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Chapter 8 Rotational Kinematics
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Chapter 8 Rotational Kinematics. Radians Angular Displacement Angle through which something is rotated Counterclockwise => positive(+) Units => radians.

Jan 03, 2016

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Page 1: Chapter 8 Rotational Kinematics. Radians Angular Displacement  Angle through which something is rotated  Counterclockwise => positive(+) Units => radians.

Chapter 8

Rotational Kinematics

Page 2: Chapter 8 Rotational Kinematics. Radians Angular Displacement  Angle through which something is rotated  Counterclockwise => positive(+) Units => radians.

Radians

θ rad =π

180θ o

Page 3: Chapter 8 Rotational Kinematics. Radians Angular Displacement  Angle through which something is rotated  Counterclockwise => positive(+) Units => radians.

Angular DisplacementAngle through which something is

rotated Counterclockwise => positive(+)

Units => radians

θ =Arc length

Radius=s

r

Page 4: Chapter 8 Rotational Kinematics. Radians Angular Displacement  Angle through which something is rotated  Counterclockwise => positive(+) Units => radians.

Angular SpeedRate of Rotation

Counterclockwise => positive(+) Clockwise => negative(-)

ωavg=ΔθΔt

Units => radians/secondAlso rev/min or rpm

Page 5: Chapter 8 Rotational Kinematics. Radians Angular Displacement  Angle through which something is rotated  Counterclockwise => positive(+) Units => radians.

Angular Acceleration

Units => radians/second2

αavg=ω2 −ω1

Δt=

ΔωΔt

Rate of change of angular speed Counterclockwise => positive(+) Clockwise => negative(-)

Page 6: Chapter 8 Rotational Kinematics. Radians Angular Displacement  Angle through which something is rotated  Counterclockwise => positive(+) Units => radians.

Linear vs. Angular Quantities Linear

x

v

a

Angular

θ

•(m)

•(m/s)

•(m/s2)

• (rad)

• (rad/s)

• (rad/s2)

Page 7: Chapter 8 Rotational Kinematics. Radians Angular Displacement  Angle through which something is rotated  Counterclockwise => positive(+) Units => radians.

Linear vs. Angular Quantities Linear Angular

f =ωi +αΔt

Δθ = iΔt +1

2α (Δt)2

f2 =ωi

2 + 2αΔθ

Δθ =1

2(ωi +ω f )Δt

Page 8: Chapter 8 Rotational Kinematics. Radians Angular Displacement  Angle through which something is rotated  Counterclockwise => positive(+) Units => radians.

Warm-upA ceiling fan’s angular speed increases

from 5.2 rad/s to 20.9 rad/s. During this constant angular acceleration, the fan moves through an angular displacement of 216 rad. How long does it take the fan to reach its final angular speed?

Page 9: Chapter 8 Rotational Kinematics. Radians Angular Displacement  Angle through which something is rotated  Counterclockwise => positive(+) Units => radians.

Tangential Velocity Instantaneous linear speed of an object

tangent to a circular pathObjects with the same angular speed,

may have different tangential speedsm/s

vt =rω

Page 10: Chapter 8 Rotational Kinematics. Radians Angular Displacement  Angle through which something is rotated  Counterclockwise => positive(+) Units => radians.

Tangential Acceleration Instantaneous linear acceleration of an

object tangent to a circular pathObjects with the same angular

acceleration, may have different tangential accelerations

m/s2

at =rα

Page 11: Chapter 8 Rotational Kinematics. Radians Angular Displacement  Angle through which something is rotated  Counterclockwise => positive(+) Units => radians.

Centripetal AccelerationAlways directed towards the center of

the circle

ac =vt

2

r

ac =rω2

Page 12: Chapter 8 Rotational Kinematics. Radians Angular Displacement  Angle through which something is rotated  Counterclockwise => positive(+) Units => radians.

Total AccelerationTangential and centripetal acceleration

are perpendicular to one another

Use Pythagorean’s theorem to find the total acceleration.Angle ϕ is measured relative to the radius.

Page 13: Chapter 8 Rotational Kinematics. Radians Angular Displacement  Angle through which something is rotated  Counterclockwise => positive(+) Units => radians.

Rolling MotionAssuming that a wheel rolls without

slipping, then The Tangential speed of a point on the

outside of the wheel will equal the linear velocity.

The tangential acceleration of a point on the outside of the wheel will equal the linear acceleration.