L=0 State: Understanding Angular Momentum and Orbital Movement

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Discussion Overview

The discussion revolves around the classical analog of the l=0 state in angular momentum, exploring the implications of zero angular momentum in both classical and quantum mechanics. Participants examine the nature of orbits, force balances, and the behavior of particles in a centrosymmetric potential.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant questions what kind of orbits correspond to an l=0 state, noting that angular momentum is zero.
  • Another participant argues that classically, an orbit with zero angular momentum cannot exist, referencing the Bohr model and the relationship between angular momentum and radius.
  • A participant observes that the l=0 state highlights significant differences between classical and quantum mechanics.
  • Some participants propose that in a centrosymmetric potential, a particle with zero angular momentum moves along a line of constant angle, potentially passing through the center, which they argue is not classically forbidden.
  • There is a discussion about the behavior of particles in quantum mechanics, including superpositions of paths and the undetermined angle phi.
  • One participant raises a question about the implications of nuclear size on electron speed, suggesting that the electrostatic attraction could lead to speeds exceeding that of light.
  • Another participant counters that relativistic effects must be considered, specifically mentioning the Dirac equation near the nucleus.

Areas of Agreement / Disagreement

Participants express differing views on the implications of zero angular momentum in classical versus quantum contexts. There is no consensus on whether the behavior of particles in this state is classically forbidden or how to reconcile classical and quantum perspectives.

Contextual Notes

The discussion includes assumptions about classical mechanics and quantum mechanics that may not be universally accepted, such as the treatment of angular momentum and the implications of particle behavior in a centrosymmetric potential.

quantum123
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What is the classical analog for l=0 state?
Angular momentum = 0 , what kind of orbits is that?
 
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Classically you cannot have an orbit with zero angular momentum. Consider a non-quantized (or classical) version of the Bohr model. Check this for exact calculations:

http://en.wikipedia.org/wiki/Bohr_model

The centrifugal force experienced by the electron will be balanced by the electrostatic attraction it experiences from the nucleus. This force balance condition will give you the velocity of the electron as a function of the radius. This functional dependence goes like [itex]1/\sqrt{r}[/itex]. The angular momentum of this electron is given by [itex]L = mvr[/itex]. Therefore, the angular momentum depends on radius as [itex]\sqrt{r}[/itex]. Consequently, the angular momentum is zero when radius is zero. Hence we do not really have an orbit.
 
Thanks.
I find the l=0 state to be one that the quantum and classical pictures differ most strikingly.
 
For angular momentum zero, in a centrosymmetric potential, the particle will move from -r to +r and back again along a line of constant angle phi. Hence it falls through the center. I do not see why this should be classically forbidden. If an obstacle (like a nucleus) happens to be in the center, the particle may or may not get reflected. In classical mechanics, the particle either gets completely reflected or not reflected at all, while in QM (like in the hydrogen atom) you usually observe a superposition of unreflected and reflected paths. Furthermore in QM, the angle phi is undetermined, which does not mean that it changes in time.
 
DrDu said:
For angular momentum zero, in a centrosymmetric potential, the particle will move from -r to +r and back again along a line of constant angle phi. Hence it falls through the center. I do not see why this should be classically forbidden. If an obstacle (like a nucleus) happens to be in the center, the particle may or may not get reflected. In classical mechanics, the particle either gets completely reflected or not reflected at all, while in QM (like in the hydrogen atom) you usually observe a superposition of unreflected and reflected paths. Furthermore in QM, the angle phi is undetermined, which does not mean that it changes in time.

Yes, that is a good example.
 
Thanks.
Nuclear size being 10-15m, the electrostatic attraction tends to negative infinity. Will the electron speed exceed speed of light?
 
No, you have to consider relativistic corrections (i.e. the Dirac equation) in the immediate vicinity of the nucleus.
 

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