chapter 4 forces and the laws of motion. aristotle’s view on motion

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Chapter 4 Forces and the Laws of Motion

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Page 1: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Chapter 4 Forces and the

Laws of Motion

Page 2: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Aristotle’s view on motion

Page 3: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Two types of Motion•Natural motion – either straight up or down

•Violent motion – was imposed motion, result of a force.

Page 4: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Force•A push or a pull exerted on some object.

Page 5: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Galileo’s view dispelled Aristotle’s • A force is not necessary

to keep an object moving.

• Introduced ‘friction’,

Page 6: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Friction• Force between materials

that are moving past one another.

• Force that opposes motion.

Page 7: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion
Page 8: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion
Page 9: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

The cause of an acceleration, or the

change in an object’s speed.

Page 10: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Newton (N)• SI/Metric unit of

force.• Is the amount of force

that, when acting on a 1 kg mass, produces an acceleration of 1 m/s2.

Page 11: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

A ‘dyne’ is the measurement of force when using

grams and centimeters.

Page 12: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

WeightIs the measure of the

magnitude of the gravitational force

exerted on an object.

Page 13: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Conversion Factor1 N = 0.225 lb

1 lb = 4.448 N

Page 14: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Figure out what your weight is in

Newton’s.

Page 15: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

190 lb 4.448 N 1 lb

845.12 N

Page 16: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Forces can act through:

1. Contact

2. At a distance

Page 17: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Contact Forces•A force that arises from the physical contact of two objects.

•Ex: Throwing a ball or pulling a sled.

Page 18: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Field ForcesA force that can exist between objects, even in the absence of physical contact between the objects.

Page 19: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

•Ex: force of gravity or attraction/repulsion of electrical charges.

Page 20: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

•The effect of a force depends upon the magnitude of the force and the direction of the force.

•Therefore, a force is a vector.

Page 21: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Force Diagram• Is a diagram, in which, all

forces acting on an object are represented by vector arrows.

• Sometimes these are called ‘free-body diagrams”.

Page 22: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Look at figures 4 – 3 & 4 – 4 on pages 126 – 128 .

Page 23: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Section 4 – 2: Newton’s First

Law

Page 24: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

An object at rest remains at rest, and an object in motion will continue in motion with a constant velocity (in a straight

line),

Page 25: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

unless the object experiences a net

external force.

Page 26: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Inertia

Is the tendency of an object to maintain its

state of motion.

Page 27: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Galileo said that every material object has a resistance to the change of its state of motion.

Page 28: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Newton’s first law is sometimes called the

‘Law of Inertia’Meaning that in the absence

of force a body will preserve its state of motion.

Page 29: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion
Page 30: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion
Page 31: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion
Page 32: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

What is “mass”?

•The amount of matter an object contains.

•Mass measures the inertia of an object.

Page 33: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

• All objects made of matter have inertia - that is, they resist accelerations (Newton’s First Law), but some objects resist more than others.

Page 34: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Mass is not Volume.• Mass is a scalar quantity.

• SI unit of mass is the kilogram (kg).

Page 35: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Mass is not Weight• Mass is a property of an object

that measures how much it resists accelerating.

• An object is difficult to accelerate because it has mass

Page 36: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Net External Force (Fnet)

Is the total force resulting from a combination of external forces on an

object; sometimes called the ‘resultant force’.

Page 37: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion
Page 38: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

The downward force due to gravity is the

object/body’s weight.The upward force is due

to the force exerted by the contact surface on

the object.

Page 39: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Ex 1: A man is pulling on his dog with a force of 70 N directed at an angle of

30 degrees to the horizontal. Find the x and y components of the force.

Page 40: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Force diagram

70 N

Page 41: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Force diagram

70 N

x

y

Page 42: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

X component: since we have a right triangle and know the angle and the hypotenuse. We will use the cosine trig function.

Page 43: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

adjcos = -----

hypFx = hyp cos

Fx = 70 cos 30

Fx = 60.6 N

Page 44: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

y component: since we have a right triangle and know the angle and the hypotenuse. We will use the sine trig function.

Page 45: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

oppsin = -----

hypFy = hyp sin

Fy = 70 sin 30

Fy = 35 N

Page 46: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Ex 2: A crate is pulled to the right with a force of 82 N, to the left with a force

115 N, upward with a force of 565 N, and

downward with a force of 236 N.

Page 47: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Force Diagram

565 N

82 N

236 N

115 N

Page 48: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

A) Find the net external force in the x direction.Remember: right is (+) and left is (-)

x = 82 N + (- 115 N) x = - 33 N

Page 49: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

B) Find the net external force in the y direction.Remember: up is (+) and down (-)

y = 565 N + (- 236 N) y = 329 N

Page 50: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

C) Find magnitude and direction of the

Fnet on the crate.

Fnet329 N

- 33 N

Page 51: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Use the Pythagorean Theorem to find Fnet

and the inverse tangent function to find the direction.

Page 52: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

22a c b

Page 53: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

22a c b22

netF yx

Page 54: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

22a c b22

netF yx 22

net 329)33(F

Page 55: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

22a c b22

netF yx 22

net 329)33(F

NFnet 7.330

Page 56: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

adj

opptan

Page 57: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

adj

opptan

adj

opp1tan

Page 58: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

33

329tan 1

Page 59: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

33

329tan 1

3.84

Page 60: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Since we are on the negative x-axis, this

is the same as an angle of 95.7o from the positive x-axis.

Page 61: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

In your notes do problems 3 & 4

on HPg 133.

Page 62: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Mass is a measurement of inertia.

Ex: A golf ball and a basketball, if the same Fnet acts on both, the golf ball will accelerate more.

Page 63: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

EquilibriumThe state in which there is no change in the body’s motion.

Page 64: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Equilibrium Means "Zero Acceleration"

Forces in balance:  

Equilibrium

Page 65: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

An object is in equilibrium when the vector sum of

the forces acting on it is equal to zero.

Page 66: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Is the object moving?

Yes, but at constant velocity.

Page 67: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Section 4-3: Newton’s Second and Third Laws

Page 68: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Force is proportional to mass and acceleration

Think about pushing a stalled car. If you try to push it by yourself, you can move it, but not very fast.

Page 69: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

However, if a couple of friends help, then it is much easier to move and you can

make it move faster quicker.

Page 70: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Newton’s 2nd LawThe acceleration of an object

is directly proportional to the Net External Force

(Fnet) acting on the object and inversely proportional

to the object’s mass.

Page 71: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

From this law we get:

m

Fa net

Normally it is written as:

maF

Page 72: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

a = F / m

Page 73: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

a = F / m

2a = 2 F / m

Page 74: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

a = F / m

2a = 2 F / m

a = 2 F / 2m

Page 75: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

a = F / m

Page 76: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

a = F / m

a/2 = F /2m

Page 77: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

a = F / m

a/2 = F /2m

a/3 = F / 3m

Page 78: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion
Page 79: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Note: remember that it is the Fnet that cause the

object to move.

Page 80: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Note:

2

kg 1 N 1s

m

Page 81: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Ex 3: Nathan applies a force of 20 N, causing the book to accelerate at a rate of 1.25 m/s2. What is the mass of

the book?

Page 82: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

G: a = 1.25 m/s2, Fnet = 20 N

U: m = ?

E: Fnet = ma or m = Fnet/a

S: m = 20 N / 1.25 m/s2

S: m = 16 kg

Page 83: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Ex 4: The Fnet on the propeller of a 3.2 kg

model airplane is 7.0 N forward. What is the acceleration of the

airplane?

Page 84: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

G: Fnet = 7.0 N, m = 3.2 kg

U: a = ?

E: Fnet= ma or a = Fnet/m

S: a = 7.0 N / 3.2 kg

S: a = 2.2 m/s2 forward

Page 85: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Remember the from Ch. 2

t

xvavg

Page 86: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Remember the from Ch. 2

2if

avg

vv

t

xv

Page 87: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Remember the from Ch. 2

t

vva if

2if

avg

vv

t

xv

Page 88: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Ex 5: A 2 kg otter starts from rest at the top of a

muddy incline 0.85 m long and slides down to the

bottom in 0.5 sec. What is the net external force?

Page 89: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

G: x = .85 m, t = 0.5s vi = 0 m/s, m = 2 kg

U: Fnet = ?We need to find the acceleration, but we need final speed first.

Page 90: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

We need to find the average speed first, than use that to find the final

speed.

t

xvavg

Page 91: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

sec5.0

85.0 mvavg

Page 92: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

sec5.0

85.0 mvavg

smvavg / 7.1

Page 93: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Using the 2nd average speed equation.

2if

avg

vvv

Rearrange for final speed

Page 94: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

iavgf vvv 2

Page 95: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

iavgf vvv 2

m/s 0m/s) 7.1(2 fv

Page 96: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

iavgf vvv 2

m/s 0m/s) 7.1(2 fv

m/s 4.3fv

Page 97: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Now we can find acceleration.

t

vva if

Page 98: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

s 5.0

m/s 0m/s 4.3 a

Page 99: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

s 5.0

m/s 0m/s 4.3 a

2m/s 8.6a

Page 100: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Now we can find Fnet

E: Fnet = ma

S: Fnet =(2 kg)(6.8 m/s2)

S: Fnet = 13.6 N

Page 101: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

On pg 138 (HP), Do Practice 4B: #

3 & 5.

Page 102: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Forces always exist in pairs.

Ex: When you push against the wall, the wall pushes

back. The forces are equal, but opposite.

Page 103: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Newton’s 3rd Law

Page 104: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

If two objects interact, the magnitude of the force exerted on object 1 by object 2 is equal

in magnitude of the force simultaneously exerted on

object 2 by object 1, and these two forces are opposite in

direction.

Page 105: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

A simpler alternative statement for

Newton’s 3rd Law:For every action,

there is an equal and opposite reaction.

Page 106: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion
Page 107: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Action-reaction pair

A pair of simultaneously equal, but opposite forces resulting from the interaction of 2 objects.

Page 108: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Action-Reaction forces each act on different objects.

They do not result in equilibrium.

Reread pg 139

Page 109: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion
Page 110: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion
Page 111: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion
Page 112: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Recoil is an example of the 3rd Law

Page 113: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Field Forces also exist in pairs.

Newton’s 3rd Law also applies to field forces.

Page 114: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

When an object is falling, its falling due to the force exerted by the earth, the reaction force is that the body is exerting an equal and opposite force on the

earth.

Page 115: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Why don’t we notice the this reaction force?

Because of Newton’s 2nd Law, the mass of the earth

is so great that the acceleration is so small it is

negligible.

Page 116: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Section 4-4: Everyday Forces

Page 117: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Weight (Fg)The magnitude of the force of gravity acting on an object.

Weight is NOT mass!

Page 118: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

The weight of an object depends on the object’s mass.

In fact, an object’s weight is directly proportional to the object’s mass.

Page 119: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

The weight of an object also depends on the object’s location.

Page 120: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

The weight of an object also depends on the object’s location.

In fact, an object’s weight is directly proportional to its free fall acceleration, g at its current location.

Page 121: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Fg= mgWhere g = 10 m/s2, unless

otherwise specified.Weight is dependent on the

force of gravity. It depends upon location. And acts downward.

Page 122: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

The farther away from the center of the earth, the less

‘g’ becomes.

Page 123: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Also, the gravitational pull of the moon is about 1/6th of the earth’s.

So if you way 180 lb or 900 N on earth you’d weigh 30 lb or 150 N on the moon.

Page 124: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

EX 6: A rocket with a mass of 10 kg is launched

vertically with a force of 150 N. What is the rocket’s

net force? What is the acceleration produced by

this net force?

Page 125: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

What forces are acting on this object?

Weight – downward

Force of Engine - upward

Page 126: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

G: m = 10 kg, g = 10 m/s2 Fengine = 150 N

U: Fnet = ?

E: Fnet = Fengine - Fg

Fnet = Fengine - mg

S: Fnet = 150 N - (10)(10)

S: Fnet = 50 N

Page 127: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Remember the net force is what accelerates the object.

U: a = ?

E: a = Fnet /mS: a = 50 N / 10 kgS: a = 5 m/s2

Page 128: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

EX 7: A 20 kg rocket is accelerated upwards

(vertically) at 3 m/s2. What is the Force that provides

this acceleration, this is the net force? What is the force

provided by the rocket’s engine?

Page 129: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

•Remember the Net Force causes the object to accelerate.

Page 130: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

G: a = 3 m/s2, m = 20 kg, g = 10 m/s2

U: Fnet = ?

E: Fnet = ma

S: Fnet = (20 kg)(3 m/s2)

S: Fnet = 60 N

Page 131: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

U: Fnet = Fengine - Fg

Fengine = Fnet + Fg

Fengine = Fnet + mg

Fengine = 60 + (20)(10)

Fengine = 260 N

Page 132: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Normal Force (FN)A force exerted by one object on another in a direction perpendicular to the surface of contact.

Page 133: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

N

Page 134: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

The normal force is always to the surface

of contact, but is not always opposite the direction of gravity.

Page 135: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion
Page 136: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

FN = Fg, but opposite if

The FN can be calculated by the equation FN = mgcos, if the object is on an inclination.

Page 137: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Fg

FN

The value for is the same for both.

Page 138: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion
Page 139: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Force of Friction

Is the force that opposes motion.

There are 2 types of friction:

Page 140: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Static Friction (Fs)

The resistive force that opposes relative motion of 2 contacting surfaces

that are at rest with respect with one another.

Page 141: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

As long as an object does not move when a force is applied:

As the applied force increase, the force of static friction increases. It increases until it reaches its max value Fs,max.

applieds FF

Page 142: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Once you exceed the max value the object begins to

move.

Page 143: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Kinetic Friction (Fk)

The resistive force that opposes the relative

motion of two contacting surfaces that are moving

past one another.

Page 144: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Since it is easier to keep an object moving than it is to start it moving, the kinetic friction is less

than static friction.kappliednet FFF

Page 145: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion
Page 146: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion
Page 147: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Frictional forces arise from the

complex interaction of the surfaces, at a microscopic level.

Page 148: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

It’s easier to push a chair than it is to move a desk

at the same speed.Since the desk is heavier,

it has a greater normal force.

Page 149: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Therefore, the force of friction is proportional to

the normal force.Also, friction depends upon the nature of the

surfaces in contact.

Page 150: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion
Page 151: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

The frictional force between a chair and tile floor is less than the the force between

a chair and carpet.

Page 152: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Coefficient of Friction

Is the ratio of the force of friction and the

normal force acting between the objects.

Page 153: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Ffriction

= ---------- Fnormal

Page 154: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Note: The coefficient of

friction has no units. From the equation

the units cancel out.

Page 155: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Coefficient of Kinetic Friction

N

kk F

F

Page 156: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Coefficient of Static Friction

N

ss F

F max,

Page 157: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

On pg 144, are values for the coefficient of

friction, for both static and kinetic.

Page 158: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion
Page 159: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Ex 8: A 19 kg crate initially at rest, on a

horizontal floor, requires a 75 N forces to set it in

motion. Find the coefficient of static

friction.

Page 160: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

G: m =19 kg, F =Fs =75 N

U: s = ?

E: Fs Fs

s = ----- = ------

FN mg

Page 161: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

S: 75 N

s= ---------------------

(19 kg)(10 m/s2)

S: s = 0.39

Page 162: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

From the Coefficient of friction what are the two surfaces in

contact?

Wood on Wood

Page 163: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Overcoming Friction Example

Page 164: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Ex 9: Andy pulls a wagon with a force of 90 N at an angle of 30o

to a horizontal surface. The mass of the wagon is 20 kg, and the coefficient of kinetic friction between the wagon and the side

walk is 0.50. Find the acceleration of the wagon due to

the net force.

Page 165: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Fg

FN

Fk

Fapplied

Page 166: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Which way does the object accelerate?

Only in the ‘x’ direction

Page 167: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

In order to find the acceleration, we will use

Newton’s 2nd Law.Fnet,x = max

We don’t know the Fnet,x, so we need to find it.

Page 168: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Since the object doesn’t move in the ‘Y’

direction the Fnet,y = 0 N. We need to find the net

force in the ‘x’ direction.

Page 169: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Fnet,x = Fapplied,x + Fk

Since the applied force is at an angle, we only want the x-

component.

Page 170: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Fapp,x = Fapp cos

Fapp,x = 90 N cos(30)

Fapp,x = 77.9 N

Page 171: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Next find the Fk

Fk = FN We need to find the Normal Force. Does it equal the weight?

Page 172: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

NO, since the Fapp

has a y-component. We know the net force in the y-direction is zero, so:

Fnet,y = FN + Fapp,y - Fg =0

Page 173: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

FN + Fapp,y - Fg = 0

FN = Fg - Fapp,y

Page 174: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Fg = mgFg = (20)(10)

Fg = 200 N

Page 175: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Fapp,y = Fapp sin

Fapp,y = 90N sin(30)

Fapp,y = 45N

Page 176: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

FN + Fapp,y - Fg = 0

FN = Fg - Fapp,y

FN= 200 N - 45N

FN = 155 N

Page 177: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Fk = kFN Fk = (0.50)(155 N)

Fk = 77.5 N to the left

So Fk = 77.5 N

Page 178: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Now, find the Fnet,x

Fnet,x = Fapp,x - Fk

Fnet,x =(77.9 N - 77.5 N)

Fnet,x = 0.4 N

Page 179: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Now, find the horizontal acceleration.

ax = Fnet,x /m

ax = 0.4 N / 20 kg

ax = 0.02 m/s2

Page 180: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Air Resistance is a form of friction (FR)

When an object moves through a fluid, that fluid provides resistance in the direction opposite of the object’s motion.

Page 181: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Terminal VelocityWhen a free falling body accelerates, the object’s

velocity increases. As the velocity increases, the object’s air resistance

increases.

Page 182: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

When the air resistance balances the force of

gravity, the net force is zero. The objects continues to move

downward at a constant maximum speed.

Page 183: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

The maximum speed a free-falling body reaches due to air resistance equaling the force of gravity.

Page 184: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Eventually, the force R of air

resistance becomes equal to the force exertedby the earth, and

the object reaches equilibrium.

Page 185: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Why does the heavierperson fall faster?

Page 186: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

What does Pressure mean to you?

• Under Pressure• Peer Pressure• Feeling Pressured• Air/Atmospheric• Tire

Page 187: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Pressure•The amount of force per unit area.

Page 188: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Force

Pressure = ----------

Area

Page 189: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion
Page 190: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Pressure Units•N/m2

•1 N/m2 = 1 Pascal (Pa)

Page 191: Chapter 4 Forces and the Laws of Motion. Aristotle’s view on motion

Ex: