Work and Energy Energy n KINETIC ENERGY KE

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Work and Energy

Work and Energy

Energy n KINETIC ENERGY (KE): energy associated with motion of an object n POTENTIAL

Energy n KINETIC ENERGY (KE): energy associated with motion of an object n POTENTIAL ENERGY (PE): energy associated with position of an object

WORK n WORK: the product of the component of the force along the direction

WORK n WORK: the product of the component of the force along the direction of displacement and the magnitude of the displacement. • W=F • dcos where d = magnitude of displacement • When the force is not in the direction of the displacement, then either sin or cos is needed. • Units of work: 1 Joule = 1 N • m

In order to do work, you must exert a force over a distance. The

In order to do work, you must exert a force over a distance. The con may expend energy when he pushes on the wall, but if it doesn’t move, no work is performed on the wall.

The force must be in the same direction as the movement. If not, you

The force must be in the same direction as the movement. If not, you have to use a vector component of the force that is in the same direction. Hence the cosine. A lot of the time, you will see the work equation written like this: W = FD cos Why?

Example: A man cleaning his apartment pulls a vacuum cleaner with a force of

Example: A man cleaning his apartment pulls a vacuum cleaner with a force of 50. N at an angle of 30. 0. A frictional force of magnitude 40. N dampens the motion, and the vacuum is pulled a distance of 3. 0 m. Calculate: a)the work done by the 50. N pull; b)the work done by the frictional force; c)the net work done on the vacuum by all forces acting on it.

Example: A man cleaning his apartment pulls a vacuum cleaner with a force of

Example: A man cleaning his apartment pulls a vacuum cleaner with a force of 50. N at an angle of 30. 0. A frictional force of magnitude 40. N dampens the motion, and the vacuum is pulled a distance of 3. 0 m. Calculate: a)the work done by the 50 N pull; b)the work done by the frictional force; c)the net work done on the vacuum by all forces acting on it. WF = (Fcos ) • d WF = (50. N)(cos 30 )(3. 0 m) WF = 130 J 50 N 30 40 N direction of displacement

Example: A man cleaning his apartment pulls a vacuum cleaner with a force of

Example: A man cleaning his apartment pulls a vacuum cleaner with a force of 50. N at an angle of 30. 0. A frictional force of magnitude 40. N dampens the motion, and the vacuum is pulled a distance of 3. 0 m. Calculate: a)the work done by the 50. N pull; b)the work done by the frictional force; c)the net work done on the vacuum by all forces acting on it. Wf = (Fcos ) • d 50 N Wf = (40. N)(cos 180 )(3. 0 m) 30 Wf = -120 J 40 N direction of displacement

Example: A man cleaning his apartment pulls a vacuum cleaner with a force of

Example: A man cleaning his apartment pulls a vacuum cleaner with a force of 50 N at an angle of 30. A frictional force of magnitude 40 N dampens the motion, and the vacuum is pulled a distance of 3 m. Calculate a)the work done by the 50 N pull; b)the work done by the frictional force; c)the net work done on the vacuum by all forces *normal force, acting on it. 50 N weight, & upward component of pull do no Wnet = WF + Wf work because they are Wnet = 130 J – 120 J perpendicular to the displacement. Wnet = 10 J 30 40 N direction of displacement

Work and Kinetic Energy

Work and Kinetic Energy

Work and Kinetic Energy Roughly speaking, energy is the ability to do work. This

Work and Kinetic Energy Roughly speaking, energy is the ability to do work. This is known as the work-energy theorem.

Work-Energy Theorem n The net work done on an object by the force or

Work-Energy Theorem n The net work done on an object by the force or forces acting on it is equal to the change in the kinetic energy of the object. – The speed of an object will increase if the net work done on it is positive; – The speed of an object will decrease if the net work done on it is negative.

KEi + Pei(s) + Workadded = KEf + Pef(s) + Worklost This is where

KEi + Pei(s) + Workadded = KEf + Pef(s) + Worklost This is where we are going with this unit. We will now break this equation down piece by piece. Note: Energy can be in all four or any combination of the four types on either side. You need to decide which pieces you will use.

Example: A 1400 -kg car has a net forward force of 4500 N applied

Example: A 1400 -kg car has a net forward force of 4500 N applied to it. The car starts from rest and travels down a horizontal highway. What are its kinetic energy and speed after it has traveled 100. m? (ignore friction and air resistance) m = 1400 kg F = 4500 N Vo = 0 d = 100. m KEf = ? KEi = 0 Vf = ? 4500 N 100 m

Example: A 1400 -kg car has a net forward force of 4500 N applied

Example: A 1400 -kg car has a net forward force of 4500 N applied to it. The car starts from rest and travels down a horizontal highway. What are its kinetic energy and speed after it has traveled 100. 0 m? (ignore friction and air resistance) 4500 N 100 m

Potential Energy n Gravitational potential energy: the energy an object has due to its

Potential Energy n Gravitational potential energy: the energy an object has due to its position in space. PE = mgh n In working problems, choose the zero level for PE (the pt. at which the grav. PE=0) so that you can easily calculate the difference in PE

Example: A 60. 0 -kg skier is at the top of a slope. At

Example: A 60. 0 -kg skier is at the top of a slope. At the initial point A, the skier is 10. 0 m vertically above point B. Find the gravitational PE of the skier at A and B, and the difference in PE between the 2 pts. choose B = 0 PEi = mghi PEi = (60. 0 kg)(9. 8 m/s 2)(10. 0 m) PEi =5880 J PEf = mghf PEf = (60. 0 kg)(9. 8 m/s 2)(0 m) B PEf =0 J A

Example: A 60. 0 -kg skier is at the top of a slope. At

Example: A 60. 0 -kg skier is at the top of a slope. At the initial point A, the skier is 10. 0 m vertically above point B. Find the gravitational PE of the skier at A and B, and the difference in PE between the 2 pts. PEi =5880 J PEf =0 J A PE = PEf - PEi PE = -5880 J B

Law of Conservation of Energy: Energy can not be created or destroyed. Actually, It’s

Law of Conservation of Energy: Energy can not be created or destroyed. Actually, It’s conservation of mass - energy

Remember E=mc 2 That is to say, energy and mass are interchangeable.

Remember E=mc 2 That is to say, energy and mass are interchangeable.

Although energy cannot be destroyed, it can go places where we can never recover

Although energy cannot be destroyed, it can go places where we can never recover it. Potential Kinetic Chemical Energy Heat RIP Electrical Sound And many more…

Conservation of Mechanical Energy Although energy may be changed into a different form, the

Conservation of Mechanical Energy Although energy may be changed into a different form, the final value will be the same as the initial value (energy is not lost). Ei = Ef KEi + PEi = KEf + PEf ½ mvi 2 + mghi = ½ mvf 2 + mghf

Kinetic vs. Potential Energy Calculate the KE and PE energy at each of the

Kinetic vs. Potential Energy Calculate the KE and PE energy at each of the 5 spots on the ski run. Assume the skier starts from rest. (m = 51 kg)

Kinetic vs. Potential Energy Calculate the KE and PE energy at each of the

Kinetic vs. Potential Energy Calculate the KE and PE energy at each of the 5 spots on the roller coaster. Assume the skater starts from rest.

Example: A diver weighing 750. N (mass = 77. 0 kg) drops from a

Example: A diver weighing 750. N (mass = 77. 0 kg) drops from a board 10. 0 m above the surface of the pool of water. A) Use the conservation of mechanical energy to find her speed at a point 5. 00 m above the water surface. 10 m B) Find the speed of the diver just before she strikes the water.

Example: A diver weighing 750. N (mass = 77. 0 kg) drops from a

Example: A diver weighing 750. N (mass = 77. 0 kg) drops from a board 10. 0 m above the surface of the pool of water. A) Use the conservation of mechanical energy to find her speed at a point 5 m above the water surface. B) Find the speed of the diver just before she strikes the water. hf = 5 m ½ mvi 2 + mghi = ½ mvf 2 + mghf ½(77)(0)+(77)(9. 8)(10)=½(77)(vf 2)+(77)(9. 8)(5) Vf = 9. 90 m/s

Example: A diver weighing 750 N (mass = 77. 0 kg) drops from a

Example: A diver weighing 750 N (mass = 77. 0 kg) drops from a board 10 m above the surface of the pool of water. A) Use the conservation of mechanical energy to find her speed at a point 5 m above the water surface. B) Find the speed of the diver just before she strikes the water. hf=0 ½ mvi 2 + mghi = ½ mvf 2 + mghf ½(77)(0)+(77)(9. 8)(10)=½(77)(vf 2)+(77)(9. 8)(0) Vf = 13. 9 m/s

Example: A sled and its rider together weigh 800. N. They move down a

Example: 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 energy to find the speed of the sled-rider system at the bottom of the hill, assuming the rider pushes off with an initial speed of 5. 00 m/s. ½ mvi 2 + mgyi = ½ mvf 2 + mgyf ½ vi 2 + gyi = ½ vf 2 + gyf ½(5)2+ (9. 8)(10)=½(vf 2)+ (9. 8)(0) vf = 14. 9 m/s 10 m

Conservative / Nonconservative Forces n A force is CONSERVATIVE if the work it does

Conservative / Nonconservative Forces n A force is CONSERVATIVE if the work it does on an object between 2 points is independent of the path the object takes between the 2 points. (The work done depends only on the initial and final positions. ) (example: Work done by gravity)

Conservative / Nonconservative Forces n A force is NONCONSERVATIVE if the work it does

Conservative / Nonconservative Forces n A force is NONCONSERVATIVE if the work it does on an object moving between 2 points depends on the path taken. (i. e. Work done by sliding friction)

Conservation of Energy with Nonconservative Forces. n A 15 kg kid, initially at rest,

Conservation of Energy with Nonconservative Forces. n A 15 kg kid, initially at rest, slides down a 8. 0 m high slide. Ideally, what is his final velocity at the bottom of the slide? n KEi + PEi = KEf + PEf n 0 + mgh = 1/2 mv 2 + 0 n (15 kg)(9. 8 m/s 2)(8. 0 m) = 1/2 (15 kg)v 2 n vf = 12. 5 m/s ~13 m/s

In reality, the final velocity of the kid is only 10 m/s. Where did

In reality, the final velocity of the kid is only 10 m/s. Where did the extra energy go? Friction is an nonconservative force which used up some of the initial potential energy. To account for friction, we need to add back in the work done by (or energy lost by) friction.

KEi + PEi + Workadded = KEf + PEf + Worklost Example: Work of

KEi + PEi + Workadded = KEf + PEf + Worklost Example: Work of someone pushing Example: Work done by friction Note: Usually work done by friction is negative (because it is in the opposite direction). But since we are ADDING BACK IN the work done by friction it is positive.

How much work was done by friction as the kid slid down the slide?

How much work was done by friction as the kid slid down the slide? (m = 15 kg, yi = 8. 0 m vf = 10 m/s) KEi + PEi + Workadded = KEf + PEf + Worklost 0 + mgh + 0 = 1/2 mvf 2 + 0 + Wfriction (15 kg)(9. 8 m/s 2)(8. 0 m) = 1/2(15 kg)(10. m/s)2 + Wf 1176 J = 750 J +Wf Wf = 426 J ~ 430 J

Potential Energy Stored in a Spring PEs = ½ kx 2 where k =

Potential Energy Stored in a Spring PEs = ½ kx 2 where k = spring constant x = distance spring is compressed or stretched (KE + PEg + PEs)i = (KE + PEg + PEs)f

Example: A block of mass 0. 500 kg rests on a horizontal, frictionless surface.

Example: A block of mass 0. 500 kg rests on a horizontal, frictionless surface. The block is pressed lightly against a spring, having a spring constant k=80. 0 N/m. The spring is compressed a distance of 2. 00 cm and released. Find the speed of the block at the instant it loses contact with the spring at the x = 0 position. 0. 500 kg (KE + PEg + PEs)i = (KE + PEg + PEs)f (PEs)i = (KE)f ½kxi 2 = ½mvf 2 ½(80)(0. 02)2 = ½(0. 5) vf 2 v = 0. 253 m/s

Example: The launching mechanism of a toy gun consists of a spring of unknown

Example: The launching mechanism of a toy gun consists of a spring of unknown spring constant. By compressing the spring a distance of 0. 120 m, the gun is able to launch a 20. 0 -g projectile to a maximum height of 20. 0 m when fired vertically from rest. Determine the value of the spring constant. (KE + PEg + PEs)i = (KE + PEg + PEs)f (PEs)i = (PEg)f ½kxi 2 = mgh ½(k)(0. 12)2 = (0. 02)(9. 8)(20) k = 544 N/m

Machines make work easier Work In = Work Out + Heat In a real

Machines make work easier Work In = Work Out + Heat In a real machine the efficiency must always be less than 100%

Types of Simple Machines: n Lever n Pulley n Ramp

Types of Simple Machines: n Lever n Pulley n Ramp

Work In Fulcrum Distance Out Distance In Work In = Work Out Force x

Work In Fulcrum Distance Out Distance In Work In = Work Out Force x Distance = Force x Distance Work Out

25 lbs 50 lbs Machines make work easier. 50 lbs 25 lbs

25 lbs 50 lbs Machines make work easier. 50 lbs 25 lbs

He lifts the package up 4 ft… 4 ft 8 ft But the work

He lifts the package up 4 ft… 4 ft 8 ft But the work stays the same. Remember…W = F x d

Power n Power: the rate at which work is done

Power n Power: the rate at which work is done

A bulldozer and a small boy can do the same amount of work. It’s

A bulldozer and a small boy can do the same amount of work. It’s just that the bulldozer can do it faster.

Units in the SI system….

Units in the SI system….

Units in the English system 1 HP = 746 Watts

Units in the English system 1 HP = 746 Watts

A new conveyor system at the local packaging plan will utilize a motorpowered mechanical

A new conveyor system at the local packaging plan will utilize a motorpowered mechanical arm to exert an average force of 890 N to push large crates a distance of 12 meters in 22 seconds. Determine the power output required of such a motor. n 490 W (rounded from 485 W)

The Taipei 101 in Taiwan is a 1667 -foot tall, 101 -story skyscraper. The

The Taipei 101 in Taiwan is a 1667 -foot tall, 101 -story skyscraper. The skyscraper is the home of the world’s fastest elevator. The elevators transport visitors from the ground floor to the Observation Deck on the 89 th floor at speeds up to 16. 8 m/s. Determine the power delivered by the motor to lift the 10 passengers at this speed. The combined mass of the passengers and cabin is 1250 kg. n 2. 06 x 105 W

Example: A 2. 00 x 103 kg car starts from rest and accelerates to

Example: A 2. 00 x 103 kg car starts from rest and accelerates to a final velocity of +20. 0 m/s in a time of 15. 0 s. Assume that the force of air resistance remains constant at a value of – 500. N during this time Find the average power developed by the engine. B) Find the instantaneous power when the car reaches its final velocity A)

Example: A 2000 kg car starts from rest and accelerates to a final velocity

Example: A 2000 kg car starts from rest and accelerates to a final velocity of +20. 0 m/s in a time of 15. 0 s. The force of the engine is 3160 N. A) Find the average power developed by the engine (average power uses average v).

Example: A 2000 kg car starts from rest and accelerates to a final velocity

Example: A 2000 kg car starts from rest and accelerates to a final velocity of +20 m/s in a time of 15 s. Assume that the force of air resistance remains constant at a value of – 500 N during this time. A) Find the average power developed by the engine (average power uses average v).

Example: A 2000 kg car starts from rest and accelerates to a final velocity

Example: A 2000 kg car starts from rest and accelerates to a final velocity of +20 m/s in a time of 15 s. Assume that the force of air resistance remains constant at a value of – 500 N during this time. B) Find the instantaneous power when the car reaches its final velocity (use velocity at instant you are solving for).

Example: An elevator has a mass of 1000. kg and carries a maximum load

Example: An elevator has a mass of 1000. kg and carries a maximum load of 800. kg. A constant frictional force of 4000. N retards its motion upward. What minimum power must the motor deliver to lift the fully-loaded elevator at a constant speed of 3. 00 m/s? (In watts and horsepower) v is constant, so a=0 FT – Ff – mg = 0 FT = Ff + mg = 4000 N + (1800 kg)(9. 8 m/s 2) FT = 2. 16 x 104 N P = FT v P = (2. 16 x 104 N)(3. 00 m/s) = 6. 48 x 104 W P = (6. 48 x 104 W)(1 hp / 746 W) = 86. 9 hp