Loading in 5 sec....

Chapter VI Dynamics of Rotational MotionPowerPoint Presentation

Chapter VI Dynamics of Rotational Motion

- By
**akamu** - Follow User

- 266 Views
- Uploaded on

Download Presentation
## PowerPoint Slideshow about ' Chapter VI Dynamics of Rotational Motion' - akamu

**An Image/Link below is provided (as is) to download presentation**

Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author.While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server.

- - - - - - - - - - - - - - - - - - - - - - - - - - E N D - - - - - - - - - - - - - - - - - - - - - - - - - -

Presentation Transcript

Chapter VIDynamics of Rotational Motion

- Rotational Kinematics
- Relating Linear and Angular Kinematics
- Moment of Inertia and Rotational Kinetic Energy
- Calculating the Moment of Inertia
- Torque
- Angular Momentum
- Work-Kinetic Energy Theorem
- Torque and Angular Acceleration for a Rigid Body
- Rolling Without Slipping
- Conservation Of Angular Momentum
- Static Equilibrium

B. Relating Linear and Angular Kinematics

Z

&

S = r

ds/dt = (d/dt) r

v = r

v = x r

dv/dt = (d/dt) r

aT = r

aT = x r

as = v2/r = (v/r)v = v

as = x v

aT & v

as

y

x

C. Moment of Inertia and Rotational Kinetic Energy

A particle

K1 = ½ m1 v12 = ½ m1 r122

System particle

K = K1 + K2 + K3 + ...

K = ½ m1 r122 + ½ m2 r222 + ...

K = ½(m1 r12 + m2 r22 + ...) 2

K = ½ ( mi ri2) 2

K = ½ I 2

moment of Inertia= I = mi ri2

D. Calculating the Moment of Inertia

moment of Inertia= I = mi ri2 discrete mass distribution

I = r2 dm continuous mass distribution

An engineer is designing a machine part consisting of three heavy disks linked by lightweight struts (Fig.). (a) What is the moment of inertia of this body about an axis through the center of disk A, perpendicular to the plane of the diagram? (b) What is the moment of inertia about an axis through the centers of disks B and C? (c) If the body rotates about an axis through A perpendicular to the plane of the diagram, with angular speed = 4.0 rad/s, what is its kinetic energy?

a)

b)

c)

I = heavy disks linked by lightweight struts (Figr2 dm

dm = dV = 2rL dr

I = r2 2rL dr = 2L r3 dr

I = 2L ¼ (r24 – r14)

I = ½ L (r22 – r12) (r22 + r12)

M = V = ( r22L - r12L)

M = L (r22 – r12)

I = ½ M (r22 + r12)

If, r1 = 0, than I = ½ M r2 solid cylinder

If, r1 = r2, than I = M r2 Thin-walled

hollow cylinder

r2

r2

r1

r1

r

dr

M

L

T heavy disks linked by lightweight struts (Fighe parallelaxis theorem

There is a simple relationship between the moment of inertia Icm of a body of mass M about an axis through its center of mass and the moment of inertia Ip about any other axis parallel to the original one but displaced from it by a distance d. This relationship, called the parallelaxis theorem, states that,

Ip = Icm + M d 2

T heavy disks linked by lightweight struts (Fighe moment of inertia Icm of the slice about the axis through the centerof mass (at 0) is

The moment of inertia of the slice about the axis through P is

We then expand the squared terms and regroup, and obtain

The second and third sums are roportional to X ern and Yern; these are zero because we have taken our origin to be the center of mass.

E. Torque heavy disks linked by lightweight struts (Fig

- = r x F
- = r F sin

y

F

r

r

x

F. Angular Momentum

y

p

r

Angular Momentum a Particle

r

l = r x p

I = r p sin

dl/dt = dr/dt x p + r x dp/dt

dl/dt = v x mv + r x F

dl/dt =

x

Angular Momentum System Particle heavy disks linked by lightweight struts (Fig

L = l1 + l2 + l3 + ...

dL/dt = dl1/dt + dl2/dt + dl3/dt + ...

dL/dt = 1 + 2 + 3 + ...

dL/dt = ext

G. Work-Kinetic Energy Theorem heavy disks linked by lightweight struts (Fig

y

F

W = F.S = F cos α r = F sin r

dW/dt = (d/dt)

Power = P =

r

r

Work-Kinetic Energy Theorem

w = K

dW/dt = dK/dt

dW/dt = d(½ I 2 )/dt

P = ½I d(2)/dt = ½I (d2/d) (d/dt)

P = ½I 2 α

P = I α

P =

= I α

x

H. heavy disks linked by lightweight struts (FigTorque and Angular Acceleration for a Rigid Body

For a particle

F1 tan = m1 a1 tan

1 z = F1 tan r1 = m1 a1 tan r1

1 z = m1 r1αz r1 = m1 r12αz

For a rigid body

z = i z = mi ri2αz

z = I αz (rotational analog of Newton's second law for a rigid body)

- = I heavy disks linked by lightweight struts (Figα T R = ½ M R2 (a/R)
- T = ½ M a ................... (1)
- Fy = m a mg – T = ma .............. (2)
- (2)
- mg – ½ M a = ma
- mg = ½ M a + ma = a (½ M + m)
- a = mg/(½ M + m)

I. Rolling Without Slipping heavy disks linked by lightweight struts (Fig

IP = ICM + M R2

K = ½ IP 2

K = ½ (ICM + M R2) 2

K = ½ ICM2 + ½ M R2 2

The total kinetic energy of a rolling object is the sum of the rotational kinetic energy about the center of mass and the translational kineticenergy of the center of mass.

M

R

Conservation of Mechanical Energy

J. CONSERVATION OF ANGULAR MOMENTUM heavy disks linked by lightweight struts (Fig

Li = Lf

Iii = Iff

Decrease in the moment of inertia of the skater causes an increase inthe angular speed.

Example. heavy disks linked by lightweight struts (Fig

An acrobatic physics professor stands at the center of a turntable, holding his arms extended horizontally with a 5.0-kg dumbbell in each hand (Fig. ). He is set rotating about a vertical axis, making one revolution in 2.0 s. Find the prof's new angular velocity ifhe pulls the dumbbells in to his stomach. His moment of inertia (without the dumbbells) is 3.0 kg . m 2 when his arms are outstretched, dropping to 2.2 kg . m 2 when his hands are at his stomach. The dumbbells are 1.0 m from the axis initially and 0.20 m from it at the end. Treat the dumbbells as particles.

We have heavy disks linked by lightweight struts (Fig1z = (0.50 rev/s)(2 rad/rev) = 3.14rad/s and

2z, = (2.5 rev/s)(2rad/rev) = 15.7rad/s.

Theinitial kinetic energy is

The extra kinetic energy came from the work that the prof did topull his arms and the dumbbells inward.

K. Static Equilibrium heavy disks linked by lightweight struts (Fig

Slippery wall

Fx = 0 ; Fy = 0 ; = 0

Fx = 0 NA – fO = 0 ................(1)

Fy = 0 NO – WL – WP = 0 .....(2)

= 0 We use theconvention that the sign of the torque resulting from a force is positive if the turning tendency of the force is counterclockwise and is negative if the turning tendency is clockwise.

When we take the torques about an axis through theorigin O at the bottom of the ladder, we have

½a WL + ⅓ a WP – b NA = 0 ......(3)

A

NA

NO

b

½ L

⅓ L

WL

WP

fO

O

a

SEKIAN heavy disks linked by lightweight struts (Fig

Download Presentation

Connecting to Server..