I have stumbled across these two identities $$ \begin{split} \cos^2(x)+\cos^2(x+2\pi/3)+\cos^2(x+4\pi/3) &= 3/2,\\ \cos^4(x)+\cos^4(x+2\pi/3)+\cos^4(x+4\pi/3) &= 9/8. \end{split} $$ There is also the more intricate $$ \begin{split} \cos^2(x)\sin^2(x)+\cos^2(x+2\pi/3)\sin^2(x+2\pi/3)+\cos^2(x+4\pi/3)\sin^2(x+4\pi/3) &= 3/8,\\ \cos^4(x)\sin^4(x)+\cos^4(x+2\pi/3)\sin^4(x+2\pi/3)+\cos^4(x+4\pi/3)\sin^4(x+4\pi/3) &= 9/128, \end{split} $$ and of course the most elementary $$ \cos(x)+\cos(x+2\pi/3)+\cos(x+4\pi/3)=0. $$
The last identity admits a rather intuitive interpretation in terms of unitary complex numbers centered about the origin. My questions are:
- Do the other identities admit similar more or less intuitive interpretations as well?
- Do such identities have names?
- Not all powers and combinations produce a constant; What is the general form of the expressions that do?
Context: The first two identities came up while calculating the elastic response of a two-dimensional truss (a planar lattice of nodes connected with springs) that is invariant by rotations of order 3, in which case $x$ describes the orientation of the truss. We know that such trusses must exhibit an isotropic response and that justifies, in a rather convoluted manner, that these expressions must be constants. The other expressions I found by trial and error. I am looking for a satisfying, non-brute-force, non-too-group-theoretic, explanation.
$\color{green}{\textbf{Version of 20.07.20.}}$
$\color{brown}{\textbf{Preliminary calculations.}}$
At first, \begin{cases} \cos\left(x+\frac{4\pi}3\right) = \cos\left(x-\frac{2\pi}3\right)\\[4pt] \sin\left(x+\frac{4\pi}3\right) = \sin\left(x-\frac{2\pi}3\right)\tag1 \end{cases} Denote \begin{cases} c= \cos x,\quad s=\sin x,\\[4pt] \mathcal S_k(f(t),x)=f^k\left(x-\frac{2\pi}3\right) +f^k(x) +f^k\left(x+\frac{2\pi}3\right)\\[4pt] \mathcal Q_k(f(t),x)=f^k\left(x-\frac{2\pi}3\right)f^k(x) +f^k(x)f^k\left(x+\frac{2\pi}3\right)\\[4pt] \mspace{93mu}+f^k\left(x+\frac{2\pi}3\right)f^k\left(x-\frac{2\pi}3\right)\\[4pt] \mathcal P_k(f(t),x)=f^k\left(x-\frac{2\pi}3\right) f^k(x) f^k\left(x+\frac{2\pi}3\right).\tag2 \end{cases} Since $$\cos\frac{2\pi}3 = -\frac12,\quad \sin\frac{2\pi}3 = \frac{\sqrt3}2,$$ then $$\cos\left(x\pm\frac{2\pi}3\right) = -\frac c2\mp\frac{s\sqrt3}2,\quad \sin\left(x\pm\frac{2\pi}3\right) = -\frac s2\pm\frac {c\sqrt3}2.\tag3$$ Applying $(3),$ easily to get
\begin{align} &\mathcal S_1(\cos t,x) = \cos\left(x-\frac{2\pi}3\right)+\cos x +\cos\left(x+\frac{2\pi}3\right)\\ & = -\frac c2+\frac{s\sqrt3}2\,+c\,-\frac c2-\frac{s\sqrt3}2 = 0,\\[4pt] &\mathcal Q_1(\cos t,x) = \cos\left(x-\frac{2\pi}3\right)\cos x + \cos x \cos\left(x+\frac{2\pi}3\right)+\cos\left(x+\frac{2\pi}3\right)\cos\left(x-\frac{2\pi}3\right)\\ &= c\left(-\frac c2+\frac{s\sqrt3}2-\frac c2-\frac{s\sqrt3}2\right) +\left(-\frac c2-\frac{s\sqrt3}2\right)\left(-\frac c2+\frac{s\sqrt3}2\right)\\ &= -\cos^2 x+\frac14\cos^2x-\frac34\sin^2x = -\frac34,\\[4pt] &\mathcal P_1(\cos t,x) = \cos\left(x-\frac{2\pi}3\right)\cos x \cos\left(x+\frac{2\pi}3\right) = \left(-\frac c2+\frac{s\sqrt3}2\right)\,c\, \left(-\frac c2-\frac{s\sqrt3}2\right)\\ & = \frac14(\cos^3x-3\cos x\sin^2 x) = \frac14\Re(\cos x + i\sin x)^3 = \frac14\cos 3x. \end{align}
At the same time, $$\sin x = \cos\left(x-\frac\pi2\right),\tag4$$ and then \begin{align} &\mathcal S_k(\sin t,x) = \sin^k\left(x-\frac{2\pi}3\right)+\sin^k x +\sin^k\left(x+\frac{2\pi}3\right) = \mathcal S_k\left(\cos t,x-\frac\pi2\right) ,\\[4pt] &\mathcal Q_k(\sin t,x) = \sin^k\left(x-\frac{2\pi}3\right)\sin^k x + \sin^k x \sin^k\left(x+\frac{2\pi}3\right)\\[4pt] &+\sin^k\left(x+\frac{2\pi}3\right)\sin^k\left(x-\frac{2\pi}3\right) =\mathcal Q_k\left(\cos t,x-\frac\pi2\right),\\ &\mathcal P_k(\sin t,x) = \sin^k\left(x-\frac{2\pi}3\right)\sin^k x \sin^k\left(x+\frac{2\pi}3\right) = \mathcal P_k\left(\cos t,x-\frac\pi2\right).\\[4pt] \end{align}
On the other hand, \begin{cases} \cos x \sin x = \frac12\sin(2x)\\[4pt] \cos\left(x-\frac{2\pi}3\right) \sin \left(x-\frac{2\pi}3\right) = \frac12\sin\left(2x-\frac{4\pi}3\right) = \frac12\sin\left(2x+\frac{2\pi}3\right)\\[4pt] \cos\left(x+\frac{2\pi}3\right) \sin \left(x+\frac{2\pi}3\right) = \frac12\sin\left(2x+\frac{4\pi}3\right) = \frac12\sin\left(2x-\frac{2\pi}3\right).\tag5 \end{cases}
then \begin{align} &\mathcal S_k(\cos t \sin t, x) = \cos^k\left(x-\frac{2\pi}3\right)\, \sin^k\left(x-\frac{2\pi}3\right)+ \cos^k x\, \sin^k x\\ & + \cos^k\left(x+\frac{2\pi}3\right)\, \sin^k\left(x+\frac{2\pi}3\right)\\ &=\frac1{2^k}\left(\sin^k\left(2x+\frac{2\pi}3\right)+ \sin^k 2x + \sin^k\left(2x-\frac{2\pi}3\right)\right) = \frac1{2^k}\mathcal S_k(\sin t,2x),\\[4pt] &\mathcal Q_k(\cos t \sin t,x) = \cos^k\left(x-\frac{2\pi}3\right)\, \sin^k\left(x-\frac{2\pi}3\right) \cos^k x\, \sin^k x\\ & + \cos^k x\, \sin^k x \cos^k\left(x+\frac{2\pi}3\right)\, \sin^k\left(x+\frac{2\pi}3\right)\\ & + \cos^k\left(x+\frac{2\pi}3\right)\, \sin^k\left(x+\frac{2\pi}3\right)\cos^k\left(x-\frac{2\pi}3\right)\, \sin^k\left(x-\frac{2\pi}3\right)\\ &=\frac1{4^k}\left(\sin^k\left(2x+\frac{2\pi}3\right)\sin^k 2x + \sin^k 2x \sin^k\left(2x-\frac{2\pi}3\right)\right.\\ &\left.+ \sin^k\left(2x-\frac{2\pi}3\right)\sin^k\left(2x+\frac{2\pi}3\right)\right)\\ & = \frac1{4^k}\mathcal Q_{k}(\sin t,2x),\\[4pt] &\mathcal P_{k}(\cos t \sin t,x) = \cos^k\left(x-\frac{2\pi}3\right)\, \sin^k\left(x-\frac{2\pi}3\right) \cos^k x\, \sin^k x\\ &\times\cos^k\left(x+\frac{2\pi}3\right)\, \sin^k\left(x+\frac{2\pi}3\right)\\ &=\frac1{8^k}\sin^k\left(2x+\frac{2\pi}3\right)\sin^k 2x \sin^k\left(2x-\frac{2\pi}3\right) = \frac1{8^k}\mathcal P_{k}(\sin t, 2x). \end{align}
Therefore, \begin{cases} \mathcal S_1(\cos t, x)=0\\ \mathcal Q_1(\cos t, x) = -\frac34\\ \mathcal P_1(\cos t, x) = \frac14\cos3x\\ \mathcal S_k(\sin t, x) = \mathcal S_k\left(\cos t,x-\frac\pi2\right)\\[4pt] \mathcal Q_k(\sin t, x) = \mathcal Q_k\left(\cos t,x-\frac\pi2\right)\\[4pt] \mathcal P_k(\sin t, x) = \mathcal P_k\left(\cos t,x-\frac\pi2\right)\\[4pt] \mathcal S_k(\cos t \sin t, x) = \frac1{2^k}\mathcal S_k(\sin t,2x)\\[4pt] \mathcal Q_k(\cos t \sin t, x) = \frac1{4^k}\mathcal Q_k(\sin t,2x)\\[4pt] \mathcal P_k(\cos t \sin t, x) = \frac1{8^k}\mathcal P_k(\sin t,2x).\tag6 \end{cases}
$\color{brown}{\textbf{Calculation of sums.}}$
$\mathcal S_1(\cos t, x),\ \mathcal Q_1(\cos t, x),\ \mathcal P_1(\cos t, x)\ $ can be considered as the elementary symmetric polynomials. In this way,
If $f(t) = \cos t,$ then $$\begin{align} &\mathcal S_2 = \mathcal S_1^2 - 2\mathcal Q_1 = \frac32,\\ &\mathcal Q_2 = \mathcal Q_1^2 - 2\mathcal S_1 \mathcal P_1 = \frac9{16},\\ &\mathcal S_4 = \mathcal S_2^2 - 2\mathcal Q_2 = \frac98. \end{align}\tag7$$ Formulas $(6)-(7)$ allow to fill the table $(8).$
Besides, $$\begin{align} &\mathcal P_2(\cos t, x) + \mathcal P_2(\sin t, x)\\ &= \cos^2\left(x-\frac{2\pi}3\right)\cos^2 x \cos^2\left(x+\frac{2\pi}3\right)+\sin^2\left(x-\frac{2\pi}3\right)\sin^2 x \sin^2\left(x+\frac{2\pi}3\right) =\frac1{16}. \end{align}$$
\begin{vmatrix} k & f(t) & \mathcal S_k(f(t),x) & \mathcal Q_k(f(t),x) & \mathcal P_k(f(t),x)\\ 1 & \cos t & 0 & -\dfrac34 & \dfrac14\cos 3x\\ 1 & \sin t & 0 & -\dfrac34 & -\dfrac14\sin 3x\\ 1 & \cos t\sin t & 0 & -\dfrac3{16} & -\dfrac1{32}\sin 6x\\ 2 & \cos t & \dfrac 32 & \dfrac9{16} & \dfrac1{16}\cos^2 3x\\ 2 & \sin t & \dfrac 32 & \dfrac9{16} & \dfrac1{16}\sin^2 3x\\ 2 & \cos t\sin t & \dfrac 38 & \dfrac9{256} & \dfrac1{1024}\sin^2 6x\\ 4 & \cos t & \dfrac98 & & \\ 4 & \sin t & \dfrac98 & & \\ 4 & \cos t\sin t & \dfrac9{128} & & \tag8 \end{vmatrix}
Any function which depends only from the considered constant polynomials, should be a constant too.
In particular, for the considered functions $f(t)$ $$\mathcal P_k = \mathcal P_1^k,\\ \mathcal S_3 - 3\mathcal P_3 = \mathcal S_1^3 - 3\mathcal S_1\mathcal Q_1 = 0.$$