17 - Work and Power in Rotational Motion.pptx
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Transcript of 17 - Work and Power in Rotational Motion.pptx
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Work and Power in Rotational Motion
Ms. Mikaela Fudolig
Physics 71 Lecture
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Work done by a torque
Suppose that the torque is along the z-axis, and that the object on which the torque is applied rotates by = f - i. The work done by the torque on the object is
f
i
zW d
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Work done by a torque
Suppose that the torque is along the z-axis, and that the object on which the torque is applied rotates by = f - i. The work done by the torque on the object is
zW CONSTANT TORQUE
![Page 4: 17 - Work and Power in Rotational Motion.pptx](https://reader036.fdocuments.in/reader036/viewer/2022082701/552dd9b04a7959395b8b47cd/html5/thumbnails/4.jpg)
Work done by a torque
Usually, the work done by an external torque is considered as part of “Wothers” in the work-energy theorem.
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Power
The power associated with the work done by a torque acting on a rotating object is
dWP
dt
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Power
If the torque is constant over time:
z
dP
dt
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Power
And we can express the power as
zP
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Example 1
A 1.50-kg grinding wheel is in the form of a solid cylinder of radius 0.100m. What constant torque will bring it from rest to an angular speed of 1200rev/min in 2.5s?
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Example 2
What is the power output of an electric motor turning at 4800 rev/min and developing a torque of 480Nm?