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Rotational Dynamics October 24, 2005.

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Presentation on theme: "Rotational Dynamics October 24, 2005."— Presentation transcript:

1 Rotational Dynamics October 24, 2005

2 Same as Bonnie’s Twice as Bonnie’s Half of Bonnie’s ¼ of Bonnie’s
Bonnie sits on the outer rim of a merry-go-round, and Klyde sits midway between the center and the rim. The merry-go-round makes one complete revolution every two seconds. Klyde’s angular velocity is: 60 Same as Bonnie’s Twice as Bonnie’s Half of Bonnie’s ¼ of Bonnie’s Four times Bonnie’s 5 w Bonnie Klyde

3 Linear velocity is zero for both of them
Bonnie sits on the outer rim of a merry-go-round, and Klyde sits midway between the center and the rim. The merry-go-round makes one revolution every two seconds. Who has the larger linear (tangential) velocity? 60 Klyde Bonnie Both the same Linear velocity is zero for both of them 5 w Bonnie Klyde

4 An object at rest begins to rotate with a constant angular acceleration. If this object rotates through an angle q in the time t, through what angle did it rotate in the time ½t? 60 ½ q ¼ q ¾ q 2 q 4 q 5

5 An object at rest begins to rotate with a constant angular acceleration. If this object has angular velocity w at time t, what was its angular velocity at the time ½t? 60 ½ w ¼ w ¾ w 2 w 4 w 5

6 Same as Bonnie’s -- The angular velocity w of any point on a solid object rotating about a fixed axis is the same. Both Bonnie & Klyde go around one revolution (2 pi radians) every two seconds. Bonnie -- Their linear speeds v will be different since v = R and Bonnie is located further out (larger radius R) than Klyde. ¼ . The angular displacement is  = ½  t 2 (starting from rest), and there is a quadratic dependence on time. Therefore, in half the time, the object has rotated through one-quarter the angle. The angular velocity is  =  t (starting from rest), and there is a linear dependence on time. Therefore, in half the time, the object has accelerated up to only half the speed.


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