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Chapter 14 – Vibrations and Waves

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1 Chapter 14 – Vibrations and Waves Every swing follows the same path This action is an example of vibrational motion vibrational motion - mechanical oscillations around an equilibrium point 14.1 Periodic Motion
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1

Chapter 14 – Vibrations and Waves

Every swing follows the same path

This action is an example of vibrational motion

vibrational motion - mechanical oscillations around an

equilibrium point

14.1 Periodic Motion

2

Each trip back and forth takes the same amount of time

This motion, which repeats in a regular cycle, is an example

of periodic motion

14.1 Periodic Motion

The simplest form of

periodic motion can be

represented by a mass

oscillating on the end of a

coil spring.

- mounted horizontally

- ignore mass of spring

- no friction

14.1 Periodic Motion

3

- Any spring has a natural

length at which it exerts no

force on the mass, m. This

is the equilibrium position

- Moving the mass

compresses or stretches the

spring, and the spring then

exerts a force on the mass in

the direction of the equilibrium

position

- This is the restoring force

14.1 Periodic Motion

- At the equilibrium

position x = 0 and F = 0

- The further the mass is

moved (in either direction)

from the equilibrium

position, the greater the

restoring force, F

- The restoring force is

directly proportional to the

displacement from the

equilibrium position

14.1 Periodic Motion

4

Hooke’s Law (restoring force of an ideal spring)

F = -kx

- The minus sign indicates the restoring force is always

opposite the direction of the displacement

- k is the “spring constant” (units of N/m)

- a stiffer spring has a larger value of k (more force is

required to stretch it)

- Note, the force changes as x changes, so the

acceleration of the mass is not constant

14.1 Periodic Motion

14.1 Periodic Motion

A spring stretches by 18 cm

when a bag of potatoes with a

mass of 5.71 kg is suspended

from its end.

a) Determine the spring

constant.

5

14.1 Periodic Motion

A 57.1 kg cyclist sits on a

bicycle seat and compresses

the two springs that support it.

The spring constant equals

2.2 x 104 N/m for each spring.

How much is each spring

compressed? (Assume each

spring bears half the weight of

the cyclist)

14.1 Periodic Motion

- The spring has the potential to do work on the ball

- The work however, is NOT W = Fx, because F varies with

displacement

- We can use the average force:

F = 1__

2(0 + kx) =

__

2

1kx

W = Fx = __

2

1kx(x) =

__

2

1kx2

6

14.1 Periodic Motion

Potential Energy in a Spring

The potential energy in a spring is equal to one-half

times the product of the spring constant and the

square of the displacement

__

2

1kx2PEsp =

14.1 Periodic Motion

A 0.5 kg block is used to compress a spring with

a spring constant of 80.0 N/m a distance of 2.0

cm (.02 m). After the spring is released, what is

the final speed of the block?

2.0 cm

7

- First, the object is stretched

from the equilibrium position a

distance x = A

- The spring exerts a force to

pull towards equilibrium

position

- Because the mass has been accelerated, it passes by the

equilibrium position with considerable speed

- At the equilibrium position, F = 0, but the speed is a

maximum

14.1 Periodic Motion

- As its momentum carries it to

the left, the restoring force now

acts to slow (decelerate) the

mass, until is stops at x = -A

- The mass then begins to

move in the opposite

direction, until it reaches x = A

The cycle then repeats

(periodic motion)

14.1 Periodic Motion

8

Terms for discussing periodic motion

Displacement – the distance of the mass from the

equilibrium point at any moment

Amplitude – the greatest distance from the equilibrium point

14.1 Periodic Motion

Cycle – a complete to-and-fro

motion (i.e. – from A to –A and back

to A)

Period (T) – the time required to

complete one cycle

Frequency (f) – the number of

cycles per second (measured in

Hertz, Hz)

14.1 Periodic Motion

9

Frequency and Period are inversely related

If the frequency is 5 cycles per second (f = 5 Hz), what is

the period (seconds per cycle)?

1__

5s

f =1__

Tand T =

1__

f

14.1 Periodic Motion

Any vibrating system for which the

restoring force is directly proportional

to the negative of the displacement is

said to exhibit simple harmonic

motion.

14.1 Periodic Motion

10

14.1 Periodic Motion

Period of a Mass-Spring System

Tm

k= 2π

14.1 Periodic Motion

A 1.0 kg mass attached to one end of a spring

completes one oscillation every 2.0 s. Find the spring

constant

What size mass will make the spring vibrate once

every 1.0 s?

11

14.1 Periodic Motion

Simple harmonic motion can also be demonstrated with a simple pendulum

The net force on the pendulum is a restoring force

x = max

v = min

a = max

x = min

v= max

a = min

14.1 Periodic Motion

12

14.1 Periodic Motion

14.1 Periodic Motion

13

14.1 Periodic Motion

14.1 Periodic Motion

14

14.1 Periodic Motion

Period of a Pendulum

The period of a pendulum is equal to two pi times the

square root of the length of the pendulum divided by

the acceleration due to gravity

Tl

g= 2π

14.1 Periodic Motion

What is the period of a 99.4 cm long pendulum?

What is the period of a 3.98 m long pendulum?

15

14.1 Periodic Motion

A desktop pendulum swings

back and forth once every

second.

How tall is this pendulum?

14.1 Periodic Motion

Resonance

The condition in which a time dependent force can

transmit large amounts of energy to an oscillating

object leading to a larger amplitude motion.

Resonance occurs when the frequency of the force

matches a natural frequency at which the object will

oscillate.


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