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Work, Energy, and Energy Conservation

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Work, Energy, and Energy Conservation. Chapter 5, Sections 1 - 3 Pg. 168-186. Σ F. d. Work. Any force that causes a displacement on an object does work (W) on that object. W= ∑ Fd. d. Work. Work is done only when components of a force are parallel to a displacement. F. θ. Σ F. - PowerPoint PPT Presentation
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Work, Energy, and Energy Conservation Chapter 5, Sections 1 - 3 Pg. 168-186
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Page 1: Work, Energy, and Energy Conservation

Work, Energy, and Energy Conservation

Chapter 5, Sections 1 - 3

Pg. 168-186

Page 2: Work, Energy, and Energy Conservation

WorkWork

W=∑Fd

Any force that causes a displacement on an object does work (W) on that object.

ΣF

d

Page 3: Work, Energy, and Energy Conservation

Work is done only when components of a force are parallel to a displacement.

W=∑Fd(cos θ)

WorkWork

F

θ

d

ΣF

Work is expressed in Newton • meters (N•m) = Joules (J)

Page 4: Work, Energy, and Energy Conservation

Sample Problem

How much work is done on a box pulled 3.0 m by a force of 50.0 N at an angle of 30.0° above the horizontal?

W=∑Fd(cos θ)

50.0 N

30.0°

d

ΣF

= (50.0 N x 3.0 m)(cos 30.0°)

W = 130 J

Page 5: Work, Energy, and Energy Conservation

EnergyEnergy

Two types of Energy:

1. Kinetic Energy (KE) - energy of an object due to its motion

2. Potential Energy (PE) - energy associated with an object due to the position of the object.

Energy is the ability to do work.

Page 6: Work, Energy, and Energy Conservation

Kinetic EnergyKinetic Energy

Kinetic energy depends on the speed and the mass of the object.

KE = ½ mv²

Page 7: Work, Energy, and Energy Conservation

Sample Problem

What is the kinetic energy of a 0.15 kg baseball moving at a speed of 38.8 m/s?

KE = ½ mv²

KE = (½)(0.15 kg)(38.8m/s)²

KE = 113 J

Page 8: Work, Energy, and Energy Conservation

Work-Kinetic Energy Theorem

The net work done on an object is equal to the change in kinetic energy of an object.

Wnet = ΔKE

Wnet = ½mvf ² - ½mvi²

Page 9: Work, Energy, and Energy Conservation

Sample Problem

A 50 kg sled is being pulled horizontally across an icy surface. After being pulled 15 m starting from rest, it’s speed is 4.0 m/s. What is the net force acting on the sled?

Wnet = ½mvf ² - ½mvi²

Vi = 0 m/s Vf = 4.0 m/s

∑Fd = ½mvf ²

∑F = (½mvf ²)/d = [(½)(50kg)(4.0m/s)²]/ 15 m

∑F ≈ 27 N

Page 10: Work, Energy, and Energy Conservation

Potential EnergyPotential Energy

Potential energy (PE) is often referred to as stored energy.

Gravitational potential energy (PEg) depends on the height (h) of the object relative to the ground.

PEg= mgh

Page 11: Work, Energy, and Energy Conservation

Sample Problem

What is the gravitational potential energy of a 0.25 kg water balloon at a height of 12.0 m?

PEg= mgh

PEg= (0.25 kg)(9.81 m/s²)(12.0 m)

PEg= 29.4 J

Page 12: Work, Energy, and Energy Conservation

Conservation of Mechanical Energy

Law of conservation of energy: Energy is neither created or destroyed. It simply changes form.

Mechanical energy (ME) is the sum of kinetic and all forms of potential energy.

ME = KE +∑PE

Page 13: Work, Energy, and Energy Conservation

h

100 % PE

0 % KE

50 % PE

50 % KE

0 % PE

100 % KE

Total mechanical energy remains constant in the absence of friction.

Page 14: Work, Energy, and Energy Conservation

Sample Problem

Starting from rest, a child zooms down a frictionless slide from an initial height of 3.00 m. What is the child’s speed at the bottom of the slide? The child’s mass is 25.0 kg.

hi = 3.00 mm = 25.0 kg

hf = 0 m

vi = 0 m/s

vf = ? m/s

Page 15: Work, Energy, and Energy Conservation

½ mvi² + mghi = ½ mvf² +mghf

(25.0 kg) (9.81 m/s²) (3.00 m) = (½)(25.0 kg) (Vf)²

736 J / (12.5 kg) = Vf ²

Vf ² = 58.9 m²/s² Vf = 7.67 m/s

hi = 3.00 mm = 25.0 kg

hf = 0 m

vi = 0 m/s

vf = ? m/s

Page 16: Work, Energy, and Energy Conservation

Mechanical Energy in the presence of friction

In the presence of friction, measured energy values at start and end points will differ.

f Fapp

KE

KE

KE

KETotal energy, however, will remain conserved.


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