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1 UCT PHY1025F: Mechanics Physics 1025F Mechanics Dr. Steve Peterson Steve.peterson@uct .ac.za NEWTON’S LAWS

Physics 1025F Mechanics

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Physics 1025F Mechanics. NEWTON’S LAWS. Dr. Steve Peterson [email protected]. Chapter 4: Newton’s Laws of Motion. Dynamics is the description of why objects move and the connection between forces and motion. Why do objects move?. - PowerPoint PPT Presentation

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Page 1: Physics 1025F Mechanics

1UCT PHY1025F: Mechanics

Physics 1025FMechanics

Dr. Steve [email protected].

za

NEWTON’S LAWS

Page 2: Physics 1025F Mechanics

2UCT PHY1025F: Mechanics

Chapter 4: Newton’s Laws of MotionDynamics is the description of why objects move and the

connection between forces and motion

Page 3: Physics 1025F Mechanics

3UCT PHY1025F: Mechanics

Why do objects move?What is the “natural state” of an object [Aristotle, ~350 BC]?

- In Motion or At Rest?

What if we remove friction (the idealized case [Galileo, ~1600 AD])?

Page 4: Physics 1025F Mechanics

4UCT PHY1025F: Mechanics

Newton’s First Law of MotionGalileo reasoned that the natural state of an object (if free of external influences) is uniform motion with a constant velocity.

Consider an object with no force acting on it. If it is at rest, it will remain at rest; if it is moving, it will continue to move in a straight line at a constant speed.

Page 5: Physics 1025F Mechanics

5UCT PHY1025F: Mechanics

Fundamental ForcesFour Basic Fundamental Forces

– Strong nuclear force (holds nucleus together)– Electromagnetic force– Weak nuclear force (radioactive decay)– Gravitational force

Characteristics– All long-range (fields) forces– Listed in order of decreasing strength– Only gravity and electromagnetic in mechanics

Page 6: Physics 1025F Mechanics

6UCT PHY1025F: Mechanics

Free Body Diagrams• Identify the object of interest

– The object whose motion you want to study• Draw a picture of the situation

– Show the object of interest and all directly-interacting objects– Choose an appropriate coordinate system

• Name and label all the forces acting on the object of interest– Contact and long-range forces

• If the free body diagram is incorrect, the solution will likely be incorrect

Page 7: Physics 1025F Mechanics

7UCT PHY1025F: Mechanics

Examples: Free Body Diagrams1. A block is dragged uphill by a rope. Identify all forces

acting on the block.

2. Block A hangs from the ceiling by a rope. Another block B hangs from A. Identify the forces acting on A.

3. A ball, hanging from the ceiling by a string, is pulled back and released. Identify the forces acting on it just after its release.

Page 8: Physics 1025F Mechanics

8UCT PHY1025F: Mechanics

Newton’s First Law of MotionA body at rest will remain at rest, and a body undergoing uniform motion will remain in uniform motion, unless a net force acts on the body.

This is sometimes referred to as the Law of Inertia.Inertia is the tendency of an object to maintain its state of rest or of uniform motion in a straight line.

Page 9: Physics 1025F Mechanics

9UCT PHY1025F: Mechanics

Newton’s First Law of MotionIf no net force is acting on a body it is said to be in “equilibrium”.• e.g. book on table

N

W

0F

Page 10: Physics 1025F Mechanics

10UCT PHY1025F: Mechanics

Static EquilibriumAn object is in equilibrium when the net force acting on it is zero. In component form, this is

- Does acceleration = 0?- Object at rest or constant v?

0

0

y

x

F

F

Page 11: Physics 1025F Mechanics

11UCT PHY1025F: Mechanics

Newton’s Second Law of MotionWhat happens if a net force is exerted on an object?

The acceleration of a body is directly proportional to the net force acting on the body, and is inversely proportional to the mass. The direction is in the same direction as the net applied force.

i.e.

aFFa

mm

or

Page 12: Physics 1025F Mechanics

12UCT PHY1025F: Mechanics

Newton’s Second Law of Motion

Note:• The mass is the property of the body which resists

acceleration, and it is referred to as “inertial mass” when measured this way.

• If a 1 kg mass is accelerating at 1 m/s2 it must be subjected to a force of 1 kg m/s2 or 1 N.

aFFa

mm

or

Page 13: Physics 1025F Mechanics

13UCT PHY1025F: Mechanics

Free Body Diagrams• Identify the object of interest

– The object whose motion you want to study• Draw a picture of the situation

– Show the object of interest and all directly-interacting objects– Choose an appropriate coordinate system

• Name and label all the forces acting on the object of interest– Contact and long-range forces

• Draw and label the net force vector Fnet.• If the free body diagram is incorrect, the solution will likely be incorrect

Page 14: Physics 1025F Mechanics

14UCT PHY1025F: Mechanics

Example: Free Body DiagramAn elevator, lifted by a cable, is going up at a steady speed.

- Identify the forces acting on the elevator.

- Is T greater than, equal to, or less than W? Or is there not enough information to tell?

Page 15: Physics 1025F Mechanics

15UCT PHY1025F: Mechanics

DynamicsAn object is in motion when the net force acting on it is not zero. In component form, this is

yy

xx

maF

maF

Page 16: Physics 1025F Mechanics

16UCT PHY1025F: Mechanics

Example: DynamicsA 10 kg block is pulled across a frictionless horizontal floor by a rope which makes an angle of 30° to the horizontal. What is the acceleration of the block if the force exerted on it by the rope is 5 N?

Page 17: Physics 1025F Mechanics

17UCT PHY1025F: Mechanics

Newton’s Third Law of MotionWhen body A exerts a force on body B, then body B will exert an equal and opposite force on A.

i.e. BAAB FF

Note: Action and reaction forces ALWAYS act on different bodies.

Page 18: Physics 1025F Mechanics

18UCT PHY1025F: Mechanics

Example: Newton’s Third LawA book is placed on a table. Are these two forces action and reaction forces?

W = Force of Earth on Book

N = Force of Table on Book

N

W

A. YES B. NO

Page 19: Physics 1025F Mechanics

19UCT PHY1025F: Mechanics

Weight: The Force of GravityA body undergoing free fall accelerated downwards under gravity with an acceleration g. From Newton’s 2nd law this means that the body must be experiencing a “force of gravity”

We refer to the gravitational force as the “weight”,

i.e.

gFmgrav

gWm

Page 20: Physics 1025F Mechanics

20UCT PHY1025F: Mechanics

MassMass is the measure of inertia of an object. In the SI system, mass is measured in kilograms.

Mass is not weight:

Mass is a property of an object. Weight is the force exerted on that object by gravity.

If you go to the moon, whose gravitational acceleration is about 1/6 g, you will weigh much less. Your mass, however, will be the same.

Page 21: Physics 1025F Mechanics

21UCT PHY1025F: Mechanics

Apparent WeightGravity is not a force that you can feel or sense directly.

The sensation of weight (how heavy you feel) is due to the contact forces pressing against you.

When you stand on a scale, the contact force is the upward spring force acting on your feet. If you and the scale are in equilibrium, the scale will read your weight. If not, it will read your “apparent weight.”

Page 22: Physics 1025F Mechanics

22UCT PHY1025F: Mechanics

Apparent Weight

aFm

Let’s define the apparent weight (Wapp) as the magnitude of the contact force (N) that supports you.

agW

mapp

agNmm

agNmm

Page 23: Physics 1025F Mechanics

23UCT PHY1025F: Mechanics

Example: Apparent WeightA 50 kg student gets in a 1000 kg elevator at rest. As the elevator begins to move, she has an apparent weight of 600 N for the first 3 s. How far has the elevator moved, and in which direction, at the end of 3 s?

Page 24: Physics 1025F Mechanics

24UCT PHY1025F: Mechanics

Normal ForceThe key is understanding the normal force is that it adjusts to the force applied by the object.

The atomic “springs” that make up the surface produce the normal force.

The harder the objects bears down on the surface, the more the normal responds, adjusting itself so the object stays on the surface

Page 25: Physics 1025F Mechanics

25UCT PHY1025F: Mechanics

Example: Normal ForceA 10.0 kg box rests on a table. (a) Calculate the normal force. (b) A rope is now tied around the box and a 40.0 N force is applied upward, calculate the normal force. (c) What happens if a 100.0 N force is applied to the rope?

Page 26: Physics 1025F Mechanics

26UCT PHY1025F: Mechanics

Example: Normal ForceA 75 kg skier starts down a 50-m-high, 10° slope on frictionless skis. What is his speed at the bottom?

Page 27: Physics 1025F Mechanics

27UCT PHY1025F: Mechanics

FrictionConsider the application of a small force to a stationary body on a rough horizontal surface.

At first the application of small force does not induce any motion.If we apply the force on the other side of the body it still does not move. (not directional dependant)We increase the applied force and the body still does not move.As we increase the applied force the body will eventually begin to move. (There is an upper limit on the frictional force)

a

F

Page 28: Physics 1025F Mechanics

28UCT PHY1025F: Mechanics

FrictionExperiments show that the size of the force needed to just cause movement of the body depends on:

- the nature of the surface (i.e. smooth / rough)

- the normal force exerted by the surface on the body

where μs is the static coefficient of friction.NF

sfr (max)

Static = two surfaces are not moving relative to each other

Page 29: Physics 1025F Mechanics

29UCT PHY1025F: Mechanics

FrictionIn general for the stationary situation

Once the body begins to move the frictional force usually reduces so

where k is the kinetic coefficient of friction and, usually, k < s.

NFsfr

NF

kfr

Kinetic = two surfaces are moving relative to each other

Page 30: Physics 1025F Mechanics

30UCT PHY1025F: Mechanics

FrictionThe static frictional force increases as the applied force increases, until it reaches its maximum. Then the object starts to move, and the kinetic frictional force takes over.

Page 31: Physics 1025F Mechanics

31UCT PHY1025F: Mechanics

Example: Friction A 2 kg block is pulled across a rough horizontal surface (k = 0.2) by a rope which makes an angle of 30 to the horizontal. What is the acceleration of the block if the force exerted by the rope is 5 N?

Page 32: Physics 1025F Mechanics

32UCT PHY1025F: Mechanics

Example: Friction A 2 kg block slides along a smooth horizontal surface at 2.4 m/s. It then encounters a rough section of the surface and travels for a further 1.5 m before it comes to rest. What is the coefficient of friction between block and table?

Page 33: Physics 1025F Mechanics

33UCT PHY1025F: Mechanics

Interacting ObjectsObjects in contact will produce Newton’s third law action/reaction pairs.

Solving two or more objects interacting via direct contact forces will require applying Newton’s second and third laws.

Two objects moving together will experience the same acceleration.

Page 34: Physics 1025F Mechanics

34UCT PHY1025F: Mechanics

Example: Interacting ObjectsA 2 kg and a 3 kg block are placed in contact with each other on a smooth frictionless surface. A 10 N force is then used to push the two blocks across the surface. What is the acceleration of the blocks? What force does the 2 kg block exert on the 3 kg? What would change if swapped around?

Page 35: Physics 1025F Mechanics

35UCT PHY1025F: Mechanics

TensionWhen a cord or rope pulls on an object, it is said to be under tension, and the force it exerts is called a tension force.Assumptions:• Ignore any frictional effects of the rope• Ignore the mass of the rope• The magnitude of the force exerted along the rope is called the

tension and is the same at all points in the rope

Page 36: Physics 1025F Mechanics

36UCT PHY1025F: Mechanics

Tension: Connected Objects

Apply Newton’s Laws separately to each object.

The magnitude of the acceleration of both objects will be the same.

The tension is the same in each diagram.

Page 37: Physics 1025F Mechanics

37UCT PHY1025F: Mechanics

Example: Connected ObjectsA block with mass m1 = 4.00 kg and a ball with mass m2 = 7.00 kg are connected by a light string that passes over a frictionless pulley. The coefficient of kinetic friction between the block and the surface is 0.300. Find the acceleration of the two objects and the tension in the string.