application of newton’s lawsnsmn1.uh.edu/cratti/phy1301-spring2015_files/ch6_claudia.pdf ·...

29
APPLICATION OF NEWTON’S LAWS Chapter 6 Copyright © 2010 Pearson Education, Inc.

Upload: others

Post on 24-Mar-2020

1 views

Category:

Documents


0 download

TRANSCRIPT

Page 1: APPLICATION OF NEWTON’S LAWSnsmn1.uh.edu/cratti/PHY1301-Spring2015_files/Ch6_Claudia.pdf · Summary of Chapter 6 Copyright © 2010 Pearson Education, Inc. • An object is in translational

APPLICATION OF NEWTON’S LAWS Chapter 6

Copyright © 2010 Pearson Education, Inc.

Page 2: APPLICATION OF NEWTON’S LAWSnsmn1.uh.edu/cratti/PHY1301-Spring2015_files/Ch6_Claudia.pdf · Summary of Chapter 6 Copyright © 2010 Pearson Education, Inc. • An object is in translational

•  Frictional forces

• Strings and springs

•  Translational Equilibrium

• Connected objects

• Circular Motion

Units of Chapter 6

Copyright © 2010 Pearson Education, Inc.

Page 3: APPLICATION OF NEWTON’S LAWSnsmn1.uh.edu/cratti/PHY1301-Spring2015_files/Ch6_Claudia.pdf · Summary of Chapter 6 Copyright © 2010 Pearson Education, Inc. • An object is in translational

6-1 Frictional forces

Copyright © 2010 Pearson Education, Inc.

•  Friction has its basis in surfaces that are not completely smooth:

Page 4: APPLICATION OF NEWTON’S LAWSnsmn1.uh.edu/cratti/PHY1301-Spring2015_files/Ch6_Claudia.pdf · Summary of Chapter 6 Copyright © 2010 Pearson Education, Inc. • An object is in translational

6-1 Frictional forces

Copyright © 2010 Pearson Education, Inc.

• Types of frictional forces:

•  Kinetic friction: the friction experienced by surfaces sliding against one another (object is moving)

•  Static friction: the friction experienced by surfaces when the object is not in motion (object is not moving)

Page 5: APPLICATION OF NEWTON’S LAWSnsmn1.uh.edu/cratti/PHY1301-Spring2015_files/Ch6_Claudia.pdf · Summary of Chapter 6 Copyright © 2010 Pearson Education, Inc. • An object is in translational

6-1 Frictional forces

Copyright © 2010 Pearson Education, Inc.

• Kinetic friction:

•  Is a vector;

•  Occurs between two objects;

•  One or both objects are in motion;

•  Occurs at the point of contact between surfaces;

•  Opposes motion, i.e. if object is sliding to the right, kinetic friction points to the left

Page 6: APPLICATION OF NEWTON’S LAWSnsmn1.uh.edu/cratti/PHY1301-Spring2015_files/Ch6_Claudia.pdf · Summary of Chapter 6 Copyright © 2010 Pearson Education, Inc. • An object is in translational

6-1 Frictional forces

Copyright © 2010 Pearson Education, Inc.

• Kinetic friction:

•  The kinetic frictional force depends on the normal force:

•  The constant is called the coefficient of kinetic friction.

Page 7: APPLICATION OF NEWTON’S LAWSnsmn1.uh.edu/cratti/PHY1301-Spring2015_files/Ch6_Claudia.pdf · Summary of Chapter 6 Copyright © 2010 Pearson Education, Inc. • An object is in translational

6-1 Frictional forces

Copyright © 2010 Pearson Education, Inc.

Page 8: APPLICATION OF NEWTON’S LAWSnsmn1.uh.edu/cratti/PHY1301-Spring2015_files/Ch6_Claudia.pdf · Summary of Chapter 6 Copyright © 2010 Pearson Education, Inc. • An object is in translational

6-1 Frictional forces

Copyright © 2010 Pearson Education, Inc.

•  The kinetic frictional force is independent of the relative speed of the surfaces, and of their area of contact.

Page 9: APPLICATION OF NEWTON’S LAWSnsmn1.uh.edu/cratti/PHY1301-Spring2015_files/Ch6_Claudia.pdf · Summary of Chapter 6 Copyright © 2010 Pearson Education, Inc. • An object is in translational

6-1 Frictional forces

Copyright © 2010 Pearson Education, Inc.

• Static friction:

•  Is a vector;

•  Occurs between two objects;

•  Objects are NOT in motion;

•  Occurs at the point of contact between surfaces;

•  Opposes direction motion would occur, i.e. if a force is applied to the right of an object but it does not move, static friction points to the left (opposite direction object would move)

Page 10: APPLICATION OF NEWTON’S LAWSnsmn1.uh.edu/cratti/PHY1301-Spring2015_files/Ch6_Claudia.pdf · Summary of Chapter 6 Copyright © 2010 Pearson Education, Inc. • An object is in translational

6-1 Frictional forces

Copyright © 2010 Pearson Education, Inc.

•  The static frictional force has a maximum value, but may take on any value from zero to the maximum, depending on what is needed to keep the sum of forces zero.

Page 11: APPLICATION OF NEWTON’S LAWSnsmn1.uh.edu/cratti/PHY1301-Spring2015_files/Ch6_Claudia.pdf · Summary of Chapter 6 Copyright © 2010 Pearson Education, Inc. • An object is in translational

6-1 Frictional forces

Copyright © 2010 Pearson Education, Inc.

where

The static frictional force is also independent of the area of contact and the relative speed of the surfaces.

Page 12: APPLICATION OF NEWTON’S LAWSnsmn1.uh.edu/cratti/PHY1301-Spring2015_files/Ch6_Claudia.pdf · Summary of Chapter 6 Copyright © 2010 Pearson Education, Inc. • An object is in translational

6-2 Strings and springs

Copyright © 2010 Pearson Education, Inc.

•  When you pull on a string or rope, it becomes taut. We say that there is tension in the string.

Page 13: APPLICATION OF NEWTON’S LAWSnsmn1.uh.edu/cratti/PHY1301-Spring2015_files/Ch6_Claudia.pdf · Summary of Chapter 6 Copyright © 2010 Pearson Education, Inc. • An object is in translational

6-2 Strings and springs

Copyright © 2010 Pearson Education, Inc.

•  The tension in a real rope will vary along its length, due to the weight of the rope.

•  Here, we will assume that all ropes, strings, wires, etc. are massless unless otherwise stated.

Page 14: APPLICATION OF NEWTON’S LAWSnsmn1.uh.edu/cratti/PHY1301-Spring2015_files/Ch6_Claudia.pdf · Summary of Chapter 6 Copyright © 2010 Pearson Education, Inc. • An object is in translational

6-2 Strings and springs

Copyright © 2010 Pearson Education, Inc.

•  An ideal pulley is one that simply changes the direction of the tension:

Page 15: APPLICATION OF NEWTON’S LAWSnsmn1.uh.edu/cratti/PHY1301-Spring2015_files/Ch6_Claudia.pdf · Summary of Chapter 6 Copyright © 2010 Pearson Education, Inc. • An object is in translational

6-2 Strings and springs

Copyright © 2010 Pearson Education, Inc.

• Hooke�s law for springs states that the force increases with the amount the spring is stretched or compressed:

•  The constant k is called the spring constant.

Page 16: APPLICATION OF NEWTON’S LAWSnsmn1.uh.edu/cratti/PHY1301-Spring2015_files/Ch6_Claudia.pdf · Summary of Chapter 6 Copyright © 2010 Pearson Education, Inc. • An object is in translational

Example Copyright © 2010 Pearson Education, Inc.

•  (a) If forces of 5.0 N applied to each end of a spring cause the spring to stretch 3.5 cm from its relaxed length, how far does a force of 7.0 N cause the same spring to stretch?

Page 17: APPLICATION OF NEWTON’S LAWSnsmn1.uh.edu/cratti/PHY1301-Spring2015_files/Ch6_Claudia.pdf · Summary of Chapter 6 Copyright © 2010 Pearson Education, Inc. • An object is in translational

Example continued Copyright © 2010 Pearson Education, Inc.

•  (b) What is the spring constant of this spring?

Page 18: APPLICATION OF NEWTON’S LAWSnsmn1.uh.edu/cratti/PHY1301-Spring2015_files/Ch6_Claudia.pdf · Summary of Chapter 6 Copyright © 2010 Pearson Education, Inc. • An object is in translational

6-3 Translational equilibrium

Copyright © 2010 Pearson Education, Inc.

• When an object is in translational equilibrium, the net force on it is zero:

•  This allows the calculation of unknown forces.

(6-5)

Page 19: APPLICATION OF NEWTON’S LAWSnsmn1.uh.edu/cratti/PHY1301-Spring2015_files/Ch6_Claudia.pdf · Summary of Chapter 6 Copyright © 2010 Pearson Education, Inc. • An object is in translational

6-3 Transational equilibrium

Copyright © 2010 Pearson Education, Inc.

Page 20: APPLICATION OF NEWTON’S LAWSnsmn1.uh.edu/cratti/PHY1301-Spring2015_files/Ch6_Claudia.pdf · Summary of Chapter 6 Copyright © 2010 Pearson Education, Inc. • An object is in translational

6-4 Connected objects

Copyright © 2010 Pearson Education, Inc.

•  When forces are exerted on connected objects, their accelerations are the same.

•  If there are two objects connected by a string, and we know the force and the masses, we can find the acceleration and the tension:

Page 21: APPLICATION OF NEWTON’S LAWSnsmn1.uh.edu/cratti/PHY1301-Spring2015_files/Ch6_Claudia.pdf · Summary of Chapter 6 Copyright © 2010 Pearson Education, Inc. • An object is in translational

6-4 Connected objects

Copyright © 2010 Pearson Education, Inc.

•  We treat each box as a separate system:

Page 22: APPLICATION OF NEWTON’S LAWSnsmn1.uh.edu/cratti/PHY1301-Spring2015_files/Ch6_Claudia.pdf · Summary of Chapter 6 Copyright © 2010 Pearson Education, Inc. • An object is in translational

6-4 Connected objects

Copyright © 2010 Pearson Education, Inc.

•  If there is a pulley, it is easiest to have the coordinate system follow the string:

Page 23: APPLICATION OF NEWTON’S LAWSnsmn1.uh.edu/cratti/PHY1301-Spring2015_files/Ch6_Claudia.pdf · Summary of Chapter 6 Copyright © 2010 Pearson Education, Inc. • An object is in translational

6-5 Circular motion

Copyright © 2010 Pearson Education, Inc.

•  An object moving in a circle must have a force acting on it; otherwise it would move in a straight line.

•  The direction of the force is towards the center of the circle.

Page 24: APPLICATION OF NEWTON’S LAWSnsmn1.uh.edu/cratti/PHY1301-Spring2015_files/Ch6_Claudia.pdf · Summary of Chapter 6 Copyright © 2010 Pearson Education, Inc. • An object is in translational

6-5 Circular motion

Copyright © 2010 Pearson Education, Inc.

• Some algebra gives us the magnitude of the acceleration, and therefore the force, required to keep an object of mass m moving in a circle of radius r.

•  The magnitude of the force is given by:

Page 25: APPLICATION OF NEWTON’S LAWSnsmn1.uh.edu/cratti/PHY1301-Spring2015_files/Ch6_Claudia.pdf · Summary of Chapter 6 Copyright © 2010 Pearson Education, Inc. • An object is in translational

6-5 Circular motion

Copyright © 2010 Pearson Education, Inc.

•  This force may be provided by the tension in a string, the normal force, or friction, among others.

Page 26: APPLICATION OF NEWTON’S LAWSnsmn1.uh.edu/cratti/PHY1301-Spring2015_files/Ch6_Claudia.pdf · Summary of Chapter 6 Copyright © 2010 Pearson Education, Inc. • An object is in translational

6-5 Circular motion

Copyright © 2010 Pearson Education, Inc.

Page 27: APPLICATION OF NEWTON’S LAWSnsmn1.uh.edu/cratti/PHY1301-Spring2015_files/Ch6_Claudia.pdf · Summary of Chapter 6 Copyright © 2010 Pearson Education, Inc. • An object is in translational

6-5 Circular motion

Copyright © 2010 Pearson Education, Inc.

•  An object may be changing its speed as it moves in a circle; in that case, there is a tangential acceleration as well:

Page 28: APPLICATION OF NEWTON’S LAWSnsmn1.uh.edu/cratti/PHY1301-Spring2015_files/Ch6_Claudia.pdf · Summary of Chapter 6 Copyright © 2010 Pearson Education, Inc. • An object is in translational

Summary of Chapter 6 Copyright © 2010 Pearson Education, Inc.

•  Friction is due to microscopic roughness.

•  Kinetic friction:

•  Static friction:

•  Tension: the force transmitted through a string.

•  Force exerted by an ideal spring:

Page 29: APPLICATION OF NEWTON’S LAWSnsmn1.uh.edu/cratti/PHY1301-Spring2015_files/Ch6_Claudia.pdf · Summary of Chapter 6 Copyright © 2010 Pearson Education, Inc. • An object is in translational

Summary of Chapter 6 Copyright © 2010 Pearson Education, Inc.

• An object is in translational equilibrium if the net force acting on it is zero.

•  Connected objects have the same acceleration.

•  The force required to move an object of mass m in a circle of radius r is: