Showing Rigid Rotor Microstates with Angular Momentum ≤ M

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Homework Help Overview

The problem involves evaluating the number of microstates available to a rigid rotor with angular momentum less than or equal to M, specifically through the integration of phase space volume. The subject area pertains to statistical mechanics and angular momentum in quantum systems.

Discussion Character

  • Exploratory, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • The original poster attempts to integrate a defined volume in phase space but notes a discrepancy in their result, questioning the limits of integration for the variable pφ. Other participants engage by clarifying the fixed nature of pθ during integration and exploring the implications of angular momentum components being negative.

Discussion Status

The discussion is ongoing, with participants providing guidance on the integration limits and questioning assumptions about the angular momentum components. There is a recognition of the need to clarify the integration setup without reaching a consensus on the specific limits.

Contextual Notes

Participants express uncertainty regarding the limits of integration for pφ and the implications of angular momentum being non-negative. The original poster also indicates difficulty in expressing equations clearly, which may affect the clarity of the discussion.

halley00
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Homework Statement


By evaluating the "volume" of the relevant region of its phase space, show that the number of microstates available to a rigid rotor with angular momentum less or equal to M is (M/ħ)2.

Homework Equations


Consider the motion in the variables θ and φ, with M^{2}=(p_{θ})2+{p_{φ}/{sin(θ)}2.

The Attempt at a Solution


I just integrated the "volume": (1/h²)∫0πdθ∫0dφ∫0Mdpθ0Msinθdpφ,

For some reason I'm missing a π. Why? I'm getting a "volume" 4π(M/h)2
Maybe I'm making a mistake in the choice of the limits of integration.

Sorry, I don't know how to write the equations in clean way.
 
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Hello. Welcome to PF!

Note that while integrating over ##p_\phi##, the variable ##p_{\theta}## is fixed at some value. Using the relation ##M^2 = p_{\theta}^2 +\frac{ p_{\phi}^2}{\sin^2 \theta}##, what are the limits for the integration over ##p_{\phi}##?

(Can the angular momenta components ##p_\theta## and ##p_\phi## be negative?)
 
No angular momentum can't be negative so those components can't be negative either. But I don't know what the limits for p_phi are supposed to be. (I'm also having trouble with this problem.)
 
Met119 said:
No angular momentum can't be negative so those components can't be negative either. But I don't know what the limits for p_phi are supposed to be. (I'm also having trouble with this problem.)
The components of angular momentum can be negative as well as positive.

For the limits of integration, it might help to consider a simpler, but similar, problem. Suppose you have a single particle moving in two dimensions. In Cartesian coordinates the magnitude of linear momentum, p, is related to the components of momentum, px and py, by

p2 = px2 + py2.

Suppose you want to integrate over the momentum portion of phase space to get the "volume" corresponding to all momentum values 0 < p < P0. How would you choose the limits of integration in ∫dpy ∫dpx?
 

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