oscillatory motion 1

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Oscillatory Motion  A very special kind of motion occurs when the force acting on a body is proportio nal to the displacement of the body from some equilibrium posi tio n. If  this force is always directed toward the equilibrium position, repetitive back- and-forth motion occurs about this position. Such motion is called periodic  moti on, ha rmoni c moti on, osci ll a ti on  , or vibration  (the four terms are comp letel y equiv alen t). Could you please mention an example of this kind of motion?

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Page 1: Oscillatory Motion 1

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Oscillatory Motion A very special kind of motion occurs when the force acting on a body is

proportional to the displacement of the body from some equilibrium position. If 

this force is always directed toward the equilibrium position, repetitive back-

and-forth motion occurs about this position. Such motion is called periodic

m o t io n , h ar m o n ic m o t io n , o s c il lat io n  , or  v i b r a t i o n   (the four terms are

completely equivalent).

Could you please mention an example of this kind of motion?

1) The oscillations of a block attached to a spring

2) The swinging of a child on a playground swing3) The motion of a pendulum

4) The vibration of a stringed musical instrument

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kx F  s

We will consider a physical system that

consists of a block of mass m attached

to the end of a spring, with the block freeto move on a horizontal, frictionless

surface. When the spring is neither 

stretched nor compressed, the block is

at the position x= 0 , called the

equilibrium position of the system. Such

a system oscillates back and forth if 

disturbed from its equilibrium position.

when the block is displaced a smalldistance x from equilibrium, the spring 

exerts on the block a force that is

proportional to the displacement and

given by Hooke’s law:where Fs is called r es t o r i n g f o r c e  

because it is always directed toward the

equilibrium position and thereforeopposite the displacement.

(Eq. 1.1)

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 xm

k a x

 Applying Newton’s second law to the motion of the block, together with Equation

1.1, we obtain

(Eq. 1.2)

The acceleration is proportional to the displacement of the block, and its

direction is opposite the direction of the displacement. Systems that behave in

this way are said to exhibit simple harmonic motion.

 xm

dt 

 xd a

2

2 Second order differentialequation for the motion of 

the block

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   t  At  x cos

In general, a particle moving along the x axis exhibits simple harmonic 

motion when x, the particle’s displacement from equilibrium, varies in timeaccording to the relationship

Equation of Motion

where A,  and  are constants.

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Some Terminology

   t  At  x cos

 Amplitude

 Angular 

frequency

Phase

constant

Phase

    }       

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Properties of Periodic Functions

The function isperiodic with T.

 

 Angular Frequency

(rad/s)

 

 21

 f  T 

Period

(s)

 

 

2 f  

Frequency

(1/s=Hz)

T t  xt  x

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Properties of Periodic Functions

The amplitude A of the motion is the maximum displacement of the particle in

either the positive or negative x direction.

The constant  is called the angular frequency of the motion and has units of 

radians per second.

The constant angle , called the phase constant (or phase angle), is determined

by the initial displacement and velocity of the particle.

The period T of the motion is the time it takes for the particle to go through one

full cycle.

The inverse of the period is called the frequency f of the motion. The frequency 

represents the number of oscillations that the particle makes per unit time.

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Simple Harmonic Motion

   t  At  x cos

    t  Adt 

dxt v sin

t  xt  Adt 

dvt a 22

cos     

 A x max

  Av max

2

max  Aa

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Properties of Simple HarmonicMotion

Displacement, velocity and

acceleration are sinusoidal

with the same frequency.

The frequency and periodof motion are independent

of the amplitude.

Velocity is 90° out-of-phase

with displacement.

 Acceleration is proportional

to displacement but in the

opposite direction.

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The Block-Spring System

   t  At  x cos

Frequency is only dependent on the

mass of the object and the force

constant of the spring

EXPLAIN WHY …??

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 An object oscillates with simple harmonic motion along the x axis. Its displacement

from the origin varies with time according to the equation

where t is in seconds and the angles in the parentheses are in radians.

(a) Determine the amplitude, frequency, and period of the motion.

(b) Calculate the velocity and acceleration of the object at any time t.

(c) Using the results of part (b), determine the position, velocity, and acceleration of 

the object at t=1.00 s.

(d) Determine the maximum speed and maximum acceleration of the object.(e) Find the displacement of the object between t = 0 s and t =1.00 s.

Example. An Oscillating Object

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Example 2. A car with a mass of 1 300 kg is constructed so that its frame is supported by

four springs. Each spring has a force constant of 20 000 N/m. If two people

riding in the car have a combined mass of 160 kg, find the frequency of vibration

of the car after it is driven over a pothole in the road and also how long does it

take the car to execute two complete vibrations?

HOMEWORK

 A block with a mass of 200 g is connected to a light spring for which the force

constant is 5.00 N/m and is free to oscillate on a horizontal, frictionless surface.The block is displaced 5.00 cm from equilibrium and released from rest (a) Find

the period of its motion; (b) Determine the maximum speed of the block; (c)

What is the maximum acceleration of the block?; (d) Express the displacement,

speed, and acceleration as functions of time.