Geodesics on Surfaces: Proving the Relationship to Particle Motion

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To prove that a particle constrained to a surface f(x,y,z)=0 moves along the surface's geodesic when no forces are acting, one must show that the particle's path and the geodesic share the same mathematical expression. The geodesic can be expressed as an integral involving the particle's speed, which remains constant due to the absence of forces. The path of the particle is derived from the Euler-Lagrange equations, indicating that the dynamics are governed by the Lagrangian. The discussion highlights the need to connect these two formulations to complete the proof. Further guidance is sought on how to proceed with the derivation.
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Homework Statement


Prove that a particle constrained to move on a surface f(x,y,z)=0 and subject to no forces, moves along the geodesic of the surface.


Homework Equations





The Attempt at a Solution


OK, we should prove that the path the particle takes and the geodesic are given by the same expression.

For the geodesic:
\int dt=\int\frac{ds}{v}=\int\frac{\sqrt{dx^2+dy^2+dz^2}}{v}
v must be constant since there are no forces - components of v may change along the path, but the speed will remain the same.

Now for the path:
\frac{d}{dt}\frac{\partial L}{\partial \dot{x}}=\frac{\partial L}{\partial x}
etc.

But where from now on??
 
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