For an infinitesimal continuous symmetry δqi=εξi(q,t), allow the Lagrangian to change by a total derivative, δL=εdF/dt. Direct variation givesOn a solution of the Euler-Lagrange equations, the first term vanishes. This proves Noether's theorem in the fixed-time form:Spatial translations yield total momentum, and rotations yield angular momentum. Time translations yield energy when the Lagrangian has no explicit time dependence; this follows either from the extended time-transformation form of the theorem or by differentiating H=∑ipiq˙i−L to obtain H˙=−∂L/∂t.
εδL=∑i(∂qi∂L−dtd∂q˙i∂L)ξi+dtd∑ipiξi.
Q=i∑piξi−F,Q˙=0.
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