[Math] Spherical Trigonometry: Spherical triangle

spherical-geometry

ABC is an equilateral spherical triangle in which small displacements are made, in the sides and angles, of such a nature that the triangle remains equilateral. Prove that
$$
\frac{da}{dA} = \cos\left({\frac{A}{2}}\right) \cot\left({\frac{a}{2}}\right)
$$

I would have mentioned my progress. But all I have been able to done is differentiate different trigonomeric formulae to get an expression which is of no use to simplify, since it never matches with answer on a numerical verification.

Please help. A hint on how to start might be enough.

NOTE: This question is Q9 of Execrcise 1 from W.M. Smart's Spherical Astronomy.

Best Answer

I don’t believe the formula is correct as quoted.

We’re dealing with an equilateral (and equiangular!) spherical triangle, and to avoid (my own) confusion, I’ll call the side-length $s$ and the angle $\theta$. Both are angles, of course. The most obvious thing is to bisect the triangle into two right triangles, each with hypotenuse $s$ and one side $s/2$, this latter side being opposite the angle $\theta/2$, while the other angle of the triangle is still $\theta$.

Now, one of the standard formulas for right spherical triangles is $$ \cos c=\cot A\cot B\,, $$ and for us, $c=s$, $A=\theta$, $B=\theta/2$. So we differentiate our relation $\cos s=\cot\theta\cot(\theta/2)$, and get \begin{align} -\sin s\frac{ds}{d\theta}&=-\cot\theta\csc^2(\theta/2)\cdot\frac12 -\csc^2\theta\cot(\theta/2)\\ \frac{ds}{d\theta}&=\frac{\frac12\cot\theta\csc^2(\theta/2)+\csc^2\theta\cot(\theta/2)}{\sin s}\,. \end{align} Now let’s test this out on the nicest possible equilateral triangle, the one whose sides and angles are both $90^\circ$. Here, the first term in the numerator drops out, ’cause $\cot90^\circ=0$, but everything else evaluates to $1$, and so even $ds/d\theta=1$ at this test-point. Yet, the formula evaluates to $\sqrt2/2$, unequal to $1$.

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