49

Chapter 10: Work and Energy

Embed Size (px)

DESCRIPTION

Chapter 10: Work and Energy. 10.1 Machines and Mechanical Advantage 10.2 Work 10.3 Energy and Conservation of Energy. Chapter 10 Objectives. Calculate the mechanical advantage for a lever or rope and pulleys. Calculate the work done in joules for situations involving force and distance. - PowerPoint PPT Presentation

Citation preview

Page 1: Chapter 10: Work and Energy
Page 2: Chapter 10: Work and Energy

Chapter 10: Work and Energy

10.1 Machines and Mechanical Advantage

10.2 Work

10.3 Energy and Conservation of Energy

Page 3: Chapter 10: Work and Energy

Chapter 10 Objectives Calculate the mechanical advantage for a lever or

rope and pulleys.

Calculate the work done in joules for situations involving force and distance.

Give examples of energy and transformation of energy from one form to another.

Calculate potential and kinetic energy.

Apply the law of energy conservation to systems involving potential and kinetic energy.

Page 4: Chapter 10: Work and Energy

Chapter Vocabulary chemical

energy

closed system

law of conservation

of energy

electrical energy

fulcrum

gears

input

input arm

input force

joule

kinetic energy

lever

machine

mechanical

advantage

mechanical energy

mechanical system

nuclear energy

output

output arm

output force

potential energy

pressure energy

radiant energy

ramp

rope and pulley

screw

simple machine

thermal energy

work

Page 5: Chapter 10: Work and Energy

Inv 10.1 Machines and Mechanical

AdvantageInvestigation Key Question:

How do simple machines work?

Page 6: Chapter 10: Work and Energy

10.1 Machines and Mechanical

Advantage The ability of humans to

build buildings and move mountains began with our invention of machines.

In physics the term “simple machine” means a machine that uses only the forces directly applied and accomplishes its task with a single motion.

Page 7: Chapter 10: Work and Energy

10.1 Machines The best way to analyze what a

machine does is to think about the machine in terms of input and output.

Page 8: Chapter 10: Work and Energy

10.1 Mechanical Advantage Mechanical advantage is the

ratio of output force to input force.

For a typical automotive jack the mechanical advantage is 30 or more.

A force of 100 newtons (22.5 pounds) applied to the input arm of the jack produces an output force of 3,000 newtons (675 pounds)— enough to lift one corner of an automobile.

Page 9: Chapter 10: Work and Energy

10.1 Mechanical Advantage

MA = Fo

Fi

Output force (N)

Input force (N)

Mechanicaladvantage

Page 10: Chapter 10: Work and Energy

10.1 Types of simple machines The lever, wheel and axle,

rope and pulleys, screw, ramp, and gears are the most common simple machines.

Complex machines, combine many simple machines into mechanical systems.

A mechanical system is an assembly of simple machines that work together to accomplish a task.

Page 11: Chapter 10: Work and Energy

10.1 Mechanical Advantage of a Lever The essential features of a lever are the input arm, output arm, and fulcrum.

Page 12: Chapter 10: Work and Energy
Page 13: Chapter 10: Work and Energy

10.1 Three types of levers

The three types of levers are classified by the location of the input and output forces relative to the fulcrum:

first class lever

second class lever

third class lever

Page 14: Chapter 10: Work and Energy

10.1 How a lever works A lever works by rotating about its fulcrum.

The mechanical advantage can be deduced by calculating the torques created by the input and output forces.

The input force creates a (positive) counterclockwise torque.

The torque created by the reaction force is clockwise (negative).

When the lever is in equilibrium the net torque must be zero.

Page 15: Chapter 10: Work and Energy

10.1 Torque and mechanical advantage

Page 16: Chapter 10: Work and Energy

1. You are asked for the location of the fulcrum2. You are given input force, lever length, mass to be lifted3. Since you are told to assume Fo = ½ Fw , use:

Fw = mg , MA = Fo ÷ Fi , MA = Li÷ Lo 4. Solve for Fo = (.5) (500 kg) (9.8 N/kg) = 2,450 N5. Solve for MA = 2,450 N ÷ 700 N = 3.56. Since Li = 3.5 Lo , and Li + Lo = 3m, then Lo = .67m

Calculating the position of the fulcrum

Where should the fulcrum of a lever be placed so one person weighing 700N can lift the edge of a stone block with a mass of 500 kg? The lever is a steel bar three meters long. Assume a person can produce an input force equal to their own weight. Assume that the output force of the lever must equal half the weight of the block to lift one edge.

Page 17: Chapter 10: Work and Energy

10.1 Mechanical advantage of ropes and pulleys A tension force is a pulling force acting along the direction of a rope or string.

Ropes and strings carry tension forces throughout their length.

If friction is small, the tension force in a rope is the same everywhere.

If you were to cut a rope in tension and insert a force scale, the scale would measure the same force at any point along the rope.

Page 18: Chapter 10: Work and Energy

10.1 Rope & Pulleys The block-and-tackle

machine is a simple machine using one rope and multiple pulleys.

The rope and pulleys can be arranged to create different amounts of mechanical advantage.

Page 19: Chapter 10: Work and Energy

10.1 Wheels, gears, & rotating machines Wheels and axles provide advantages.

Friction occurs where the wheel and axle touch or where the wheel touches a surface.

Rolling motion creates less wearing away of material compared with two surfaces sliding over each other.

With gears the trade-off is made between torque and rotation speed.

An output gear will turn with more torque when it rotates slower than the input gear.

Page 20: Chapter 10: Work and Energy

10.1 Ramps and Screws

Ramps reduce input force by increasing the distance over which the input force needs to act.

A screw is a simple machine that turns rotating motion into linear motion.

A thread wraps around a screw at an angle, like the angle of a ramp.

Page 21: Chapter 10: Work and Energy

Chapter 10 Work and Energy

10.1 Machines and Mechanical Advantage

10.2 Work

10.3 Energy and Conservation of Energy

Page 22: Chapter 10: Work and Energy

Inv 10.2 Work

Investigation Key Question:

What is the trade-off for multiplying forces in a machine?

Page 23: Chapter 10: Work and Energy

10.2 Work

In physics, work has a very specific meaning.

In physics, work represents a measurable change in a system, caused by a force.

Page 24: Chapter 10: Work and Energy

10.2 Work

If you push a box with a force of one newton for a distance of one meter, you have done exactly one joule of work.

Page 25: Chapter 10: Work and Energy

10.2 Work (force is parallel to distance)

W = F x dDistance (m)

Force (N)

Work (joules)

Page 26: Chapter 10: Work and Energy

10.2 Work (force at angle to distance)

W = Fd cos ()

Distance (m)

Force (N)

Work (joules) Angle

Page 27: Chapter 10: Work and Energy

10.2 Work done against gravity

W = mgh

Height object raised (m)

Gravity (m/sec2)

Work (joules)

Mass (g)

Page 28: Chapter 10: Work and Energy
Page 29: Chapter 10: Work and Energy

1. You are asked for the work and time it takes to do work.

2. You are given mass, height, and work done per second.

3. Use: W = mgh.

4. Solve: W = (1,500 kg) ( 9.8 N/kg) (50 m) = 735,000 J

5. At a rate of 10,000 J/s, it takes 73.5 s to lift the beam.

Calculate work done against gravityA crane lifts a steel beam with a mass of 1,500 kg. Calculate how much work is done against gravity if the beam is lifted 50 meters in the air. How much time does it take to lift the beam if the motor of the crane can do 10,000 joules of work per second?

Page 30: Chapter 10: Work and Energy

10.2 Work done by a machine

Work is usually done when a force is applied to a simple machine.

All machines can be described in terms of input work and output work.

In any machine, some of the input work goes to overcoming friction.

The output work is always less than the input work because of the energy lost to friction.

Page 31: Chapter 10: Work and Energy
Page 32: Chapter 10: Work and Energy

Chapter 10 Work and Energy

10.1 Machines and Mechanical Advantage

10.2 Work

10.3 Energy and Conservation of Energy

Page 33: Chapter 10: Work and Energy

Inv 10.3 Energy and Conservation of EnergyInvestigation Key

Question:

How is motion on a track related to energy?

Page 34: Chapter 10: Work and Energy

10.3 Energy and Conservation of Energy Energy describes a system’s ability to

cause change. A system that has energy has the

ability to do work. Energy is measured in the same units

as work because energy is transferred during the action of work.

Page 35: Chapter 10: Work and Energy

10.3 Different forms of energy Mechanical energy is the energy possessed

by an object due to its motion or its position.

Radiant energy includes light, microwaves, radio waves, x-rays, and other forms of electromagnetic waves.

Nuclear energy is released when heavy atoms in matter are split up or light atoms are put together.

The electrical energy we use is derived from other sources of energy.

Page 36: Chapter 10: Work and Energy

The workings of the universe can be viewed as energy flowing from one place to another and changing back and forth from one form to another.

Page 37: Chapter 10: Work and Energy

10.3 Potential Energy

Objects that have potential energy do not use the energy until they move.

An object’s potential energy comes from the gravity of Earth.

Technically, energy from height is called gravitational potential energy.

Other forms of potential energy also exist, such as potential energy stored in springs.

Page 38: Chapter 10: Work and Energy

10.3 Potential Energy

Ep = mgh Height (m)

Mass (kg)

Potential Energy (joules)

Accelerationof gravity (m/sec2)

Page 39: Chapter 10: Work and Energy

1. You are asked for potential energy and time.

2. You are given mass, height and work done per second.

3. Use: Ep = mgh.

4. Solve for Ep = (102 kg) (9.8 N/kg) (4 m) = 3,998 J.

5. At a rate fof 50 J/s, it takes 80 s to push the cart up the ramp.

Calculating potential energyA cart with a mass of 102 kg is pushed up a ramp. The top of the ramp is 4 meters higher than the bottom. How much potential energy is gained by the cart? If an average student can do 50 joules of work each second, how much time does it take to get up the ramp?

Page 40: Chapter 10: Work and Energy

10.3 Kinetic Energy Energy of motion is called kinetic energy.

The kinetic energy of a moving object depends on two things: mass and speed.

Kinetic energy is proportional to mass.

Page 41: Chapter 10: Work and Energy

10.3 Kinetic Energy Mathematically, kinetic energy

increases as the square of speed. If the speed of an object doubles, its

kinetic energy increases four times (mass is constant).

Page 42: Chapter 10: Work and Energy

10.3 Kinetic Energy

Ek = 1 mv2

2

Speed (m/sec)

Mass (kg)

Kinetic Energy (joules)

Page 43: Chapter 10: Work and Energy

10.3 Kinetic Energy

Kinetic energy becomes important in calculating braking distance.

Page 44: Chapter 10: Work and Energy

10.3 The formula for kinetic energy A force (F) is applied to mass (m) and

creates acceleration (a). After a distance (d), the ball has reached speed

(v), therefore the work done is its mass times acceleration time distance: W= fd = (ma) x d = mad Also: d = ½ at2

Replace d in the equation for work, combine similar terms: W= ma (½ at2) = ½ ma2t2 Also: v = at, so v2 = a2t2

Replace a2t2 by v2 shows that the resulting work is the formula for kinetic energy: W = ½ mv2

Page 45: Chapter 10: Work and Energy

1. You are asked for kinetic energy and stopping distance

2. You are given mass, speed and force of brakes.

3. Use Ek = 1/2mv2 and W= fd

4. Solve for Ek = ½ (1,300 kg) ( 30 m/s)2 = 585,000 J To stop the car, work done by brakes = Ek of car, so W = Ek

Solve for distance = W ÷ f = 585,000J ÷ 9,500 N = 62 m

Calculating kinetic energyA car with a mass of 1,300 kg is going straight ahead at a speed of 30 m/s (67 mph). The brakes can supply a force of 9,500 N.Calculate:

a) The kinetic energy of the car.b) The distance it takes to stop.

Page 46: Chapter 10: Work and Energy

10.3 Law of Conservation of Energy As energy takes different forms and

changes things by doing work, nature keeps perfect track of the total.

No new energy is created and no existing energy is destroyed.

Page 47: Chapter 10: Work and Energy

10.3 Energy in a closed system

The conservation of energy is most useful when it is applied to a closed system.

Because of the conservation of energy, the total amount of matter and energy in your system stays the same forever.

Page 48: Chapter 10: Work and Energy

10.3 Energy in a closed system

The total energy in the system is the potential energy of the ball at the start.

Later, the ball is at a lower height (h) moving with speed (v) and has both potential and kinetic energy.

Page 49: Chapter 10: Work and Energy

Every day in the United States the average person uses about 90 million joules of electrical energy.

This energy comes from many sources, including burning coal, gas and oil, nuclear power, and hydroelectric power.

Hydroelectric Power

In hydroelectric power, the potential energy of falling water is converted to electricity.

No air pollution is produced, nor hazardous wastes created.