Department of Physics and Applied Physics 95.141, F2010, Lecture 8 Physics I 95.141 LECTURE 8...

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Transcript of Department of Physics and Applied Physics 95.141, F2010, Lecture 8 Physics I 95.141 LECTURE 8...

Page 1: Department of Physics and Applied Physics 95.141, F2010, Lecture 8 Physics I 95.141 LECTURE 8 9/29/10.

Department of Physics and Applied Physics95.141, F2010, Lecture 8

Physics I95.141

LECTURE 89/29/10

Page 2: Department of Physics and Applied Physics 95.141, F2010, Lecture 8 Physics I 95.141 LECTURE 8 9/29/10.

Department of Physics and Applied Physics95.141, F2010, Lecture 8

Exam Prep Problem

• A 5kg block (A) sits on an inclined plane tilted at an angle of 30º. It is attached via a massless cord to a block of mass 2kg (B) lying on a flat surface. Ignore friction.– (10pts) Draw a free body diagram for each block (include

coordinate system).– (8pts) What are the magnitude of the Normal Forces on each

block?– (10pts) What is the acceleration of the blocks?– (7pts) What is the tension in the cord?

A

B

θ =30°

Page 3: Department of Physics and Applied Physics 95.141, F2010, Lecture 8 Physics I 95.141 LECTURE 8 9/29/10.

Department of Physics and Applied Physics95.141, F2010, Lecture 8

Exam Prep Problem

• A 5kg block (A) sits on an inclined plane tilted at an angle of 30º. It is attached via a massless cord to a block of mass 2kg (B) lying on a flat surface. Ignore friction.– (10pts) Draw a free body diagram for each block (include coordinate

system).

Page 4: Department of Physics and Applied Physics 95.141, F2010, Lecture 8 Physics I 95.141 LECTURE 8 9/29/10.

Department of Physics and Applied Physics95.141, F2010, Lecture 8

Exam Prep Problem

• A 5kg block (A) sits on an inclined plane tilted at an angle of 30º. It is attached via a massless cord to a block of mass 2kg (B) lying on a flat surface. Ignore friction.– (8pts) What are the magnitude of the Normal Forces on each block?

Page 5: Department of Physics and Applied Physics 95.141, F2010, Lecture 8 Physics I 95.141 LECTURE 8 9/29/10.

Department of Physics and Applied Physics95.141, F2010, Lecture 8

Exam Prep Problem

• A 5kg block (A) sits on an inclined plane tilted at an angle of 30º. It is attached via a massless cord to a block of mass 2kg (B) lying on a flat surface. Ignore friction.– (5pts) What is the acceleration of the blocks?

Page 6: Department of Physics and Applied Physics 95.141, F2010, Lecture 8 Physics I 95.141 LECTURE 8 9/29/10.

Department of Physics and Applied Physics95.141, F2010, Lecture 8

Exam Prep Problem

• A 5kg block (A) sits on an inclined plane tilted at an angle of 30º. It is attached via a massless cord to a block of mass 2kg (B) lying on a flat surface. Ignore friction.– (4pts) What is the tension in the cord?

Page 7: Department of Physics and Applied Physics 95.141, F2010, Lecture 8 Physics I 95.141 LECTURE 8 9/29/10.

Department of Physics and Applied Physics95.141, F2010, Lecture 8

Common Mistakes

• Orientation of mass on plane.

• Direction of Normal Force.

• Confusing sin and cos.

Page 8: Department of Physics and Applied Physics 95.141, F2010, Lecture 8 Physics I 95.141 LECTURE 8 9/29/10.

Department of Physics and Applied Physics95.141, F2010, Lecture 8

Administrative Issues

• EXAM 1: Monday, IN CLASS!– Equation sheet given

• If you rely on this, you will run out of time!!

– Wait outside class– Practice Exams– Pens/Pencils and Calculators are all that are allowed!– No iPods/mp3 players

• Exam Review session– Thursday evening, OH218, 6:30 pm. – Come with questions!! I will work out whatever you ask,

but session ends when you run out of questions.

Page 9: Department of Physics and Applied Physics 95.141, F2010, Lecture 8 Physics I 95.141 LECTURE 8 9/29/10.

Department of Physics and Applied Physics95.141, F2010, Lecture 8

Outline

• Friction • Velocity dependent Forces

• What do we know?– Units– Kinematic equations– Freely falling objects– Vectors– Kinematics + Vectors = Vector Kinematics– Relative motion– Projectile motion– Uniform circular motion– Newton’s Laws– Force of Gravity and Normal Force– Free Body Diagrams– Problem Solving

Page 10: Department of Physics and Applied Physics 95.141, F2010, Lecture 8 Physics I 95.141 LECTURE 8 9/29/10.

Department of Physics and Applied Physics95.141, F2010, Lecture 8

Review Problem

50m

250m

Page 11: Department of Physics and Applied Physics 95.141, F2010, Lecture 8 Physics I 95.141 LECTURE 8 9/29/10.

Department of Physics and Applied Physics95.141, F2010, Lecture 8

Solve for acceleration, velocity

• Geometry

• Free-body diagram

• Forces

Page 12: Department of Physics and Applied Physics 95.141, F2010, Lecture 8 Physics I 95.141 LECTURE 8 9/29/10.

Department of Physics and Applied Physics95.141, F2010, Lecture 8

Zip-Line problem

• a, vf

Page 13: Department of Physics and Applied Physics 95.141, F2010, Lecture 8 Physics I 95.141 LECTURE 8 9/29/10.

Department of Physics and Applied Physics95.141, F2010, Lecture 8

Up to now…

• We have worked with frictionless surfaces and no air resistance.

• Not particularly realistic!

• If I apply a Force to an object on this table, does it keep moving forever?

Page 14: Department of Physics and Applied Physics 95.141, F2010, Lecture 8 Physics I 95.141 LECTURE 8 9/29/10.

Department of Physics and Applied Physics95.141, F2010, Lecture 8

Friction

• Friction is actually a microscopic effect.– The roughness of two surfaces sliding against one

another provides a Force opposite to the direction of motion.

– The magnitude of this force depends on two things:• The properties of the two surfaces• The Normal Force between the two surfaces.

Page 15: Department of Physics and Applied Physics 95.141, F2010, Lecture 8 Physics I 95.141 LECTURE 8 9/29/10.

Department of Physics and Applied Physics95.141, F2010, Lecture 8

Coefficient of Kinetic Friction

• Sliding Friction• Force acting against sliding motion of object on

a surface

Nkfr FF

k Coefficient of kinetic friction

Depends on surfaces

Magnitude of Ffr depends on FN, but direction is ALWAYS against direction of motion.

Not a fundamental law Experimental Result

Page 16: Department of Physics and Applied Physics 95.141, F2010, Lecture 8 Physics I 95.141 LECTURE 8 9/29/10.

Department of Physics and Applied Physics95.141, F2010, Lecture 8

Friction Example

• Suppose we consider the 3 examples from last lecture. Let’s rank the Frictional Forces for a mass sliding on a surface with coefficient of static friction k

ov ov ov

-FH +FH

FFR FFR FFR

A B C

Page 17: Department of Physics and Applied Physics 95.141, F2010, Lecture 8 Physics I 95.141 LECTURE 8 9/29/10.

Department of Physics and Applied Physics95.141, F2010, Lecture 8

In Class Demo

• Pull on book from rest

– What is Force required to start book moving?

– What is Force required to keep book moving once it has started?

– What happens to the magnitude of this Force if I press down on the book?

Page 18: Department of Physics and Applied Physics 95.141, F2010, Lecture 8 Physics I 95.141 LECTURE 8 9/29/10.

Department of Physics and Applied Physics95.141, F2010, Lecture 8

Two Types of Friction

• Kinetic Friction: associated with movement• Static Friction: Friction at rest

– If I push on an object on the ground and it doesn’t move, I am exerting a Force, and since the object isn’t moving, there must be a second Force opposing my Force. This Force is the Force of Static Friction

• The expression for Static Friction is slightly different than for Kinetic Friction.

• Still depends on FN

NsSfr FF

Page 19: Department of Physics and Applied Physics 95.141, F2010, Lecture 8 Physics I 95.141 LECTURE 8 9/29/10.

Department of Physics and Applied Physics95.141, F2010, Lecture 8

Static Friction

• I push a little harder (F=40N)…Does it move?

• Imagine a 10.2kg box on the ground, at rest. The system has a coefficients friction μs=0.5, and μk=0.3.

• I push (horizontally) with a Force 20N. What is acceleration?

• I push with a Force of 60N. What is acceleration now?

Page 20: Department of Physics and Applied Physics 95.141, F2010, Lecture 8 Physics I 95.141 LECTURE 8 9/29/10.

Department of Physics and Applied Physics95.141, F2010, Lecture 8

Static Friction• Imagine a 10.2kg box on the ground, at rest. The system

has a coefficients friction μs=0.5, and μk=0.3. • I push (horizontally) with a Force 50N. Does it move?

What is acceleration?

• I push with a Force of 60N. What is acceleration now?

Page 21: Department of Physics and Applied Physics 95.141, F2010, Lecture 8 Physics I 95.141 LECTURE 8 9/29/10.

Department of Physics and Applied Physics95.141, F2010, Lecture 8

Demo: Static Friction

• Case 1: only a couple of pages overlap

• 10 pages overlap

• Every other page

Page 22: Department of Physics and Applied Physics 95.141, F2010, Lecture 8 Physics I 95.141 LECTURE 8 9/29/10.

Department of Physics and Applied Physics95.141, F2010, Lecture 8

Example I (Kinetic and Static Friction)

• A block lies on an inclined plane (μk=0.3, μs=0.5). At what angle do you see the block start to move? What is the acceleration when θ=45º?

• Choose coordinate system• Draw Free Body Diagram

Page 23: Department of Physics and Applied Physics 95.141, F2010, Lecture 8 Physics I 95.141 LECTURE 8 9/29/10.

Department of Physics and Applied Physics95.141, F2010, Lecture 8

Example I (Kinetic and Static Friction)• A block lies on an inclined plane (μk=0.3, μs=0.5). At

what angle do you see the block start to move? • Write out Force components

27max

0cos mgFF Ny

cossin

sinsin

mgmg

FmgFmgF

s

Nsfrx

Page 24: Department of Physics and Applied Physics 95.141, F2010, Lecture 8 Physics I 95.141 LECTURE 8 9/29/10.

Department of Physics and Applied Physics95.141, F2010, Lecture 8

Die Hard with a Physics Vengeance

Page 25: Department of Physics and Applied Physics 95.141, F2010, Lecture 8 Physics I 95.141 LECTURE 8 9/29/10.

Department of Physics and Applied Physics95.141, F2010, Lecture 8

Die Hard with a Physics Vengeance

40º

0.1S8.0k

What is acceleration with a) wheels spinning?b) wheels locked?

Page 26: Department of Physics and Applied Physics 95.141, F2010, Lecture 8 Physics I 95.141 LECTURE 8 9/29/10.

Department of Physics and Applied Physics95.141, F2010, Lecture 8

Die Hard with a Physics Vengeance

40º

8.0k

Page 27: Department of Physics and Applied Physics 95.141, F2010, Lecture 8 Physics I 95.141 LECTURE 8 9/29/10.

Department of Physics and Applied Physics95.141, F2010, Lecture 8

Die Hard with a Physics Vengeance

40º

0.1s

Page 28: Department of Physics and Applied Physics 95.141, F2010, Lecture 8 Physics I 95.141 LECTURE 8 9/29/10.

Department of Physics and Applied Physics95.141, F2010, Lecture 8

Velocity-Dependent Forces

• Friction is relatively easy, it just has two values, depending on whether the object is moving or at rest.

• Friction does not depend on the velocity of the object!

• Some forces, however, do depend on the velocity of the object.

Page 29: Department of Physics and Applied Physics 95.141, F2010, Lecture 8 Physics I 95.141 LECTURE 8 9/29/10.

Department of Physics and Applied Physics95.141, F2010, Lecture 8

Drag Forces

• Force acting on an object as it moves through a Fluid or Gas.– Boat in water– Any motion in air

• Cars• Skydivers• Projectile motion

• Mathematics of velocity dependent Forces is tricky, but a good approximations are:

bvFD 2bvFD

Page 30: Department of Physics and Applied Physics 95.141, F2010, Lecture 8 Physics I 95.141 LECTURE 8 9/29/10.

Department of Physics and Applied Physics95.141, F2010, Lecture 8

Terminal Velocity

• If we assume drag force is:• What is terminal velocity of a skydiver?

bvFD

Page 31: Department of Physics and Applied Physics 95.141, F2010, Lecture 8 Physics I 95.141 LECTURE 8 9/29/10.

Department of Physics and Applied Physics95.141, F2010, Lecture 8

Terminal Velocity II

• If we assume drag force is:• What is terminal velocity of a skydiver?

2bvFD

Page 32: Department of Physics and Applied Physics 95.141, F2010, Lecture 8 Physics I 95.141 LECTURE 8 9/29/10.

Department of Physics and Applied Physics95.141, F2010, Lecture 8

Now we Know

• Force problems with friction– Draw diagram– Draw free body diagram– Divide Forces into components– Obtain equations of motion for each dimension

• Velocity Dependent Forces– Terminal Velocity