query: Information contained in Lagrangians and actions
positive_passages.docid: 24896
positive_passages.text: The meaning of action
negative_passages.docid: 82166
negative_passages.text: How are constraint forces represented in Lagrangian mechanics?
negative_passages.docid: 90626
negative_passages.text: Work in circular motions
negative_passages.docid: 72721
negative_passages.text: Do an action and its Euler-Lagrange equations have the same symmetries?
negative_passages.docid: 56446
negative_passages.text: A kind of converse of Lagrange's Theorem
negative_passages.docid: 87125
negative_passages.text: Does action really have to be Lorentz-invariant in SR?
negative_passages.docid: 146853
negative_passages.text: Do we need inertial frames in Lagrangian mechanics?
negative_passages.docid: 3603
negative_passages.text: Lagrangian and Hamiltonian EOM with dissipative force
negative_passages.docid: 27016
negative_passages.text: Is the Lagrangian density a functional or a function?
negative_passages.docid: 150081
negative_passages.text: Deriving Lagrangian density for electromagnetic field
negative_passages.docid: 46053
negative_passages.text: How to find Hamiltonian from this simple Lagrangian? (tricky)
negative_passages.docid: 69199
negative_passages.text: How to find the continuous transformations which leave the action invariant?
negative_passages.docid: 25728
negative_passages.text: A second isomorphism theorem for action on cosets
negative_passages.docid: 103613
negative_passages.text: Two Claims about Symplectic Group Actions
negative_passages.docid: 68422
negative_passages.text: Understanding Lagrange's Theorem (Group Theory)
negative_passages.docid: 28946
negative_passages.text: Derivation of Spin Lagrangian
negative_passages.docid: 12175
negative_passages.text: Applying the principle of equivalence to an accelerated frame