Notes on Mechanics of General Physics
Statics, the study of (mechanical) equilibrium and its relation to forces.
Kinematics, the study of motion (position, velocity, acceleration).
Historically, the study of motion and its relation to forces has been called kinetics. The term has largely been superseded by analytical dynamics, or simply dynamics.
Newton’s law includes nonconservative forces. It is only right non-relativistically.
Case studies:
The fundamental laws in theoretical physics can be put in the form of a principle of stationary action.
Principle of stationary action (平稳作用量原理): The evolution of a system between two specified states at two specified times is a stationary point of the action functional. \( \mathcal{S}: \mathbf{q}(t) \rightarrow \int_{t_1}^{t_2} \mathcal{L}(\mathbf{q},\dot{\mathbf{q}},t) \mathrm{d}t \). \[ \frac{\delta \mathcal{S}}{\delta \mathbf{q}(t)}=0 \]
Hamilton's Principle is Hamilton's formulation of the Principle of Stationary Action for classical mechanics, where the Lagrangian is the kinetic energy minus the potential energy. \( \mathcal{L} = \text{KE}-\text{PE} \)
Generalized coordinates, generalized velocities, and Lagrange's equations: Notes from Intermediate Classical Mechanics
\[ \frac{d}{dt} \frac {\partial L}{\partial \dot{q}} = \frac {\partial L}{\partial q} \]
Canonical coordinates, canonical momenta, and Hamilton's equations: Notes from Advanced Dynamics
\[ \mathrm{d}\mathcal{H} = -\dot{p} \mathrm{d}q + \dot{q} \mathrm{d}p + \frac{\partial \mathcal{H}}{\partial t} \mathrm{d}t \]
The Hamiltonian \( \mathcal{H}(q,p,t) \) is the Legendre transform of the Lagrangian \( \mathcal{L}(q,\dot{q},t) \), while the coordinates and time are held constant and the canonical momenta are conjugate to the generalized velocities.
\[ \mathcal{H} + \mathcal{L} = p \dot{q} \]
Advantages of Hamiltonian mechanics over Lagrangian mechanics: