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

It is a special case of the more general identity

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

since

Similar identities
A similar identity for the sine function also holds:

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

Proof
Geometric proof of Morrie's law
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
Recall the double angle formula for the sine function

Solve for

It follows that:
![{\displaystyle {\begin{aligned}\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{aligned}}}](./60bd81aaf5f880106a8afbd298449d2818660709.svg)
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
References
Further reading
External links