Angular Momentum Dimensional Analysis

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SUMMARY

The discussion centers on determining the angular momentum of a particle of mass m moving in a circle of radius R using dimensional analysis. The established formula for angular momentum is L = mvr, which has the dimensionality of ML2T-1. Participants emphasize the importance of starting with the units of angular momentum and constructing an equation that aligns with these units, ultimately leading to the conclusion that L = m v R is valid, albeit correct up to a dimensionless constant.

PREREQUISITES
  • Understanding of angular momentum and its formula L = mvr
  • Familiarity with dimensional analysis and unit conversion
  • Basic knowledge of physics concepts such as mass, velocity, and radius
  • Ability to manipulate equations and interpret physical dimensions
NEXT STEPS
  • Study dimensional analysis techniques in classical mechanics
  • Explore the concept of dimensionless constants in physics
  • Learn about angular momentum in different coordinate systems
  • Investigate the applications of angular momentum in rotational dynamics
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Students of physics, educators teaching classical mechanics, and anyone interested in mastering dimensional analysis and angular momentum concepts.

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Homework Statement


"A particle of mass m moves in a circle of radius R. Using dimensional argument,
determine the particle angular momentum."

Homework Equations


L = mvr


The Attempt at a Solution


Because L = mvr, the dimensionality would be ML2T-1. I don't know where to go from here so if someone could point me in the right direction it'd be appreciated.

Thanks!
 
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You need to take the problem backward, compared to what you wrote.

To use a "dimensional argument," you start by the units, and then figure out how to construct an equation (with parameters you know) that will have the correct units.

So start with the fact that the units of angular momentum are ML2T-1, and find a way to argue that this means that ##L = m v R##.
 
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I should add that dimensional arguments are, at best, correct up to a dimensionless constant.
 

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