Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics...

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Chapter 8 Rotational Motion

Transcript of Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics...

Page 1: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

Chapter 8

Rotational Motion

Page 2: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

Objectives

• state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion.

• describe torque.

• solve word problems related to angular kinematics.

Page 3: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

Torque

• A torque is an action that causes objects to rotate.

• Torque is not the same thing as force.

• For rotational motion, the torque is what is most directly related to the motion, not the force.

Page 4: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

TORQUE

• To make an object rotate, a force must be applied in the right place.

• the combination of force and point of application is called TORQUE

Force, F

lever arm, L

Axle

Page 5: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

Torque = force times lever arm

Torque = F L

Page 6: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

Torque

• Motion in which an entire object moves is called translation.

• Motion in which an object spins is called rotation.

• The point or line about which an object turns is its center of rotation.

• An object can rotate and translate.

Page 7: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

8-4 TorqueTo make an object start rotating, a force is needed; the position and direction of the force matter as well.

The perpendicular distance from the axis of rotation to the line along which the force acts is called the lever arm.

Page 8: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

8-4 Torque

A longer lever arm is very helpful in rotating objects.

Page 9: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

Torque

• Torque is created when the line of action of a force does not pass through the center of rotation.

• The line of action is an imaginary line that follows the direction of a force and passes though its point of application.

Page 10: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

Torque

• To get the maximum torque, the force should be applied in a direction that creates the greatest lever arm.

• The lever arm is the perpendicular distance between the line of action of the force and the center of rotation

Page 11: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.
Page 12: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

Torque Period 1 stopped here

• Hewitt video

Page 13: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

Why things fall over• Every object has a special point called the

center of gravity (CG). The CG is usually right smack in the center of the object.

• if the center of gravity is supported, the object will not fall over.

• You generally want a running back with a low CG then it’s harder to knock him down.

• The lower the CG the more stable an object is. stable not easy to knock over!

Page 14: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

Condition for stability

If the CG is above the edge, the objectwill not fall

CG

Page 15: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

when does it fall over?

CG CG

STABLE NOT STABLE

If the vertical lineextending down fromthe CG is inside theedge the object willreturn to its uprightposition the torquedue to gravity bringsit back.

Page 16: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

Stable and Unstable

stable unstable

torque due to gravitypulls object back

torque due to gravitypulls object down

Page 17: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

Stable structures

Structures arewider at their

base to lower theircenter of gravity

Page 18: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

If the center of gravityis supported, the blocksdo not fall over

Playing with your blocks

CG

Page 19: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

Object with low CG

Stay low to the ground!

300 lb fullback who is4 ft, 10 inches talland runs a 4-40

Page 20: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

As more and more stuff is loaded into asemi, its center of gravity moves upward.It could be susceptible to tipping over.

High ProfileVehicles

wind

Page 21: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

Enrichment

Linear and Rotational Motion of Cars.

Page 22: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

8-4 Torque

Here, the lever arm for FA is the distance from the knob to the hinge; the lever arm for FD is zero; and the lever arm for FC is as shown.

Page 23: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

Torque

t = r x F

Lever arm length (m)

Force (N)

Torque (N.m)

Page 24: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

Sign Convention for Sign Convention for TorqueTorque

By convention, counterclockwise torques are positive and clockwise

torques are negative.Positive torque:

Counter-clockwise, out of

pagecw

ccw

Negative torque: clockwise, into page

Page 25: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

8-4 Torque

The torque is defined as:

(8-10a)

(8-10c)

Page 26: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

Net Force = 0 , Net Torque ≠ 0

10 N

10 N

• > The net force = 0, since the forces are applied in opposite directions so it will not accelerate.

• > However, together these forces will make the rod rotate in the clockwise direction.

Page 27: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

Net torque = 0, net force ≠ 0

The rod will accelerate upward under thesetwo forces, but will not rotate.

Page 28: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

Balancing torques

10 N20 N

1 m 0.5 m

Left torque = 10 N x 1 m = 10 n mRight torque = 20 N x 0.5 m = 10 N m

Page 29: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

Torque Lab

Page 30: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

Torque example

F

L

What is the torque on a boltapplied with a wrench that has a lever arm of 30 cmwith a force of 10 N?

Torque = F L = 30 N 0.30 m = 9 N m

For the same force, you get more torquewith a bigger wrench the job is easier!

Page 31: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

Example 1:Example 1: An An 80-N80-N force acts at the end of force acts at the end of a a 12-cm12-cm wrench as shown. Find the torque. wrench as shown. Find the torque.

• Extend line of action, draw, calculate r.

= (80 N)(0.104 m) = 8.31 N m

= (80 N)(0.104 m) = 8.31 N m

r = 12 cm sin 600 = 10.4 cm

r = 12 cm sin 600 = 10.4 cm

Page 32: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

Example 2:Example 2: Find resultant torque Find resultant torque about axis about axis AA for the arrangement for the arrangement shown below:shown below:

300300

6 m 2 m4 m

20 N30 N

40 NA

Find due to each force. Consider 20-N force first:

Find due to each force. Consider 20-N force first:

r = (4 m) sin 300 = 2.00 m

= Fr = (20 N)(2 m) = 40 N m, cw

The torque about A is clockwise and negative.

20 = -40 N m20 = -40 N m

r

negative

Page 33: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

Example 2 (Cont.):Example 2 (Cont.): Next we find Next we find torque due to torque due to 30-N30-N force about force about same axis same axis AA..

300300

6 m 2 m4 m

20 N30 N

40 NA

Find due to each force. Consider 30-N force next.

Find due to each force. Consider 30-N force next.

r = (8 m) sin 300 = 4.00 m

= Fr = (30 N)(4 m) = 120 N m, cw

The torque about A is clockwise and negative.

30 = -120 N m30 = -120 N m

rnegative

Page 34: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

Example 2 (Cont.):Example 2 (Cont.): Finally, we Finally, we consider the torque due to the consider the torque due to the 40-N40-N force.force.

Find due to each force. Consider 40-N force next:

Find due to each force. Consider 40-N force next:

r = (2 m) sin 900 = 2.00 m

= Fr = (40 N)(2 m) = 80 N m, ccw

The torque about A is CCW and positive.

40 = +80 N m40 = +80 N m

300300

6 m 2 m4 m

20 N30 N

40 NA

r

positive

Page 35: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

Example 2 (Conclusion):Example 2 (Conclusion): Find Find resultant torque about axis resultant torque about axis AA for the for the arrangement shown below:arrangement shown below:

300300

6 m 2 m4 m

20 N30 N

40 NA

Resultant torque is the sum of individual torques.

Resultant torque is the sum of individual torques.

R = - 80 N mR = - 80 N m Clockwise

R = 20 + 20 + 20 = -40 N m -120 N m + 80 N m

Page 36: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

Practice Problem #1Practice Problem #1

A person exerts a force of 45N on A person exerts a force of 45N on the end of a door 84cm wide. the end of a door 84cm wide. What is the magnitude of the What is the magnitude of the torque if the force is exerted (a) torque if the force is exerted (a) perpendicular to the door, and (b) perpendicular to the door, and (b) at a 60at a 6000 angle to the face of the angle to the face of the door? door? 

Page 37: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

Practice Problem #1 SolutionPractice Problem #1 SolutionAA person exerts a force of 45N on the end of a door 84cm person exerts a force of 45N on the end of a door 84cm wide. What is the magnitude of the torque if the force is wide. What is the magnitude of the torque if the force is exerted (a) perpendicular to the door, and (b) at a 60exerted (a) perpendicular to the door, and (b) at a 6000 angle angle to the face of the door? to the face of the door? 

a.a.The formula for torque is:The formula for torque is:r x F = rFsinr x F = rFsinSo for the 60So for the 60oo angle:  angle: = (.84 m)(45 N)sin= (.84 m)(45 N)sin6060ooNm = 33 NmNm = 33 Nm

b.b.If the force is applied at a 90If the force is applied at a 90oo angle to the radius, the factor angle to the radius, the factor sinsinbecomes 1, and really the torque is:becomes 1, and really the torque is:rF = (.84 m)(45 N) = 37.8 Nm = 38 NmrF = (.84 m)(45 N) = 37.8 Nm = 38 Nm

Page 38: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

Practice Problem 2

If the coefficient of static friction between tires and pavement is 0.75, calculate the minimum torque that must be applied to the 66-cm-diameter tire of a 1080kg automobile in order to "lay rubber" (make the wheel spin, slipping as the car accelerates). Assume each tire supports an equal share of the weight. 

Page 39: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

Practice Problem 2If the coefficient of static friction between tires and pavement is 0.75, calculate the minimum torque that must be applied to the 66-cm-diameter tire of a 1080kg automobile in order to "lay rubber" (make the wheel spin, slipping as the car accelerates). Assume each tire supports an equal share of the weight. 

If each wheel supports an equal share of the weight, thenF = maF = (1080 kg)(9.80 N/kg) = 10584 N is divided into four equal parts, so the normal force at each tire isFN = (10584 N)/4 = 2646 N

This means that the maximum static force of friction tangential to the drive wheels must be:Ffr µsFN = (.75)(2646 N) = 1984.5 N

The formula for torque is:r x F = rFsinSince the road must be tangential to the tire,  the force is applied at a 90o angle to the radius, so the factor sinbecomes 1, and really the torque is:rF = (.33 m)(1984.5 N) = 654.9 Nm = 650 Nm(They gave you the diameter - .66 m diameter, .33m radius)

Page 40: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

Practice Problem 3The bolts on the cylinder head of an engine require tightening to a torque of 80m.N. If a wrench is 30cm long, what force perpendicular to the wrench must the mechanic exert at its end? If the six-sided bolt head is 15mm in diameter, estimate the force applied near each of the six points by a rocket wrench.

Page 41: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

Practice Problem 3

The bolts on the cylinder head of an engine require tightening to a torque of 80m.N. If a wrench is 30cm long, what force perpendicular to the wrench must the mechanic exert at its end? If the six-sided bolt head is 15mm in diameter, estimate the force applied near each of the six points by a rocket wrench.

The formula for torque is:r x F = rFsinSince force is applied at a 90o angle to the radius, so the factor sinbecomes 1, and really the torque is:rF = 80 Nmr = .30 mF = (80 Nm)/(.30 m) = 266.67 N

This force is much greater at the locale of the bolt head itself, with a diameter of 15 mm, or radius of 7.5 mm:rF = 80 Nmr = 7.5x10-3 mF = (80 Nm)/(7.5x10-3 m) = 10666.7 N, which divided by the six sides is:F = 1777.8 N = 1800 N per side

Page 42: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

Elaboration

• Torque Magnitude

Page 43: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

Homework

• Chapter 8 Problems

• #s 22, 24, and 25

Page 44: Chapter 8 Rotational Motion Objectives state the meaning of the symbols used in the kinematics equations for uniformly accelerated angular motion. describe.

Closure

• Kahoot 8-4