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Chapter 13 - Hamiltonian Mechanics

Section 13.1 - The Basic Variables

Definition. Consider a Laplacian defined as \mathcal{L} = \mathcal{L}(q_1, \ldots, q_n, \dot{q}_1, \ldots, \dot{q}_n, t). Then, the set of coordinates q_1, \ldots, q_n are the configuration space while the set of coordinates q_1, \ldots, q_n, \dot{q}_1, \ldots, \dot{q}_n are known as the state space.

Recall that the generalized momenta p_i is also defined such that

p_i = \frac{\partial \mathcal{L}}{\partial \dot{q}_i}

Definition. The generalized momenta is also called the canonical momentum or the momentum conjugate to $q_i$.

Definition. The Hamiltonian is defined as

\mathcal{H} = \sum_{i = 1}^n p_i \dot{q_i} - \mathcal{L}

Section 13.2 - Hamilton's Equations for One-Dimensional Systems

Section 13.3 - Hamilton's Equations in Several Dimensions

Section 13.4 - Ignorable Coordinates

Section 13.5 - Lagrange's Equations vs. Hamilton's Equations

Section 13.6 - Phase-Space Orbits

Section 13.7 - Lioville's Theorem