Then at the critical point, t'(x)=\dfrac{1}{c_1}\dfrac{x}{\sqrt{h_1^2+x^2}}-\dfrac{1}{c_2}\dfrac{a-x}{\sqrt{h_2^2+(a-x)^2}}=0.
Now comes the surprising moment: \dfrac{x}{\sqrt{h_1^2+x^2}}=\sin \alpha_1,\quad \dfrac{x}{\sqrt{h_1^2+x^2}}=\sin \alpha_2.
This actually gives us \dfrac{\sin \alpha_1}{c_1}=\dfrac{\sin \alpha_2}{c_2}
or \dfrac{\sin \alpha_1}{\sin \alpha_2}=\dfrac{c_1}{c_2},
which is Snell's law. In words, it says that when the sines of the angles in the different media are in the same proportion as the propagation velocities, the time of travel from A_1 to A_2 is minimised.
Reference:
Mathematical Analysis I by Vladimir A. Zorich
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