chapter 4 – forces and newton’s laws of motion

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Chapter 4 – Forces and Newton’s Laws of Motion

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Chapter 4 – Forces and Newton’s Laws of Motion. Newton’s First Law ( aka Law of Inertia). Objects maintain their state of motion unless acted on by a net external force. Inertia – resistance to change in motion. Mass – measure of an object’s inertia (in kg). Newton’s Second Law. - PowerPoint PPT Presentation

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Page 1: Chapter 4  – Forces and Newton’s Laws of Motion

Chapter 4 – Forces and Newton’s Laws of Motion

Page 2: Chapter 4  – Forces and Newton’s Laws of Motion

Newton’s First Law(aka Law of Inertia)

Objects maintain their state of motion unless acted on by a net

external force.

Page 3: Chapter 4  – Forces and Newton’s Laws of Motion

Inertia – resistance to change in motion.

Mass – measure of an object’s inertia (in kg)

Page 4: Chapter 4  – Forces and Newton’s Laws of Motion

Newton’s Second Law

maF net force mass acceleration(Newtons) (kg) (m/s2)

The net force is the total (vector) force on the object

Page 5: Chapter 4  – Forces and Newton’s Laws of Motion

Newton’s Second Lawin words…

The net force on object equals the mass of the object x it’s acceleration.

The acceleration of an object is inversely proportional to its mass.

Given the same net force, a small mass will accelerate more than a larger mass.

Page 6: Chapter 4  – Forces and Newton’s Laws of Motion

Units for Mass, Acceleration, and Force

System Mass Accel. Force

SI kg m/s2 newton (N)

CGS g cm/s2 dyne (dyn)

BE slug foot/s2 pound (lb)

Page 7: Chapter 4  – Forces and Newton’s Laws of Motion

Weight – force of gravity on a mass (Newtons)

F = ma

W = mg

A 1 kg object has a weight of W = mg

W = (1 kg)(9.8 m/s2)W= 9.8 N

Page 8: Chapter 4  – Forces and Newton’s Laws of Motion

Newton’s Third LawFor every action there is an equal

and opposite reaction.

Forces always occur in pairs.

Page 9: Chapter 4  – Forces and Newton’s Laws of Motion

Newton’s Third Law

Fhammer on nail = -Fnail on hammer

Page 10: Chapter 4  – Forces and Newton’s Laws of Motion

Newton’s Third LawIf one object exerts a force on

another, then the second object also exerts a force on the first; these

forces are equal in magnitude and opposite in direction. FA on B = -FB on A

Remember that the forces act on different objects and DO NOT cancel

out!

When determining the motion of an object, only consider the forces

acting ON the object.

Page 11: Chapter 4  – Forces and Newton’s Laws of Motion
Page 12: Chapter 4  – Forces and Newton’s Laws of Motion
Page 13: Chapter 4  – Forces and Newton’s Laws of Motion

An unfortunate box elder bug splatters against the windshield of a moving car. Compared to the force of the car on the bug, the force of the bug on the car is

a. largerb. smallerc. the samed. need more information to say

c. the same

Compared to the deceleration of the car, the deceleration of the windshield-hitting bug is

a. largerb. smallerc. the samed. need more information to say

a. larger

Page 14: Chapter 4  – Forces and Newton’s Laws of Motion

A box weighing 600 lbs is pushed along a horizontal floor at constant velocity with a force of 250 lbs parallel to the floor.

What is the net force on the box?

The net force is zero since the velocity is constant (no accel.)

A car weighs 2193 lb.

(a) What is the weight of the car in N? (b) What is the mass of the car in kg ?

(a) 9754 N (1 lb = 4.45 N)(b) 995 kg (W = mg, g = 9.8 m/s2)

Page 15: Chapter 4  – Forces and Newton’s Laws of Motion

ASSIGN: Chapter 4 #1-13 (odds), p. 121Due Thursday

Page 16: Chapter 4  – Forces and Newton’s Laws of Motion
Page 17: Chapter 4  – Forces and Newton’s Laws of Motion

Chapter 4 Conceptual Questions #1-18Page 118

Page 18: Chapter 4  – Forces and Newton’s Laws of Motion

An object must be moving for it to have inertia.

In a tug of war, the person who pulls with the most force wins.

If the net force on an object is zero, it can’t be moving.

In order for you to jump off the ground, you need to exert a force on the floor that is greater than the force the floor exerts on you.

Constant velocity requires that the acceleration be zero.

As a ball falls freely, the distance it falls each second is the same.

If a horse pulls on a wagon at rest, the wagon pulls back equally as much on the horse.

When given the same force, a heavy mass will have a larger acceleration than a lighter mass.

Neglecting air resistance, all objects fall at the same rate.

FALSE

FALSE

FALSE

FALSE

TRUE

TRUE

TRUE

FALSE

FALSE

Page 19: Chapter 4  – Forces and Newton’s Laws of Motion

If a horse pulls on a wagon at rest, the wagon pulls back equally as much on the horse. Will the wagon be set into motion?

a. No, because the forces cancel each other out.b. Yes, because there is a net force acting on the wagon.c. Yes, because there is time delay between action and reaction.d. Yes, only if the horse’s pull on the wagon is larger than the wagon’s pull on the horse.

b. Yes, because there is a net force acting on the wagon.

An object of mass 5 kg is acted upon by exactly four forces, each of magnitude 10 N. Which of the following could NOT be the resulting acceleration of the object?a. 0 m/s2

b. 2 m/s2

c. 4 m/s2

d. 8 m/s2

e. 10 m/s2

e. The maximum net force would be 40 N; 40N/5kg = 8 m/s2

Page 20: Chapter 4  – Forces and Newton’s Laws of Motion

Clearly state Newton’s Three Laws of Motion in your own words.

First Law – Objects maintain their state of motion until acted upon by a net external force.

Second Law – Given the same force, a more massive object will have a smaller acceleration than a less massive object.

F = ma

Third Law – Every force has an equal and opposite force.

Page 21: Chapter 4  – Forces and Newton’s Laws of Motion

Section 4.7 – The Gravitational Force

Newton’s Law of Universal Gravitation

All masses attract each other with a force determined by

1 22

mmF G

r

2

2-11 6.67259 10 N m

kgG x

masses (in kg)

distance b/w mass centers (m)

force of attraction

(in N)

Page 22: Chapter 4  – Forces and Newton’s Laws of Motion

Universal Gravitational Constant (G)

2

2-11 6.67259 10 N m

kgG x

Page 23: Chapter 4  – Forces and Newton’s Laws of Motion

The force of gravity between masses depends on The value of each massThe distance between their center of masses

Page 24: Chapter 4  – Forces and Newton’s Laws of Motion

Inverse Square Law – The force of gravity becomes 4x

less when r doubles.

Page 25: Chapter 4  – Forces and Newton’s Laws of Motion

True or False –

1.You exert the same amount of force on the earth as it exerts on you.

2. If you threw something fast enough it would never land.

3. The sun exerts more of a force on you than the moon.

TRUE!

TRUE!

TRUE!How many more

times?

Page 26: Chapter 4  – Forces and Newton’s Laws of Motion

Weightlessness – feeling experienced during free-fall due to lack of support force.

Apparent Weight – Weight read by a scale; reaction force applied to the person.

True Weight – Actual weight due to gravitational force.

Zero g or micro g – Zero acceleration of gravity experienced by astronaut; Not zero gravity, gravity holds them in orbit!

Page 27: Chapter 4  – Forces and Newton’s Laws of Motion

True or False –

1.There is barely any gravity in an orbiting space shuttle.

2. The earth exerts the same gravitational force on a falling penny as it does on a ton of bricks.3. Neglecting air resistance, a falling ton of bricks will fall faster than a falling penny.

FALSE!

FALSE!

FALSE!

Page 28: Chapter 4  – Forces and Newton’s Laws of Motion

Weight of objects on the surface of the earth

2E

E

m mW G

r

W m g g = 9.80 m/s2

Page 29: Chapter 4  – Forces and Newton’s Laws of Motion

ASSIGNMENT:Ch. 4 #18, 20, 24, 30

Due Friday

Page 30: Chapter 4  – Forces and Newton’s Laws of Motion
Page 31: Chapter 4  – Forces and Newton’s Laws of Motion

Section 4.8 – The Normal Force

The normal force (FN) is a support force that a surface exerts on an object.

FN = W since net force on box is zero.

Page 32: Chapter 4  – Forces and Newton’s Laws of Motion

Section 4.8 – The Normal Force

FN > W since box is being pressed down.

Page 33: Chapter 4  – Forces and Newton’s Laws of Motion

Section 4.8 – The Normal Force

FN < W since box is being lifted up.

Page 34: Chapter 4  – Forces and Newton’s Laws of Motion

Section 4.8 – The Normal Force

FN is always perpendicular to the surface.

Page 35: Chapter 4  – Forces and Newton’s Laws of Motion

Section 4.8 – The Normal Force

Apparent Weight – weight read by the scale.

True Weight – weight due to gravity.

Page 36: Chapter 4  – Forces and Newton’s Laws of Motion

Section 4.8 – The Normal Force

F ma y NF F mg

NF mg ma Apparent

Weight

TrueWeight

NF mg ma

Page 37: Chapter 4  – Forces and Newton’s Laws of Motion

Section 4.9 – Friction

Friction – force that opposes motion.

Depends on

1. Types of surfaces in contact

2. Amount of force pressing surfaces together (the normal force)

Does NOT depend on contact surface area (according to the books)

Page 38: Chapter 4  – Forces and Newton’s Laws of Motion

Static Friction (fs) – friction holding an object in place.

Kinetic Friction (fk) – friction while object is moving.

k k Nf F

coefficient of

static frictions

coefficient of

kinetic frictionk

MAXs s Nf F

Page 39: Chapter 4  – Forces and Newton’s Laws of Motion
Page 40: Chapter 4  – Forces and Newton’s Laws of Motion
Page 41: Chapter 4  – Forces and Newton’s Laws of Motion

ASSIGNMENT:

Read 4.8 – 4.9

Chapter 4 #34 – 39 (p. 123)

Page 42: Chapter 4  – Forces and Newton’s Laws of Motion

Help with solving problems…1. Draw a picture of the object; include all forces drawn with the

correct direction.2. Write an expression for the net force (ΣF). Have a separate

expression for the horizontal (x) and vertical (y) direction.3. Set the net force expression

equal to ma.4. Try substituting to eliminate the

number of variables. Keep trying!!

Page 43: Chapter 4  – Forces and Newton’s Laws of Motion

Tension (T) – the reaction force of a pulling on an object.

Pull w/ 100 N, box pulls back / 100 N.

Tension in rope is 100 N, not 200 N

Page 44: Chapter 4  – Forces and Newton’s Laws of Motion

Spring scale reads 100 N

What does spring scale read now?

100 N

Page 45: Chapter 4  – Forces and Newton’s Laws of Motion

Applying Newton’s 2nd Law

Equilibrium (a = 0)

Non-Equilibrium (a ≠ 0)

ΣFx = 0ΣFy = 0

ΣFx = max

ΣFy = may

Page 46: Chapter 4  – Forces and Newton’s Laws of Motion

Free-Body Diagrams – Show relative magnitudes and directions of all forces acting on an object.

Free-Body Diagrams help to visualize all the forces acting to determine the net force.

Don’t forget that ΣF = ma

Page 47: Chapter 4  – Forces and Newton’s Laws of Motion

Free-Body Diagram Examples…

A book is at rest on a table top.

A girl is suspended motionless from the ceiling by two ropes.

Page 48: Chapter 4  – Forces and Newton’s Laws of Motion

Free-Body Diagram Examples…

A rightward force is applied to a book in order to move it across a desk with a rightward acceleration. Consider

frictional forces. Neglect air resistance.

A rightward force is applied to a book in order to move it across a desk at constant velocity. Consider frictional forces. Neglect air resistance.

Page 49: Chapter 4  – Forces and Newton’s Laws of Motion

Free-Body Diagram Examples…

A car is coasting to the right and slowing down.

An leave is free-falling from a tree. Neglect air resistance.

Page 50: Chapter 4  – Forces and Newton’s Laws of Motion

Free-Body Diagram Examples…

A block on an inclined plane.

Page 51: Chapter 4  – Forces and Newton’s Laws of Motion

ASSIGNMENT: Ch. 4 #46,47,50,51,53,58,63,67

due Tuesday