Assume is differentiable along the ray, with sufficient regularity for the following variation, and fix the endpoints. Fermat principle makes the travel time stationary:
For the variational integrand , the Euler-Lagrange equation is
Expanding the derivative and multiplying by gives
and therefore
Equivalently, the Beltrami identity gives . Mere continuity of , as stated in the wording, does not by itself justify the appearance of ; the displayed classical ray equation requires this additional differentiability.

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