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Work and Power Chapter 5

Work and Power Chapter 5. Work Work is done when a force causes a displacement in the direction of the force W = Fd (force and displacement parallel)

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Page 1: Work and Power Chapter 5. Work Work is done when a force causes a displacement in the direction of the force W = Fd (force and displacement parallel)

Work and Power

Chapter 5

Page 2: Work and Power Chapter 5. Work Work is done when a force causes a displacement in the direction of the force W = Fd (force and displacement parallel)

Work

• Work is done when a force causes a displacement in the direction of the force

• W = Fd (force and displacement parallel)

• Unit is newton x meter = joule (J)

• If force is at angle to displacement must find component of force in that direction

• W = Fd(cos)

Page 3: Work and Power Chapter 5. Work Work is done when a force causes a displacement in the direction of the force W = Fd (force and displacement parallel)
Page 4: Work and Power Chapter 5. Work Work is done when a force causes a displacement in the direction of the force W = Fd (force and displacement parallel)

Work

• Equations assume force is constant.

• If force is not constant a graph of force vs. displacement can be used.

• On graph of force vs. distance, work equals area under curve

• Work can be done against gravity, friction, spring, etc.

Page 5: Work and Power Chapter 5. Work Work is done when a force causes a displacement in the direction of the force W = Fd (force and displacement parallel)

Power

• Rate of doing work

• P = W/t = F(d/t) = Fv

• Unit is watt (W) = J/s

• Often expressed as kilowatts (kW)

• English unit is horsepower (hp)

• 1hp = 746 W

Page 6: Work and Power Chapter 5. Work Work is done when a force causes a displacement in the direction of the force W = Fd (force and displacement parallel)

Energy

• The ability to do work or move

• Mechanical energy is involved with the motion of objects

• Two types of mechanical energy– Potential energy– Kinetic energy

Page 7: Work and Power Chapter 5. Work Work is done when a force causes a displacement in the direction of the force W = Fd (force and displacement parallel)

Kinetic Energy

• Energy due to motion

• Since speed is squared, kinetic energy is always positive.

• To double speed, energy must be quadrupled

2

2

1mvKE

Page 8: Work and Power Chapter 5. Work Work is done when a force causes a displacement in the direction of the force W = Fd (force and displacement parallel)

Work – Kinetic Energy Theorem

• Work done on object to change speed equals change in kinetic energy

• W = KE

• Positive work increases speed, negative work decreases speed

• Kinetic energy of object equals amount of work it can do in coming to rest

Page 9: Work and Power Chapter 5. Work Work is done when a force causes a displacement in the direction of the force W = Fd (force and displacement parallel)

Gravitational Potential Energy

• Stored energy due to position in gravitational field

• Equals work done to reach elevated position

• Must be referenced to some zero point

• PEg = mgy

Page 10: Work and Power Chapter 5. Work Work is done when a force causes a displacement in the direction of the force W = Fd (force and displacement parallel)

Elastic Potential Energy

• Equals work done to stretch or compress spring or other elastic material

• Energy stored depends on stiffness of spring and distance stretched or compressed

• Spring constant, k (in N/m) describes stiffness

Page 11: Work and Power Chapter 5. Work Work is done when a force causes a displacement in the direction of the force W = Fd (force and displacement parallel)

Elastic Potential Energy

• Force from spring: F = -kx

• Negative sign shows force is in direction opposite x

• Energy stored in spring or work done on spring:

PEe = W = ½ Fx= ½ kx2

Page 12: Work and Power Chapter 5. Work Work is done when a force causes a displacement in the direction of the force W = Fd (force and displacement parallel)

Figure 1c. In both cases shown in Figures 1a and 1b, the effect of the spring force is to return the system to the equilibrium position. At this position, x = 0 and the

spring is unstretched, signifying Fs = 0.

When the displacement is to the right ( x > 0) the spring force Fs is directed to the left ( x < 0).  

When the displacement is to the left (x < 0) the spring force Fs is directed to the right ( x > 0).

Page 13: Work and Power Chapter 5. Work Work is done when a force causes a displacement in the direction of the force W = Fd (force and displacement parallel)

Other types of Potential Energy

• Electrical and magnetic potential energy are due to position in electrical or magnetic field

• Chemical potential energy due to chemical composition of material

Page 14: Work and Power Chapter 5. Work Work is done when a force causes a displacement in the direction of the force W = Fd (force and displacement parallel)

Conservative Forces• Work done by conservative forces does not

depend on the path taken: gravitation• For conservative forces, total work done on

closed path is zero.• Conservative forces have no energy losses• Example: lifting object from floor to table

involves same amount of work no matter what route is taken. When returned to floor, same amount of work can be extracted.

Page 15: Work and Power Chapter 5. Work Work is done when a force causes a displacement in the direction of the force W = Fd (force and displacement parallel)

Dissipative Forces

• Total work around closed path is not zero.

• Work done depends on length of path

• Main dissipative force is friction

• Dissipative forces cause energy loss as heat

• Work done against friction = force of friction times distance moved = energy lost to heat: Wf = fkd

Page 16: Work and Power Chapter 5. Work Work is done when a force causes a displacement in the direction of the force W = Fd (force and displacement parallel)

Conservation of Energy

• In a closed system with no dissipative forces (friction), total mechanical energy remains constant

• Energy can change forms but can’t be created or destroyed

• System must be closed: nothing enters or leaves

Page 17: Work and Power Chapter 5. Work Work is done when a force causes a displacement in the direction of the force W = Fd (force and displacement parallel)

Examples of Energy Conservation

• Potential energy converts to kinetic when object falls, converts back to potential if it rises again: roller coaster or pendulum

• Energy stored in spring can convert to kinetic energy if used to launch object: catapult

Page 18: Work and Power Chapter 5. Work Work is done when a force causes a displacement in the direction of the force W = Fd (force and displacement parallel)

Energy Conservation and Work

• Work input to system increases total energy by amount of work done

• Work done by system decreases energy by amount of work done

• With friction, change in mechanical energy equals work done against friction

Page 19: Work and Power Chapter 5. Work Work is done when a force causes a displacement in the direction of the force W = Fd (force and displacement parallel)

Power and Energy

• Power in terms of energy is the rate energy is provided or the rate energy is used

• A 60 W light bulb converts 60 J of electrical energy each second into light and heat energy

• A 10 kW generator provides 10,000 J of energy each second

Page 20: Work and Power Chapter 5. Work Work is done when a force causes a displacement in the direction of the force W = Fd (force and displacement parallel)

Vocabulary

• elastic potential energy

• gravitational potential energy

• kinetic energy• law of conservation of

energy

• work• power• conservative force• dissipative force

Page 21: Work and Power Chapter 5. Work Work is done when a force causes a displacement in the direction of the force W = Fd (force and displacement parallel)

Summary

• Work = displacement times force in that direction; unit is joule

• Work = area under force vs. displacement graph

• Kinetic energy is due to motion

• Power is rate of doing work or the rate energy is provided or used

Page 22: Work and Power Chapter 5. Work Work is done when a force causes a displacement in the direction of the force W = Fd (force and displacement parallel)

Summary

• Gravitational potential energy is due to elevated position and equals work done lifting object.

• Elastic potential energy depends on force constant and distance spring is stretched.

• Conservation of energy means sum of all types of energy in closed system is constant.