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[Model Hierarchy]

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The root page Model Hierarchy could not be found in space Modeling Applied to Problem Solving.
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Description and Assumptions

This model applies to a single point particle moving in a circle of fixed radius (assumed to lie in the xy plane with its center at the origin) with constant speed. It is a subclass of the Rotational Motion model defined by α=0 and r = R.

Problem Cues

Usually uniform circular motion will be explicitly specified if you are to assume it. (Be especially careful of vertical circles, which are generally nonuniform circular motion because of the effects of gravity. Unless you are specifically told the speed is constant in a vertical loop, you should not assume it to be.) You can also use this model to describe the acceleration in instantaneously uniform circular motion, which is motion along a curved path with the tangential acceleration instantaneously equal to zero. This will usually apply, for example, when a particle is at the top or the bottom of a vertical loop, when gravity is not changing the speed of the particle.


Page Contents


Prerequisite Knowledge

Prior Models

Vocabulary and Procedures


System

Constituents

A single point particle.

State Variables

Time (t), radius of circle (R), tangential speed (v), angular position (θ), angular velocity (ω).


Interactions

Relevant Types

The system must be subject to an acceleration (and so a net force) that is directed radially inward to the center of the circular path, with no tangential component.

Interaction Variables

Centripetal acceleration (ac).


Model

Relevant Definitions

Initial conditions:
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\begin

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[ x_

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= x(t=0)]
[ y_

= y(t=0) ]
[\theta_

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= \theta(t=0)]\end

Centripetal acceleration:


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\begin

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[ \vec

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_

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= -\frac{v^{2}}

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\hat

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= -\omega^

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R\;\hat

]\end


Phase:


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\begin

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[ \phi = \cos^{-1}\left(\frac{x_{0}}

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\right) = \sin^{-1}\left(\frac{y_

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}

\right) ]\end

Laws of Change


Angular Position:


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\begin

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[ \theta(t) = \theta_

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+\omega t]\end


Position:


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\begin

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[ x(t) = R\cos(\omega t + \phi)]\end


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\begin

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[ y(t) = R\sin(\omega t + \phi)]\end


Velocity:


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\begin

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[ \vec

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= -R\omega\sin(\omega t+\phi) \;\hat

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+ R\omega\cos(\omega t +\phi)\;\hat

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= \omega R \hat

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]\end



Diagrammatical Representations


Relevant Examples

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RELATE wiki by David E. Pritchard is licensed under a Creative Commons Attribution-Noncommercial-Share Alike 3.0 United States License.

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