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University Physics I - Classical Mechanics, 2019

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176 CHAPTER 8. MOTION IN TWO DIMENSIONS<br />

on whatever value is necessary to keep the object from moving, up to a maximum value of<br />

F s max = μ sF n .<br />

5. An object moving in an arc of a circle of radius R withaspeedv experiences a centripetal<br />

acceleration of magnitude a c = v 2 /R. “Centripetal” means the corresponding vector points<br />

towards the center of the circle. Accordingly, to get an object of mass m to move on such a<br />

path requires a centripetal force F c = mv 2 /R.<br />

6. To describe the motion of a particle on a circle of radius R, we use an angular position variable<br />

θ(t), in terms of which we define angular displacement Δθ, angular velocity ω = dθ/dt, and<br />

angular acceleration α = dω/dt. The equations for motion in one dimension with constant<br />

acceleration apply to circular motion with constant α with the changes x → θ, v → ω and<br />

a → α.<br />

7. The displacement along the circle, s, corresponding to an angular displacement Δθ, is(in<br />

magnitude) s = R|Δθ|. Similarly, the (linear) speed of the particle (magnitude of its velocity<br />

vector) is equal to v = R|ω|, and the tangential component of its acceleration vector has<br />

magnitude a t = R|α|. In addition to this, the particle always has a radial acceleration<br />

component a r equal to the centripetal acceleration of point 5 above.

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