chapter 5: displacement and force in two dimensions physics principles and problems

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Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

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Page 1: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Chapter 5: Displacement and Force in Two Dimensions

Chapter 5: Displacement and Force in Two Dimensions

PHYSICS Principles and

Problems

Page 2: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

BIG IDEA

Forces in two dimensions can be described using vector addition and vector resolution.

CHAPTER

5 Displacement and Force in Two Dimensions

Page 3: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Section 5.1 Vectors

Section 5.2 Friction

Section 5.3 Force in Two Dimensions

CHAPTER

5 Table Of Contents

Click a hyperlink to view the corresponding slides. Exit

Page 4: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

MAIN IDEA

All vectors can be broken into x- and y- components.

Essential Questions• How are vectors added graphically?

• What are the components of a vector?

• How are vectors added algebraically?

SECTION5.1

Vectors

Page 5: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Review Vocabulary

• Vector a quantity that has magnitude and direction.

New Vocabulary

• Components

• Vector resolution

SECTION5.1

Vectors

Page 6: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• So far in this course, we have only discussed vectors in one dimension but how can you set up a coordinate system for a net force when you are dealing with more than one dimension? And what happens when the forces are not at right angles to each other?

• Recall in previous discussions of adding vectors along a straight line, you learned the resultant vector always points from the tail of the first vector to the tip of the final vector.

• This process of adding vectors works even when the vectors do not point along the same straight line.

Vectors in Two Dimensions

SECTION5.1

Vectors

Page 7: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• If you are solving one of these two-dimensional problems graphically, you will need to use a protractor, both to draw the vectors at the correct angle and also to measure the direction and magnitude of the resultant vector.

• You can add vectors by placing them tip-to-tail and then drawing the resultant of the vector by connecting the tail of the first vector to the tip of the second vector.

SECTION5.1

Vectors

Vectors in Two Dimensions (cont.)

Page 8: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• If you move one of the vectors so that its tail is at the same place as the tip of the other vector, its length and direction do not change.

Vectors in Two Dimensions (cont.)

SECTION5.1

Vectors

Page 9: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• If you move a vector so that its length and direction are unchanged, the vector is unchanged.

• You can draw the resultant vector pointing from the tail of the first vector to the tip of the last vector and measure it to obtain its magnitude.

• Use a protractor to measure the direction of the resultant vector.

SECTION5.1

Vectors

Vectors in Two Dimensions (cont.)

Page 10: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• Sometimes you will need to use trigonometry to determine the length or direction of resultant vectors.

• If you are adding together two vectors at right angles, vector A pointing north and vector B pointing east, you could use the Pythagorean theorem to find the magnitude of the resultant, R.

SECTION5.1

Vectors

Vectors in Two Dimensions (cont.)

Page 11: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• If vector A is at a right angle to vector B, then the sum of the squares of the magnitudes is equal to the square of the magnitude of the resultant vector.

SECTION5.1

Vectors

Vectors in Two Dimensions (cont.)

Page 12: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• If you are adding two vectors that are at an angle other than 90°, then you can use the law of sines or the law of cosines.

Law of sines

• The magnitude of the resultant, divided by the sine of the angle between two vectors, is equal to the magnitude of one of the vectors divided by the angle between that component vector and the resultant vector.

SECTION5.1

Vectors

Vectors in Two Dimensions (cont.)

Page 13: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Law of cosines

• The square of the magnitude of the resultant vector is equal to the sum of the magnitude of the squares of the two vectors, minus two times the product of the magnitudes of the vectors, multiplied by the cosine of the angle between them.

SECTION5.1

Vectors

Vectors in Two Dimensions (cont.)

Page 14: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Finding the Magnitude of the Sum of Two VectorsFind the magnitude of the sum of a 15-km displacement and a 25-km displacement when the angle between them is 90° and when the angle between them is 135°.

SECTION5.1

Vectors

Page 15: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Step 1: Analyze and Sketch the Problem

Finding the Magnitude of the Sum of Two Vectors (cont.)

• Sketch the two displacement vectors, A and B, and the angle between them.

SECTION5.1

Vectors

Page 16: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Identify the known and unknown variables.

Known:

A = 25 km

B = 15 km

θ1 = 90°

θ2 = 135°

Unknown:

R = ?

SECTION5.1

Vectors

Finding the Magnitude of the Sum of Two Vectors (cont.)

Page 17: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Step 2: Solve for the Unknown

SECTION5.1

Vectors

Finding the Magnitude of the Sum of Two Vectors (cont.)

Page 18: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

When the angle is 90°, use the Pythagorean theorem to find the magnitude of the resultant vector.

SECTION5.1

Vectors

Finding the Magnitude of the Sum of Two Vectors (cont.)

Page 19: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Substitute A = 25 km, B = 15 km

SECTION5.1

Vectors

Finding the Magnitude of the Sum of Two Vectors (cont.)

Page 20: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

When the angle does not equal 90°, use the law of cosines to find the magnitude of the resultant vector.

SECTION5.1

Vectors

Finding the Magnitude of the Sum of Two Vectors (cont.)

Page 21: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Substitute A = 25 km, B = 15 km, θ2 = 135°.

SECTION5.1

Vectors

Finding the Magnitude of the Sum of Two Vectors (cont.)

Page 22: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Step 3: Evaluate the Answer

SECTION5.1

Vectors

Finding the Magnitude of the Sum of Two Vectors (cont.)

Page 23: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Are the units correct?

Each answer is a length measured in kilometers.

Do the signs make sense?

The sums are positive.

SECTION5.1

Vectors

Finding the Magnitude of the Sum of Two Vectors (cont.)

Page 24: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Are the magnitudes realistic?

The magnitudes are in the same range as the two combined vectors, but longer. This is because each resultant is the side opposite an obtuse angle. The second answer is larger than the first, which agrees with the graphical representation.

SECTION5.1

Vectors

Finding the Magnitude of the Sum of Two Vectors (cont.)

Page 25: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

The steps covered were:

Step 1: Analyze and Sketch the Problem

Sketch the two displacement vectors, A and B, and the angle between them.

SECTION5.1

Vectors

Finding the Magnitude of the Sum of Two Vectors (cont.)

Page 26: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

The steps covered were:Step 2: Solve for the Unknown

When the angle is 90°, use the Pythagorean theorem to find the magnitude of the resultant vector.

When the angle does not equal 90°, use the law of cosines to find the magnitude of the resultant vector.

SECTION5.1

Vectors

Finding the Magnitude of the Sum of Two Vectors (cont.)

Page 27: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

The steps covered were:

Step 3: Evaluate the answer

SECTION5.1

Vectors

Finding the Magnitude of the Sum of Two Vectors (cont.)

Page 28: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• What is the direction of the vector shown in the figure to the right?

• To determine the exact direction, we need to choose a coordinate system.

Vector Components

SECTION5.1

Vectors

Page 29: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• This coordinate system, such as the one in the center panel below, is similar to laying a grid drawn on a sheet of transparent plastic on top of a vector problem.

• You have to choose where to put the center of the grid (the origin) and establish the directions in which the axes point.

Vector Components (cont.)

SECTION5.1

Vectors

Page 30: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• When the motion you are describing is confined to the surface of Earth, it is often convenient to have the x-axis point east and the y-axis point north.

• When the motion involves an object moving through the air, the positive x-axis is often chosen to be horizontal and the positive y-axis vertical (upward).

• If the motion is on a hill, it’s convenient to place the positive x-axis in the direction of the motion and the y-axis perpendicular to the x-axis.

Vector Components (cont.)

SECTION5.1

Vectors

Page 31: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Click image to view movie.

Vector Components (cont.)

SECTION5.1

Vectors

Page 32: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Vector Components (cont.)

SECTION5.1

Vectors

Page 33: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• Two or more vectors (A, B, C, etc.) may be added by first resolving each vector into its x- and y-components.

• The x-components are added to form the x-component of the resultant:

Rx = Ax + Bx + Cx.

Algebraic Addition of Vectors

SECTION5.1

Vectors

Page 34: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• Similarly, the y-components are added to form the y-component of the resultant:

Ry = Ay + By + Cy.

Algebraic Addition of Vectors (cont.)

SECTION5.1

Vectors

Page 35: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• Because Rx and Ry are at a right angle (90°), the magnitude of the resultant vector can be calculated using the Pythagorean theorem, R2 = Rx

2 + Ry2.

SECTION5.1

Vectors

Algebraic Addition of Vectors (cont.)

Page 36: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• To find the angle or direction of the resultant, recall that the tangent of the angle that the vector makes with the x-axis is given by the following:

Angle of the Resultant Vector

SECTION5.1

Vectors

Algebraic Addition of Vectors (cont.)

Page 37: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• You can find the angle by using the tan−1 key on your calculator.

• Note that when tan θ > 0, most calculators give the angle between 0° and 90°, and when tan θ < 0, the angle is reported to be between 0° and −90°.

• You will use these techniques to resolve vectors into their components throughout your study of physics.

• Resolving vectors into components allows you to analyze complex systems of vectors without using graphical methods.

SECTION5.1

Vectors

Algebraic Addition of Vectors (cont.)

Page 38: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Jeff moved 3 m due north, and then 4 m due west to his friend’s house. What is the displacement of Jeff?

A. 3 + 4 m

B. 4 – 3 m

C. 32 + 42 m

D. 5 m

SECTION5.1

Section Check

Page 39: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Answer

Reason: When two vectors are at right angles to each other as in this case, we can use the Pythagorean theorem of vector addition to find the magnitude of the resultant, R.

SECTION5.1

Section Check

Page 40: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Reason: The Pythagorean theorem of vector addition states

If vector A is at a right angle to vector B, then the sum of squares of magnitudes is equal to the square of the magnitude of the resultant vector.

Answer

That is, R2 = A2 + B2

R2 = (3 m)2 + (4 m)2 = 5 m

SECTION5.1

Section Check

Page 41: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

C. 42 – 32 units

Calculate the resultant of the three vectors A, B, and C as shown in the figure.

(Ax = Bx = Cx = Ay = Cy = 1 units and By = 2 units)

A. 3 + 4 units

B. 32 + 42 units

SECTION5.1

D.

Section Check

Page 42: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Answer

Reason: Add the x-components to form, Rx = Ax + Bx + Cx.

Add the y-components to form, Ry = Ay + By + Cy.

SECTION5.1

Section Check

Page 43: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Answer

Reason: Since Rx and Ry are perpendicular to each other we can apply the Pythagorean theorem of vector addition:

R2 = Rx2 + Ry

2

SECTION5.1

Section Check

Page 44: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

If a vector B is resolved into two components Bx and By, and if is the angle that vector B makes with the positive direction of x-axis, which of the following formulae can you use to calculate the components of vector B?

A. Bx = B sin θ, By = B cos θ

B. Bx = B cos θ, By = B sin θ

C.

D.

SECTION5.1

Section Check

Page 45: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Answer

Reason: The components of vector B are calculated using the equation stated below.

SECTION5.1

Section Check

Page 46: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Answer

Reason:

SECTION5.1

Section Check

Page 47: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems
Page 48: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

MAIN IDEA

Friction is a type of force between two touching surfaces.

Essential Questions

• What is the friction force?

• How do static and kinetic friction differ?

SECTION5.2

Friction

Page 49: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Review Vocabulary

• Force push or pull exerted on an object.

New Vocabulary

• Kinetic friction

• Static friction

• Coefficient of kinetic friction

• Coefficient of static friction

SECTION5.2

Friction

Page 50: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• Push your hand across your desktop and feel the force called friction opposing the motion.

• So far, you have not considered friction in solving problems, but friction is all around you.

• There are two types of friction, and both always oppose motion.

Kinetic and Static Friction

SECTION5.2

Friction

Page 51: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• When you push a book across the desk, it experiences a type of friction that acts on moving objects.

• This force is known as kinetic friction, and it is exerted on one surface by another when the two surfaces rub against each other because one or both of them are moving.

Kinetic and Static Friction (cont.)

SECTION5.2

Friction

Page 52: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• To understand the other kind of friction, imagine trying to push a heavy couch across the floor. You give it a push, but it does not move.

• Because it does not move, Newton’s laws tell you that there must be a second horizontal force acting on the couch, one that opposes your force and is equal in size.

• This force is static friction, which is the force exerted on one surface by another when there is no motion between the two surfaces.

SECTION5.2

Friction

Kinetic and Static Friction (cont.)

Page 53: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• You might push harder and harder, as shown in the figure below, but if the couch still does not move, the force of friction must be getting larger.

SECTION5.2

Friction

Kinetic and Static Friction (cont.)

Page 54: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• This is because the static friction force acts in response to other forces.

• Finally, when you push hard enough, as shown in the figure below, the couch will begin to move.

SECTION5.2

Friction

Kinetic and Static Friction (cont.)

Page 55: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• Evidently, there is a limit to how large the static friction force can be. Once your force is greater than this maximum static friction, the couch begins moving and kinetic friction begins to act on it instead of static friction.

SECTION5.2

Friction

Kinetic and Static Friction (cont.)

Page 56: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• Frictional force depends on the materials that the surfaces are made of.

• For example, there is more friction between skis and concrete than there is between skis and snow.

• The normal force between the two objects also matters. The harder one object is pushed against the other, the greater the force of friction that results.

SECTION5.2

Friction

Kinetic and Static Friction (cont.)

Page 57: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• If you pull a block along a surface at a constant velocity, according to Newton’s laws, the frictional force must be equal and opposite to the force with which you pull.

• You can pull a block of known mass along a table at a constant velocity and use a spring scale, as shown in the figure, to measure the force that you exert.

SECTION5.2

Friction

Kinetic and Static Friction (cont.)

Page 58: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• You can then stack additional blocks on the block to increase the normal force and repeat the measurement.

SECTION5.2

Friction

Kinetic and Static Friction (cont.)

Page 59: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• Plotting the data will yield a graph like the one shown here. There is a direct proportion between the kinetic friction force and the normal force.

SECTION5.2

Friction

Kinetic and Static Friction (cont.)

Page 60: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• The different lines correspond to dragging the block along different surfaces.

• Note that the line corresponding to the sandpaper surface has a steeper slope than the line for the highly polished table.

SECTION5.2

Friction

Kinetic and Static Friction (cont.)

Page 61: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• You would expect it to be much harder to pull the block along sandpaper than along a polished table, so the slope must be related to the magnitude of the resulting frictional force.

SECTION5.2

Friction

Kinetic and Static Friction (cont.)

Page 62: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• The slope of this line, designated μk, is called the coefficient of kinetic friction between the two surfaces and relates the frictional force to the normal force, as shown below.

• The kinetic friction force is equal to the product of the coefficient of the kinetic friction and the normal force.

Kinetic Friction Force

SECTION5.2

Friction

Kinetic and Static Friction (cont.)

Page 63: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• The maximum static friction force is related to the normal force in a similar way as the kinetic friction force.

• The static friction force acts in response to a force trying to cause a stationary object to start moving. If there is no such force acting on an object, the static friction force is zero.

• If there is a force trying to cause motion, the static friction force will increase up to a maximum value before it is overcome and motion starts.

SECTION5.2

Friction

Kinetic and Static Friction (cont.)

Page 64: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• The static friction force is less than or equal to the product of the coefficient of the static friction and the normal force.

• In the equation for the maximum static friction force, μs is the coefficient of static friction between the two surfaces, and μsFN is the maximum static friction force that must be overcome before motion can begin.

Static Friction Force

SECTION5.2

Friction

Kinetic and Static Friction (cont.)

Page 65: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• Note that the equations for the kinetic and maximum static friction forces involve only the magnitudes of the forces.

• The forces themselves, Ff and FN, are at right angles to each other.

SECTION5.2

Friction

Kinetic and Static Friction (cont.)

Page 66: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• The table here shows coefficients of friction between various surfaces.

• Measurements of coefficients of friction are quite sensitive to the conditions of the surface: Surface impurities can affect the measurements.

SECTION5.2

Friction

Kinetic and Static Friction (cont.)

Page 67: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Balanced Friction Forces

You push a 25.0 kg wooden box across a wooden floor at a constant speed of 1.0 m/s. The coefficient of kinetic friction is 0.20. How large is the force that you exert on the box?

SECTION5.2

Friction

Page 68: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Step 1: Analyze and Sketch the Problem

Balanced Friction Forces (cont.)

• Identify the forces and establish a coordinate system.

SECTION5.2

Friction

Page 69: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• Draw a motion diagram indicating constant v and a = 0.

Step 1: Analyze and Sketch the Problem (cont.)

SECTION5.2

Friction

Balanced Friction Forces (cont.)

Page 70: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• Draw the free-body diagram.

Step 1: Analyze and Sketch the Problem (cont.)

SECTION5.2

Friction

Balanced Friction Forces (cont.)

Page 71: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Identify the known and unknown variables.

Known:

m = 25.0 kg

v = 1.0 m/s

a = 0.0 m/s2

μk = 0.20

Unknown:

Fp = ?

SECTION5.2

Friction

Balanced Friction Forces (cont.)

Page 72: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Step 2: Solve for the Unknown

SECTION5.2

Friction

Balanced Friction Forces (cont.)

Page 73: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

The normal force is in the y-direction, and there is no acceleration.

FN = - Fg

= - mg

SECTION5.2

Friction

Balanced Friction Forces (cont.)

Page 74: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Substitute m = 25.0 kg, g = -9.80 m/s2

FN = - 25.0 kg(-9.80 m/s2)

= 245 N

SECTION5.2

Friction

Balanced Friction Forces (cont.)

Page 75: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

The pushing force is in the x-direction; v is constant, thus there is no acceleration.

Fperson on box = μkFN

SECTION5.2

Friction

Balanced Friction Forces (cont.)

Page 76: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Substitute μk = 0.20, FN = 245N

Fperson on box = (0.20)(245N)

= 49 N

SECTION5.2

Friction

Balanced Friction Forces (cont.)

Page 77: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Step 3: Evaluate the Answer

SECTION5.2

Friction

Balanced Friction Forces (cont.)

Page 78: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Are the units correct?

Performing dimensional analysis on the units verifies that force is measured in kg·m/s2 or N.

Does the sign make sense?

The positive sign agrees with the sketch.

Is the magnitude realistic?

The force is reasonable for moving a 25.0 kg box.

SECTION5.2

Friction

Balanced Friction Forces (cont.)

Page 79: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

The steps covered were:

Step 1: Analyze and Sketch the Problem

Identify the forces and establish a coordinate system.

Draw a motion diagram indicating constant v and a = 0.

Draw the free-body diagram.

SECTION5.2

Friction

Balanced Friction Forces (cont.)

Page 80: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

The steps covered were:

Step 2: Solve for the Unknown

The normal force is in the y-direction, and there is no acceleration.

The pushing force is in the x-direction; v is constant, thus there is no acceleration.

Step 3: Evaluate the answer

SECTION5.2

Friction

Balanced Friction Forces (cont.)

Page 81: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Define friction force.

SECTION5.2

Section Check

Page 82: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

A force that opposes motion is called friction force. There are two types of friction force:

Answer

1) Kinetic friction—exerted on one surface by another when the surfaces rub against each other because one or both of them are moving.

2) Static friction—exerted on one surface by another when there is no motion between the two surfaces.

SECTION5.2

Section Check

Page 83: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Juan tried to push a huge refrigerator from one corner of his home to another, but was unable to move it at all. When Jason accompanied him, they where able to move it a few centimeters before the refrigerator came to rest. Which force was opposing the motion of the refrigerator?

A. static friction

B. kinetic friction

C. Before the refrigerator moved, static friction opposed the motion. After the motion, kinetic friction opposed the motion.

D. Before the refrigerator moved, kinetic friction opposed the motion. After the motion, static friction opposed the motion.

SECTION5.2

Section Check

Page 84: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Answer

Reason: Before the refrigerator started moving, the static friction, which acts when there is no motion between the two surfaces, was opposing the motion. But static friction has a limit. Once the force is greater than this maximum static friction, the refrigerator begins moving. Then, kinetic friction, the force acting between the surfaces in relative motion, begins to act instead of static friction.

SECTION5.2

Section Check

Page 85: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

On what does a friction force depend?

A. the material of which the surface is made

B. the surface area

C. speed of the motion

D. the direction of the motion

SECTION5.2

Section Check

A. the material of which the surface is made

B. the surface area

C. speed of the motion

D. the direction of the motion

Page 86: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Answer

Reason: The materials that the surfaces are made of play a role. For example, there is more friction between skis and concrete than there is between skis and snow.

SECTION5.2

Section Check

Page 87: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

A player drags three blocks in a drag race: a 50-kg block, a 100-kg block, and a 120-kg block with the same velocity. Which of the following statements is true about the kinetic friction force acting in each case?

A. The kinetic friction force is greatest while dragging the 50-kg block.

B. The kinetic friction force is greatest while dragging the 100-kg block.

C. The kinetic friction force is greatest while dragging the 120-kg block.

D. The kinetic friction force is the same in all three cases.

SECTION5.2

Section Check

Page 88: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Answer

Reason: Kinetic friction force is directly proportional to the normal force, and as the mass increases the normal force also increases. Hence, the kinetic friction force will be the most when the mass is the most.

SECTION5.2

Section Check

Page 89: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems
Page 90: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

MAIN IDEA

An object is in equilibrium if the net forces in the x-direction and in the y-direction are zero.

Essential Questions

• How can you find the force required for equilibrium?

• How do you resolve force vector components for motion along an inclined plane?

SECTION5.3

Forces in Two Dimensions

Page 91: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Review Vocabulary

• Equilibrium the condition in which the net force on an object is zero.

New Vocabulary

• Equilibrant

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Forces in Two Dimensions

Page 92: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• Now you will use your skill in adding vectors to analyze situations in which the forces acting on an object are at angles other than 90°.

• Recall that when the net force on an object is zero, the object is in equilibrium.

• According to Newton’s laws, the object will not accelerate because there is no net force acting on it; an object in equilibrium moves at constant velocity (Remember that being at rest is a state of constant velocity).

Equilibrium Revisited

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Forces in Two Dimensions

Page 93: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• It is important to realize that equilibrium can occur no matter how many forces act on an object. As long as the resultant is zero, the net force is zero and the object is in equilibrium.

• The figure here shows three forces exerted on a point object. What is the net force acting on the object?

Equilibrium Revisited (cont.)

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Forces in Two Dimensions

Page 94: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• Remember that vectors may be moved if you do not change their direction (angle) or length.

• To find the net force, you must add all the vectors together.

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Forces in Two Dimensions

Equilibrium Revisited (cont.)

Page 95: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• The figure here shows the addition of the three forces, A, B, and C.

• Note that the three vectors form a closed triangle.

• There is no net force; thus, the sum is zero and the object is in equilibrium.

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Forces in Two Dimensions

Equilibrium Revisited (cont.)

Page 96: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• Suppose that two forces are exerted on an object and the sum is not zero.

• How could you find a third force that, when added to the other two, would add up to zero, and therefore cause the object to be in equilibrium?

• To find this force, first find the sum of the two forces already being exerted on the object.

• This single force that produces the same effect as the two individual forces added together, is called the resultant force.

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Forces in Two Dimensions

Equilibrium Revisited (cont.)

Page 97: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• The force that you need to find is one with the same magnitude as the resultant force, but in the opposite direction.

• A force that puts an object in equilibrium is called an equilibrant.

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Forces in Two Dimensions

Equilibrium Revisited (cont.)

Page 98: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

The figure below illustrates the procedure for finding the equilibrant for two vectors.

This general procedure works for any number of vectors.

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Forces in Two Dimensions

Equilibrium Revisited (cont.)

Page 99: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Inclined Planes

Click image to view movie.

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Forces in Two Dimensions

Page 100: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• Because an object’s acceleration is usually parallel to the slope, one axis, usually the x-axis, should be in that direction.

• The y-axis is perpendicular to the x-axis and perpendicular to the surface of the slope.

• With this coordinate system, there are two forces—normal and frictional forces. These forces are in the direction of the coordinate axes. However, the weight is not.

Inclined Planes (cont.)

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Forces in Two Dimensions

Page 101: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• This means that when an object is placed on an inclined plane, the magnitude of the normal force between the object and the plane will usually not be equal to the object’s weight.

• You will need to apply Newton’s laws once in the x-direction and once in the y-direction.

• Because the weight does not point in either of these directions, you will need to break this vector into its x- and y-components before you can sum your forces in these two directions.

Inclined Planes (cont.)

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Forces in Two Dimensions

Page 102: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

If three forces A, B, and C are exerted on an object as shown in the following figure, what is the net force acting on the object? Is the object in equilibrium?

SECTION5.3

Section Check

Page 103: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

We know that vectors can be moved if we do not change their direction and length.

The three vectors A, B, and C can be moved (rearranged) to form a closed triangle.

Answer

SECTION5.3

Section Check

Page 104: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Since the three vectors form a closed triangle, there is no net force. Thus, the sum is zero and the object is in equilibrium. An object is in equilibrium when all the forces add up to zero.

SECTION5.3

Section Check

Answer

Page 105: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

How do you decide the coordinate system when the motion is along a slope? Is the normal force between the object and the plane the object’s weight?

SECTION5.3

Section Check

Page 106: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

An object’s acceleration is usually parallel to the slope. One axis, usually the x-axis, should be in that direction. The y-axis is perpendicular to the x-axis and perpendicular to the surface of the slope. With these coordinate systems, you have two forces—the normal force and the frictional force. Both are in the direction of the coordinate axes. However, the weight is not. This means that when an object is placed on an inclined plane, the magnitude of the normal force between the object and the plane will usually not be equal to the object’s weight.

Answer

SECTION5.3

Section Check

Page 107: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

A skier is coming down the hill. What are the forces acting parallel to the slope of the hill?

A. normal force and weight of the skier

B. frictional force and component of weight of the skier along the slope

C. normal force and frictional force

D. frictional force and weight of the skier

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Section Check

Page 108: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Reason: There is a component of the weight of the skier along the slope, which is also the direction of the skier’s motion. The frictional force will also be along the slope in the opposite direction from the direction of motion of the skier.

Answer

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Section Check

Page 109: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems
Page 110: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Physics Online

Study Guide

Chapter Assessment Questions

Standardized Test Practice

CHAPTER

5

Resources

Displacement and Force in Two Dimensions

Page 111: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• Vectors are added graphically by placing the tail of the second vector on the tip of the first vector. The resultant is the vector pointing from the tail of the first vector to the tip of the final vector.

Vectors

Study Guide

SECTION5.1

Page 112: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• The components of a vector are projections of the component vectors onto axes. Vectors can be summed by separately adding the x- and y- components.

Vectors

Study Guide

SECTION5.1

Page 113: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• When two vectors are at right angles, you can use the Pythagorean theorem to determine the magnitude of the resultant vector. The law of cosines and the law of sines can be used to find the resultant of any two vectors.

Vectors

Study Guide

SECTION5.1

Page 114: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• A frictional force acts when two surfaces touch.

• The kinetic friction force is equal to the coefficient of kinetic friction times the normal force. The static friction force is less than or equal to the coefficient of static friction times the normal force.

Frictions

Study Guide

SECTION5.2

Page 115: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

• The equilibrant is a force of the same magnitude but opposite direction as the sum of all the other forces acting on an object.

• Friction forces are parallel to an inclined plane but point up the plane if the motion of the object is down the plane. An object on an inclined plane has a component of the force of gravity parallel to the plane; this component can acceleration the object down the plane.

Forces in Two Dimensions

Study Guide

SECTION5.3

Page 116: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

If a vector R is resolved into two components Rx and Ry, what is the measure of the angle () formed between R and the positive direction of the x-axis?

A.

B.

C.

D.

Chapter Assessment

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5 Displacement and Force in Two Dimensions

Page 117: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Reason: To find the measure of the angle () formed between R and the positive direction of the x-axis, we make use of the tangent law.

Chapter Assessment

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5 Displacement and Force in Two Dimensions

Page 118: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Which of the following is the “Law of Sines” to find the magnitude of resultant vectors?

A.

B. 2 2 2= + 2 sin R A B AB θ

C.

D.

Chapter Assessment

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5 Displacement and Force in Two Dimensions

Page 119: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Reason: The “Law of Sines” is:

The magnitude of the resultant, divided by the sine of the angle between two vectors, is equal to the magnitude of one of the vectors divided by the angle between that component vector and the resultant vector.

That is,

Chapter Assessment

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5 Displacement and Force in Two Dimensions

Page 120: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

A force of 110 N is required to move a table of 120 kg. What is the coefficient of static friction (μs) between the table and the floor?

A.

B.

C.

D.

Chapter Assessment

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5 Displacement and Force in Two Dimensions

Page 121: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Reason: The coefficient of static friction is the ratio of the friction force to the normal force, or μs = Ff/FN.

Here .

Chapter Assessment

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5 Displacement and Force in Two Dimensions

Page 122: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Reason:

Here, FN = mg= (120 kg) (9.80 m/s2)

Chapter Assessment

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5 Displacement and Force in Two Dimensions

Page 123: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

If Ff, static is the static friction force, s is the coefficient of static friction, and FN is the normal force, which of the following formulae is correct?

A. Ff, static sFN

B. Ff, static = sFN

C. Ff, static sFN

D. Ff, static sFN

Chapter Assessment

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5 Displacement and Force in Two Dimensions

Page 124: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Reason: If there is a force trying to cause motion, the static friction force will increase up to a maximum value before it is overcome and motion starts, therefore Ff, static μsFN.

Where μsFN is the maximum static friction force that must be overcome before motion can begin.

Chapter Assessment

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5 Displacement and Force in Two Dimensions

Page 125: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

The magnitude of the force of friction depends on which of the following factors?

A. magnitude of normal force between the rubbing surfaces

B. the weights of the objects

C. direction in which the force is applied

D. surface area in contact

Chapter Assessment

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5 Displacement and Force in Two Dimensions

Page 126: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Reason: From the equations Ff, kinetic = μk FN and Ff,

static μsFN, we can state that the friction

force (Ff) is directly proportional to the

normal force (FN) between the rubbing

surfaces. That is, the magnitude of force of friction depends on the magnitude of the normal force between the rubbing surfaces.

Chapter Assessment

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5 Displacement and Force in Two Dimensions

Page 127: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Two tractors pull against a 1.00×103 kg log. If the angle of the tractor’s chains in relation to each other is 18.0°, and each tractor pulls with a force of 8×102 N, what forces will they be able to exert?

A. 250 N

B. 1.52×103 N

C. 1.58×103 N

D. 1.60×103 N

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Standardized Test Practice

Page 128: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

An airplane pilot tries to fly directly east with a velocity of 800.0 km/h. If a wind comes from the southwest at 80.0 km/h, what is the relative velocity of the airplane to the surface of Earth?

A. 804 km/h, 5.7° N of E

B. 804 km/h, 8.4° N of E

C. 859 km/h, 4.0° N of E

D. 880 km/h, 45° N of E

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Standardized Test Practice

Page 129: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

For a winter fair, some students decide to build 30-kg wooden pull-carts on sled skids. If two 90-kg passengers get in, how much force will the puller have to exert to move the pull-cart? The coefficient of maximum static friction between the cart and the snow is 0.15.

A. 1.8×102 N

B. 3.1×102 N

C. 2.1×103 N

D. 1.4×104 N

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5 Displacement and Force in Two Dimensions

Standardized Test Practice

Page 130: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

It takes a minimum force of 280 N to move a 5.0-kg crate. What is the coefficient of maximum static friction between the crate and the floor?

A. 0.18

B. 0.57

C. 1.8

D. 5.6

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5 Displacement and Force in Two Dimensions

Standardized Test Practice

Page 131: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

What is the y component of a 95.3-N force that is exerted at 57.1° to the horizontal?

A. 51.8 N

B. 80.0 N

C. 114 N

D. 175 N

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5 Displacement and Force in Two Dimensions

Standardized Test Practice

Page 132: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Calculators Are Only Machines

Test-Taking Tip

If your test allows you to use a calculator, use it wisely. Figure out which numbers are relevant, and determine the best way to solve the problem before you start punching keys.

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5 Displacement and Force in Two Dimensions

Standardized Test Practice

Page 133: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Magnitude of the Sum of Two Vectors

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5 Displacement and Force in Two Dimensions

Chapter Resources

Page 134: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Finding the Magnitude of the Sum of Two Vectors

Find the magnitude of the sum of a 15-km displacement and a 25-km displacement when the angle between them is 90° and when the angle between them is 135°.

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5 Displacement and Force in Two Dimensions

Chapter Resources

Page 135: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Coordinate System and Component Vectors

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Chapter Resources

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Sign of a Component Depends on the Quadrant

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Chapter Resources

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Algebraic Addition of Vectors

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Chapter Resources

Page 138: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Understanding Static Friction

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Chapter Resources

Page 139: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Pulling a Block Using a Spring Scale

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5 Displacement and Force in Two Dimensions

Chapter Resources

Page 140: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Coefficient of Kinetic Friction for Different Surfaces

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Chapter Resources

Page 141: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Balanced Friction Forces

You push a 25.0 kg wooden box across a wooden floor at a constant speed of 1.0 m/s. How much force do you exert on the box?

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5 Displacement and Force in Two Dimensions

Chapter Resources

Page 142: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Pushing a Wooden Box

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Chapter Resources

Page 143: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

Motion and Free-body Diagram for Pushing a Wooden Box

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5 Displacement and Force in Two Dimensions

Chapter Resources

Page 144: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

An Object in Equilibrium

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Chapter Resources

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The Equilibrant Forces

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5 Displacement and Force in Two Dimensions

Chapter Resources

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Skier Sliding Down a Slope

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5 Displacement and Force in Two Dimensions

Chapter Resources

Page 147: Chapter 5: Displacement and Force in Two Dimensions PHYSICS Principles and Problems

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