Simple Harmonic Motion 16 th October 2008. Quick review… (Nearly) everything we’ve done so far...

13
Simple Harmonic Motion 16 th October 2008

Transcript of Simple Harmonic Motion 16 th October 2008. Quick review… (Nearly) everything we’ve done so far...

Page 1: Simple Harmonic Motion 16 th October 2008. Quick review… (Nearly) everything we’ve done so far in this course has been about a single equation a = constant.

Simple Harmonic Motion

16th October 2008

Page 2: Simple Harmonic Motion 16 th October 2008. Quick review… (Nearly) everything we’ve done so far in this course has been about a single equation a = constant.

Quick review…

(Nearly) everything we’ve done so far in this course has been about a single equation

F ma=a = constant

210 2

( )x t v t at= +a = f(t)

( ) ( )d dx t f t t t= ò

a is central

Circular motion…

Page 3: Simple Harmonic Motion 16 th October 2008. Quick review… (Nearly) everything we’ve done so far in this course has been about a single equation a = constant.

What we’re doing now…

Consider new type of force, to extend the types of situations we can deal with

F kx= -

ma kx

ß

= -

Page 4: Simple Harmonic Motion 16 th October 2008. Quick review… (Nearly) everything we’ve done so far in this course has been about a single equation a = constant.

Example… Particle on a spring

ˆspring

kx= -F ir

2

2

d

d

xma m kx

t= = -

Page 5: Simple Harmonic Motion 16 th October 2008. Quick review… (Nearly) everything we’ve done so far in this course has been about a single equation a = constant.

Solutions…

You saw yesterday that one solution to this problem was

( ) cosk

x t A tm

æ ö÷ç ÷ç= ÷ç ÷ç ÷çè ø

However, this is not the only solution… It turns out that the following solution also

works

( ) sink

x t B tm

æ ö÷ç ÷ç= ÷ç ÷ç ÷çè ø

Page 6: Simple Harmonic Motion 16 th October 2008. Quick review… (Nearly) everything we’ve done so far in this course has been about a single equation a = constant.

Most general solution

It turns out that the most general solution is given by (see 18.03…)

( ) cos sink k

x t A t B tm m

æ ö æ ö÷ ÷ç ç÷ ÷ç ç= +÷ ÷ç ç÷ ÷ç ç÷ ÷ç çè ø è ø

km

w=2

Tpw

= Ü

Angular frequency

Period

Page 7: Simple Harmonic Motion 16 th October 2008. Quick review… (Nearly) everything we’ve done so far in this course has been about a single equation a = constant.

What is the period?

Consider the oscillator at t = 0

( ) ( )( ) cos sinx t tt A Bw w= +

( ) ( )(0) cos 0 sin 0x A B= +

(0)x A=

Consider the oscillator at t = T = 2/2 2

( ) cos sinxT A Bp p

w ww w

æ ö æ ö÷ ÷ç ç÷ ÷= +ç ç÷ ÷ç ç÷ ÷ç çè ø è ø

( ) ( )( ) cos 2 sin 2xT A B Ap p= + =

Page 8: Simple Harmonic Motion 16 th October 2008. Quick review… (Nearly) everything we’ve done so far in this course has been about a single equation a = constant.

What does the motion look like?

( ) ( )( ) cos sinx t A t B tw w= +

T

Page 9: Simple Harmonic Motion 16 th October 2008. Quick review… (Nearly) everything we’ve done so far in this course has been about a single equation a = constant.

Velocity and acceleration

We can differentiate our expression to find velocity and acceleration

( ) ( )

( ) ( )

( ) ( )2 2 2

( ) cos sin

( ) sin cos

( ) cos sin ( )

x t A t B t

v t A t B t

a t A t B t x t

w w

w w w w

w w w w w

= +

= - +

= - - = -

Page 10: Simple Harmonic Motion 16 th October 2008. Quick review… (Nearly) everything we’ve done so far in this course has been about a single equation a = constant.

How to find A and B?

Use initial conditions

Since there are two constants, we need two initial conditions

These can be anything, but let’s try an example with initial position x(0) and

initial velocity v(0)

( ) ( )( ) cos sinx t A t B tw w= +

Page 11: Simple Harmonic Motion 16 th October 2008. Quick review… (Nearly) everything we’ve done so far in this course has been about a single equation a = constant.

Initial Position

( ) ( )( ) cos sinx t tt A Bw w= +

If t = 0

( ) ( )( ) ( )

(0) cos sin

(0) cos

0

sin

(0

0 0

)

0x A B

x A B

x A

w w

+

´ +

=

´=

=

So the constant A is simply equal to the original displacement

Page 12: Simple Harmonic Motion 16 th October 2008. Quick review… (Nearly) everything we’ve done so far in this course has been about a single equation a = constant.

Initial velocity

( ) ( )( ) cos sinx t A t B tw w= +

To find the velocity, we need to differentiate

( ) ( )d ( )( ) sin cos

dx t

v A Bt

tt tw ww w= = - +

At t = 0

(0)v Bw=

And so B is equal to (0) /v w

Page 13: Simple Harmonic Motion 16 th October 2008. Quick review… (Nearly) everything we’ve done so far in this course has been about a single equation a = constant.

Summary

We’ve learnt how to deal with forces like

kF kx a x

m= - Þ = -

We found that the solution looks like

( ) ( )( ) cos sin /x t A t B t k mw w w= + =

We can use initial conditions to find A and B

We can use this expression to find out anything we want about the motion