chapters 10 -11 energy, work, and conservation

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Chapters Chapters 10 -11 10 -11 Energy, Work, Energy, Work, and and Conservation Conservation

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Page 1: Chapters 10 -11 Energy, Work, and Conservation

Chapters Chapters 10 -1110 -11

Energy, Work, Energy, Work, and and ConservationConservation

Page 2: Chapters 10 -11 Energy, Work, and Conservation
Page 3: Chapters 10 -11 Energy, Work, and Conservation

Some Energy Some Energy ConsiderationsConsiderationsEnergy can be transformed from one

form to another.◦ The total amount of energy in the Universe

never changes.◦ This is also true for isolated system.◦ Energy transformations are essential to the

study of physics, chemistry, biology, geology, astronomy.

Can be used in place of Newton’s laws to solve certain problems more simply

Page 4: Chapters 10 -11 Energy, Work, and Conservation

Mechanical EnergyMechanical EnergyThe focus of this chapter is on

mechanical energy.“Mechanical energy is the energy

that is possessed by an object due to its motion or due to its position.”

Mechanical Energy

Kinetic Energy(KE)

Potential Energy(PE)

Page 5: Chapters 10 -11 Energy, Work, and Conservation

Force, Energy, and WorkForce, Energy, and Work

With this relationship we can find expressions for different forms of PE and discuss the principle of conservation of energy and apply it to solving problems.

The connection between work and energy can be used in place of Newton’s 2nd law to solve for certain problems involving force.

Force

Work

Energy

Page 6: Chapters 10 -11 Energy, Work, and Conservation

What is work?What is work?“Work” is the link that ties force and energy together.

In physics, work is defined differently than in everyday life.

“The work, W, done by a constant force on an object is defined as the product of the component of the force along the direction of displacement and the magnitude of the displacement.”

Page 7: Chapters 10 -11 Energy, Work, and Conservation

Work: General CaseWork: General Case

◦F is the magnitude of the force◦Δ x is the magnitude of the object’s

displacement◦ is the angle between and F x

W = (F cos )x

Page 8: Chapters 10 -11 Energy, Work, and Conservation

Work: Specific CaseWork: Specific Case

◦This equation applies when the force is in the same direction as the displacement.

◦ are in the same direction.and F x

W = F x

Page 9: Chapters 10 -11 Energy, Work, and Conservation

Sample ProblemSample Problem

A man cleaning his apartment pulls the canister of a vacuum cleaner with a force of magnitude F = 55.0 N. The force makes an angle of 30.0o with the horizontal. The canister is displaced 3.00 m to the right. Calculate the work done by the 55.0 N force on the vacuum cleaner.

Page 10: Chapters 10 -11 Energy, Work, and Conservation

More About WorkMore About Work

This definition of work gives no information about:◦The time it took for the displacement

to occur.◦The velocity or acceleration of the

object.◦These value can be obtained indirectly

from work and then use of PE, KE, and the conservation of energy.

◦More on this later.

Page 11: Chapters 10 -11 Energy, Work, and Conservation

NO Displacement = NO NO Displacement = NO Work!!Work!!

As long as an object does not change its position, no work is being done.

There are two other cases when no work is done. Can you think of them?

Page 12: Chapters 10 -11 Energy, Work, and Conservation

Force & Displacement Force & Displacement Perpendicular = NO Work!!Perpendicular = NO Work!!If displacement is

horizontal and the applied force is vertical, the angle between them will be 90o.

cos 90° = 0Whenever the

displacement and the applied force are perpendicular to each other no work is done.

Page 13: Chapters 10 -11 Energy, Work, and Conservation

No Applied Force = NO No Applied Force = NO Work!!Work!!No applied force means no work is done.

ΣF = 0 N, W = 0 J

Page 14: Chapters 10 -11 Energy, Work, and Conservation

Multiple Forces and WorkMultiple Forces and Work

If there are multiple forces acting on an object, the total work done is the algebraic sum of the amount of work done by each force.

∆x

WT = (ΣFcosθ) ∆x

Page 15: Chapters 10 -11 Energy, Work, and Conservation

A Quick Summary of WorkA Quick Summary of WorkWork doesn’t happen by itself.

◦A net force must be acting on an object and causing a displacement for work to be done.

Work is done by something in the environment, on the object of interest.

The forces discussed here are constant.◦The forces could be variable.

Work is related to energy as well.◦This will be covered in the next section.

Page 16: Chapters 10 -11 Energy, Work, and Conservation

Work and EnergyWork and EnergyIn the previous section we looked

at the link between work and force. ◦W = (F cos )x

In this section we will look at the relationship between work and energy.◦We can use this relationship as an

alternative to solving problems involving Newton’s 2nd law.

◦From which we can solve for velocity, displacement, and acceleration.

Page 17: Chapters 10 -11 Energy, Work, and Conservation

Work Causes Work Causes DisplacementDisplacementWork does not occur unless

displacement occurs.Displacement does not occur unless

speed/velocity is involved.Thus, work and speed/velocity are

also related.Using work, we can determine the

speed of an object if we know its displacement and the net forces acting on it.

Page 18: Chapters 10 -11 Energy, Work, and Conservation

Determining an object’s Determining an object’s speed given the net force speed given the net force acting on it and the work acting on it and the work done to it.done to it.

Page 19: Chapters 10 -11 Energy, Work, and Conservation

Kinetic EnergyKinetic Energy

Energy associated with the motion of an object.

Scalar quantity with the same dimensions as work.◦SI Units: J

Work is related to kinetic energy.◦Wnet = ∆KE = KEf – KEi

2mv2

1KE

Page 20: Chapters 10 -11 Energy, Work, and Conservation

Work-Kinetic Energy Work-Kinetic Energy TheoremTheorem

When work is done by a net force on an object and the only change in the object is its speed, the work done is equal to the change in the object’s kinetic energy.◦ Speed will increase if work is positive.◦ Speed will decrease if work is negative.

net fiW KE KE KE

Page 21: Chapters 10 -11 Energy, Work, and Conservation

Work and Kinetic EnergyWork and Kinetic EnergyAn object’s

kinetic energy can also be thought of as the amount of work a moving object could do in coming to rest.◦The moving

hammer has kinetic energy and can do work on the nail.

Page 22: Chapters 10 -11 Energy, Work, and Conservation

Work and Kinetic EnergyWork and Kinetic EnergyWork can also

be used to impart KE to an object. ◦The golf ball

at rest is given a velocity and thus KE because of the work done by the club.

Page 23: Chapters 10 -11 Energy, Work, and Conservation

Sample ProblemSample Problem

A car of mass 1.40x103 kg being towed has a net forward force of 4.50x103 N applied to it. The car starts from rest and travels down a horizontal highway. Find the speed of the car after it has traveled 100.0 m. (Ignore kinetic energy losses caused by friction and air resistance.)

Page 24: Chapters 10 -11 Energy, Work, and Conservation

Potential EnergyPotential EnergyPotential energy (PE)is

associated with the position of the object within some system.◦Potential energy is a property of the

system, not the object.◦A system is a collection of objects

interacting via forces or processes that are internal to the system.

◦PE again is only associated with conservative forces.

Page 25: Chapters 10 -11 Energy, Work, and Conservation

Gravitational Potential Gravitational Potential EnergyEnergy

Gravitational Potential Energy is the energy associated with the relative position of an object in space near the Earth’s surface.◦Objects interact with

the earth through the gravitational force.

◦The potential energy is for the earth-object system.

Page 26: Chapters 10 -11 Energy, Work, and Conservation

Work and Gravitational Work and Gravitational Potential EnergyPotential Energy

An expression for PE can be derived using work.

The expression for PE shows that it is determined by the mass of the object, the gravitational acceleration at the Earth’s surface, and the vertical location of the object.◦This expression for PE is only valid for

object near the Earth’s surface.

Page 27: Chapters 10 -11 Energy, Work, and Conservation

Work and Gravitational Work and Gravitational Potential EnergyPotential Energy

figrav ity PEPEW

PE = mgy

◦ This equation relates work to PE.

◦ The work done by PE depends only on the height of the object.

A “zero” point must be established.◦ More on this in a

moment.

Page 28: Chapters 10 -11 Energy, Work, and Conservation

Reference Levels for Reference Levels for Gravitational Potential EnergyGravitational Potential Energy

A location where the gravitational potential energy is zero must be chosen for each problem.◦The choice is arbitrary since the change

in the potential energy is the important quantity.

◦Choose a convenient location for the zero reference height. Often the Earth’s surface. May be some other point suggested by the

problem.◦Once the position is chosen, it must

remain fixed for the entire problem.

Page 29: Chapters 10 -11 Energy, Work, and Conservation

Example of Reference Example of Reference LevelsLevelsAt location A, the

desk may be the convenient reference level.

At location B, the floor could be used.

At location C, the ground would be the most logical reference level.

The choice is arbitrary, though.

Page 30: Chapters 10 -11 Energy, Work, and Conservation

Sample ProblemSample Problem

How much work does a bricklayer do to carry 30.2 kg of bricks from the ground up to the height of 11.1 m.? What is the potential energy of the bricks when the bricklayer reaches this height?

Page 31: Chapters 10 -11 Energy, Work, and Conservation

ConservationConservationConservation in

general:◦ To say a physical

quantity is conserved is to say that the numerical value of the quantity remains constant throughout any physical process although the quantities may change form. The form of a physical

quantity may change but the overall numeric value (or magnitude) will not.

◦ Conservation plays an important role in physics and in other sciences.

Page 32: Chapters 10 -11 Energy, Work, and Conservation

Conservation of Mechanical Conservation of Mechanical EnergyEnergyIn conservation of mechanical energy, the

total mechanical energy remains constant.◦ In any isolated system of objects interacting only

through conservative forces, the total mechanical energy of the system remains constant.

Total mechanical energy is the sum of the kinetic and potential energies in the system.

◦ Other types of potential energy functions can be added to modify this equation

ffii

fi

PEKEPEKE

EE

Page 33: Chapters 10 -11 Energy, Work, and Conservation

Problem Solving with Problem Solving with Conservation of EnergyConservation of Energy

Define the system◦ Verify that only conservative forces are present.

Select the location of zero gravitational potential energy, where y = 0.◦ Do not change this location while solving the problem.

Identify two points the object of interest moves between.◦ One point should be where information is given.◦ The other point should be where you want to find out

something.Apply the conservation of energy equation to

the system.◦ Immediately substitute zero values, then do the

algebra before substituting the other values.Solve for the unknown:

◦ Typically a speed or a position◦ Substitute known values ◦ Calculate result

Page 34: Chapters 10 -11 Energy, Work, and Conservation

Sample ProblemSample Problem

A sled and its rider together weigh 800 N. They move down a frictionless hill through a vertical distance of 10.0 m. Use conservation of mechanical energy to find the speed of the sled at the bottom of the hill, assuming the rider pushes with an initial speed of 5.00 m/s. Neglect air resistance.

Page 35: Chapters 10 -11 Energy, Work, and Conservation

Potential Energy Stored in a Potential Energy Stored in a SpringSpringSpring force is also a conservative

force.◦Thus a PE expression can be derived for

the spring force and the work a spring does is not path dependent.

◦Let’s 1st look at the spring force.Involves the spring constant, kHooke’s Law gives the force

◦F = - k x F is the restoring force F is in the opposite direction of x k depends on how the spring was formed, the

material it is made from, thickness of the wire, etc.

Page 36: Chapters 10 -11 Energy, Work, and Conservation

Potential Energy in a Potential Energy in a SpringSpringElastic Potential Energy

◦Related to the work required to compress a spring from its equilibrium position to some final, arbitrary, position x.

◦We can relate this PE to kinetic energy in the same way we related gravitational PE to kinetic energy.

2s kx

2

1PE

Page 37: Chapters 10 -11 Energy, Work, and Conservation

Spring Potential EnergySpring Potential Energy

A) The spring is in equilibrium, neither stretched or compressed.

B) The spring is compressed, storing potential energy.

C) The block is released and the potential energy is transformed to kinetic energy of the block.

Page 38: Chapters 10 -11 Energy, Work, and Conservation

Conservation of Mechanical Conservation of Mechanical Energy Including a SpringEnergy Including a SpringThe PE of the spring is added to

both sides of the conservation of mechanical energy equation to give:

The same problem-solving

strategies apply to these problems as well.

fsgisg )PEPEKE()PEPEKE(

Page 39: Chapters 10 -11 Energy, Work, and Conservation

Sample ProblemSample ProblemA 0.50 kg block rests on a horizontal, frictionless surface as seen in the figure. The block is pressed against a light spring having a spring constant of k=80.0 N/m. The spring is compressed a distance of 2.0 cm and released. Consider the system to be the spring, block, and Earth and find the speed of the block when it is at the bottom of the incline.

Page 40: Chapters 10 -11 Energy, Work, and Conservation

Energy TransfersEnergy TransfersBy Work

◦ By applying a force.◦ Produces a displacement of the system.◦

Heat◦ The process of transferring heat by

collisions between atoms or molecules.◦ For example, when a spoon rests in a cup

of coffee, the spoon becomes hot because some of the KE of the molecules in the coffee is transferred to the molecules of the spoon as internal energy.

( ) ( )nc fi fiW KE KE PE PE

Page 41: Chapters 10 -11 Energy, Work, and Conservation

More Energy TransfersMore Energy TransfersMechanical Waves

◦ A disturbance propagates through a medium.

◦ Examples include sound, water, seismic.

Electrical transmission◦ Transfer by means of electrical current.◦ This is how energy enters any electrical

device.

Page 42: Chapters 10 -11 Energy, Work, and Conservation

More Energy TransfersMore Energy TransfersElectromagnetic radiation

◦Any form of electromagnetic waves. Light, microwaves, radio waves.

◦For example Cooking something in your microwave

oven. Light energy traveling from the Sun to

the Earth.

Page 43: Chapters 10 -11 Energy, Work, and Conservation

CollisionsCollisionsMomentum is conserved in any collision.Total KE is not always conserved.

◦ Some KE is converted to other forms of energy (i.e. internal energy, sound energy, etc.) or is used to do the work needed to deform an object.

Two broad categories of collisions:◦ Elastic collisions◦ Inelastic collisions: Perfectly inelastic and

inelasticElastic and perfectly inelastic collisions

represent ideal cases of collisions.Most real world cases fit somewhere

between these two extremes.

Page 44: Chapters 10 -11 Energy, Work, and Conservation

Inelastic CollisionsInelastic CollisionsMomentum is conserved.Kinetic energy is not conserved.Two categories: inelastic and

perfectly inelastic.◦Perfectly inelastic collisions occur

when the objects stick together. Not all of the KE is necessarily lost. Colliding objects have different initial

velocities but the same final velocities.

Use: 1 1 2 2 1 1 2 2i i ffm m m m v v v v

Page 45: Chapters 10 -11 Energy, Work, and Conservation

Perfectly Inelastic Perfectly Inelastic CollisionsCollisionsWhen two objects stick together after the collision, they have undergone a perfectly inelastic collision.

Conservation of momentum becomes:

f21i22i11 v)mm(vmvm

Page 46: Chapters 10 -11 Energy, Work, and Conservation

Elastic CollisionsElastic CollisionsMostly occurs at the atomic and

subatomic levels.◦Macroscopic collisions can only

approximate elastic collisions.Both momentum and kinetic

energy are conserved for both objects.◦No KE is lost as sound, heat, light, etc.

Typically have two unknowns.◦Solve the equations simultaneously

2f22

2f11

2i22

2i11

f22f11i22i11

vm2

1vm

2

1vm

2

1vm

2

1

vmvmvmvm

Page 47: Chapters 10 -11 Energy, Work, and Conservation

Sample problemSample problemTwo billiard balls move towards one another as in the figure. The balls have identical masses, and assume that the collision between them is perfect elastic. If the initial velocities of the balls are 30 cm/s and -20cm/s, what is the velocity of each ball after the collision?

Page 48: Chapters 10 -11 Energy, Work, and Conservation

Summary of Types of Summary of Types of CollisionsCollisionsIn an elastic collision, both momentum

and kinetic energy are conserved.In an inelastic collision, momentum is

conserved but kinetic energy is not.In a perfectly inelastic collision,

momentum is conserved, kinetic energy is not, and the two objects stick together after the collision, so their final velocities are the same.

Page 49: Chapters 10 -11 Energy, Work, and Conservation

Final Notes About Final Notes About Conservation of EnergyConservation of EnergyWe can neither create nor destroy

energy.◦The total energy of the universe must

always remain the same.◦Another way of saying energy is

conserved.◦If the total energy of the system does

not remain constant, the energy must have crossed the boundary by some mechanism.

◦Applies to areas other than physics.

Page 50: Chapters 10 -11 Energy, Work, and Conservation

PowerPowerOften also interested in the rate at

which the energy transfer takes place.Power is defined as this rate of energy

transfer.

SI units for power are Watts (W).

WFv

t

2

2

J kg mW

s s

Page 51: Chapters 10 -11 Energy, Work, and Conservation

PowerPowerUS Customary units are generally hp.

◦ Need a conversion factor

◦ Can define units of work or energy in terms of units of power: kilowatt hours (kWh) are often used in electric

bills. This is a unit of energy, not power.

W746s

lbft550hp1

Page 52: Chapters 10 -11 Energy, Work, and Conservation

Chapters Chapters 10 -1110 -11

Energy, Work, Energy, Work, and and ConservationConservation

THE END