Chapter 10 Rotation of a Rigid Object about a Fixed Axis Putaran Objek Tegar Terhadap Paksi Tetap.
Lecture 30 Rigid-body Rotation About a Moving Axis
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Transcript of Lecture 30 Rigid-body Rotation About a Moving Axis
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Lecture 30: Rigid-‐body Rotation about a Moving Axis
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Lecture Objectives 1. Compare translational and rotational kinetic energies of a rolling object. 2. Apply Newton’s second law of rotation and conservation of energy to physical systems that involves rotation about a moving axis.
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Rigid-‐body rotation about a moving axis
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Speed of a primitive yo-‐yo
Given: mass, M radius, R height, h target variable, vcm 7
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Solution: U1 = mgh, U2 = 0 K1 = 0 I = 1/2 MR2
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Race of the rolling objects
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Solution: U1 = mgh, U2 = 0 K1 = 0 I = cMR2
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Acceleration of a rolling sphere
Given: Isolid sphere = 2/5 MR2
Angle of inclination, target variables, acm-‐x and f
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FBD of the solid ball
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Equations of Motion
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Rolling without slipping so may write (2) as
(1)
(2)
Solve for f in (1) and substitute to (2):
(3)
(4)
(5)
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Work in rotational motion
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Work in rotational motion
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Power in rotational motion
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Seatwork
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Seatwork 1
Note: 1rev = 2πrad
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Seatwork
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Seatwork (yes or no)
4.Is it possible to change the translational kinetic energy of an object without changing its rotational energy?
5.Must an object be rotating to have a non-‐zero moment of inertia?
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Seatwork answers
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Seatwork 1
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Seatwork
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Seatwork (yes or no)
4.Is it possible to change the translational kinetic energy of an object without changing its rotational energy? NO; v = Rω
5.Must an object be rotating to have a non-‐zero moment of inertia? NO; ex: I = mR2 (no rotation)