2.2 Energy and Conserved Vectors
For a phase point \(z = (q, p)\), define:
\[ H(q,p) = \frac{\| p\| ^2}{2m} - \frac{\mu }{\| q\| }, \qquad L = q \times p, \qquad A = p \times L - \frac{m\mu }{\| q\| }q. \]
Here \(H\) is the total energy (kinetic minus potential), \(L\) is the angular momentum vector, and \(A\) is the Laplace–Runge–Lenz vector. All three are proved constant along every non-collision solution in Chapter 4.