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Copyright © by Holt, Rinehart and Winston. All rights reserved.
Resources
Chapter menu
GUIDELINES FOR NOTE-TAKING
• Key terms in blue pen. Definitions in black pen.
• Sample Problem (Titles) in red pen.
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Resources
Chapter menu
Chapter 4
FORCE
• A force is an action exerted on an object which may change the object’s state
of rest or motion.
• Forces can cause accelerations.
• The SI unit of force is the newton, N.
• Forces can act through contact or at a distance.
Section 1 Changes in Motion
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Resources
Chapter menu
Chapter 4
FORCE DIAGRAMS
• The effect of a force depends on both magnitude and direction.Thus, force is
a vector quantity.
• Diagrams that show force vectors as arrows are called force diagrams.
• Force diagrams that show only the forces acting on a single object are called
free-body diagrams.
Section 1 Changes in Motion
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Resources
Chapter menu
Chapter 4
FORCE DIAGRAMS, CONTINUED
In a force diagram, vector
arrows represent all the forces
acting in a situation.
Section 1 Changes in Motion
A free-body diagram shows
only the forces acting on the
object of interest—in this case,
the car.
Force Diagram Free-Body Diagram
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Resources
Chapter menu
Chapter 4
NEWTON’S FIRST LAW
• An object at rest remains at rest, and an object in motion continues in motion
with constant velocity (that is, constant speed in a straight line) unless the
object experiences a net external force.
Section 2 Newton’s First Law
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Resources
Chapter menu
Chapter 4
NET FORCE
• Newton's first law refers to the net force on an object.
• The net force is the vector sum of all forces acting on an
object.
• The net force on an object can be found by using the
methods for finding resultant vectors.
Section 2 Newton’s First Law
Although several forces are acting on this car,
the vector sum of the forces is zero. Thus, the
net force is zero, and the car moves at a
constant velocity.
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Resources
Chapter menu
Chapter 4
INERTIA
• Inertia is the tendency of an object to resist being moved or, if the object is
moving, to resist a change in speed or direction.
• Newton’s first law is often referred to as the law of inertia because it states that
in the absence of a net force, a body will preserve its state of motion.
• Mass is a measure of inertia.
In other words, a more massive object will have more inertia; a less massive object
will have less inertia.
Section 2 Newton’s First Law
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Resources
Chapter menu
Chapter 4
EQUILIBRIUM
• Equilibrium is the state in which the net force on an object is zero.
• Objects that are either at rest or moving with constant velocity
are said to be in equilibrium.
• Newton’s first law describes objects in equilibrium.
Tip: To determine whether a body is in equilibrium, find the net force. If the net
force is zero, the body is in equilibrium. If there is a net force, a second force
equal and opposite to this net force will put the body in equilibrium.
Section 2 Newton’s First Law
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Resources
Chapter menu
Chapter 4
NEWTON’S SECOND LAW
The acceleration of an object is directly proportional to the net force
acting on the object and inversely proportional to the object’s mass.
SF = ma
net force = mass  acceleration
Section 3 Newton’s Second and Third Laws
Where:
SF = the vector sum or the net force.
m = mass (kg)
a = acceleration (m/s ) 2
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Resources
Chapter menu
Chapter 4
NEWTON’S THIRD LAW
• If two objects interact, the magnitude of the force exerted on object 1 by
object 2 is equal to the magnitude of the force simultaneously exerted on
object 2 by object 1, and these two forces are opposite in direction.
• In other words, for every action, there is an equal and opposite reaction.
• Because the forces coexist, either force can be called the action or the
reaction.
Section 3 Newton’s Second and Third
Laws
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Resources
Chapter menu
Chapter 4
ACTION AND REACTION FORCES
• Action-reaction pairs do not imply that the net force on
either object is zero.
• The action-reaction forces are equal and opposite, but
either object may still have a net force on it.
Section 3 Newton’s Second and Third
Laws
Consider driving a nail into wood with a
hammer. The force that the nail exerts on
the hammer is equal and opposite to the
force that the hammer exerts on the nail.
But there is a net force acting on the nail,
which drives the nail into the wood.
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Resources
Chapter menu
Chapter 4
WEIGHT
• The gravitational force (Fg) exerted on an object by Earth is a vector quantity,
directed toward the center of Earth.
• The magnitude of this force (Fg) is a scalar quantity called weight.
• Weight changes with the location of an object in the universe.
Section 4 Everyday Forces
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Resources
Chapter menu
Chapter 4
WEIGHT, CONTINUED
• Calculating weight at any location:
Fg = mag
ag = free-fall acceleration at that location
• Calculating weight on Earth's surface:
ag = g = 9.81 m/s2
Fg = mg = m(9.81 m/s2)
Section 4 Everyday Forces
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Resources
Chapter menu
Chapter 4
NORMAL FORCE
• The normal force acts on a surface in a direction
perpendicular to the surface.
• The normal force is not always opposite in direction to
the force due to gravity.
Section 4 Everyday Forces
– In the absence of other forces, the
normal force is equal and opposite
to the component of gravitational
force that is perpendicular to the
contact surface.
– In this example, Fn = mg cos q.
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Resources
Chapter menu
Chapter 4
FRICTION
• Static friction is a force that resists the initiation of sliding
motion between two surfaces that are in contact and at rest.
• Kinetic friction is the force that opposes the movement of two
surfaces that are in contact and are sliding over each other.
• Kinetic friction is always less than the maximum static
friction.
Section 4 Everyday Forces
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Resources
Chapter menu
Chapter 4
FRICTION FORCES IN FREE-BODY DIAGRAMS
• In free-body diagrams, the force of friction is always parallel to the surface of contact.
• The force of kinetic friction is always opposite the direction of motion.
• To determine the direction of the force of static friction, use the principle of
equilibrium. For an object in equilibrium, the frictional force must point in the direction
that results in a net force of zero.
Section 4 Everyday Forces
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Resources
Chapter menu
Chapter 4
THE COEFFICIENT OF FRICTION
• The quantity that expresses the dependence of
frictional forces on the particular surfaces in contact is
called the coefficient of friction, m.
• Coefficient of kinetic friction:
Section 4 Everyday Forces
mk 
Fk
Fn
ms 
Fs,max
Fn
• Coefficient of static friction:
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Resources
Chapter menu
Chapter 4 Section 4 Everyday Forces
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Resources
Chapter menu
Chapter 4
AIR RESISTANCE
• Air resistance is a form of friction. Whenever an object
moves through a fluid medium, such as air or water, the
fluid provides a resistance to the object’s motion.
• For a falling object, when the upward force of air
resistance balances the downward gravitational force, the
net force on the object is zero. The object continues to move
downward with a constant maximum speed, called the
terminal speed.
Section 4 Everyday Forces
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Resources
Chapter menu
Chapter 4
FUNDAMENTAL FORCES
• There are four fundamental forces:
• Electromagnetic force
• Gravitational force
• Strong nuclear force
• Weak nuclear force
• The four fundamental forces are all field forces.
Section 4 Everyday Forces
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Resources
Chapter menu
SAMPLE PROBLEM 1: INERTIA
(LEAVE 1 FULL PAGE FOR EXPLANATION PROCESS)
• Which object has more inertia?
a) A 2.5 lb book
b) A 1.15 kg bag of rice
c) A 40 oz bag of nuts
d) 1050 g of cat food
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Resources
Chapter menu
SAMPLE PROBLEM 2: FREE-BODY DIAGRAM (FBD)
(LEAVE ½ PAGE FOR EXPLANATION PROCESS)
• Earth exerts a downward gravitational force of 8.9 N
on a cake that is resting on a plate. The plate exerts a
force of 11.0 N upward on the cake, and a knife exerts
a downward force of 2.1 N on the cake.
Draw a free-body diagram of the cake.
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Resources
Chapter menu
SAMPLE PROBLEM 3: FREE-BODY DIAGRAM (FBD)
(LEAVE ½ PAGE FOR EXPLANATION PROCESS)
• A chair is pushed forward with a force of 185 N.
The gravitational force of Earth on the chair is 155 N
downward, and the floor exerts a force of 155 N upward on the chair.
Draw a free-body diagram showing the forces acting on the chair.
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Resources
Chapter menu
SAMPLE PROBLEM 4: NEWTON’S II LAW OF
MOTION
(LEAVE ½ PAGE FOR EXPLANATION PROCESS)
• Roberto and Lucía are studying across from each other at a wide table. Laura
slides a 2.2 kg book toward Roberto. If the net force acting on the book is 1.6
N to the right, what is the book’s acceleration?
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Resources
Chapter menu
SAMPLE PROBLEM 5: NEWTON’S II LAW OF
MOTION
(LEAVE ½ PAGE FOR EXPLANATION PROCESS)
• Space-shuttle astronauts experience accelerations of about 35 m/s2 during
takeoff. What force does a 75-kg astronaut experience during an
acceleration of this magnitude?
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Resources
Chapter menu
SAMPLE PROBLEM 6: NEWTON’S II LAW OF
MOTION
(LEAVE ½ PAGE FOR EXPLANATION PROCESS)
• An 8.5-kg bowling ball initially at rest is dropped from the top of an 11-m
building. The ball hits the ground 1.5 s later. Find the net force on the falling
ball.
Copyright © by Holt, Rinehart and Winston. All rights reserved.
Resources
Chapter menu
SAMPLE PROBLEM 7: NEWTON’S II LAW OF
MOTION
(LEAVE 1 FULL PAGE FOR EXPLANATION
PROCESS)
Two forces are applied to a car in an effort to accelerate it, as shown below.
a. What is the resultant of these two forces?
b. If the car has a mass of 3200 kg, what acceleration does it have? (Disregard
friction.)

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Ch. 4 Physics PPTX.pdf

  • 1. Copyright © by Holt, Rinehart and Winston. All rights reserved. Resources Chapter menu GUIDELINES FOR NOTE-TAKING • Key terms in blue pen. Definitions in black pen. • Sample Problem (Titles) in red pen.
  • 2. Copyright © by Holt, Rinehart and Winston. All rights reserved. Resources Chapter menu Chapter 4 FORCE • A force is an action exerted on an object which may change the object’s state of rest or motion. • Forces can cause accelerations. • The SI unit of force is the newton, N. • Forces can act through contact or at a distance. Section 1 Changes in Motion
  • 3. Copyright © by Holt, Rinehart and Winston. All rights reserved. Resources Chapter menu Chapter 4 FORCE DIAGRAMS • The effect of a force depends on both magnitude and direction.Thus, force is a vector quantity. • Diagrams that show force vectors as arrows are called force diagrams. • Force diagrams that show only the forces acting on a single object are called free-body diagrams. Section 1 Changes in Motion
  • 4. Copyright © by Holt, Rinehart and Winston. All rights reserved. Resources Chapter menu Chapter 4 FORCE DIAGRAMS, CONTINUED In a force diagram, vector arrows represent all the forces acting in a situation. Section 1 Changes in Motion A free-body diagram shows only the forces acting on the object of interest—in this case, the car. Force Diagram Free-Body Diagram
  • 5. Copyright © by Holt, Rinehart and Winston. All rights reserved. Resources Chapter menu Chapter 4 NEWTON’S FIRST LAW • An object at rest remains at rest, and an object in motion continues in motion with constant velocity (that is, constant speed in a straight line) unless the object experiences a net external force. Section 2 Newton’s First Law
  • 6. Copyright © by Holt, Rinehart and Winston. All rights reserved. Resources Chapter menu Chapter 4 NET FORCE • Newton's first law refers to the net force on an object. • The net force is the vector sum of all forces acting on an object. • The net force on an object can be found by using the methods for finding resultant vectors. Section 2 Newton’s First Law Although several forces are acting on this car, the vector sum of the forces is zero. Thus, the net force is zero, and the car moves at a constant velocity.
  • 7. Copyright © by Holt, Rinehart and Winston. All rights reserved. Resources Chapter menu Chapter 4 INERTIA • Inertia is the tendency of an object to resist being moved or, if the object is moving, to resist a change in speed or direction. • Newton’s first law is often referred to as the law of inertia because it states that in the absence of a net force, a body will preserve its state of motion. • Mass is a measure of inertia. In other words, a more massive object will have more inertia; a less massive object will have less inertia. Section 2 Newton’s First Law
  • 8. Copyright © by Holt, Rinehart and Winston. All rights reserved. Resources Chapter menu Chapter 4 EQUILIBRIUM • Equilibrium is the state in which the net force on an object is zero. • Objects that are either at rest or moving with constant velocity are said to be in equilibrium. • Newton’s first law describes objects in equilibrium. Tip: To determine whether a body is in equilibrium, find the net force. If the net force is zero, the body is in equilibrium. If there is a net force, a second force equal and opposite to this net force will put the body in equilibrium. Section 2 Newton’s First Law
  • 9. Copyright © by Holt, Rinehart and Winston. All rights reserved. Resources Chapter menu Chapter 4 NEWTON’S SECOND LAW The acceleration of an object is directly proportional to the net force acting on the object and inversely proportional to the object’s mass. SF = ma net force = mass  acceleration Section 3 Newton’s Second and Third Laws Where: SF = the vector sum or the net force. m = mass (kg) a = acceleration (m/s ) 2
  • 10. Copyright © by Holt, Rinehart and Winston. All rights reserved. Resources Chapter menu Chapter 4 NEWTON’S THIRD LAW • If two objects interact, the magnitude of the force exerted on object 1 by object 2 is equal to the magnitude of the force simultaneously exerted on object 2 by object 1, and these two forces are opposite in direction. • In other words, for every action, there is an equal and opposite reaction. • Because the forces coexist, either force can be called the action or the reaction. Section 3 Newton’s Second and Third Laws
  • 11. Copyright © by Holt, Rinehart and Winston. All rights reserved. Resources Chapter menu Chapter 4 ACTION AND REACTION FORCES • Action-reaction pairs do not imply that the net force on either object is zero. • The action-reaction forces are equal and opposite, but either object may still have a net force on it. Section 3 Newton’s Second and Third Laws Consider driving a nail into wood with a hammer. The force that the nail exerts on the hammer is equal and opposite to the force that the hammer exerts on the nail. But there is a net force acting on the nail, which drives the nail into the wood.
  • 12. Copyright © by Holt, Rinehart and Winston. All rights reserved. Resources Chapter menu Chapter 4 WEIGHT • The gravitational force (Fg) exerted on an object by Earth is a vector quantity, directed toward the center of Earth. • The magnitude of this force (Fg) is a scalar quantity called weight. • Weight changes with the location of an object in the universe. Section 4 Everyday Forces
  • 13. Copyright © by Holt, Rinehart and Winston. All rights reserved. Resources Chapter menu Chapter 4 WEIGHT, CONTINUED • Calculating weight at any location: Fg = mag ag = free-fall acceleration at that location • Calculating weight on Earth's surface: ag = g = 9.81 m/s2 Fg = mg = m(9.81 m/s2) Section 4 Everyday Forces
  • 14. Copyright © by Holt, Rinehart and Winston. All rights reserved. Resources Chapter menu Chapter 4 NORMAL FORCE • The normal force acts on a surface in a direction perpendicular to the surface. • The normal force is not always opposite in direction to the force due to gravity. Section 4 Everyday Forces – In the absence of other forces, the normal force is equal and opposite to the component of gravitational force that is perpendicular to the contact surface. – In this example, Fn = mg cos q.
  • 15. Copyright © by Holt, Rinehart and Winston. All rights reserved. Resources Chapter menu Chapter 4 FRICTION • Static friction is a force that resists the initiation of sliding motion between two surfaces that are in contact and at rest. • Kinetic friction is the force that opposes the movement of two surfaces that are in contact and are sliding over each other. • Kinetic friction is always less than the maximum static friction. Section 4 Everyday Forces
  • 16. Copyright © by Holt, Rinehart and Winston. All rights reserved. Resources Chapter menu Chapter 4 FRICTION FORCES IN FREE-BODY DIAGRAMS • In free-body diagrams, the force of friction is always parallel to the surface of contact. • The force of kinetic friction is always opposite the direction of motion. • To determine the direction of the force of static friction, use the principle of equilibrium. For an object in equilibrium, the frictional force must point in the direction that results in a net force of zero. Section 4 Everyday Forces
  • 17. Copyright © by Holt, Rinehart and Winston. All rights reserved. Resources Chapter menu Chapter 4 THE COEFFICIENT OF FRICTION • The quantity that expresses the dependence of frictional forces on the particular surfaces in contact is called the coefficient of friction, m. • Coefficient of kinetic friction: Section 4 Everyday Forces mk  Fk Fn ms  Fs,max Fn • Coefficient of static friction:
  • 18. Copyright © by Holt, Rinehart and Winston. All rights reserved. Resources Chapter menu Chapter 4 Section 4 Everyday Forces
  • 19. Copyright © by Holt, Rinehart and Winston. All rights reserved. Resources Chapter menu Chapter 4 AIR RESISTANCE • Air resistance is a form of friction. Whenever an object moves through a fluid medium, such as air or water, the fluid provides a resistance to the object’s motion. • For a falling object, when the upward force of air resistance balances the downward gravitational force, the net force on the object is zero. The object continues to move downward with a constant maximum speed, called the terminal speed. Section 4 Everyday Forces
  • 20. Copyright © by Holt, Rinehart and Winston. All rights reserved. Resources Chapter menu Chapter 4 FUNDAMENTAL FORCES • There are four fundamental forces: • Electromagnetic force • Gravitational force • Strong nuclear force • Weak nuclear force • The four fundamental forces are all field forces. Section 4 Everyday Forces
  • 21. Copyright © by Holt, Rinehart and Winston. All rights reserved. Resources Chapter menu SAMPLE PROBLEM 1: INERTIA (LEAVE 1 FULL PAGE FOR EXPLANATION PROCESS) • Which object has more inertia? a) A 2.5 lb book b) A 1.15 kg bag of rice c) A 40 oz bag of nuts d) 1050 g of cat food
  • 22. Copyright © by Holt, Rinehart and Winston. All rights reserved. Resources Chapter menu SAMPLE PROBLEM 2: FREE-BODY DIAGRAM (FBD) (LEAVE ½ PAGE FOR EXPLANATION PROCESS) • Earth exerts a downward gravitational force of 8.9 N on a cake that is resting on a plate. The plate exerts a force of 11.0 N upward on the cake, and a knife exerts a downward force of 2.1 N on the cake. Draw a free-body diagram of the cake.
  • 23. Copyright © by Holt, Rinehart and Winston. All rights reserved. Resources Chapter menu SAMPLE PROBLEM 3: FREE-BODY DIAGRAM (FBD) (LEAVE ½ PAGE FOR EXPLANATION PROCESS) • A chair is pushed forward with a force of 185 N. The gravitational force of Earth on the chair is 155 N downward, and the floor exerts a force of 155 N upward on the chair. Draw a free-body diagram showing the forces acting on the chair.
  • 24. Copyright © by Holt, Rinehart and Winston. All rights reserved. Resources Chapter menu SAMPLE PROBLEM 4: NEWTON’S II LAW OF MOTION (LEAVE ½ PAGE FOR EXPLANATION PROCESS) • Roberto and Lucía are studying across from each other at a wide table. Laura slides a 2.2 kg book toward Roberto. If the net force acting on the book is 1.6 N to the right, what is the book’s acceleration?
  • 25. Copyright © by Holt, Rinehart and Winston. All rights reserved. Resources Chapter menu SAMPLE PROBLEM 5: NEWTON’S II LAW OF MOTION (LEAVE ½ PAGE FOR EXPLANATION PROCESS) • Space-shuttle astronauts experience accelerations of about 35 m/s2 during takeoff. What force does a 75-kg astronaut experience during an acceleration of this magnitude?
  • 26. Copyright © by Holt, Rinehart and Winston. All rights reserved. Resources Chapter menu SAMPLE PROBLEM 6: NEWTON’S II LAW OF MOTION (LEAVE ½ PAGE FOR EXPLANATION PROCESS) • An 8.5-kg bowling ball initially at rest is dropped from the top of an 11-m building. The ball hits the ground 1.5 s later. Find the net force on the falling ball.
  • 27. Copyright © by Holt, Rinehart and Winston. All rights reserved. Resources Chapter menu SAMPLE PROBLEM 7: NEWTON’S II LAW OF MOTION (LEAVE 1 FULL PAGE FOR EXPLANATION PROCESS) Two forces are applied to a car in an effort to accelerate it, as shown below. a. What is the resultant of these two forces? b. If the car has a mass of 3200 kg, what acceleration does it have? (Disregard friction.)