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**Review Chap. 10 Dynamics of Rotational Motion**

PHYS 218 sec Review Chap. 10 Dynamics of Rotational Motion

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**What you have to know Dynamics of rotational motion Torque**

Equation of motion for a rotational motion Rotation about a moving axis Work & power Angular momentum and its conservation

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**Translational motion: governed by forces**

Torque Translational motion: governed by forces Rotational motion: governed by torques When you define a rotational motion, you should specify the axis of rotation. Therefore, physical quantities in rotational motion must include information about the location of the axis of rotation. This makes the definitions of those physical quantities include x or r. For example, even if the same force (same magnitude & same direction) is applied, the rotational motion depends on where the force exerts on, i.e., the distance between the axis of ration and the point where the force exerts on. When you have a rotational motion, determine whether the rotation is clockwise or counterclockwise.

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**This force causes counterclockwise rotation. (So, t is positive)**

Torque definition This force causes counterclockwise rotation. (So, t is positive) Axis of rotation

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**Line of action of the force F**

Torque Line of action of the force F Lever arm Only the tangential force can give a torque.

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**Note the similarity of the two equations.**

Torque for a rigid body Note the similarity of the two equations. Rotational analog of Newton’s 2nd law for a rigid body

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**Reproduce the result of Ex 9.8 as explained in the class **

Same situation as in Ex 9.8 Free-body diagram Reproduce the result of Ex 9.8 as explained in the class Direction of the rotation & sing of the torque

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Ex 10.3 Same situation as in Ex 9.9 Free-body diagram cylinder block Obtain v !

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**Rigid-body rotation about a moving axis**

Extend the analysis to the case where the axis of rotation moves Translation + Rotation cm

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**Rolling without slipping**

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**Translation + Rotation**

For translation, concentrate the mass of the object on its CM g same as the motion of a point-like particle For rotation, consider the rotation about CM g same as the rotational motion when the CM is fixed. The second equation is valid, if The axis through the CM must be an axis of symmetry The axis must not change direction

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**Speed of a primitive yo-yo**

Ex 10.4 Speed of a primitive yo-yo initial final

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**Race of the rolling bodies**

Ex 10.5 Race of the rolling bodies

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**Acceleration of a primitive yo-yo (cf. Ex 10.4)**

Rolling without slipping Try to reproduce the result of Ex 10.4

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**Solid bowling ball (rolling without slipping)**

Ex 10.7 Solid bowling ball (rolling without slipping) Free-body diagram If b is small, the friction force which is required to have the rolling is small. If b is large, the ball easily slips, then we need a large friction force to make it roll.

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**Work & Power in rotational motion**

To rotate a body, a force should be applied. Then this force do work on it.

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Work –energy theorem

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**Similarly, we define angular momentum L**

(linear) momentum p Similarly, we define angular momentum L This is defined with r, so it depends on the choice of the origin. This is a vector product. Therefore, the angular momentum is perpendicular to the plane spanned by r and p. If r and p lie on the xy-plane, L is in the z-direction. This is always true.

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Note the similarity.

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**Angular momentum of a rigid-body**

This is valid if the rigid-body lies on the xy-plane.

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**Angular momentum of a rigid-body**

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**Angular momentum of a rigid-body**

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**Conservation of angular momentum**

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**Collision problem including rotational motion. **

Ex 10.14 Collision problem including rotational motion. g use angular momentum conservation d after before Use the numbers given in the textbook to verify the result. Also check the change in kinetic energies.

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**Gyroscopes & precession**

The motion of gyroscope was discussed in the class. Here I do not repeat it. But you should understand that the gyroscope has precession and this is due to the vector nature of angular momentum.

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