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Definition of Work W=F . d This is Fundamental to Engineering Work and Energy

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Page 1: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the

Definition of Work

W=F.d

• This is Fundamental to Engineering

Work and Energy

Page 2: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the

Work done and Work experienced

• Something subtle: The amount of work YOU do on a body may not be the same as the work done ON a body.

• Only the NET force on the object is used in the total work calculation

• Add up all the work done on an object to find the total work done!

Page 3: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the

Examples• Holding a bag of groceries

– Is it heavy?– Will you get tired holding it?– Are you doing “Work?”

• Moving a bag of groceries with constant speed across a room– Is it heavy?– Will you get tired doing it?– Are you doing “Work?”

• Lifting a bag of groceries a height h with constant speed?– Work by you?– Work on the bag?

Page 4: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the

Hiker with a backpack

Determine:

•The work done by the hiker

•The work done by gravity

•The work on the backpack

Page 5: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the
Page 6: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the

Does the Earth do work on the Moon?

Page 7: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the

Work by IntegrationTo find the total work, we must sum up all the little pieces of work (i.e., F.d). If the force is continually changing, then we have to take smaller and smaller lengths to add. In the limit, this sum becomes anintegral.

∫ •b

ai xdF

Page 8: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the

W=F.dWork and Energy

W=∆K

Page 9: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the

Force to stop a car

What constant net force is required to bring a car of mass m to rest from a speed of Vwithin a distance of D?

X0 = 0 XF = D

V0 = V V = 0

Page 10: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the

Force to stop a car

Page 11: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the

Kicking a ball

Page 12: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the
Page 13: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the

Water SlideWho hits the bottom with a faster speed?

Page 14: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the

Multiple ways to calculate work

1. If the force and direction is constant– F.d

2. If the force isn’t constant– Integrate

3. If we don’t know much about the forces

– Look at the change in kinetic energy

Page 15: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the

Potential Energy

U = W

Is a measure of work that a system COULD do.

Page 16: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the

Last time we considered a hiker carrying a backpack of mass M with constant speed up a hill of angle Θand height h.

We have determined:

•The work done by the hiker

•The work done by gravity

•The work on the backpack

Page 17: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the

Subtlety: Potential energy is relative to somewhere!Example: What is the potential energy of a brick 2

meters above a 1 meter high table? 3 meters above the floor?

Only change in potential energy is really meaningful!

Gravitational Potential EnergyI lift up a brick from the ground to a height h, and let it go. How much work will be done by gravity by the time the brick hits the ground?

U=mgh

Page 18: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the

Springs

• Hooke’s Law

• Force is NOT CONSTANT over a distance

Some constantDisplacement

xkF −=

Page 19: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the
Page 20: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the

Potential Energy of a Spring

How much work do we exert to compress a spring by a distance x?

How much potential energy does it now have?

U(x) = ½kx2

Page 21: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the

Mechanical Energy

E≡K+U

For some types of problems,Mechanical Energy is conserved:

K2+U2 = K1+U1

Page 22: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the

Problem Solving

As objects move, their potential energy gets converted into kinetic energy, and back.

It’s often useful to draw “before” and “after” diagrams.

Page 23: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the
Page 24: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the
Page 25: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the

A Roller Coaster of mass M starts at the top, height h, with an initial speed V0=0.

a) What is the energy at the top?b) What is the speed at the bottom?c) How much work is done by gravity in going from the top to

the bottom?d) At what height is it at half the max speed?

Rollercoaster Problem

h

Page 26: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the
Page 27: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the

If there were no friction, the roller coaster would go back up to height h.Would it go as high, if there were friction?

Three different types of forces acting:–Gravity: Conserves mechanical energy–Normal Force: Conserves mechanical energy

–Friction: Doesn’t conserve mechanical energyFriction is a Non-Conservative force!

Page 28: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the

Energy Conservation

Friction turns mechanical energy into heat

E = Kinetic Energy + Potential Energy ++ Heat + Others… -- This is what

is really conserved!

One can use “lost” mechanical energy to estimate things about friction

Page 29: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the

Emma Noether(23 March 1882 – 14 April 1935)

Noether's (first) theorem states that any differentiable symmetryof the action of a physical system has a corresponding conservation law.

Page 30: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the

EHeat+Light+Sound = -WNC

If work is done by a non-conservative force, take this into account in the total energy. (Friction causes mechanical energy to be lost.)

K1+U1 = K2+U2+EHeat…

K1+U1 = K2+U2-WNC

Page 31: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the

Roller Coaster Again!A roller coaster of mass m starts at rest at height y1 and

falls down the path, then back up until it hits height y2(y1 > y2). An odometer tells us that the total scalar distance traveled is d.

Assuming we don’t know anything about the friction or the path, how much work is done by friction on this path?

Assuming that the magnitude of the force of friction, F, between the car and the track is constant, find F.

Page 32: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the
Page 33: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the

Force and Potential Energy

If we know the potential energy, U(x), we can find the force

dxdU

xF −=

Page 34: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the

Potential Energy Diagrams

• For Conservative forces we can draw energy diagrams

• Equilibrium points:– If placed there with

no energy, an object will just stay (no force) 0=−= dx

dUxF

Page 35: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the

Stable vs. Unstable Equilibrium Points

The force is zero at both maxima and minima

Page 36: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the

Another definition:A force is conservative if the net work done by the force on an object moving around any closed path is zero.This definition is equivalent to the previous one.

A force is conservative if the work done by a force on an object moving from one point to another point depends only on the initial and final positions and is independent of the particular path taken.

Page 37: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the

Friction a Non-Conservative Force

Is the force, applied by the person who moves the box, conservative?

Page 38: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the

Robot ArmA robot arm has a funny Force equation in 1-dimension

where F0 and X0 are constants.What is the work done to move a block from position X1 to position X2?

+= 2

0

2

0 x3x1F F(x)

Page 39: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the

Problem

We drop a ball of mass m from a height h above the uncompressed spring and observe that it compresses a distance Y.

What is k?

Page 40: Definition of Work W=Fdpeople.physics.tamu.edu/sokol/Work+Energy.pdf · Work by Integration To find the total work, we must sum up all the little pieces of work (i.e., F.d). If the