Hamiltonian: Definition, Equations & Explanation

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SUMMARY

The Hamiltonian is a function that summarizes equations of motion and represents the total energy of a system, applicable in both classical and quantum mechanics. It is derived from the Lagrangian by defining canonical momentum \( p_a(t) \) for each coordinate \( q_a(t) \) using the equation \( p_a = \frac{\partial L}{\partial \dot q_a} \). The Hamiltonian is expressed as \( H = \left(\sum_a p_a \dot q_a \right) - L \) and is governed by Hamilton's equations of motion: \( \dot q_a = \frac{\partial H}{\partial p_a} \) and \( \dot p_a = - \frac{\partial H}{\partial q_a} \). Notably, if the Hamiltonian lacks explicit time dependence, it remains constant over time.

PREREQUISITES
  • Understanding of Lagrangian mechanics
  • Familiarity with canonical coordinates and momenta
  • Knowledge of classical mechanics principles
  • Basic concepts of quantum mechanics
NEXT STEPS
  • Study the derivation of the Lagrangian for various physical systems
  • Explore Hamilton's equations in detail
  • Learn about the implications of time independence in Hamiltonian systems
  • Investigate applications of the Hamiltonian in quantum mechanics
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Students and professionals in physics, particularly those focusing on mechanics, theoretical physicists, and anyone interested in the mathematical foundations of energy systems.

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Definition/Summary

The Hamiltonian, like the Lagrangian, is a function that summarizes equations of motion. It has the additional interpretation of giving the total energy of a system.

Though originally stated for classical mechanics, it is also an important part of quantum mechanics.

Equations

Start from the Lagrangian and define a canonical momentum p_a(t) for each canonical coordinate q_a(t):
p_a = \frac{\partial L}{\partial \dot q_a}

The Hamiltonian is given by
\left(\sum_a p_a \dot q_a \right) - L

Hamilton's equations of motion are
\dot q_a = \frac{\partial H}{\partial p_a}
\dot p_a = - \frac{\partial H}{\partial q_a}

The Hamiltonian has the interesting property that
\dot H = \frac{\partial H}{\partial t}

meaning that if the Hamiltonian has no explicit time dependence, it is a constant of the motion.

Extended explanation

To illustrate the derivation of the Hamiltonian, let us start with the Lagrangian for a particle with Newtonian kinetic energy and potential energy V(q):
L = T - V

where
T = \frac12 m \left( \frac{dq}{dt} \right)^2

For canonical coordinate q, we find canonical momentum p:
p = m \frac{dq}{dt}

and from that, we find the Hamiltonian:
H = T + V

where the kinetic energy is now given by
T = \frac{p^2}{2m}

* This entry is from our old Library feature. If you know who wrote it, please let us know so we can attribute a writer. Thanks!
 
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Thanks for sharing this useful information! I didn't know that the Hamiltonian is a function which summarizes equations of motion and gives the total energy of a system. It's great to learn the equations and extended explanation to understand it better.
 
I do not have a good working knowledge of physics yet. I tried to piece this together but after researching this, I couldn’t figure out the correct laws of physics to combine to develop a formula to answer this question. Ex. 1 - A moving object impacts a static object at a constant velocity. Ex. 2 - A moving object impacts a static object at the same velocity but is accelerating at the moment of impact. Assuming the mass of the objects is the same and the velocity at the moment of impact...

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