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Lecture 3 - Jeffrey McCallum - Circular Motion.pdf - School of ...

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3/24/10<br />

<strong>Circular</strong> <strong>Motion</strong>: Ball on String<br />

<strong>Circular</strong> <strong>Motion</strong>: Ball on String<br />

Similar Triangles<br />

R<br />

θ<br />

R<br />

?<br />

<strong>Circular</strong> <strong>Motion</strong>: Ball on String<br />

Newton’s Laws<br />

! Newton 2: An object <strong>of</strong> mass m subjected to<br />

a net force F net will undergo acceleration a<br />

given by:<br />

The acceleration vector is in the same direction as the<br />

net force vector.<br />

<strong>Circular</strong> <strong>Motion</strong>: Ball on String<br />

Newton’s Laws<br />

For uniform circular motion we<br />

require a net force directed toward<br />

the centre <strong>of</strong> the circle.<br />

! Newton 3: When two objects interact, the<br />

forces that the objects exert on each other<br />

(action/reaction forces) are always equal in<br />

magnitude and opposite in direction.<br />

4

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