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Work

When you hold something, are you exerting a

force on the object? Yes.

When you hold something, are you doing

work?

If you set the object on a table, does the table

exert a force on the object? Yes. Does the

table do any work? No.

When you hold something, then, you are not

doing work either.

Work

What can you do that the table can’t do? You

can lift the object up - which is work!

We define the concept of WORK as the

exertion of force through a distance.

There is one more consideration, however. In

tether ball, the pole exerts a force on the

moving ball (via the rope). Does the pole

do work?

Work

The pole does NOT do work!

Does the player who hits the tether ball do

work? YES.

What is the difference between what the pole

does and what the player does?

Work

The difference is in the direction. The pole

was pulling on the tether ball perpendicular

to the motion of the tether ball. The player

was pushing on the tether ball in the same

direction as the motion.

In part two, however, we also had torque as

being force across a distance. What is the

difference?

Work and Torque

In applying torque, the direction of the force

had to be perpendicular to the distance.

This caused a turning force: t = r F sin(qrF)

In doing work, the direction of the force has to

be parallel (or anti-parallel) to the distance

moved. We write this this way:

Work = F s

where the dot indicates the cosine of the angle

between F and s: Work = F s cos(qFs) .

Work

Work = F s

Although F and s are vectors (with magnitude

and direction), Work is a scalar

(magnitude only).

Can we have positive and negative work? If

the Force and distance are parallel, the

amount of work is positive, but if the two

vectors are anti-parallel, then the work is

negative.

Energy

We can now define the concept of energy:

Energy is the capacity to do work (in ideal

circumstances).

We all know that we can do work: exert a

force through a distance. But to do that

requires food. Thus we convert the energy

in food into work. The same thing happens

when we burn coal to generate heat which

can be converted into electricity which can

be converted into lots of useful work.

Conservation of Energy

A Natural Law

Many such examples as we just saw lead us to

propose a natural law. Remember that a

natural law is a statement of how nature

seems to work - it is not “derived” from

anything more basic, it is observed to fit the

results of observations (experiments).

Energy can neither be created nor

destroyed (that is, energy is conserved).

However, it can be transformed from one

form into another.

Conservation of Energy

The equation that comes from this law of

conservation of energy is:

S Energiesinitially = S Energiesfinally .

Our job now is to find out how the amount of

energy in different forms relates to the

various parameters associated with that

form. That is, we need to derive formulas

for various kinds of energy.

Units

The units of energy (and work) are:

Nt*m = Joule.

A British unit of energy is the BTU (British

Thermal Unit). 1 BTU = 1054 Joules

Another unit of energy is the calorie.

1 calorie = 4.186 Joules

However, the calorie we refer to when we eat

is really a kilocalorie = 4186 Joules.

Units

The units of torque are: Nt*m = Nt*m.

Note that even though torque and energy both

have units of Nt*m, they are different

quantities, and so they have different formal

names. Energy units are in Joules, while

torque units are simply specified as Nt*m.

In the British system, the unit of torque is

simply called the foot-pound (ft-lb).

Positive and Negative

Can we have energies that are negative?

First, can we have negative money? Yes - it’s

called debt. You need to earn money to pay

off the debt and reach up to zero.

In the same way, some energies can be

negative - we need to gain some energy to

reach what we define as zero energy.

Forms of Energy

Kinetic Energy

Energy of motion, called Kinetic Energy:

should depend on mass and speed of object.

Your car has energy when it is moving.

The wind has energy when it is moving, and

we can convert this wind energy into

electric energy via windmills.

Potential Energies

Energy of position, called Potential Energy:

should depend on why that position has

energy.

The water stored behind a dam has energy due

to it’s height above the base of the dam.

We can use this to run a hydroelectric

station. The energy in food is due to the

molecular binding of the atoms in the food.

The same is true for coal, oil and gas.

There is also energy stored in the nucleus of

atoms - nuclear energy.

Some other forms

• Heat: should depend on temperature, type

and amount of material. We burn coal to

get heat to turn water into steam and use the

steam pressure to get work (or electricity).

• Light: should depend on type and intensity

of the light.

• Sound: should depend on type and

intensity of the sound.

Kinetic Energy - derivation

If we let an object fall, it gains speed. It also

gains what we call kinetic energy. By the

Conservation of Energy law, the amount of

work going into the object (from gravity)

will equal the amount of energy the object

has (kinetic): F s cos(q) = mg h (1). But if

an object falls a distance h with an

acceleration of g, how fast is it going?

Kinetic Energy - derivation

KE(m,v) = mgh (The amount of kinetic energy,

which depends on the quantities mass and speed in

this case equals the amount of work done by

gravity, mgh).

From our motion equations, v = vo + gt and

h = ho + vot + (1/2)gt2 or in this case (ho=0,

vo=0): h = (1/2)gt2, or t = (2h/g)1/2 so v = gt =

g(2h/g)1/2, or v = (2hg)1/2, or h = (1/2)v2/g; thus

mgh = mg(1/2)v2/g = (1/2)mv2 = KE .

Kinetic Energy - formula

KE = (1/2)mv2 . Note that the kinetic energy

depends on m (the more mass the more

kinetic energy) and on v2 (if you double the

speed, you quadruple the kinetic energy).

Also note that the kinetic energy must always

be either zero or positive - it can’t be

negative. (This is like cash in the money

analogy.)

Kinetic Energy - considerations

You’ve probably heard the expression: “speed

kills”. This comes from the fact that KE

depends on the square of the speed. If you

double your speed, you quadruple the

amount of energy of the object. And

remember that energy is the capacity to do

work - for either good or bad. Uncontrolled

energy can exert large forces through

significant distances - which can be very

dangerous!

Kinetic Energy - considerations

Note that the difference between (1 m/s)2 and

(2 m/s)2 is 3 m2/s2, whereas the difference

between (99 m/s)2 and (100 m/s)2 is 199

m2/s2 . What this indicates is that it takes

more and more energy to move faster and

faster. This explains why there is so little

difference between first and tenth in a speed

race between trained athletes!

Gravitational Potential Energy

If we let the force of gravity act on an object

as it moves, gravity is exerting a force

through a distance and may add or subtract

energy from the object. We can work with

this near the earth (where gravity is

constant) with PEgravity = mgh . Farther

from the earth’s surface, gravity changes,

and we need a different formula (from

calculus): PEgravity = -Gm1m2/r12 .

PEgravity Considerations

In the simpler formula near the earth’s

surface, PEgravity = mgh both m and g are

positive numbers, but h is a height

measured from some point that you

determine. It can be the ground, but doesn’t

have to be. Note that h can be either

positive or negative!

PEgravity Considerations

In the more general form,

PEgravity = -Gm1m2/r12 , the PE is always

negative, with the highest (least negative)

value being when PE=0 or r12 goes to

infinity.

Note in particular, that while the force of

gravity goes as r122, the PE of gravity goes

only as r12.

Problems

Having KE and PEgravity, we can start solving

some problems using the Conservation of

Energy.

Problem: How high will a ball go if it is

thrown with a speed of 25 m/s?

We could solve this problem using Newton’s

Second Law and the equations for constant

acceleration, or we could use Conservation

of Energy.

Tossing a ball up

Let’s try this problem using Conservation of

Energy:

We recognize that we have kinetic energy (since we

have motion), and we recognize that we have

gravitational potential energy (since we have

gravity); also vi=25 m/s; hi=0 m (start from the

ground); vf=0 (highest point). These are all

related by the Conservation of Energy:

Tossing a Ball Up

S Energiesinitially = S Energiesfinally .

KEi + PEi = KEf + PEf

(1/2)mvi2 + mghi = (1/2)mvf2 + mghf

(1/2)*m*(25 m/s)2 + m*(9.8 m/s2)*(0 m) =

(1/2)*m*(0 m/s)2 + m*(9.8 m/s2)*hf .

Here we see that the mass cancels out, and we

have one equation in one unknown (hf):

hf = (1/2)*(25 m/s)2 / (9.8 m/s2) = 31.89 m.

Observations

We should note two things from this example:

Conservation of Energy is a scalar equation,

and so has no information about directions.

This makes it easier to solve, but gives less

information in the answer.

Conservation of Energy makes no mention of

time (only initial and final). This removes t

from the problem - making it easier but also

giving us less information in the answer.

Escape Speed

In the previous example, we threw something up that

went about 32 meters high. How fast would we

have to throw something to make it escape

from the earth altogether?

We can use Conservation of Energy again, but

we need the more general form for potential

energy due to gravity.

To escape the earth, rf = infinity!

We start with ri = Rearth = 6.4 x 106m.

Escape Speed

S Energiesinitially = S Energiesfinally .

KEi + PEi = KEf + PEf

(1/2)mvi2 - Gmearthm/ri = (1/2)mvf2 - Gmearthm/rf

We see that m is in each term, so we cancel it.

(1/2)*(vi)2 - (6.67x10-11 Nt*m2/kg2) *(6.0 x 1024

kg)/(6.4x106m) = (1/2)*(0 m/s)2 - (6.67x10-11

Nt*m2/kg2) *(6.0 x 1024 kg)/(infinity)

We again have one equation in one unknown (vi).

Escape Speed

We have used vf = 0 m/s since this is the

minimum speed we need at the end. We

could have more speed when we escape, but

we’re looking for the lowest speed for the

object to still escape; this means that both

the terms on the right side = 0.

Solving for vi = vescape = [2*G*Mearth /Rearth ]1/2

= 11,180 m/s = 25,000 mph.

Friction and Energy Loss

Can we use Conservation of Energy if we

have friction? What happens with friction?

We convert kinetic energy into heat!

What “formula” do we use for how much

energy is “lost” to friction, that is, how

much energy is converted from kinetic to

heat?

Friction

We start from the basic definition of energy:

the capacity to do work, where work =

Force thru a distance:

Elost = Ffriction * s. We still have Ffriction = mFc.

Where does this Elost go in the equation for

Conservation of Energy: on the initial or

final side? Is it a positive or negative

amount of energy?

Friction

Since some of the initial kinetic energy will

go (transform) into some heat, the Elost

should be a positive term if it is on the final

side, or a negative term if it is on the initial

side.

S Energiesinitially = S Energiesfinally .

KEi + PEi = KEf + PEf + Elost

where Elost = + Ffriction*s = + mFcs .

Friction - example

Problem: If the coefficient of friction

between a block of wood and the concrete

floor is 0.50, how far will a block of wood

slide on the floor before coming to rest if it

starts with a speed of 10 m/s ?

We recognize this as a Conservation of

Energy problem with kinetic energy and

with friction (Elost).

Friction - an example

We are given: vi = 10 m/s; vf = 0 m/s; m = .5

We are looking for s (the distance of slide).

S Energiesinitially = S Energiesfinally .

KEi = KEf + Elost

where Elost = + Ffriction*s = + mFcs .

From S Fy = 0, we have Fc = mg. Therefore:

(1/2)*m*vi2 = (1/2)*m*vf2 + m*m*g*s .

Friction - an example

(1/2)*m*vi2 = (1/2)*m*vf2 + m*m*g*s

We notice that there is an m in each term so it

cancels out!

(1/2)*(10 m/s)2 = 0 + (.5)*(9.8 m/s2)*s

This is one equation in one unknown (s):

s = (1/2)*(10 m/s)2 / (.5)*(9.8 m/s2) = 10.2 m.

Power

We now know what Force and Energy are, but

what is Power?

Power

We now know what Force and Energy are, but

what is Power?

The definition of Power is that it is the rate of

change of Energy from one form into

another: Power = DEnergy / Dt .

The units of power are: Joule/sec = Watt.

Another common unit is the horsepower, hp.

The conversion factor is: 1 hp = 746 Watts.

Example: Power

What is your power output when you climb

stairs?

In this case, you are changing your potential

energy (mgh) in time, so … P = Dmgh / Dt

if your mass = 70 kg, gravity is 9.8 m/s2, and

you climb steps of height 10 meters in a

time of 20 seconds:

P = 70 kg * 9.8 m/s2 * 10 m / 20 sec = 343 W

or 343 W * (1 hp / 746 W) = .46 hp .

Example #2: Power

What is your average power output per day?

If you eat 2000 Calories per day, (and

assuming you do not gain or lose weight),

that energy must be converted into energy

you use throughout the day.

P = 2,000 Calories / day = (2000 Cal)*(4186

joule/Cal) / [(24 hours)*(60 min/hr)*(60

sec/min)] = 97 Watts.

Example #3: Power

How powerful must a car engine be (on

average) if it is to accelerate a 2000 kg car

from zero to 65 mph in 20 seconds?

This is a power question. The change in

energy is in the form of kinetic energy. We

should convert 65 mph into metric form:

vf = 65 mph * (1 m/s / 2.24 mph) = 29 m/s.

vi = 0 (starts at rest); Dt = 20 sec.

Example #3: Power

Power = DEnergy / Dt =

[(1/2)*m*vf2 - (1/2)*m*vi2] / t =

[(1/2)*(2000 kg)*(29 m/s)2 - 0 ] / 20 sec =

42,000 Watts * (1 hp / 746 Watts) = 56 hp.

Note that this is the average power.

Force and Power

We know how force is related to energy, and

how energy is related to power. Can we

relate power to force?

Work = F s , Power = DWork /Dtime =

F Ds /Dt (but Ds/Dt = v), so Power = F v .

Power, like work, is a scalar.

Note that if F is constant, Power must go up

as speed (v) goes up! If Power is constant,

F must go down as v goes up.

Force and Power

At very low speeds, even a small power will

give a rather large force!

On cars with manual transmissions, you

normally don’t rev up the engine (high

power), and then pop the clutch! This

causes tremendous forces that can break the

car!

What do you pay for:

Force, Energy, or Power?



What do you pay MLG&W (for example) for:

force, energy or power?



What do you pay the gas station for:

force, energy or power?

What do you pay for:

Force, Energy, or Power?

What do you pay MLG&W (for example) for:

force, energy or power?

What do you pay the gas station for: force,

energy or power?

In both cases you pay for ENERGY!

Cost of Energy

What is the cost of energy?

We saw before that we could do work at the

rate of a couple 100 Watts, but that was

hard work!. If we worked for 40 hours a

week, how much useful work would we

perform?

Work = Energy = Power * time.

The MKS unit of energy is the Joule, but this

is a very small unit. Another common unit

of energy is the Kilowatt*hour.

Cost of Energy

In terms of kilowatt-hours, if you worked at

the rate of 200 Watts for 40 hours, you

would do 8 KW-Hrs of work.

How much does the power company charge

for a KW-hr of energy?

How much would you make for your 8 KW-

Hrs of work (assuming MLG&W paid you

exactly what it charges us for that same amount of

energy)?

Cost of Energy

In Memphis, MLG&W charges about 9 cents

per KW-hr. Thus, if you were to work for

the power company providing power, you

would earn about 8 KW-hr/week * $.09 =

$.72/week (72 cents per week)!

As we see, energy is quite cheap! The reason

our utility bills are so high is that we use so

much energy - especially when we heat (or

cool) things (like air and water)!

Computer Homework

The computer homework program, Energy

and Power, is the first program on

Volume 2. This program has questions

about the concepts we have covered in this

set of slides.

The labs on Atwood Machine and Hooke’s

Law also deal with these concepts.



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