newton’s laws of motion. review equations for motion along one dimension

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NEWTON’S LAWS OF MOTION

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Page 1: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

NEWTON’S LAWS OF MOTION

Page 2: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Review

Equations for Motion Along One Dimension

dt

dx

t

xv

t

xv

t

ave

0lim

dt

dv

t

va

t

va

t

ave

0lim

Page 3: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Review

Motion Equations for Constant Acceleration

•1.

•2.

•3.

•4.

atvv 0

221

00 attvxx

20vv

vave

xavv 220

2

Page 4: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Dynamics vs Kinematics

So far we’ve been studying kinematics, we’ve been describing how things move.

We were only concerned with a particles position, velocity or acceleration.

But why do things move? What gives objects motion?

Page 5: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

What is Force?

Page 6: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

What is Force?

Force is either a push or a pull. It is an interaction between two bodies.

Force is a vector. It has both magnitude and direction.

When force is a result of two objects touching, we call that a contact force.

Aside from that there are also long-range forces or field forces

Page 7: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Examples of Contact Forces

Normal Force

Frictional Force

Tension Force

Page 8: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Examples of Field Forces

Gravitational Force Magnetic Force Electric Attraction

Page 9: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Fundamental Forces

Gravitational Forces – weakest of the four forces

Electromagnetic Forces – force between electrically charged particles.

Weak Nuclear Forces – responsible for some nuclear phenomena like beta decay

Strong Nuclear Forces – only holds inside an atomic nucleus.

Page 10: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Superposition of Forces

Throwing a basketball into the hoop What are the forces involved?

Page 11: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Superposition of Forces

Throwing a basketball into the hoop What are the forces involved?

Force of your hand on the ball Force of gravity (i.e. weight)

Page 12: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Superposition of Forces

If we can add forces, we can also separate a force into its components!

yx AAA cosAAx sinAAy

Page 13: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Examples

Young and Freedman 4.4 A man is dragging a trunk up a loading

the loading ramp of a mover’s truck. The ramp has a slope angle of 20.0o, and the man pulls upward with a force F, who’s direction makes an angle of 30o with the ramp. (a) How large a force F is necessary for the component Fx parallel to the ramp to be 60.0 N? (b) How large will the component Fy perpendicular to the ramp then be?

Page 14: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Isaac Newton

Born January 4, 1643 (December 25, 1642 under old calendar)

He was a physicist, mathematician, astronomer, natural philosopher, alchemist and theologian.

Considered by many to be the “greatest scientist who ever lived”.

He published the “Philosophiæ Naturalis Principia Mathematica” in 1687 which laid the foundations for classical mechanics.

Page 15: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

He also invented calculus

Page 16: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Isaac Newton – lesser known facts Was a religious nut

He published more papers on scripture than science.

He poured over the bible looking for secret codes.

He also poured a lot of effort into alchemy and the philosophers stone

Page 17: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Isaac Newton – questionable facts Invented the cat door (pet door) Apple hitting Newton on the head

Page 18: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Principia was written due to a bet

Christopher Wren was with some astronomers when he bet 40 shillings (around 4,000 php now) that no one could explain elliptical orbits.

It took Newton years to find the answer so he didn’t get any money.

But he expanded his answers and published Principia.

Included in Principia are the Three Laws of Motion

Page 19: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

First Law of Motion

Lets examine an object at rest If there are no forces acting on it the

object what will happen to the object?

If the sum of forces on an abject equal zero, what will happen to the object?

Page 20: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

First Law of Motion

Lets examine an object in motion If there are no forces acting on it the

object what will happen to the object?

If the sum of forces on an abject equal zero, what will happen to the object?

Page 21: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

First Law of Motion

Every object continues in its state of rest or of uniform velocity as long as no net force acts on it.

Inertia – the tendency of an object to maintain its state of rest or uniform motion

Law of inertia

A body is in equilibrium if 0F

Page 22: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

But wait

If you’re in a decelerating car, your body gets thrown forward, but there is no net force acting on you!!!

Page 23: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Inertial Frames of Reference

Frames of reference where First Law of Motion holds

Frames fixed on the Earth can be considered to be inertial frames of reference

Frames of reference travelling at constant velocity relative to another inertial frame are also inertial frames (a=0).

Page 24: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Mass

Mass is usually defined as quantity of matter an object has.

We need to be a bit more specific here Mass is a measure of inertia of an object. Uses SI unit kg

Page 25: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Mass vs Weight

Mass and weight are used interchangeably in everyday language

In physics, mass and weight are different Mass is the measure of inertia. It is an

intrinsic property of matter. No matter where you are, or where the observer is, your mass will be the same.

Weight is the force of gravity on an object. Your weight will be different here than on the moon or in space.

Page 26: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Young and Freedman 4.20

An astronauts pack weighs 17.5N on earth and 3.24N on an asteroid. (a) what is the acceleration due to gravity on the asteroid? (b) what is the mass of the pack on the asteroid?

Page 27: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

What happens then if net Force is not equal to 0

0F

F

Page 28: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Newton’s Second Law of Motion The acceleration of an object is directly

proportional to the net force acting on it and indirectly proportional to its mass. The direction of the acceleration is in the direction of the net force acting on the object.

m

Fa

maF

Page 29: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Force

We now define the Newton 1 Newton is the amount of force needed

to accelerate a 1kg object by 1m/s2

1N=1kg m /s2

It is the SI unit for Force

Page 30: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Force

We now define the Newton 1 Newton is the amount of force needed

to accelerate a 1kg object by 1m/s2

1N=1kg m /s2

It is the SI unit for Force Pull of the earth is a force

Weight has SI unit of N

Page 31: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Example

What average force is required to stop an 1,100 kg car in 8.0 s if the car is travelling at 95 km/h

Page 32: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Example

We have mass, we need accelerationmaF

st

v

v

sm

sm

hkm

0.8

0

389.26950

Page 33: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Example

NF

kgF

maF

a

a

t

vva

atvv

sm

sm

600,3

)298.3)(1100(

298.38

389.260

2

2

0

0

Page 34: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Newton’s Third Law of Motion Force is an interaction between two

objects It always comes in pairs

Page 35: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Newton’s Third Law of Motion Whenever one object exerts a force on a

second object, the second exerts an equal force in the opposite direction on the first.

BonAAonB FF

Page 36: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Newton’s Third Law of Motion To every action there is an equal but

opposite reaction

Remember the action and reaction forces are acting on different objects

BonAAonB FF

Page 37: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Horse and Cart Paradox

Page 38: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Example

Giancoli 4-19 A box weighing 77.0N is

resting on a table. A rope tied to the box runs vertically upward over a pulley and a weight is hung from the other end. Determine the force the table exerts on the box if the weight on the other side of the pulley weighs (a) 30.0N (b) 60.0N (c) 90.0N

77N

Page 39: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Example

Force table exerts on the box is just normal force

Normal Force = Weight of box on table

77N

Page 40: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Application of Newton’s Laws Serway 5-18 A bag of cement

weighs 325 N and hangs from three wires. Two of the wires make angles 60.0o and 25.0o with the horizontal. If the system is in equilibrium, find the tensions, T1, T2, T3 in the wires.

Page 41: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Young & Freedman 5.10

A 1130 kg car is held in place by a light cable on a very smooth (frictionless) ramp. The cable makes an angle of 31.0o above the surface of the ramp. The ramp itself rises 25.0o above the horizontal. (a) find the tension in the cable. (c) How hard does the surface of the ramp push on the car?

Page 42: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Giancoli 4-30

At the instant a race began a 65kg sprinter exerted a force of 720N on the starting block at an angle of 22o with respect to the ground. (a) What is the horizontal acceleration of the sprinter? (b) if the force was exerted for 0.32s with what speed did the sprinter leave the starting block?

Page 43: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Serway 5-24

A 5.00 kg object placed on a frictionless, horizontal table is connected to a string that passes over a pulley and then is fastened to a hanging 9.00-kg object. Find the acceleration of the two objects and the tension in the string.

Page 44: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Giancoli 4-34

Two masses each initially 1.80 m above the ground, and the massless fricitonless pulley is 4.8m above the ground. What maximum height does the lighter mass reach after the system is released?

2.2

3.2

1.80 m

4.80 m

Page 45: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Friction

Results from contact between two surfaces.

Parallel to the surface of contact.

Always opposite to the relative motion of the two surfaces.

Page 46: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Kinetic Friction

Frictional force can be approximated to be proportional to normal force

Where µk is the coefficient of kinetic friction

Note: friction is not dependent on surface area

Nf kk

Page 47: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Static Friction

Force of friction that arises even when objects are not in relative motion.

Where µs is the coefficient of Static friction

Nf ss

sk

Page 48: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Friction Graph

Page 49: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Young & Freedman 5.30

A box of bananas weighs 40.0N and rests on a horizontal surface. µs=0.40 while µk =0.20. (a) if no horizontal force is being applied and the box is at rest, what is the friction force exerted on the box. (b) What is the magnitude of friction is a monkey exerts a force of 6.0 N on the box. (c) What is the minimum horizontal force the monkey needs to apply to start the box in motion? (d) What is the minimum horizontal force the monkey needs to keep the box in motion? (e) If the monkey applies a horizontal force of 18.0N what is the magnitude of friction force and the boxes acceleration.

Page 50: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Young & Freedman 5.30

FN=40.0N (a) = 0 (b) max fs=0.4*40=16N => fs=6N (c) 16N (d) fk=0.2*40=8N (e) Fnet=ma=F-fk

ma=18-8=10N a=10/m=10*9.8/40=2.45m/s2

Page 51: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Serway 5-44

Three objects are connected as shown. Table has µk =0.350. (a) determine the acceleration of each object in the system (b) Determine the tensions in the two chords.

Page 52: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Serway 5-49

A block weighing 75.0N rests on a plane inclined at 25.0o to the horizontal. A force F is applied at 40.0o to the horizontal pushing it upward on the plane. If µs =0.363 and µk =0.156 (a) What is the minimum value of F to prevent the block from slipping down the plane. (b) what is the minimum value of F that will start the block up the plane. (c) What value of F will move the block up at constant velocity.

Page 53: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Apparent Weight

Tension in an elevator cable Elevator has a total mass of 800 kg. its

moving downwards at 10 m/s but slows to a stop at constant acceleration for 25.0m. Find the tension T while the elevator is being brought to rest.

Page 54: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Apparent Weight

Elevator has a total mass of 800 kg. its moving downwards at 10 m/s but slows to a stop at constant acceleration for 25.0m. Find the tension T while the elevator is being brought to rest.

A woman is on a scale while riding the elevator. Mass of the woman is 50.0 kg, what is the reading on the scale?

Page 55: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Common Movie Mistakes

Page 56: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Seat Work/Home Work (time dependent)

A block with mass 15.0kg is placed on a frictionless inclined plane with slope 20.0o

and is connected to a second block with mass 6.00kg hanging over a small, frictionless pulley. (a) Will the first block accelerate to the left or to the right? (b) What is the magnitude of the acceleration?

kg15

kg6

Page 57: NEWTON’S LAWS OF MOTION. Review  Equations for Motion Along One Dimension

Seat Work/Home Work (time dependent)

A block with mass 15.0kg is placed on an inclined plane with slope 20.0o and is connected to a second block with mass 6.00kg hanging over a small, frictionless pulley. If µs= 0.300 and µk= 0.150 (a) Will the system accelerate? Why or why not? (b) If yes, what is the magnitude of the acceleration?

kg15

kg6