MHB How is the Equation Derived for an Isosceles Triangle with a specific Angle?

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The discussion focuses on deriving the equation for an isosceles triangle with given sides and angle. Starting with triangle $PQR$, where $QR = m$, $PQ = PR = n$, and $\angle P = \frac{\pi}{7}$, the relationship $\sin\left(\frac{\pi}{14}\right) = \frac{m}{2n}$ is established. Utilizing the Chebyshev polynomial, the equation $\sin(7\theta) = 1$ leads to a polynomial in terms of $\sin\left(\frac{\pi}{14}\right)$. This results in the equation $m^4 - 3m^2n^2 - mn^3 + n^4 = 0$, confirming the derived relationship for the triangle's dimensions. The solution is recognized as elegant and mathematically satisfying.
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Given a triangle $PQR$ where $QR=m$, $PQ=PR=n$ and $\angle P=\dfrac{\pi}{7}$.

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Show that $m^4-3m^2n^2-mn^3+n^4=0$.
 

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[sp]Half the angle at $P$ is $\dfrac{\pi}{14}$. The triangle is isosceles, so it follows that $\sin\Bigl(\dfrac\pi{14}\Bigr) = \dfrac{m/2}n = \dfrac m{2n}.$

If $\theta = \frac\pi{14}$ then $\sin(7\theta) = 1.$ But if $s = \sin\theta$ then $\sin(7\theta) = 7s - 56s^3 + 112s^5 - 64s^7$ (using the Chebyshev polynomial $T_7(s)$). So the equation $\sin(7\theta) = 1$ can be written as $64s^7 - 112s^5 + 56s^3 - 7s + 1 = 0$. That can be factored as $$\begin{aligned} 0 &= 64s^7 - 112s^5 + 56s^3 - 7s + 1\\ &= (s+1)(64s^6 - 64s^5 - 48s^4 + 48s^3 + 8s^2 - 8s + 1) \\ &= (s+1)(8s^3 - 4s^2 - 4s + 1)^2.\end{aligned}$$ So if $\sin(7\theta) = 1$ but $s\ne-1$ then $8s^3 - 4s^2 - 4s + 1 = 0.$

Now put $s = \sin\bigl(\frac\pi{14}\bigr) = \frac m{2n}$ to see that $$ 0 = 8s^3 - 4s^2 - 4s + 1 = \frac{8m^3}{8n^3} - \frac{4m^2}{4n^2} - \frac{4m}{2n} + 1 = \frac{m^3 - m^2n - 2mn^2 + n^3}{n^3},$$ and therefore $m^3 - m^2n - 2mn^2 + n^3 = 0.$ Finally, multiply that by $m+n$ to see that $0 = (m+n)(m^3 - m^2n - 2mn^2 + n^3) = m^4 - 3m^2n^2 - mn^3 + n^4.$[/sp]
 
Opalg said:
[sp]Half the angle at $P$ is $\dfrac{\pi}{14}$. The triangle is isosceles, so it follows that $\sin\Bigl(\dfrac\pi{14}\Bigr) = \dfrac{m/2}n = \dfrac m{2n}.$

If $\theta = \frac\pi{14}$ then $\sin(7\theta) = 1.$ But if $s = \sin\theta$ then $\sin(7\theta) = 7s - 56s^3 + 112s^5 - 64s^7$ (using the Chebyshev polynomial $T_7(s)$). So the equation $\sin(7\theta) = 1$ can be written as $64s^7 - 112s^5 + 56s^3 - 7s + 1 = 0$. That can be factored as $$\begin{aligned} 0 &= 64s^7 - 112s^5 + 56s^3 - 7s + 1\\ &= (s+1)(64s^6 - 64s^5 - 48s^4 + 48s^3 + 8s^2 - 8s + 1) \\ &= (s+1)(8s^3 - 4s^2 - 4s + 1)^2.\end{aligned}$$ So if $\sin(7\theta) = 1$ but $s\ne-1$ then $8s^3 - 4s^2 - 4s + 1 = 0.$

Now put $s = \sin\bigl(\frac\pi{14}\bigr) = \frac m{2n}$ to see that $$ 0 = 8s^3 - 4s^2 - 4s + 1 = \frac{8m^3}{8n^3} - \frac{4m^2}{4n^2} - \frac{4m}{2n} + 1 = \frac{m^3 - m^2n - 2mn^2 + n^3}{n^3},$$ and therefore $m^3 - m^2n - 2mn^2 + n^3 = 0.$ Finally, multiply that by $m+n$ to see that $0 = (m+n)(m^3 - m^2n - 2mn^2 + n^3) = m^4 - 3m^2n^2 - mn^3 + n^4.$[/sp]

What a beautiful solution it is, Mr. Opalg! (Sun)(Clapping)

My solution:

My solution used the "identity" that states $\cos \dfrac{\pi}{7}+\cos \dfrac{3\pi}{7}+\cos \dfrac{5\pi}{7}=\dfrac{1}{2}$.

By applying the Cosine Rule to the triangle $PQR$, we get:

$\cos \dfrac{\pi}{7}=\dfrac{2n^2-m^2}{2n^2}$,

$\cos \dfrac{3\pi}{7}=\dfrac{m}{2n}$ and finally,

$\cos \dfrac{5\pi}{7}=\cos \left( \pi-\dfrac{2\pi}{7} \right)=-\cos \dfrac{2\pi}{7}=-\left( 2\cos^2 \dfrac{\pi}{7}-1 \right)=1-2\left(\dfrac{2n^2-m^2}{2n^2} \right)^2$

Now, by adding these three we get:

$\dfrac{2n^2-m^2}{2n^2}+\dfrac{m}{2n}+1-2\left(\dfrac{2n^2-m^2}{2n^2} \right)^2=\dfrac{1}{2}$

and simplifying these we get:

$m^4-3m^2n^2-mn^3+n^4=0$

But I'm not sure if I have to show how does one get the identity of $\cos \dfrac{\pi}{7}+\cos \dfrac{3\pi}{7}+\cos \dfrac{5\pi}{7}=\dfrac{1}{2}$ before using it or it's a well-known identity that one can just refer to it when needed...
 
Insights auto threads is broken atm, so I'm manually creating these for new Insight articles. In Dirac’s Principles of Quantum Mechanics published in 1930 he introduced a “convenient notation” he referred to as a “delta function” which he treated as a continuum analog to the discrete Kronecker delta. The Kronecker delta is simply the indexed components of the identity operator in matrix algebra Source: https://www.physicsforums.com/insights/what-exactly-is-diracs-delta-function/ by...

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