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Phy 201: General Physics I

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Phy 201: General Physics I. Chapter 4: Forces & Newton’s Laws of Motion Lecture Notes. Newton’s 1 st Law. Every object continues in its state of rest, or of motion unless compelled to change that state by forces impressed upon it. Also known as the “Law of Inertia” Key Points: - PowerPoint PPT Presentation
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Phy 201: General Physics I Chapter 4: Forces & Newton’s Laws of Motion Lecture Notes
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Page 1: Phy 201: General Physics I

Phy 201: General Physics I

Chapter 4: Forces & Newton’s Laws of Motion

Lecture Notes

Page 2: Phy 201: General Physics I

Newton’s 1st Law

• Also known as the “Law of Inertia” • Key Points:

– When an object is moving in uniform linear motion it has no net force acting on it

– When there is no net force acting on an object, it will stay at rest or maintain its constant speed in a straight line

• This property of matter to maintain uniform motion is called inertia

• Stated a simpler way: Nature is lazy! {i.e. matter resists changes in motion}

F=0 a = 0 {v = constant}

Every object continues in its state of rest, or of motion unless compelled to change that state by forces impressed upon it.

Page 3: Phy 201: General Physics I

Newton’s 2nd Law• When a net force is exerted on an object its velocity will

change:

• The time rate of change of motion (acceleration) is related to:– Proportional to the size of the net force– Inversely proportional to the mass of the object (i.e. its inertia)

• The relationship between them is

or

• The direction of will always correspond to the direction of

ˆ ˆx y

F 1a= = F x + F y

m m

ˆ ˆ

x yF = ma= m a x + a y

...1 2 3F=F F F dv

dt

a

F

Page 4: Phy 201: General Physics I

Newton’s 3rd LawWhen an object exerts a force on a second object, the second

object exerts an equal but oppositely directed force on the first object

where:

Consequences:• Forces always occur in action-reaction pairs (never by themselves)• Each force in an action-reaction pair acts on a different object

Important: • Newton’s 3rd law identifies the forces produced by interactions

between bodies• Newton’s 2nd law defines the accelerations that each object

undergoes

1 on 2FBody 1 Body 2

2 on 1F

2 on 1 1 on 2F F

Page 5: Phy 201: General Physics I

Free-Body Diagrams• Simplified drawing of a body with only the forces acting on

it specified• The forces are drawn as vectors• Free-Body diagrams facilitate the application of Newton’s

2nd Law

Examples:

Joey

W

Joey in “Free Fall”

Joey

W

floorF

Joey standing on a floor

Joey

W

floorF

Joey getting slapped while standing on a floor

slapF

Page 6: Phy 201: General Physics I

Types of Forces

Non-Contact:• Gravitational• Electric• Magnetic

Contact:• Normal• Frictional• Tension

In our world, forces can be categorized as one of 2 types:

• Non-Contact: force is exerted over a distance of space with out direct contact (a.k.a. “action-at-a-distance” forces)

• Contact: forces is exerted due to direct contact

(Note: at the microscopic level, ALL forces are non-contact)

• In either case, Newton’s 3rd law still applies to the forces present

Examples of each type of force:

Page 7: Phy 201: General Physics I

Mass vs. Weight• The “weight” of an object is the gravitational force

exerted on it by the gravitational attraction between the object and its environment:

• On the surface of the Earth, the gravitational force is referred to as weight:

• Mass is a measure of an object’s inertia (measured in kg)

– Independent of object location• Weight is the effect of gravity on an object’s mass

(measured in N)– Determined by the local gravitational acceleration

surrounding the object

ˆG G G G G G GF =ma =ma y F =m a F =ma

ˆG GF = W = (-mg)y F = W = mg

Notes:• Mass is a measure of an object’s inertia (measured in kg)

– Independent of object location• Weight is the effect of gravity on an object’s mass (measured in N)

– Determined by the local gravitational acceleration surrounding the object

Page 8: Phy 201: General Physics I

Normal Force

• The “support” force between 2 surfaces in contact• Direction is always perpendicular (or normal) to the plane of the

area of contactExample: the force of floor that supports your weight

Consider standing on a scale on the floor of an elevator. The reading of the scale is equal to the normal force it exerts on you:Task: Construct free body diagrams for the scale:

1. At rest2. Constant velocity3. Accelerating upward4. Accelerating downward

Page 9: Phy 201: General Physics I

Examples of Normal Force

Page 10: Phy 201: General Physics I

Surface Frictional Forces• When an object moves or tends to move along a surface, there

is an interaction between the microscopic contact points on the 2 surfaces. This interaction results in a frictional force, that is– parallel to the surface– opposite to the direction of the motion

• There are 2 types of surface friction:– Static (sticking)– Kinetic (sliding)

Page 11: Phy 201: General Physics I

Static Friction• Static (or sticking) friction ( ) is the frictional force

exerted when the object tends to move, but the external force is not yet strong enough to actually move the object.

• Increasing the applied force, the static frictional force increases as well (so the net force is zero) . The force just before breakaway is the maximum static frictional force.

• The direction of the static friction force is always in opposition to the external forces(s) acting on the body

• The magnitude of the maximum static friction force is:

Where:– is the coefficient (maximum) of static friction– FN is the normal force

max maxs s Nf =μ F

sf

maxsμ

Page 12: Phy 201: General Physics I

Kinetic Friction• Kinetic frictional force ( ) is the frictional force exerted by the

surface on an object that is moving along the surface• Kinetic frictional force:

– always opposes the direction of the motion– the direction is along the surface (parallel to the surface)

• The magnitude of the kinetic frictional force depends only on the normal force and the properties of the 2 surfaces in contact

Where:– k is the coefficient of kinetic friction– FN is the normal force

Notes:– Kinetic friction is independent to the rate of travel of the sliding body– Kinetic friction is independent to the surface area of contact

k k Nf =μ F

kf

Page 13: Phy 201: General Physics I

Tension Force

• Force applied through a rope or cable• When the rope or cable is mass-less (negligible

compared to the bodies it is attached to) it can be treated as a connection between 2 bodies– No mass means no force needed to accelerate rope– Force of pull transfers unchanged along the rope – Action force at one end is the same as the Reaction

force at the other end

• When attached to a pulley the tension force can be used to change the direction of force acting on a body

• Calculation of a tension force is usually an intermediate step to connecting the free-body diagrams between 2 attached objects

Page 14: Phy 201: General Physics I

Tension Applications

• With Pulley (flat surface):

• Inclined Plane:

• Atwood Machine:

M1

M2

M1

M2

M1 M2

Page 15: Phy 201: General Physics I

Sir Isaac Newton (1642-1727)• Greatest scientific mind of the late 17th century• Invented the “calculus” (independently but

simultaneously with Gottfried Wilhelm Leibnitz)

• Among his accomplishments included:– A Particle Theory Light & Optics– A Theory of Heat & Cooling

• Established 3 Laws of Motion• Proposed the Law of Universal Gravitation (to

settle a parlor bet proposed by Christopher Wren!!)– The competition was actually between Edward

Haley & Robert Hooke– This theory successfully explained planetary motion

and elliptical orbits

“If I have seen further it is by standing on the shoulders of giants.”


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