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WORK AND CONSERVATION OF WORK AND CONSERVATION OF ENERGY ENERGY STYMVERLY GAWAT JENERUS JUAN AND ALWEN AGYAM
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WORK AND WORK AND CONSERVATION OF CONSERVATION OF

ENERGYENERGYSTYMVERLY GAWAT

JENERUS JUAN

AND ALWEN AGYAM

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Work is the transfer of energy through motion. In order for work to take place, a force must be exerted through a distance. The amount of work done depends on two things: the amount of force exerted and the distance over which the force is applied. There are two factors to keep in mind when deciding when work is being done: something has to move and the motion must be in the direction of the applied force. Work can be calculated by using the following formula: Work=force x distance

WorkWork

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Work is done on the books when they are being lifted, but no work is done on them when they are being held or carried horizontally.

WorkWork

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Work can be positive Work can be positive or negativeor negative

• Man does positive work lifting box

Man does negative work

lowering box

Gravity does positive work when box lowers

Gravity does negative work when box is raised

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Work done by a constant ForceWork done by a constant Force

Ekin = Wnet

• W = F s = |F| |s| cos = Fs s

|F| : magnitude of force |s| = s : magnitude of displacement Fs = magnitude of force in direction of displacement :

Fs = |F| cos

: angle between displacement and force vectors• Kinetic energy : Ekin= 1/2 m v2

• Work-Kinetic Energy Theorem:

F

s

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Conservation of Mechanical EnergyConservation of Mechanical Energy

Total mechanical energy of an object remains constant

provided the net work done by non-conservative forces

is zero: Etot = Ekin + Epot = constantor

Ekin,f+Epot,f = Ekin,0+Epot,0

Otherwise, in the presence of net work done bynon-conservative forces (e.g. friction):

Wnc = Ekin,f – Ekin,0 + Epot,f-Epot,i

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Example ProblemExample Problem

Suppose the initial kinetic and potential energies of a system are 75J and 250J respectively, and that the final kinetic and potential energies of the same system are 300J and -25J respectively. How much work was done on the system by non-conservative forces? 1. 0J 2. 50J 3. -50J 4. 225J 5. -225J

correct

Work done by non-conservative forces equals the difference between final and initial kinetic energies plus the difference between the final and initial gravitational potential energies.

W = (300-75) + ((-25) - 250) = 225 - 275 = -50J.

Samar HathoutSamar Hathout

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ExampleExample

Samar Hathout

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Conservation of EnergyConservation of Energy

Conservative forces:• Gravity, electrical, QCD…Non-conservative forces:• Friction, air resistance…Non-conservative forces still conserve energy!Energy just transfers to thermal energy

PE f KE f PEi KEiKE PE

Samar Hathout

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ExampleExample

A diver of mass m drops from a board 10.0 m above the water surface, as in the Figure. Find his speed 5.00 m above the water surface. Neglect air resistance.

9.9 m/s

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ExampleExample

A skier slides down the frictionless slope as shown. What is the skier’s speed at the bottom?

H=40 m

L=250 m

start

finish

28.0 m/s

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Example Example

Three identical balls are thrown from the top of a building with the same initial speed. Initially, Ball 1 moves horizontally. Ball 2 moves upward. Ball 3 moves downward.

Neglecting air resistance, which ball has the fastest speed when it hits the ground?A) Ball 1

B) Ball 2C) Ball 3D) All have the same speed.

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Springs (Hooke’s Law)Springs (Hooke’s Law)

Proportional to displacement from equilibrium

F kx

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Potential Energy of Potential Energy of SpringSpring

PE=-Fx

x

F

PE 1

2(kx)x

PE 1

2kx2

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x

Example Example

b) To what height h does the block rise when moving up the incline?

A 0.50-kg block rests on a horizontal, frictionless surface as in the figure; it is pressed against a light spring having a spring constant of k = 800 N/m, with an initial compression of 2.0 cm.

3.2 cm

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Power Power

Average power is the average rate at which a net force

does work:

Pav = Wnet / tSI unit: [P] = J/s = watt (W)

Or Pav = Fnet s /t = Fnet vav

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Example Example

A 1967 Corvette has a weight of 3020 lbs. The 427 cu-in engine was rated at 435 hp at 5400 rpm.a) If the engine used all 435 hp at 100% efficiency during acceleration, what speed would the car attain after 6 seconds?b) What is the average acceleration? (in “g”s)

a) 120 mph b) 0.91g

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Example Example

Consider the Corvette (w=3020 lbs) having constantacceleration of a=0.91ga) What is the power when v=10 mph?b) What is the power output when v=100 mph?

a) 73.1 hp b) 732 hp (in real world a is larger at low v)


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