chapter 5 work and energy. 6-1 work done by a constant force the work done by a constant force is...

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Chapter 5 Work and Energy

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Page 1: Chapter 5 Work and Energy. 6-1 Work Done by a Constant Force The work done by a constant force is defined as the distance moved multiplied by the component

Chapter 5

Work and Energy

Page 2: Chapter 5 Work and Energy. 6-1 Work Done by a Constant Force The work done by a constant force is defined as the distance moved multiplied by the component

6-1 Work Done by a Constant ForceThe work done by a constant force is defined as the distance moved multiplied by the component of the force in the direction of displacement:

(6-1)

Page 3: Chapter 5 Work and Energy. 6-1 Work Done by a Constant Force The work done by a constant force is defined as the distance moved multiplied by the component

6-1 Work Done by a Constant Force

In the SI system, the units of work are joules:

For person walking at constant velocity:

•Force and displacement are orthogonal, therefore the person does no work on the grocery bag

•Is this true if the person begins to accelerate?

Page 4: Chapter 5 Work and Energy. 6-1 Work Done by a Constant Force The work done by a constant force is defined as the distance moved multiplied by the component

Example 6-1. A 50-kg crate is pulled along a floor. Fp=100N and Ffr=50N. A) Find the work done by each force acting on th crateB)Find the net work done on the crate when it is dragged 40m.

Wnet = Wg + Wn + Wpy + Wpx + Wfr

Page 5: Chapter 5 Work and Energy. 6-1 Work Done by a Constant Force The work done by a constant force is defined as the distance moved multiplied by the component

Mechanical Energy

Types of Mechanical Energy

•Kinetic Energy = ½ mv2

•Potential Energy (gravitational) = mgh

•Potential Energy (stored in springs) = ½ kx2

Page 6: Chapter 5 Work and Energy. 6-1 Work Done by a Constant Force The work done by a constant force is defined as the distance moved multiplied by the component

6-3 Kinetic Energy, and the Work-Energy Principle

Wnet = Fnetd

but Fnet = ma

Wnet = mad

v22 = v1

2 + 2ad

a = v22 - v1

2 2dWnet = m (v2

2 - v12)

2We define the kinetic energy:

Page 7: Chapter 5 Work and Energy. 6-1 Work Done by a Constant Force The work done by a constant force is defined as the distance moved multiplied by the component

6-3 Kinetic Energy, and the Work-Energy Principle

The work done on an object is equal to the change in the kinetic energy:

• If the net work is positive, the kinetic energy increases.

• If the net work is negative, the kinetic energy decreases.

(6-4)

Page 8: Chapter 5 Work and Energy. 6-1 Work Done by a Constant Force The work done by a constant force is defined as the distance moved multiplied by the component

Example: A 145g baseball is accelrated from rest to 25m/s.A) What is its KE when released?B) What is the work done on the ball?

Page 9: Chapter 5 Work and Energy. 6-1 Work Done by a Constant Force The work done by a constant force is defined as the distance moved multiplied by the component

Potential Energy

• Potential energy is associated with the position of the object within some system

• Gravitational Potential Energy is the energy associated with the position of an object to the Earth’s surface

Page 10: Chapter 5 Work and Energy. 6-1 Work Done by a Constant Force The work done by a constant force is defined as the distance moved multiplied by the component

6-4 Potential Energy

In raising a mass m to a height h, the work done by the external force is

We therefore define the gravitational potential energy:

(6-5a)

(6-6)

Page 11: Chapter 5 Work and Energy. 6-1 Work Done by a Constant Force The work done by a constant force is defined as the distance moved multiplied by the component

6-4 Potential Energy

Potential energy can also be stored in a spring when it is compressed; the figure below shows potential energy yielding kinetic energy.

Page 12: Chapter 5 Work and Energy. 6-1 Work Done by a Constant Force The work done by a constant force is defined as the distance moved multiplied by the component

6-4 Potential Energy

The force required to compress or stretch a spring is:

where k is called the spring constant, and needs to be measured for each spring. k is measured in N/m.

(6-8)

Page 13: Chapter 5 Work and Energy. 6-1 Work Done by a Constant Force The work done by a constant force is defined as the distance moved multiplied by the component

Conservation of Energy

• Energy cannot be created or destroyed• In the absence of non-conservative forces

such as friction and air resistance:

Ei = Ef = constant

• E is the total mechanical energy

fsgisg )PEPEKE()PEPEKE(

Page 14: Chapter 5 Work and Energy. 6-1 Work Done by a Constant Force The work done by a constant force is defined as the distance moved multiplied by the component

Example: A marble having a mass of 0.15 kg rolls along the path shown below. A) Calculate the Potential Energy of the marble at A (v=0)B) Calculate the velocity of the marble at B.C) Calculate the velocity of the marble at C

A

C

B

10m

3m

Page 15: Chapter 5 Work and Energy. 6-1 Work Done by a Constant Force The work done by a constant force is defined as the distance moved multiplied by the component

Ex. 6-11 Dart Gunmdart = 0.1kgk = 250n/mx = 6cmFind the velocity of the dart when it releases from the spring at x = 0.

Page 16: Chapter 5 Work and Energy. 6-1 Work Done by a Constant Force The work done by a constant force is defined as the distance moved multiplied by the component

A marble having a mass of 0.2 kg is placed against a compressed spring as shown below. The spring is initially compressed 0.1m and has a spring constant of 200N/m. The spring is released. Calculate the height that the marble rises above its starting point. Assume the ramp is frictionless.

h

Page 17: Chapter 5 Work and Energy. 6-1 Work Done by a Constant Force The work done by a constant force is defined as the distance moved multiplied by the component

Nonconservative Forces

• A force is nonconservative if the work it does on an object depends on the path taken by the object between its final and starting points.

• Examples of nonconservative forces– kinetic friction, air drag, propulsive forces

• Examples of conservative forces– Gravitational, elastic, electric

Page 18: Chapter 5 Work and Energy. 6-1 Work Done by a Constant Force The work done by a constant force is defined as the distance moved multiplied by the component

Power• Often also interested in the rate at which the

energy transfer takes place• Power is defined as this rate of energy transfer

– SI units are Watts (W)

2

2

s

mkg

s

JW

P = W = FΔx = Fvavg

t t

Page 19: Chapter 5 Work and Energy. 6-1 Work Done by a Constant Force The work done by a constant force is defined as the distance moved multiplied by the component

Power, cont.

• US Customary units are generally hp– need a conversion factor

– Can define units of work or energy in terms of units of power:

• kilowatt hours (kWh) are often used in electric bills

W746s

lbft550hp1