities

[edit]

A similar identity for the sine function also holds:

Moreover, dividing the second identity by the first, the following identity is evident:

Proof

[edit]

Geometric proof of Morrie's law

[edit]
Regular nonagon with being the center of its circumcircle. Computing of the angles:

Consider a regular nonagon with side length and let be the midpoint of , the midpoint and the midpoint of . The inner angles of the nonagon equal and furthermore , and (see graphic). Applying the cosinus definition in the right angle triangles , and then yields the proof for Morrie's law:[2]

Algebraic proof of the generalised identity

[edit]

Recall the double angle formula for the sine function

Solve for

It follows that:

Multiplying all of these expressions together yields:

The intermediate numerators and denominators cancel leaving only the first denominator, a power of 2 and the final numerator. Note that there are n terms in both sides of the expression. Thus,

which is equivalent to the generalization of Morrie's law.

See also

[edit]

References

[edit]
  1. ^ W. A. Beyer, J. D. Louck, and D. Zeilberger, A Generalization of a Curiosity that Feynman Remembered All His Life, Math. Mag. 69, 43–44, 1996. (JSTOR)
  2. ^ Samuel G. Moreno, Esther M. García-Caballero: "'A Geometric Proof of Morrie's Law". In: American Mathematical Monthly, vol. 122, no. 2 (February 2015), p. 168 (JSTOR)

Further reading

[edit]
  • Glen Van Brummelen: Trigonometry: A Very Short Introduction. Oxford University Press, 2020, ISBN 9780192545466, pp. 79–83
  • Ernest C. Anderson: Morrie's Law and Experimental Mathematics. In: Journal of recreational mathematics, 1998
[edit]