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1 Newton’s 3 rd Law Momentum Prentice Hall Chapters 7 & 8

1 Newton’s 3 rd Law Momentum Prentice Hall Chapters 7 & 8

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Page 1: 1 Newton’s 3 rd Law Momentum Prentice Hall Chapters 7 & 8

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Newton’s 3rd LawMomentum

Prentice HallChapters 7 & 8

Page 2: 1 Newton’s 3 rd Law Momentum Prentice Hall Chapters 7 & 8

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Ch 7 & 8 assignments

– Complete Packets for the chapters. On the problem sections, you must follow the problem solving method: write givens with symbols and units, working equation, work with units and answer with units. Use more paper if there is not enough room.

Page 3: 1 Newton’s 3 rd Law Momentum Prentice Hall Chapters 7 & 8

Newton’s 3rd Law

• For every action there is an opposite and equal reaction.

• This is applied to momentum and collisions.

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Page 4: 1 Newton’s 3 rd Law Momentum Prentice Hall Chapters 7 & 8

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Chapter 8 Momentum and Its Conservation

Momentum, = mass of an object times its velocity = mv units: kgm/s

Impulse is an object’s difference in final momentum and initial momentumF t = m v = f – i units: ns, kgm/s

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Conservation of Momentum

This is used in collisions

where Newton’s third law

is related to conservation

of momentum.

See figure 8.11 on page 132

i = f

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Page 7: 1 Newton’s 3 rd Law Momentum Prentice Hall Chapters 7 & 8

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Recoil occurs when objects are at rest initially.

Example problem on page 135

General formula

i = f but I (small fish) = 0

Page 8: 1 Newton’s 3 rd Law Momentum Prentice Hall Chapters 7 & 8

Collision Types

• Elastic – when objects collide and rebound from each other without a loss in energy (no permanent change in shape and no heat change). Fig 8.11 (pg. 132)

• Inelastic – when objects collide and become distorted. Vehicle crashes.

• Perfectly inelastic – when objects collide and stick together after impact. Freight cars coupling on train track.

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Page 9: 1 Newton’s 3 rd Law Momentum Prentice Hall Chapters 7 & 8

Asgn:

• 142/55,57,58 due tomorrow.

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Page 11: 1 Newton’s 3 rd Law Momentum Prentice Hall Chapters 7 & 8

Now we begin:

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WorkPower Energy

Page 12: 1 Newton’s 3 rd Law Momentum Prentice Hall Chapters 7 & 8

Objectives*Differentiate among the various forms of energy and how they can be transformed from one into another.

*Explore the Law of Conservation of Energy by differentiating among open, closed, and isolated systems and explain that the total energy in an isolated system is a conserved quantity.

*Compare and contrast work and power both qualitatively and quantitatively.

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Work is the transfer of energy by mechanical means.

• In this section you will calculate work and power used.

• Terms/Units:

Work/joule,j energy/joule,j

kinetic energy/joule,j

work-energy theorem

Power/joule/sec or watt

746 w = 1 hp

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Work = Force x distance

• W = Fd units: nm or joule, j

• Work is equal to a constant force exerted on an object in the direction of motion, times the object’s displacement

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Kinetic Energy – the energy of motion

• KE = ½ m v 2

• units: kg (m/s) 2 = (kgm/s2) m

• = nm = joule

• Work Energy Theorem: W = KE

• Work = the change in kinetic energy of a system.

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Work at an angle

• W = Fd cos • Work = the product of force and

displacement, times the cosine of the angle between the force and the direction of the displacement.

• How much work is done pulling with a 15 N force applied at 20.o over a distance of 12 m?

Page 17: 1 Newton’s 3 rd Law Momentum Prentice Hall Chapters 7 & 8

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How much work is done pulling with a 15 N force applied at 20.o over a distance of 12

m?

• W = Fdcos • W = 15 N (12 m) (cos 20)

• W = 169 170 J

20o

15 N

Page 18: 1 Newton’s 3 rd Law Momentum Prentice Hall Chapters 7 & 8

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Power

Power = Work / time

j/s = watt or w

Power is “The rate of doing work.”

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Sample Problem:

• Together, two students exert a force of 825 n in pushing a car a distance of 35 m.

• A. How much work do they do on the car?

• W = Fd = 825n (35m) =

• B. If the force was doubled, how much work would they do pushing the car the same distance?

• W = 2Fd = 2(825n)(35m) =

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A rock climber wears a 7.5 kg backpack while scaling a cliff. After 30.0 min, the climber is 8.2 m above the starting point.

a.How much work does the climber do on the backpack?

W = Fd = mgd = 7.5kg(9.8m/s2)(8.2m)

b. How much power did the climber expend?

P = W = 6.0x102 j x 1min = 0.33 = 3.3x10-1 w

t 30.0min 60sec

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Machines

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Actual Mechanical Advantage – comparing torques or forces

MA = resistance (or load) force effort force

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• Calculated Actual Mechanical Advantage:

• Fr / Fe = 200nm / 300 nm = .67

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Ideal Mechanical Advantage, comparing

distances: IMA = d effort / d resistance

IMA = 2.4 m / 1.2 m = 2

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Efficiency

Efficiency, e = work out = AMA x 100

work in IMA

Sample problem on next slide.

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Two people use a wheel and axle to raise a mass of 750. kg. The radius of the wheel is 0.50 m and the radius of the axle is 0.040 m. If the efficiency of the machine is 62% and each person exerts and equal force, how much force must each apply?

Efficiency, e = work out = AMA x 100

work in IMA

e = 0.62 IMA = R =0.50m =

r 0.040m

AMA = f effort f effort = f resist AMA f effort = ?

f resistance

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Page 27: 1 Newton’s 3 rd Law Momentum Prentice Hall Chapters 7 & 8

Efficiency, e = work out = AMA x 100

work in IMA

e = 0.62 IMA = R =0.50m =

r 0.040mAMA = f effort f effort = f resist AMA f effort = ?

fresistance

f effort = f resis r = 750. kg x 10.nkg-1 x 0.040m

e x R 0.62 x 0.50 m

f effort = 968 n Per person: 968 = 484 n

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Chapter 11 Energy & Its Conservation

• Kinetic Energy: KE = ½ m v2

• KE for a Spring: KE = ½ k (d)2

k = F / d• Potential Energy: PE = mgh• Rest Energy: E = mc2

• Mechanical Energy, E = KE + PE• Conservation of Energy (collisions, etc.)

• KEi + PEi = KEf + PEf

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The total energy of a closed, isolated system is constant. The energy can

change form.

20.0J

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Examples: Collisions

• Elastic Collisions: ones in which initial KE = final KE

• Inelastic Collisions: ones in which energy is changed into another form (i.e., KE into heat or sound)

Page 31: 1 Newton’s 3 rd Law Momentum Prentice Hall Chapters 7 & 8

A 98.0 –N sack of grain is hoisted to a storage room 50.0 m above the ground floor of a grain elevator.

a.How much work was done?

W = Fd

W = 98.0 – N ( 50.0m)

W = 4900 = 4.90 x 103 j

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Page 32: 1 Newton’s 3 rd Law Momentum Prentice Hall Chapters 7 & 8

A 98.0 –N sack of grain is hoisted to a storage room 50.0 m above the ground floor of a grain elevator.

b. What is the increase in potential energy of the sack of grain at this height?

PE = mgh = Fd

PE = 98.0 N (50.0 m)

PE = 4900 j = 4.90 x 103 j

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Page 33: 1 Newton’s 3 rd Law Momentum Prentice Hall Chapters 7 & 8

A 98.0 –N sack of grain is hoisted to a storage room 50.0 m above the ground floor of a grain elevator.

c.The rope being used to lift the sack of grain breaks just as the sack rached the storage room. What kinetic energy does the sack have just before it strikes the ground floor?

Ans.: KEbottom = PEtop

KEbottom = 4.90 x 103 J

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11/73

73a. W = Fd = 98.0 N (50.0 m)

W = 4.90 x 103 J

73b. PE = mgh = Fd

PE = W = 4.90 x 103 J