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Angular Momentum and External Torque about a Single Axis

DescriptionandAssumptions"> Description and Assumptions

ProblemCues"> Problem Cues

PriorModels"> Prior Models

VocabularyandProcedures"> Vocabulary and Procedures

Model

Compatible Systems "> Compatible Systems

The system can be composed of any number of rigid bodies and point particles. The system must either be constrained to move in such a way that the angular momentum will be one-dimensional, or else the symmetries of the situation (system plus interactions) must guarantee that the angular momentum will remain one dimensional.


Relevant Interactions "> Relevant Interactions

External interactions must be explicitly given as torques, or as forces with their point of application or moment arm about a chosen axis of rotation specified along with their magnitude and direction.  (Internal interactions do not change the angular momentum of the system.)


Relevant Definitions "> Relevant Definitions

Angular momentum about axis a:

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\begin

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[ L_

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= I_

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\omega + m\vec

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_{{\rm cm},a}\times \vec

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_\rm cm ]\end


Laws of Change "> Laws of Change


Differential Form


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\begin

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[ \sum_

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\frac{dL_{a}}

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= \sum_

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\tau_

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]\end


Integral Form


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\begin

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[ \sum_

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L_

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= \sum_

L_

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+ \int \:\sum_

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\tau_

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\:dt ]\end

where the last term is called the "angular impulse"


Diagrammatic Representations "> Diagrammatic Representations


Relevant Examples

ExamplesInvolvingConstantAngularMomentum"> Examples Involving Constant Angular Momentum

ExamplesInvolvingRollingwithoutSlipping"> Examples Involving Rolling without Slipping

ExamplesInvolvingtheParallelAxisTheorem"> Examples Involving the Parallel Axis Theorem

AllExamplesUsingthisModel"> All Examples Using this Model



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Pictures courtesy of:
Wikimedia Commons user Dobromila
Wikimedia Commons user Vmenkov

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