chapter 4: forces in one dimension physics principles and problems

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Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

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Page 1: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Chapter 4: Forces in One DimensionChapter 4: Forces in One Dimension

PHYSICS Principles and

Problems

Page 2: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Net forces cause changes in motion.

BIG IDEA

CHAPTER

4 Forces in One Dimension

Page 3: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Section 4.1 Force and Motion

Section 4.2 Weight and Drag Force

Section 4.3 Newton’s Third Law

Table Of ContentsCHAPTER

4

Click a hyperlink to view the corresponding slides. Exit

Page 4: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

MAIN IDEA

A force is a push or a pull.

• What is a force?

• What is the relationship between force and acceleration?

• How does motion change when the net force is zero?

Essential Questions

SECTION4.1

Force and Motion

Page 5: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Review Vocabulary

• Acceleration the rate at which the velocity of an object changes.

New Vocabulary

• Force

• System

• Free-body diagram

• Newton’s second law

• Newton’s first law

• Inertia

• Equilibrium

SECTION4.1

Force and Motion

Page 6: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• Consider a textbook resting on a table. To cause it to move, you could either push or pull on it.

• A force is defined as a push or pull exerted on an object.

Force

SECTION4.1

Force and Motion

Page 7: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• If you push harder on an object, you have a greater effect on its motion.

• The direction in which force is exerted also matters. If you push the book to the right, the book moves to the right.

• The symbol F is a vector and represents the size and direction of a force, while F represents only the magnitude.

Force (cont.)

SECTION4.1

Force and Motion

Page 8: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• Forces can cause objects to speed up, slow down, or change direction as they move.

• Based on the definitions of velocity and acceleration, a force exerted on an object causes that object’s velocity to change; that is, a force causes an acceleration.

• All accelerations are the result of an unbalanced force acting on an object.

Force (cont.)

SECTION4.1

Force and Motion

Page 9: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• When considering how a force affects motion, it is important to identify the object of interest. This object is called the system.

• Everything around the object that exerts forces on it is called the external world.

Force (cont.)

SECTION4.1

Force and Motion

Page 10: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• Think about the different ways in which you could move a textbook.

• You could touch it directly and push or pull it, or you could tie a string around it and pull on the string. These are examples of contact forces.

Force (cont.)

SECTION4.1

Force and Motion

Page 11: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• A contact force exists when an object from the external world touches a system and thereby exerts a force on it.

Force (cont.)

SECTION4.1

Force and Motion

Page 12: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• There are other ways in which the motion of the textbook can change.

• If you drop a book, the gravitational force of Earth causes the book to accelerate, whether or not Earth is actually touching it. This is an example of a field force.

• Field forces are exerted without contact.

Force (cont.)

SECTION4.1

Force and Motion

Page 13: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• Forces result from interactions; thus, each force has a specific and identifiable cause called the agent.

• Without both an agent and a system, a force does not exist.

• A physical model which represents the forces acting on a system, is called a free-body diagram.

Force (cont.)

SECTION4.1

Force and Motion

Page 14: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Click image to view movie.

Force (cont.)

SECTION4.1

Force and Motion

Page 15: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• When the force vectors are in the same direction, they can be replaced by a vector with a length equal to their combined length.

• If the forces are in opposite directions, the resulting vector is the length of the difference between the two vectors, in the direction of the greater force.

• Vector sum of all the forces on an object is net force.

Combining Forces

SECTION4.1

Force and Motion

Page 16: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• To explore how forces affect an object’s motion, consider the situation explored in the figure, in which, a horizontal force is exerted on an object.

Acceleration and Force

SECTION4.1

Force and Motion

Page 17: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• Notice, in order to reduce complications resulting from the object rubbing against the surface, the investigation was performed on a smooth, well-polished table and the cart has wheels.

Acceleration and Force (cont.)

SECTION4.1

Force and Motion

Page 18: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• To exert a constant force, a spring scale was used to pull the cart.

• The velocity of the cart was measured for a period of time.

• Using the data, a velocity-time graph was constructed.

Acceleration and Force (cont.)

SECTION4.1

Force and Motion

Page 19: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• The data indicates for a constant force there is a constant acceleration on an object.

• Thus, indicating the relationship between force and acceleration is linear and allowing the application of the equation for a straight line:

• The y-intercept is 0, so the linear equation simplifies to y=kx. The y-variable is acceleration and x-variable is force.

Acceleration and Force (cont.)

SECTION4.1

Force and Motion

Page 20: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• What is the physical meaning of the slope of the acceleration-force graph?

• To determine this, increase the number of carts gradually.

Acceleration and Force (cont.)

SECTION4.1

Force and Motion

Page 21: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• A plot of the force versus acceleration for one, two, and three carts indicates that if the same force is applied in each situation, the acceleration of two carts is the acceleration of one cart and the acceleration of three carts is the acceleration of one cart.

Acceleration and Force (cont.)

SECTION4.1

Force and Motion

Page 22: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• This means that as the number of carts is increased, a greater force is needed to produce the same acceleration.

• The slopes of the lines in the graph depend upon the number of carts; that is, the slope depends on the total mass of the carts.

Acceleration and Force (cont.)

SECTION4.1

Force and Motion

Page 23: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Acceleration and Force (cont.)

SECTION4.1

Force and Motion

Page 24: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• The formula, F = ma, tells you that if you double the force, you will double the object’s acceleration.

• If you apply the same force to several different objects, the one with the most mass will have the smallest acceleration and the one with the least mass will have the greatest acceleration.

• One unit of force causes a 1-kg mass to accelerate at 1 m/s2, so one force unit has the dimensions 1 kg·m/s2 or one newton and is represented by N.

Acceleration and Force (cont.)

SECTION4.1

Force and Motion

Page 25: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• The observation that acceleration of an object is proportional to the net force exerted on it and inversely proportional to its mass is Newton’s second law, which can be represented in the following equation.

• Newton’s second law states that the acceleration of an object is equal to the sum of the forces (the net force) acting on the object, divided by the mass of the object.

Newton’s Second Law

SECTION4.1

Force and Motion

Page 26: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• One of the most important steps in correctly applying Newton’s second law is determining the net force acting on the object.

• Draw a free-body diagram showing the direction and relative strength of each force acting on the system.

• Then add the force vectors to find the net force.

Newton’s Second Law (cont.)

SECTION4.1

Force and Motion

Page 27: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• Next, use Newton’s second law to calculate the acceleration.

• Finally, if necessary, use what you know about accelerated motion to find the velocity or position of the object.

Newton’s Second Law (cont.)

SECTION4.1

Force and Motion

Page 28: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Anudja is holding a stuffed dog with a mass of 0.30 kg, when Sarah decides that she wants it and tries to pull it away from Anudja. If Sarah pulls horizontally on the dog with a force of 10.0 N and Anudja pulls with a horizontal force of 11.0 N, what is the horizontal acceleration of the dog?

Fighting Over a Toy

SECTION4.1

Force and Motion

Page 29: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Step 1: Analyze and Sketch the Problem• Sketch the situation. • Identify the stuffed dog as

the system and the direction in which Anudja pulls as positive.

• Draw the free-body diagram. Label the force.

Fighting Over a Toy

SECTION4.1

Force and Motion

Page 30: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Step 2: Solve for the Unknown

Fighting Over a Toy

SECTION4.1

Force and Motion

Page 31: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Identify known and unknown variables.

Unknown:

a = ?

Known:

m = 0.30 kg

FAnudja on dog = 11.0 N

FSarah on dog = 10.0 N

Fighting Over a Toy

SECTION4.1

Force and Motion

Page 32: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Use Newton’s second law to solve for a.

Fnet = FAnudja on dog + (-FSarah on dog)

Fighting Over a Toy

SECTION4.1

Force and Motion

Page 33: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Substitute Fnet= FAnudja on dog+ (–FSarah on dog)

Fighting Over a Toy

SECTION4.1

Force and Motion

Page 34: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Substitute FAnudja on dog = 11.0 N, FSarah on dog = 10.0 N, m

= 0.30 kg

Fighting Over a Toy

SECTION4.1

Force and Motion

Page 35: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Step 3: Evaluate the Answer

Fighting Over a Toy

SECTION4.1

Force and Motion

Page 36: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Are the units correct?

m/s2 is the correct unit for acceleration.

Does the sign make sense?

The acceleration is in the positive direction because Anudja is pulling in the positive direction with a greater force than Sarah is pulling in the negative direction.

Fighting Over a Toy

SECTION4.1

Force and Motion

Page 37: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Is the magnitude realistic?

It is a reasonable acceleration for a light, stuffed toy.

Fighting Over a Toy

SECTION4.1

Force and Motion

Page 38: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

The steps covered were:

Step 1: Analyze and Sketch the Problem

Sketch the situation.

Identify the stuffed dog as the system and the direction in which Anudja pulls as positive.

Draw the free-body diagram. Label the forces.

Fighting Over a Toy

SECTION4.1

Force and Motion

Page 39: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

The steps covered were:

Step 2: Solve for the Unknown

Step 3: Evaluate the Answer

Fighting Over a Toy

SECTION4.1

Force and Motion

Page 40: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• What is the motion of an object with no net force acting on it?

– Newton’s second law states says that if net force is zero, then acceleration equal zero.

– If acceleration is zero, then velocity does not change.

• A stationary object with no net force acting on it will stay at rest.

Newton’s First Law

SECTION4.1

Force and Motion

Page 41: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• What about a moving object like a rolling ball? How long will it roll? – Depends on the surface: thick carpet exerts more force

than a smooth hard surface like a bowling alley.– So the ball will stop rolling sooner on the carpet than

the bowling alley.

Newton’s First Law (cont.)

SECTION4.1

Force and Motion

Page 42: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• Galileo did many experiments, and he concluded that in the ideal case of zero resistance, horizontal motion would never stop.

• Galileo was the first to recognize that the general principles of motion could be found by extrapolating experimental results to the ideal case, in which there is no resistance to slow down an object’s motion.

Newton’s First Law (cont.)

SECTION4.1

Force and Motion

Page 43: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• In the absence of a net force, the motion (or lack of motion) of both the moving object and the stationary object continues as it was. Newton recognized this and generalized Galileo’s results in a single statement.

• This statement, “an object that is at rest will remain at rest, and an object that is moving will continue to move in a straight line with constant speed, if and only if the net force acting on that object is zero,” is called Newton’s first law.

Newton’s First Law (cont.)

SECTION4.1

Force and Motion

Page 44: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• Newton’s first law is sometimes called the law of inertia.

• Inertia is the tendency of an object to resist change.

• If an object is at rest, it tends to remain at rest.

• If it is moving at a constant velocity, it tends to continue moving at that velocity.

• Forces are results of interactions between two objects; they are not properties of single objects, so inertia cannot be a force.

Newton’s First Law (cont.)

SECTION4.1

Force and Motion

Page 45: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• If the net force on an object is zero, then the object is in equilibrium.

• An object is in equilibrium if its velocity is not changing.

• Newton’s first law identifies a net force as something that disturbs the state of equilibrium.

• Thus, if there is no net force acting on the object, then the object does not experience a change in speed or direction and is in equilibrium.

Newton’s First Law (cont.)

SECTION4.1

Force and Motion

Page 46: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• Some of the common types of forces are displayed on the right.

• When analyzing forces and motion, it is important to keep in mind that the world is dominated by resistance. Newton’s ideal, resistance-free world is not easy to visualize.

Newton’s First Law (cont.)

SECTION4.1

Force and Motion

Page 47: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Two horses are pulling a 100-kg cart in the same direction, applying a force of 50 N each. What is the acceleration of the cart?

A. 2 m/s2

B. 1 m/s2

C. 0.5 m/s2

D. 0 m/s2

SECTION4.1

Section Check

Page 48: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Reason: If we consider positive direction to be the direction of pull then, according to Newton’s second law,

SECTION4.1

Section Check

Answer

Page 49: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Two friends Mary and Maria are trying to pull a 10-kg chair in opposite directions. If Maria applied a force of 60 N and Mary applied a force of 40 N, in which direction will the chair move and with what acceleration?

SECTION4.1

Section Check

Page 50: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

A. The chair will move towards Mary with an acceleration of 2 m/s2.

B. The chair will move towards Mary with an acceleration of 10 m/s2.

C. The chair will move towards Maria with an acceleration of 2 m/s2.

D. The chair will move towards Maria with an acceleration of 10 m/s2.

SECTION4.1

Section Check

Page 51: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Reason: Since the force is applied in opposite directions, if we consider Maria’s direction of pull to be positive, then net force = 60 N – 40 N = 20 N . Thus, the chair will accelerate towards Maria.

Answer

SECTION4.1

Section Check

Page 52: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

State Newton’s first law.

Answer: Newton’s first law states that “an object that is at rest will remain at rest, and an object that is moving will continue to move in a straight line with constant speed, if and only if the net force acting on that object is zero”.

SECTION4.1

Section Check

Page 53: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems
Page 54: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

MAIN IDEA

Newton’s second law can be used to explain the motion of falling objects.

• How are the weight and the mass of an object related?

• How do actual weight and apparent weight differ?

• What effect does air have on falling objects?

Essential Questions

SECTION4.2

Weight and Drag Force

Page 55: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Review Vocabulary

• viscosity a fluid’s resistance to flowing.

New Vocabulary

• Weight

• Gravitational pull

• Apparent weight

• Weightlessness

• Drag force

• Terminal velocity

SECTION4.2

Weight and Drag Force

Page 56: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• Weight is the gravitational force experienced by an object.

• This gravitational force is a field force whose magnitude is directly proportional to the mass of the object experiencing the force:

Fg = mg, where m is the mass of the object and g is the gravitational field.

• Because weight is a force, the proper unit used to measure weight is the newton.

Weight

SECTION4.2

Weight and Drag Force

Page 57: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• Gravitational field is a vector quantity that relates the mass of an object to the gravitational force it experiences at a given location.

– Near Earth’s surface, g is 9.8N/kg toward Earth’s center.

• When you step on a scale, the scale exerts an upward force on you equal in magnitude to the gravitational force pulling down on you.

SECTION4.2

Weight and Drag Force

Weight (cont.)

• The scale is calibrated to convert the stretch of the springs, the upward force necessary to give a net force of zero, to weight .

Page 58: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Click image to view movie.

• Apparent weight and weightlessness.

SECTION4.2

Weight and Drag Force

Weight (cont.)

Page 59: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• When an object moves through any fluid, such as air or water, the fluid exerts a drag force on the moving object in the direction opposite to its motion.

• A drag force is the force exerted by a fluid on the object moving through the fluid.

• This force is dependent on the motion of the object, the properties of the object, and the properties of the fluid (viscosity and temperature) that the object is moving through.

SECTION4.2

Weight and Drag Force

Drag Force

Page 60: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• As a dropped tennis ball’s velocity increases, so does the drag force. The constant velocity that is reached when the drag force equals the force of gravity is called the terminal velocity.

SECTION4.2

Weight and Drag Force

Drag Force (cont.)

Page 61: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Click image to view movie.

SECTION4.2

Weight and Drag Force

Drag Force (cont.)

Page 62: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

If the mass of a person on Earth is 20 kg, what will be his mass on the Moon? (Gravity on the Moon is six times less than the gravity on Earth.)

SECTION4.2

Weight and Drag Force

Page 63: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Reason: The mass of an object does not change with the change in gravity, only the weight changes.

SECTION4.2

Weight and Drag Force

Answer

Page 64: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Your mass is 100 kg, and you are standing on a bathroom scale in an elevator. What is the scale reading when the elevator is falling freely?

SECTION4.2

Weight and Drag Force

Page 65: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Reason: Since the elevator is falling freely with acceleration g, the contact force between the elevator and you is zero. As scale reading displays the contact force, it would be zero.

SECTION4.2

Weight and Drag Force

Answer

Page 66: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

In which of the following cases will your apparent weight be greater than your real weight?

A. The elevator is at rest.

B. The elevator is accelerating upward.

C. The elevator is accelerating downward.

D. Apparent weight is never greater than real weight.

SECTION4.2

Weight and Drag Force

Page 67: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Reason: When the elevator is moving upward, your apparent weight Fapparent = ma + Fg (where m is your mass and a is the acceleration of the elevator). So your apparent weight becomes more than your real weight.

SECTION4.2

Weight and Drag Force

Answer

Page 68: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems
Page 69: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

MAIN IDEA

All forces occur in interaction pairs.

• What is Newton’s third law?

• What is the normal force?

Essential Questions

SECTION4.3

Newton’s Third Law

Page 70: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Review Vocabulary

• symmetry correspondence of parts on opposite sides of a dividing line.

New Vocabulary

• Interaction pair

• Newton’s third law

• Tension

• Normal force

SECTION4.3

Newton’s Third Law

Page 71: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• The forces FA on B and FB on A are an interaction pair.

• An interaction pair is two forces that are in opposite directions and have equal magnitude.

• When you exert a force on your friend to push him forward, he exerts an equal and opposite force on you, which causes you to move backward.

Interaction Pairs

SECTION4.3

Newton’s Third Law

Page 72: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• An interaction pair is also called an action-reaction pair of forces.

• This might suggest that one causes the other; however, this is not true.

• For example, the force of you pushing your friend doesn’t cause your friend to exert a force on you.

• The two forces either exist together or not at all.

• They both result from the contact between the two of you.

SECTION4.3

Newton’s Third Law

Interaction Pairs (cont.)

Page 73: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• The force of you on your friend is equal in magnitude and opposite in direction to the force of your friend on you.

• This is summarized in Newton’s third law, which states that all forces come in pairs.

SECTION4.3

Newton’s Third Law

Interaction Pairs (cont.)

Page 74: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• Newton’s Third Law states that the force of A on B is equal in magnitude and opposite in direction of the force of B on A.

• The two forces in a pair act on different objects and are equal and opposite.

• Numerically, FA on B = – FB on A

SECTION4.3

Newton’s Third Law

Interaction Pairs (cont.)

Page 75: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• When identifying an interaction pair, remember that they always occur in two different free-body diagrams and they always have the symmetry in subscripts noted on the previous slide.

SECTION4.3

Newton’s Third Law

Interaction Pairs (cont.)

Page 76: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Earth’s Acceleration

A softball has a mass of 0.18 kg. What is the gravitational force on Earth due to the ball, and what is Earth’s resulting acceleration? Earth’s mass is 6.0×1024 kg.

SECTION4.3

Newton’s Third Law

Page 77: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Step 1: Analyze and Sketch the Problem

• Draw free-body diagrams for the two systems: the ball and Earth.

• Connect the interaction pair by a dashed line.

SECTION4.3

Newton’s Third Law

Earth’s Acceleration (cont.)

Page 78: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Identify known and unknown variables.

Known:

mball = 0.18 kg

mEarth = 6.0×1024 kg

g = -9.80 m/s2

Unknown:

FEarth on ball = ?

aEarth = ?

SECTION4.3

Newton’s Third Law

Earth’s Acceleration (cont.)

Page 79: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Step 2: Solve for the Unknown

SECTION4.3

Newton’s Third Law

Earth’s Acceleration (cont.)

Page 80: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Use Newton’s second law to find the weight of the ball.

FEarth on ball = mballg

SECTION4.3

Newton’s Third Law

Earth’s Acceleration (cont.)

Page 81: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Substitute mball = 0.18 kg, g = -9.80 m/s2

FEarth on ball = (0.18 kg)(-9.80 m/s2)

= -1.8 N

SECTION4.3

Newton’s Third Law

Earth’s Acceleration (cont.)

Page 82: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Use Newton’s third law to solve for Fball on Earth.

Fball on Earth = –FEarth on ball

SECTION4.3

Newton’s Third Law

Earth’s Acceleration (cont.)

Page 83: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Substitute FEarth on ball = –1.8 N

Fball on Earth = – (– 1.8 N)

= +1.8N

SECTION4.3

Newton’s Third Law

Earth’s Acceleration (cont.)

Page 84: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Use Newton’s second and third laws to find aEarth.

SECTION4.3

Newton’s Third Law

Earth’s Acceleration (cont.)

Page 85: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Substitute Fnet = 1.8 N, mEarth= 6.0×1024 kg

SECTION4.3

Newton’s Third Law

Earth’s Acceleration (cont.)

Page 86: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Step 3: Evaluate the Answer

SECTION4.3

Newton’s Third Law

Earth’s Acceleration (cont.)

Page 87: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Are the units correct?

Dimensional analysis verifies force in N and acceleration in m/s2.

Does the sign make sense?

Force and acceleration should be positive.

SECTION4.3

Newton’s Third Law

Earth’s Acceleration (cont.)

Page 88: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Is the magnitude realistic?

Because of Earth’s large mass, the acceleration should be small.

SECTION4.3

Newton’s Third Law

Earth’s Acceleration (cont.)

Page 89: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

The steps covered were:

Step 1: Analyze and Sketch the Problem

Draw free-body diagrams for the two systems: the ball and Earth.

Connect the interaction pair by a dashed line.

Step 2: Solve for the Unknown

Step 3: Evaluate the Answer

SECTION4.3

Newton’s Third Law

Earth’s Acceleration (cont.)

Page 90: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

The force exerted by a string or rope is called tension.

At any point in a rope, the tension forces are pulling equally in both directions.

SECTION4.3

Newton’s Third Law

Tension

Page 91: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

SECTION4.3

Newton’s Third Law

Tension (cont.)

Page 92: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• The normal force is the perpendicular contact force exerted by a surface on another object.

• The normal force is important when calculating resistance.

The Normal Force

SECTION4.3

Newton’s Third Law

Page 93: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Explain Newton’s third law.

SECTION4.3

Section Check

Page 94: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Answer: Suppose you push your friend. The force of you on your friend is equal in magnitude and opposite in direction to the force of your friend on you. This is summarized in Newton’s third law, which states that forces come in pairs. The two forces in a pair act on different objects and are equal in strength and opposite in direction.

Newton’s third law FA on B = – FB on A

The force of A on B is equal in magnitude and opposite in direction of the force of B on A.

SECTION4.3

Answer

Section Check

Page 95: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

If a stone is hung from a rope with no mass, at which place on the rope will there be the most tension?

A. The top of the rope, near the hook.

B. The bottom of the rope, near the stone.

C. The middle of the rope.

D. The tension will be the same throughout the rope.

SECTION4.3

Section Check

Page 96: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Reason: Because the rope is assumed to be without mass, the tension everywhere in the rope is equal to the stone’s weight.

SECTION4.3

Section Check

Answer

Page 97: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems
Page 98: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Resources

Physics Online

Study Guide

Chapter Assessment Questions

Standardized Test Practice

CHAPTER

4 Forces in One Dimension

Page 99: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• A force is a push or a pull. Forces have both direction and magnitude. A force might be either a contact force or a field force.

• Newton’s second law states that the acceleration of a system equals the net force acting on it divided by its mass.

SECTION4.1

Force and Motion

Study Guide

Page 100: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• Newton’s first law states that an object that is at rest will remains at rest and an object that is moving will continue to move in a straight line with constant speed, if and only if the net force acting on that object is zero. An object with zero net force acting on it is in equilibrium.

SECTION4.1

Force and Motion

Study Guide

Page 101: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• The object’s weight (Fg) depends on the object’s mass and the gravitational field at the object’s location.

• An object’s apparent weight is the magnitude of the support force exerted on it. An object with no apparent weight experiences weightlessness.

SECTION4.2

Weight and Drag Force

Study Guide

Page 102: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• A falling object reaches a constant velocity when the drag force is equal to the object’s weight. The constant velocity is called the terminal velocity. The drag force on an object is determined by the object’s weight, size and shape as well as the fluid through which it moves.

SECTION4.2

Weight and Drag Force

Study Guide

Page 103: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• Newton’s third law states that the two forces that make up an interaction pair of forces are equal in magnitude, but opposite in direction and act on different objects. In an interaction pair, FA on B does not cause FB on A. The two forces either exist together or not at all.

SECTION4.3

Newton’s Third Law

Study Guide

Page 104: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

• The normal force is a support force resulting from the contact between two objects. It is always perpendicular to the plane of contact between the two objects.

SECTION4.3

Newton’s Third Law

Study Guide

Page 105: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

If you and your friend exert a force of 100 N each on a table, first in the same direction and then in opposite directions, what is the net force?

Combining Forces

CHAPTER

4 Forces in One Dimension

Chapter Assessment

Page 106: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

In the first case, your friend is pushing with a negative force of 100 N. Adding them together gives a total force of 0 N.

CHAPTER

4 Forces in One Dimension

Chapter Assessment

Combining Forces

Page 107: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

In the second case, your friend’s force is 100 N, so the total force is 200 N in the positive direction and the table accelerates in the positive direction.

CHAPTER

4 Forces in One Dimension

Chapter Assessment

Combining Forces

Page 108: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Newton’s second law can be rearranged to the form F = ma, which you learned about previously.

Assume that the table that you and your friend were pushing was 15.0 kg and the two of you each pushed with a force of 50.0 N in the same direction.

To find out what the acceleration of the table would be, calculate the net force, 50.0 N + 50.0 N = 100.0 N, and apply Newton’s second law by dividing the net force of 100.0 N by the mass of the table, 15.0 kg, to get an acceleration of 6.67 m/s2.

Newton’s Second Law

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4 Forces in One Dimension

Chapter Assessment

Page 109: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Tension forces are at work in a tug-of-war.

If team A, on the left, is exerting a force of 500 N and the rope does not move, then team B, must also be pulling with 500 N.

Forces of Ropes and Strings

CHAPTER

4 Forces in One Dimension

Chapter Assessment

Tim Fuller

Page 110: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Fighting Over a Toy

Anudja is holding a stuffed dog, with a mass of 0.30 kg, when Sarah decides that she wants it and tries to pull it away from Anudja. If Sarah pulls horizontally on the dog with a force of 10.0 N and Anudja pulls with a horizontal force of 11.0 N, what is the horizontal acceleration of the dog?

CHAPTER

4 Forces in One Dimension

Chapter Assessment

Page 111: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Earth’s Acceleration

When a softball with a mass of 0.18 kg is dropped, its acceleration toward Earth is equal to g, the acceleration due to gravity. What is the force on Earth due to the ball, and what is Earth’s resulting acceleration? Earth’s mass is 6.0×1024 kg.

CHAPTER

4 Forces in One Dimension

Chapter Assessment

Page 112: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

If a golf ball, baseball and bowling ball are thrown with the same force, which ball will move with a greater acceleration?

A. Golf ball

B. Baseball

C. Bowling ball

D. The three balls will have equal acceleration.

CHAPTER

4 Forces in One Dimension

Chapter Assessment

Page 113: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Reason: As , the lesser the

mass the greater the acceleration.

Since the golf ball has the least mass,

it will move with the greatest

acceleration.

CHAPTER

4 Forces in One Dimension

Chapter Assessment

Page 114: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Jack is boating in a river applying a contact force of 30 N, in a direction opposite to the flow of water. At the same time, the water is exerting a force of 30 N on the boat. In which direction will the boat move?

A. The boat will move in the direction of the flow of water.

B. The boat will not move at all.

C. The boat will move back and forth within a particular distance.

D. The boat will move in the direction opposite to the flow of water.

CHAPTER

4 Forces in One Dimension

Chapter Assessment

Page 115: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Reason: Since two equal and opposite forces are acting together, the net force is zero. Hence, the boat will not move at all.

CHAPTER

4 Forces in One Dimension

Chapter Assessment

Page 116: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

What is inertia?

A. Force.

B. The tendency of a body to stay only at rest

C. The tendency of a body to move with constant acceleration

D. The tendency of a body to move with constant velocity

CHAPTER

4 Forces in One Dimension

Chapter Assessment

Page 117: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Reason: Inertia of a body is the tendency of a body to stay at rest and/or to move with a constant velocity. Remember being at rest is simply a special case of constant velocity, v = 0 m/s.

CHAPTER

4 Forces in One Dimension

Chapter Assessment

Page 118: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

If the weight of a person on Earth is 120 N, what will his weight be on the Moon? (Gravity on the Moon is six times less than the gravity on Earth.)

A.

B.

C.

D.

CHAPTER

4 Forces in One Dimension

Chapter Assessment

Page 119: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Reason: Gravity on the Moon is .

Mass of the person is (since mass =

weight/g).

CHAPTER

4 Forces in One Dimension

Chapter Assessment

Page 120: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Weight of person on the Moon = Gravity on the Moon × mass of person

Reason:

So, the weight of the person on the

Moon .

CHAPTER

4 Forces in One Dimension

Chapter Assessment

Page 121: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

What happens when the drag force is equal to the force of gravity?

A. The object comes to rest.

B. The object moves with constant acceleration.

C. The object moves with constant velocity.

D. The velocity of the object increases.

CHAPTER

4 Forces in One Dimension

Chapter Assessment

Page 122: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Reason: When drag force equals the force due to gravity, the net force acting on the object is zero. As a result of this, the object moves with constant velocity, which is called terminal velocity.

CHAPTER

4 Forces in One Dimension

Chapter Assessment

Page 123: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

What is the acceleration of the car described by the graph on the right?

A. 0.20 m/s2

B. 0.40 m/s2

C. 1.0 m/s2

D. 2.5 m/s2

CHAPTER

4 Forces in One Dimension

Standardized Test Practice

Page 124: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

What distance will the car described by the above graph have traveled after 4.0 s?

A. 13 m

B. 40 m

C. 80 m

D. 90 m

CHAPTER

4 Forces in One Dimension

Standardized Test Practice

Page 125: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

If the car in the graph on the right maintains a constant acceleration, what will its velocity be after 10 s.

A. 10 km/h

B. 25 km/h

C. 90 km/h

D. 120 km/h

CHAPTER

4 Forces in One Dimension

Standardized Test Practice

Page 126: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

In a tug-of-war, 13 children, with an average mass of 30 kg each, pull westward on a rope with an average force of 150 N per child. Five parents, with an average mass of 60 kg each, pull eastward on the other end of the rope with an average force of 475 N per adult. Assuming that the whole mass accelerates together as a single entity, what is the acceleration of the system?

A. 0.62 m/s2 E

B. 2.8 m/s2 W

C. 3.4 m/s2 E

D. 6.3 m/s2 W

CHAPTER

4 Forces in One Dimension

Standardized Test Practice

Page 127: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

What is the weight of a 225-kg space probe on the Moon? The acceleration of gravity on the Moon is 1.62 m/s2.

A. 139 N

B. 364 N

C. 1.35×103 N

D. 2.21×103 N

CHAPTER

4 Forces in One Dimension

Standardized Test Practice

Page 128: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Maximize Your Score

If possible, find out how your standardized test will be scored. In order to do your best, you need to know if there is a penalty for guessing, and if so, what the penalty is. If there is no random-guessing penalty at all, you should always fill in an answer, even if you have not read the question.

CHAPTER

4 Forces in One Dimension

Standardized Test Practice

Test-Taking Tip

Page 129: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Forces Exerted on the Book

CHAPTER

4 Forces in One Dimension

Chapter Resources

Page 130: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Ball Tied to a String

CHAPTER

4 Forces in One Dimension

Chapter Resources

Page 131: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Ball Held in Your Hand

CHAPTER

4 Forces in One Dimension

Chapter Resources

Page 132: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

The Cart’s Motion Shown in a Linear Relationship

CHAPTER

4 Forces in One Dimension

Chapter Resources

Page 133: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Acceleration of Cart

CHAPTER

4 Forces in One Dimension

Chapter Resources

Page 134: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Force-Acceleration Graph

CHAPTER

4 Forces in One Dimension

Chapter Resources

Page 135: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Combining Forces

CHAPTER

4 Forces in One Dimension

Chapter Resources

Page 136: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Fighting Over a Toy

CHAPTER

4 Forces in One Dimension

Chapter Resources

Page 137: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

An Elevator Accelerating Upward

CHAPTER

4 Forces in One Dimension

Chapter Resources

Page 138: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

A Soccer Ball on a Table on Earth

CHAPTER

4 Forces in One Dimension

Chapter Resources

Page 139: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

Earth’s Acceleration

CHAPTER

4 Forces in One Dimension

Chapter Resources

Page 140: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

The Normal Force on an Object

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4 Forces in One Dimension

Chapter Resources

Page 141: Chapter 4: Forces in One Dimension PHYSICS Principles and Problems

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