Lecture 19 More on 2 D rotation Rotational

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Lecture 19 More on 2 D rotation • Rotational kinetic energy • Rotation and

Lecture 19 More on 2 D rotation • Rotational kinetic energy • Rotation and COM motion • Angular momentum with respective to different reference point • Dynamical equation with arbitrary reference point. 1

Rotational kinetic energy around a fixed center • 2

Rotational kinetic energy around a fixed center • 2

Turn-table example • 3

Turn-table example • 3

Dependence of AM and Torque on the reference point • When defining angular momentum

Dependence of AM and Torque on the reference point • When defining angular momentum L and torque τ, they depend on the reference point. • In general we consider the reference point as the origin of the coordinate. • Sometimes, however, it is convenient to consider the reference point on the Rigid Body itself, such as its center of mass, or any point on the rigid body. • In this case, the dynamical equations are different. 4

A general motion in 2 D • Consider a two dimensional motion of a

A general motion in 2 D • Consider a two dimensional motion of a disk Or 3 D motion of a cylinder • A general motion can be considered as a motion of center of mass and rotation (COM) around the COM • A general motion can also be considered a translational motion of an arbitrary point on the rigid body and rotation around that point. 5

An example • 6

An example • 6

Kinetic energy of rotation in general case General Movement: the COM velocity vc, and

Kinetic energy of rotation in general case General Movement: the COM velocity vc, and rotation around the COM This, however, is not true for any reference point! 7

An example of translation plus rotation 8

An example of translation plus rotation 8

Rotation around any point P • We can in fact consider rotation around any

Rotation around any point P • We can in fact consider rotation around any reference point P on the rigid body. • It can be shown that the angular velocity around any point P is the same. (this is a challenge!) • However, the dynamical equation with torque becomes different. • One cannot write down a simple energy expression in this case. 9

2 D rotation with a general reference point P • 10

2 D rotation with a general reference point P • 10

Choosing q as the instant rotation center 11

Choosing q as the instant rotation center 11

Choosing COM as the instant rotation center 12

Choosing COM as the instant rotation center 12

Pulling the wheel solving the acceleration 13

Pulling the wheel solving the acceleration 13