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4.5 Elastic potential energy and Simple Harmonic Motion (SHM)
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4.5 Elastic potential energy and Simple Harmonic Motion (SHM)

Dec 13, 2015

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Holly McGee
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Page 1: 4.5 Elastic potential energy and Simple Harmonic Motion (SHM)

4.5 Elastic potential energy and Simple

Harmonic Motion (SHM)

Page 2: 4.5 Elastic potential energy and Simple Harmonic Motion (SHM)

How does a rubber band reflect the link between energy and forces?

Think carefully about the behaviour of stretchy objects like rubber bands and springs

What happens to them?

Page 3: 4.5 Elastic potential energy and Simple Harmonic Motion (SHM)

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FeFaFe

Fe

Fa FeFaVmax

V = 0 m/s

V = 0 m/s

Page 4: 4.5 Elastic potential energy and Simple Harmonic Motion (SHM)

Stretchy stuff responds to forces by storing energy

When you apply force to an elastic object like a spring or elastic band

The force does work on the object because it causes a displacement

This gives the spring energy The spring releases this energy when it is

given the chance to return to equilibrium length

Page 5: 4.5 Elastic potential energy and Simple Harmonic Motion (SHM)

How do we know it releases energy?

Well, what were to happen if you placed something in front of that spring?

Page 6: 4.5 Elastic potential energy and Simple Harmonic Motion (SHM)

Elastic potential energy

Energy stored in springs are a type of potential energy

Like gravity, once the energy is put into the spring, it can be released if the conditions are right

In fact, elastic potential energy is similar to gravity

You can compare pulling on a spring to Eg

Page 7: 4.5 Elastic potential energy and Simple Harmonic Motion (SHM)

In gravitational potential energy, stored energy from raised objects is released when the gravity pulls the object back down – similar to what the spring does when it “pulls” the mass back to equilibrium point.

Page 8: 4.5 Elastic potential energy and Simple Harmonic Motion (SHM)

Ideal spring

An ideal spring is one that doesn’t deform when stretched or depressed

That means it doesn’t get damaged and can return back to normal shape

An ideal spring that we study also assumes that external forces like friction do not interfere with it – nor does the spring experience any internal forces

Page 9: 4.5 Elastic potential energy and Simple Harmonic Motion (SHM)

Reality vs. ideal conditions

What happens eventually to a bouncing mass on a spring in real conditions?

If you had an ideal spring, what happens eventually to the bouncing mass?

Page 10: 4.5 Elastic potential energy and Simple Harmonic Motion (SHM)

Hooke’s Law

An ideal spring follows Hooke’s Law, which states that the force required to deform a spring per unit length is always constant

Where: F = -kx F = force applied in Newtons (N) k = spring constant in N/m x = position of spring relative to equilibrium in

metres (m)

Page 11: 4.5 Elastic potential energy and Simple Harmonic Motion (SHM)

Why the negative?

The negative is supposed to make up for the relativity in direction of forces

Hooke’s law is written from the spring’s point of view

Page 12: 4.5 Elastic potential energy and Simple Harmonic Motion (SHM)

Hooke’s Law is written from the point of view of the spring

Page 13: 4.5 Elastic potential energy and Simple Harmonic Motion (SHM)

Simple Harmonic Motion

SHM is created when the force (and therefore acceleration) is proportional to the displacement

In the previous animation of the spring’s motion, notice that the net force on the mass is the greatest when the displacement is greatest from equilibrium

Page 14: 4.5 Elastic potential energy and Simple Harmonic Motion (SHM)

Fa

FeFa

FeFe

Fa FeFaVmax

V = 0 m/s

V = 0 m/s

Page 15: 4.5 Elastic potential energy and Simple Harmonic Motion (SHM)

SHM creates periodic motion

This relationship is periodic – like waves, it exhibits regular, repeated motion that can be described using many of the same properties that you use to describe wave functions

Imagine the spring that we discussed earlier, but this time it moves along a track

The mass is attached to a writing device that can sketch out the path of the mass

Page 16: 4.5 Elastic potential energy and Simple Harmonic Motion (SHM)
Page 17: 4.5 Elastic potential energy and Simple Harmonic Motion (SHM)

Mathematically…

In order to make a clear relationship between the spring and the forces associated with it, you can compare the movement of the bouncing mass to a handle on a rotating disc

Page 18: 4.5 Elastic potential energy and Simple Harmonic Motion (SHM)

Direction of rotation

Page 19: 4.5 Elastic potential energy and Simple Harmonic Motion (SHM)

Direction of rotation

Page 20: 4.5 Elastic potential energy and Simple Harmonic Motion (SHM)

Direction of rotation

Page 21: 4.5 Elastic potential energy and Simple Harmonic Motion (SHM)

Direction of rotation

Page 22: 4.5 Elastic potential energy and Simple Harmonic Motion (SHM)

Direction of rotation

Page 23: 4.5 Elastic potential energy and Simple Harmonic Motion (SHM)

Conservation of energy still applies

If you analyze the motion of a mass on a spring, the speed gained by the mass and lost by the mass is traceable back to the total amount of elastic potential energy put into the system

A spring with a mass that is stretched or compressed will store energy

Once released, the mass will move As the kinetic energy of the mass increases, the

energy in the spring decreases, and vice versa

Page 24: 4.5 Elastic potential energy and Simple Harmonic Motion (SHM)

Dampened Harmonic Motion

DAMPENED HARMONIC MOTION occurs when the spring system loses energy over time causing the displacement to decrease in the spring

This energy is dissipated to other forms This is desirable in some mechanical

systems like shock absorbers – or else your car would continue to bounce up and down after the shock absorber is depressed