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Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

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Page 1: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Work and Energy

So far, we have viewed motion in terms of Newton’s 3 Laws.

What are they?

Page 2: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

• Law of Inertia – a body at rest stays at rest & a body in motion continues in its straight line motion at a constant v unless a net external force acts on it.

Page 3: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Law of Acceleration -An Fnet will cause a mass to accelerate F = ma.

Page 4: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Action- Reaction - If a force is applied to a particle by a body, the particle will apply an

equal but opposite force to the body.

Page 5: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Work, Power, & Energy

Energy, E offers an alternative analysis of motion and its causes.

Changes in E is valuable in analyzing motion in systems i.e. roller coasters, engines, power plants, transformers.

What are some types of energy?

What is energy? Define it.

Page 6: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Def: Energy is ability to do work.

Work is done when force applied to an object or particle causes motion parallel to force direction.

Work and Energy are Scalar quantities.

Page 7: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

W = F net x d cos.

• F = parallel l l to displacement N.• . = angle between force and displacement. • . = 0, W = Fd.

• d = displacement – m.

• If Fap has no component parallel to motion W=0!

• Remember Fnet = F, if more than 1parallel force, they add.

Page 8: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Units W = Fd = (N m)

kg m m . s2

kg m 2.s2

Joules (J)

Page 9: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

• When a force F is applied to an object, it may produce a displacement d.

W = F d = F d cos()

Page 10: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Work can be zero even if force is applied.

W = Fd cos

• The work done is zero if:

– d = 0 m (no displacement)

– force perpendicular to the displacement.

Page 11: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Work is positive when the force component causing the displacement is in the same direction as the displacement.

Work is Scalar but:

Page 12: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Work is negative when the force component causing the displacement is in the opposite direction as the displacement.

Page 13: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

• There are many important examples of forces that do not do any work.

• For example, the gravitational force between the earth and the moon does not do any work!

Zero Work

Page 14: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Moving horizontally while applying an upward force is not work. Yeah – right!!

Page 15: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Examples

• How much work is done to lift a 10 N chair 1 meter?

• How much work is done to hold a 44 N weight at a constant height of 2.0 m?

W = Fd10N x 1m

10-J

W = Fd 44N x 0 W = 0

Page 16: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Forces acting at angles to motion

Consider the Force Component parallel to displacement.

Page 17: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Ex 1: A man pulls a cart with a ropethat makes a 20o angle to the horizontal. If he exerts a 100 N force, how much work is done is he pulls the cart 8.0 meters?

Page 18: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

W = F cos d = 100 N (cos 20o)(8.0m)

= 752 Nm = 752 J

100 N

20o

FII

Page 19: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Ex 2. A student lifts a 1.5-kg box 2-m straight up.

a. How much work did she do on the box?

b. How much work did gravity do on the box?

Page 20: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

The force on the box was:Fg = mg (1.5 kg)(10 m/s2) = 15-N.

The work done by the student was W = Fd(15-N)(2-m) = +30 J.

Gravity did negative 30 J of work b/c it was pulling in the opposite direction of the displacement.

Page 21: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Hwk: Worksheet “intro work”

• Hwk Work Prb’s Text read 168 – 171

• Do 170 all

• Pg 193 #2, 3, 4, 5, 7-9.

Page 22: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

• Hwk Work Prb’s Text read 168 – 171

• Do 170 all

• Pg 193 # 3, 4, 5, 7-9.

Page 23: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Energy

Page 24: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Energy = Ability to do work.Energy is measured in Joules.

E measured in terms of amount of work it can do.

If a battery has 9 J of E, it can do 9 J of work.

Page 25: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Relationship between Work and Energy.

• It takes work to change an object’s energy from one form to another, or to increase or decrease it.

• What are some forms of energy?

Page 26: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Common Energy Types:

Kinetic (KE) – energy of motion

Gravitational Potential (GPE) – energy due to height in gravitational field.

Chemical- energy stored in chemical bonds

Elastic Potential – energy stored in shape deformations.

Page 27: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Electrical Energy – due to charge separation.

Internal or Heat Energy (Q) – due to vibration of atoms.

Mass/Nuclear Energy = Stored between subatomic particles. E = mc2.

Page 28: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Kinetic Energy, KE is energy associated with object in motion.

The amount of KE = ½ mv2.

m = mass in kg.

v = velocity in m/s.

KE in Joules (J) or Nm.

Page 29: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Derivation of KE equation.

• KE = W

• KE = Fd

• KE = mad

• KE = m (v) d = m v d

t t

= m v v

= m(vf - vi) (vf + vi) where vi = 0

2

KE = ½ mv2.

Page 30: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Ex 3: Calculate the speed of a 80,000-kg airplane with KE = 1.1 x 109 J.

Page 31: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

KE = ½ mv2

mKEv /2

kgJx 000,80/)101.1(2 9

= 170 m/s

Page 32: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Work must be done to change the E of an object.

W = KE. W = KEf - KEi

Page 33: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Ex 3: A pitcher does work to accelerate a 145g baseball from rest to 25 m/s.

a) What is its KE?

b) How much work was done to reach this speed?

Page 34: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

KE = 1/2mv2.

• a) ½(0.145kg)(25m/s)2 = 45 J

• b) since the KE is 45 J and the initial KE was zero:

KE =KEf – KEi

KE = 45 J – 0 J = 45 J of work

Page 35: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

In order to change the velocity of an object (KE), work must be done.

The amount of work done is equal to the change in KE.

Work – KE Theorem Wnet = KE

Page 36: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Ex 4: How much work is required to accelerate a 1000 kg car from 20 m/s to 30m/s?

Page 37: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

KE = KE2- KE1.

•W = 1/2mv2f - 1/2mv2

i.

•=1/2(1000kg)(30m/s)2 -1/2(1000kg)(20m/s)2. = 2.5 x 105 J.

The work needed is equal to the KE.

Page 38: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Ex 4: On a frozen pond, a person kicks a 10-kg sled giving it an initial speed of 2.2 m/s. It slides and eventually comes to a stop.

• How much work is done bringing it to a stop?

• What force does work to stop the sled?

• How far will the sled move after being kicked if the coefficient of kinetic friction is 0.10 between the ice and the sled?

Page 39: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Listm = 10kgvi = 2.2 m/s vf = 0 = 0.1d = ?

W = KE = KEf – KEi

W = 0 - 1/2mvi2.

W = ½(10kg)(2.2)2.= 24.2 J

Friction stops the sled.

Page 40: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

• W = 24.2 J

• Fd = 24.2 JFnd=24.2 J

mgd = 24.2 J

• 0.1(10kg)(9.81m/s2)d = 24.2 J

• d = 2.48 m.

Page 41: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

In the past we’ve used velocity, acceleration equations to solve

for distance, velocity etc.

We can consider using KE and work equations.

Page 42: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

• Text Pg 176 #1, 2, 4 and

• pg 193 #5-10 12-14.

Page 43: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Force/distance GraphsArea under curve = work or E.

Page 44: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Do Now: A constant force is applied over a distance to an object & graphed. How

would we calculate work from the graph?

Find the work done at 8-m.

Page 45: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Find the work done between 4 – 8m.

4mx5N = 20 Nm

What if the force is not constant but varies over distance? How would we find the work done from

the graph?

½ (4mx5N) = 10 Nm

Wtot = 20+10=30 Nm

Page 46: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

How much work between 8 – 14 m?

• 25J

Page 47: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Potential Energy – Stored Energy

An object can store energy as the result of its position.

Page 48: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Gravitational Potential Energy (GPE or PEg)

Energy due to position of object above some base level (lowest available point).

Page 49: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

PEg = work done to raise some distance against gravity.

W = Fd

W = mgd

PEg = mgh

Page 50: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Examples of work done by GPE

Pile driver

Dam or waterfalls

See Saw Circus Act.

Page 51: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Ex 2: A 12 N weight fell 2-m. How much PE did it lose? What agent did work on the weight? Was the work positive or negative?

PE = (mg) h

(12N)(2m) = 24 J

Positive F and d same

Page 52: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

As objects fall under gravity, they lose PEg but gain KE. (They go faster)

Page 53: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Ex 3: A 50 N weight falls for 10-m. How much PE does it lose? 

How much KE does it gain? 

What is its velocity at that point?

• 50N x 10m = 500 J

• 500 J

• KE = ½ mv2.

• 500J = ½ (5kg) v2.

• 14 m/s.

Page 54: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Elastic PE

Page 55: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Elastic materials store energy when stretched or compressed. The further they are deformed, the more E they will store (the more work they can do).

It takes a force to stretch or compress a spring.

Each spring has a constant, k, which indicates how much force is needed to deform it.

Page 56: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Hooke’s Law

• How much force is needed to deform elastic material.

• Hooke’s Law – Fs = kx.

• Force on spring, N (=weight),

• x is L (m),

• k is constant in N/m.

Page 57: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Ex 4: A 12-N weight stretches a spring 25- cm when hung from it. What is k for the spring?

• F = kx

• F/x = k

• 12-N/0.25m = 48 N/m.

Page 58: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Graph F vs. x is direct linear

Slope = k

Fs = kx.

Page 59: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Elastic Energy PEs.

• PEs= ½ kx2.

– x is the dif btw relaxed length and new length in meters sometime x.

– k is a constant for the material N/m.

– PE in joules.

Page 60: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Ex 5. A 2.0 kg mass is attached to a vertical spring, the spring is stretched 10.0 cm such that the mass is 50.0 cm above the table.

1. What is the GPE relative to the table?

2. What is the spring’s PEs if k = 400.0 N/m?

3. What is the total PE of the system?

9.81 J

2.0 J

11.8 J

Page 61: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Ex 6: A spring with a force constant of 5.2-N/m has a relaxed length of 2.45-m. When a mass is attached to it the vertical length of the spring is 3.57-m. Calculate the PEs stored in the spring.

3.3 J

Page 62: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

• W = PEs

• W = ½ kx2.

• =1/2 (500)(0.03m)2.

• W = 0.225 J

7. A spring has a constant of 500 N/m. What is the work required to compress it 3.0-cm?

Page 63: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Derive the PEs equation.Energy is area under curve for F vs. x graph.

Area = E or W

W = ½ F x

But Fs = kx so

W = ½ (kx) x

E = ½ k x2.

Page 64: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Hwk: Rev Bk Read pg 169-171

Do Pg 173 # 1 - 14, 21-23

Separate Sheet.

Page 65: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Mechanical Energy & Non-mechanical Energy

Mechanical Energy =KE, GPE, EPE.

Page 66: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Non-mechanical/ Internal = heat, light, chemical, nuclear, magnetic, electric, sound.

Page 67: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

If no E is lost to non-mechanical, then

Conservation of Mechanical Energy.

Before After Mechanical Energy = Mechanical Energy

KE 1 + GPE 1 + EPE 1= KE 2 + GPE 2 + EPE 2.

Page 68: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Energy Transformations What are the energy transformations in

the following situations?

• Tossing a ball into the air and catching it.

• Bouncing a ball on the floor.

• Driving a car into a brick wall.

Page 69: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Calculations Using Conservation of Energy

• Identify the energy/work transformations.

• Set up equalities.

• Break down equations if necessary.

Page 70: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Common Conservation Concepts

• E constant at every point in system.

• If ball has 100-J PEg at 2-m is dropped from rest, how much Etot does it have at 1-m?

• 100-J

• How much KE does it have a 1-m?

• PEg = KE or

• PEg lost = KE gained.

• 50-J

• W done on system = E.

• If ball gains 150-J PEg by being raised up, how much work was done to raise it?

• 150-J

Page 71: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Ex 1: A small 10 g (0.01 kg) ball is held to a slingshot stretched 6.0 cm. The spring constant is 200 N/m. It is released and allowed to rise to its highest point.

a. What are the energy transformations?

b. What is the PEs before it is released?

c. What is the KE of the ball just as it leaves the slingshot?

d. What is the ball’s speed at that instant?

e. How high does the ball rise if it is shot directly upward?

1/2kx2 = 0.36J

PEs lost = KE gained = 0.36J

KE = 0.36J = 1/2mv2 v = 8.5 m/s

PEs KE PEg

KE lost = PEg gained 0.36J=mgh h= 1.5m

Page 72: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Ex 2. A bike rider approaches a hill at a speed of 6.1 m/s. The mass of the bike and rider is 95 kg.

• What are the E transformations as it coasts uphill?

• How high can it coast up the hill? Ignore friction.

• ½ mv2 = mgh• v2/2g = h• (6.1m/s)2 /2(9.81 m/s2)• h = 1.9 m.

Page 73: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Ex 3. An apple of mass 1.47 kg is dropped by a student to the ground.

If the apple’s velocity a moment before hitting the ground is 5.42 m/s, from what height was it dropped?

~ 1.5 m

Page 74: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Ex 4. A skier starts from rest at the top of a 45 m high hill. He skis down the hill which is at a 30o incline, down into a valley, and coasts 40m up to the top of the next hill.

• How fast is he going at the valley bottom? Ignore friction.

• What is his speed at the top of the 2nd hill?

Page 75: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

How fast is he going at the valley bottom?

• At top all PEg, at bottom all KE.

• PEgi = KEf.

• mgh = ½ mv2.• gh = ½ v2.• v = 30 m/s.

45-m 40-m

Page 76: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

What is his speed at the top of the 2nd hill?

• On hill 1 he has only PEg .

• On hill 2 he has both PEg and KE.

• PEg lost = KE gained.

• PE1 – PE2 = KE.

• mgh = ½ mv2.• gh = ½ v2.

• (9.81 m/s2) (45-40)m = ½ v2.• v = 9.9 m/s.

45-m 40-m

Page 77: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Ex 5: An archer puts a 0.3 kg arrow to the bowstring. She exerts an average force of 201-N to draw the bowstring back 1.3-m.

• What is the speed of the arrow as it leaves the bow?

• If the arrow is shot straight up, how high will it rise?

Fd = (201 N)(1.3m) = 261.3 J

h = 90 m

W = E = KE

261.3 J = KE =½ mv2

W = PEg

42 m/s

261.3 J = PE =mgh

Page 78: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Pendulum Problems

PE to KE to PE

Page 79: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Compare the PE & KE at the top & bottom of the swing.

• Top KE =0

• PEg maximum

• Bottom of swing PEg = 0

• KE is maximum

Page 80: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Ex 6. A 0.4-kg pendulum bob has 10-J of PEg at the top of its swing.

• What is its KE at the bottom of the swing?

• What is its velocity at the bottom?

• What is its velocity when it is halfway between the top and bottom?

• 10-J• 10-J = ½ mv2 v2 = 50 • v = 7.1 m/s. • 5 m/s.

Page 81: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Hwk read Txt 5-3do pg 185 1, 2, 5 and

Pg 195 #33, 38, 39, 50, 57, 59Show all equations, work, units, circle

answers.Counts for double hwk due D4

(Tuesday)

Page 82: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Roller CoastersSafari Film Clip “Physics of Fun” 23 min

• While you watch:

• List any physics concepts we’ve covered.

• Give as many examples of how they’re used in “fun” as you can.

• List physics concepts that are new.

• Give examples of those.

Page 83: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

PowerDef: Rate at which work is done.

Power = work/time = W J Nm

t s s

1 J/s = 1 Watt (W)

If it takes 10 seconds to do 50 J of work, then

P = 50J10s

5 J/s or 5W.

Page 84: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Power is related to speed that work gets done.Watts are commonly used to describe how fast motors & engines will do work.

P = W Fd Fvt t

1 watt is the rate at which a 1N forcedoes work if it moves a body 1m/s.

1 horsepower (HP) = 746 watts.

Page 85: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Ex 2: A motor exerting a steady force of 10N on an object keeps the object moving forward at 2m/s. What is the power of the motor?

Page 86: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

P = Fv

P = (10N)(2m/s) = 20 Nm = 20 W. s

Page 87: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Ex 3: An engine exerts a force 1000 N and expends 12 kW of power to keep a car moving at constant speed. What is the car’s velocity?

Page 88: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

P = Fv v = P/F

12 kW = 12,000 W = 12,000 Nm/s

So 12,000Nm/s = 12 m/s 1000 N

Page 89: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Hwk: Text pg 187 – 189Do Prac Prb 189 #1, 3-5, and Sec Review PRb #1-3.

Page 90: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Energy Lost to Friction (or other internal forms)

• Often Mech. E is converted to heat because of friction or can be converted to other forms of internal E like sound.

• Think about a box being pushed on the ground at a constant velocity by an applied force of 20-N. What force is friction exerting on the box?

Page 91: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Ex 1. A girl pushes a box at a constant speed 10-m by doing 15-J of work. How much work was done by friction?

• 15 J

Hint: Sketch the free body diagram.

Page 92: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

• If some ME is “missing” after your calculations are done, it was probably “lost” to frictional heating.

• The “lost” ME is the difference between the the total initial ME the total final ME.

• Set up an energy transformation equation and take the difference between the two energies.

Page 93: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Ex 2. A 5 kg box slides down a hill from a height of 6-m. If its KE at the bottom of the hill is 200-J, how much energy was lost to friction?

• PE = mgh should equal gain in KE

• =(5kg)(9.81m/s2)(6m)

• =294 J but KE only 200J

294 J – 200 J = 94 J Lost

Page 94: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Ex 3: A workman uses a pulley to raise a 12-N box 12-m. If he does 200-J of work in raising the box, how much energy was lost to friction?

• 200 J – 144 J .

• 56 J

Page 95: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Energy & Work Something for Nothing?

Why do people use a ramp rather than steep stairs to push a box or shopping cart?

• If a box gains 4 J of GPE, it takes 4 J of work to give it the GPE regardless of whether you lift it straight up or push it up a (frictionless) ramp!

Page 96: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Consider sliding a box up a ramp to change its PEg.

force you apply is to overcome the weight.

(no friction).

As the ramp angle gets lower the distance to raise the object must get longer to attain the same PE.

So F gets less, d gets proportionally longer.

Page 97: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

For the same PE, the distance can be shorter or longer. But work Fd is the same.Either large F & short d, or small F & long d.

h2h1d1

d2

larg

e F

small F

h1 h2

Page 98: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Hwk Packet.

Page 99: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Efficiency IB only

Usually, some energy is lost to heat, light, sound, etc. We must do extra work.

Efficiency is a percentage:

useful work done x 100%

actual work done

Page 100: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Ex 4 reg: An engine with a power output of 1.2 kW pulls an object with weight of 1000 N at a constant speed straight up. A constant frictional force of 300 N acts on the engine. The object is lifted a distance of 8.0 m.

1.Find the speed of the object .

2.the efficiency of the engine.

Page 101: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Ex 4: An engine with a power output of 1.2 kW drags an object with weight of 1000 N at a constant speed up a 30o incline. A constant frictional force of 300 N acts between the object and the plane. The object is dragged a distance of 8.0 m.

1. Find the speed of the object and the efficiency of the engine.

2. calculate the energy output per second of the fuel used.

Page 102: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

The downhill weight component is: 1000 N (sin 30o) = 500 N.

The total force the engine must overcome is weight + friction:

500 N + 300 N = 800 N.

P = Fv v = P 1200 W v = 1.5 m/s. F 800 N

Speed of the Object

Page 103: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

The machine lifts the weight to a height: 8.0m (sin30o) = 4.0 m.

The useful work is (mg)h:(1000 N)(4.0 m) = 4000 J.

The actual work done is: (800 N)(8.0m)= 6400 J.

Eff: useful work x 100% 4000 J x 100%actual work 6400 J

=63 %

Page 104: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

You can calculate the energy output per second of the fuel used.

Since the machine has a power output of 1.2 kW and is 63% efficient, the fuel must produce energy at a rate of:

1.2 x 103 J/s = 1.9 x 103 J/s.

0.63

Page 105: Work and Energy So far, we have viewed motion in terms of Newton’s 3 Laws. What are they?

Work done by non-constant force.Area under curve of F vs d = work done

W = Fd = ½ kx2.