Can L be conserved if its magnitude is conserved?

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Homework Help Overview

The discussion revolves around a problem in classical mechanics, specifically focusing on angular momentum in a system described by a modified form of Newton's second law. Participants are tasked with demonstrating the conditions under which angular momentum L is not conserved, while its magnitude |L| is conserved.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the derivation of the time derivative of angular momentum and its implications for conservation laws. There are attempts to express the magnitude of angular momentum and explore the conditions under which its magnitude remains constant.

Discussion Status

The discussion is ongoing, with participants sharing their attempts and seeking hints on how to show the conservation of the magnitude of angular momentum. Some guidance has been offered regarding the use of the product rule and the relationship between the time derivative of L and its perpendicularity to L.

Contextual Notes

Participants are working under the constraints of a specific problem setup involving a function h(r) and its derivative, which influences the dynamics of the system. There is an emphasis on understanding the implications of the derived equations without providing direct solutions.

subzero0137
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Problem: Consider a system for which Newton's second law is $$ \frac {d \vec v}{dt} = - [ \frac {h(r)h'(r)}{r} + \frac {k}{r^3} ] \vec r- \frac {h'(r)}{r} \vec L $$ where k is a constant, h(r) is some function of r, h'(r) is its derivative and L = r x v is the angular momentum. Show that $$ \frac {d \vec L}{dt} = - \frac {h'(r)}{r} \vec r × \vec L$$ and use this equation to prove that L is not generally conserved, but its magnitude L is conserved.

Attempt: I've done the first part of the question, but I don't know how I should go about showing that L is not conserved but its magnitude is conserved. Any hints would be appreciated.
 
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subzero0137 said:
Problem: Consider a system for which Newton's second law is $$ \frac {d \vec v}{dt} = - [ \frac {h(r)h'(r)}{r} + \frac {k}{r^3} ] \vec r- \frac {h'(r)}{r} \vec L $$ where k is a constant, h(r) is some function of r, h'(r) is its derivative and L = r x v is the angular momentum. Show that $$ \frac {d \vec L}{dt} = - \frac {h'(r)}{r} \vec r × \vec L$$ and use this equation to prove that L is not generally conserved, but its magnitude L is conserved.

Attempt: I've done the first part of the question, but I don't know how I should go about showing that L is not conserved but its magnitude is conserved. Any hints would be appreciated.

The magnitude squared is given by the dot product of L with itself. Can you show the time derivative of that is 0?
 
So |L|^2 = (r×v)⋅(r×v) = (rr)(vv) - (vr)(vr) = |r|^2 |v|^2 right? But how would I show the time derivative of this to be 0? [itex]\frac {dL}{dt} = r \frac {dv}{dt} + v \frac {dr}{dt}[/itex], but how do I make this equal 0?
 
subzero0137 said:
So |L|^2 = (r×v)⋅(r×v) = (rr)(vv) - (vr)(vr) = |r|^2 |v|^2 right? But how would I show the time derivative of this to be 0? [itex]\frac {dL}{dt} = r \frac {dv}{dt} + v \frac {dr}{dt}[/itex], but how do I make this equal 0?

You want to show the time derivative of ##L \cdot L## is zero. Use the product rule and your given expression for dL/dt. Can you tell me why dL/dt must be perpendicular to L?
 
Last edited:

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