PX285 - D3 - the conservation of energy
- taking
, the hamiltonian is defined as:
for a system is usually defined as energy, - therefore, the conservation for energy is stated as:
- if energy is conserved,
, ie: is a constant of motion:
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constant energy is also defined as 'an integral of the motion'
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this only contains the first-order time derivatives of the coordinates, whereas the euler-lagrange equation is second-order
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a none on notation:
is used, in place of , because it is reserved for the expression of energy in terms of coordinates stands for the constant value it keeps