Hamiltonian in spherical coordinates

In summary, the conversation discusses the use of spherical coordinates to describe the dynamics of a free particle in a three-dimensional space. It is mentioned that the Hamiltonian in this system includes terms related to both linear and angular momenta. The reason for this is explained to be the rotational symmetry of the space, with rotations corresponding to angles and points corresponding to circles and spheres. The question of why the kinetic energy in the Hamiltonian is not expressed in terms of linear momenta in spherical coordinates is also raised, with the answer being related to the presence of rotational symmetry. The conversation ends with a request for more information on the specific area of mathematics or physics related to this topic.
  • #1
Syrus
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Homework Statement



The total energy may be given by the hamiltonian in terms of the coordinates and linear momenta in Cartesian coordinates (that is, the kinetic energy term is split into the familiar pi2/2m. When transformed to spherical coordinates, however, two terms are angular momentum terms.

Why do these angular componenets arise, and how come it is not possible to derive this expression in terms of linear momentum in spherical coordinates. In other words, if we resolve the velocity in terms of, say, θ by taking the time derivative of the position vector in spherical coordinates and dotting it with the θ unit vector, and then multiply this velocity by m and do the same for the r and phi components, the outcome is not the same as that of the Hamiltonian transformed in terms of the angular momenta.

Can anyone elaborate on this peculiarity?

Homework Equations





The Attempt at a Solution

 
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  • #2
My point, hopefully correct and helpful, is:

That the space (R^3) or the dynamics of a free pointlike particle in such an infinite space is rotationally invariant (or isotropic) is best exhibited in spherical coordinates, a generalization to 3 dimensions of the plane polar coordinates which can be used to describe R^2 or free dynamics in R^2. It's just the connection: rotation -> angle and point -> circle -> sphere -> hypersphere (for at least 4 dimensions). R^2 is the disk of infinite radius, R^3 is the ball with infinite radius. This fact sets the Hamiltonian to be rotationally invariant, hence it commutes (in the Poisson bracket) with the generator of rotations, the orbital angular momentum. Under rotations of coordinate axis (or rotation of inertial observers) energy is conserved.

There's no coincidence that a space (time) with rotational symmetry has 2,3,... observables hidden in it. We don't see them in cartesian coordinates, since there's no natural description of rotations in cartesian coordinates.
 
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  • #3
Dex, thank you for your response. Can you tell me what specific area of mathetmatics or physics I should search for more detail?

Perhaps the question I wish to satisfy is: what is the theta (extend this to include r and phi) component of the linear velocity of a particle in spherical coordinates? Once we have these velocities, why is the kinetic energy in the hamiltonian not expressed in terms of these linear momenta (rather than their angular analogues)?
 

Related to Hamiltonian in spherical coordinates

1. What is the Hamiltonian in spherical coordinates?

The Hamiltonian in spherical coordinates is a mathematical expression that describes the total energy of a particle in a three-dimensional space. It takes into account the particle's kinetic energy and potential energy, and is an important concept in classical mechanics and quantum mechanics.

2. How is the Hamiltonian in spherical coordinates different from Cartesian coordinates?

In spherical coordinates, the Hamiltonian takes into account the radial distance, polar angle, and azimuthal angle of a particle, while in Cartesian coordinates, it only takes into account the particle's position in the x, y, and z directions. This makes the Hamiltonian in spherical coordinates more suitable for systems with spherical symmetry.

3. What is the physical significance of the Hamiltonian in spherical coordinates?

The Hamiltonian in spherical coordinates represents the total energy of a particle in a three-dimensional space. It is a fundamental concept in physics and is used in various fields such as classical mechanics, quantum mechanics, and electromagnetism.

4. How is the Hamiltonian in spherical coordinates derived?

The Hamiltonian in spherical coordinates can be derived from the Lagrangian function, which describes the dynamics of a system in terms of generalized coordinates and their time derivatives. By using the Lagrangian function, one can obtain the equations of motion for the system, and from these equations, the Hamiltonian can be derived.

5. Can the Hamiltonian in spherical coordinates be used for all kinds of systems?

Yes, the Hamiltonian in spherical coordinates can be used for all kinds of systems, as long as they have spherical symmetry. This includes systems such as planetary orbits, atoms, and molecules. However, for systems without spherical symmetry, a different coordinate system may be more suitable for describing the dynamics of the system.

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