r. field 11/7/2013 university of florida phy 2053page 1 simple harmonic motion: shm energy...

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R. Field 11/7/2013 Univer PHY 2053 Page 1 Simple Harmonic Motion: SHM ) ( ) ( t x m k t a x Energy Conservation: Linear Restoring Force: kx ma F x x At x max = A v x = 0 hence 2 2 1 2 2 1 kx mv U KE E x Spring Constant k 2 2 1 2 2 1 2 2 1 kx mv kA E x constant (independent of time) A m k x m k a max max 2 2 2 ) ( ) ( A t x t v k m x (true at any time t) Amplitude A The maximum speed v max occurs when x = 0. ) cos( ) ( ) sin( ) ( ) cos( ) ( 2 t A t a t A t v t A t x x x m k spring General Solution! A m k v max The phase angle determines where the mass m is at t = 0, x(t=0) = Acos. If x(t=0) = A then = 0. Ideal Spring

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Page 1: R. Field 11/7/2013 University of Florida PHY 2053Page 1 Simple Harmonic Motion: SHM Energy Conservation: Linear Restoring Force: At x max = A v x = 0 hence

R. Field 11/7/2013 University of Florida

PHY 2053 Page 1

Simple Harmonic Motion: SHM

)()( txm

ktax

• Energy Conservation:

• Linear Restoring Force:

kxmaF xx

At xmax = A vx = 0 hence

2212

21 kxmvUKEE x

Spring Constant k

2212

212

21 kxmvkAE x

constant (independent of time)

Am

kx

m

ka maxmax

222 )()( Atxtvk

mx

(true at any time t)

Amplitude A

The maximum speed vmax occurs when x = 0.

)cos()(

)sin()(

)cos()(

2

tAta

tAtv

tAtx

x

x

m

kspring

General Solution!

Am

kv max

The phase angle determines where the mass m is at t = 0, x(t=0) = Acos. If x(t=0) = A then = 0.

Ideal Spring

Page 2: R. Field 11/7/2013 University of Florida PHY 2053Page 1 Simple Harmonic Motion: SHM Energy Conservation: Linear Restoring Force: At x max = A v x = 0 hence

R. Field 11/7/2013 University of Florida

PHY 2053 Page 2

Uniform Circular Motion & SHM

x-axis x(t)

(t)

A • Uniform Circular Motion:

Time t

x(t)

tt )(

Tf

1

)cos()](cos[)( tAtAtx

Project uniform circular motion (constant angular velocity ) of a vector with length A onto the x-axis and you get SHM!

2

T f 2

)cos()(

)sin()(

)cos()(

2 tAta

tAtv

tAtx

x

x

If x(t=0) = A then

The period T is the time is takes for one circular revolution:

• Simple Harmonic Motion (SHM):

)()()( 2 txm

ktxtaspring

x m

kspring

Aa

Av

Ax

2max

max

max

Amplitude

T = period (in s) f = frequency (in Hz) = angular frequency (in rad/sec)

Page 3: R. Field 11/7/2013 University of Florida PHY 2053Page 1 Simple Harmonic Motion: SHM Energy Conservation: Linear Restoring Force: At x max = A v x = 0 hence

R. Field 11/7/2013 University of Florida

PHY 2053 Page 3

SHM: Graphical Representation

)cos()(

)sin()(

)cos()(

max

max

tata

tvtv

tAtx

x

x

If x(t=0) = A then

m

kspring

Aa

Av

Ax

2max

max

max

Tf

1

2

T f 2

Page 4: R. Field 11/7/2013 University of Florida PHY 2053Page 1 Simple Harmonic Motion: SHM Energy Conservation: Linear Restoring Force: At x max = A v x = 0 hence

R. Field 11/7/2013 University of Florida

PHY 2053 Page 4

SHM: General Solution

)cos()(

)sin()(

)cos()(

max

max

tata

tvtv

tAtx

x

x

If the acceleration ax(t) and the position x(t) are related as follows:

C

CAa

ACv

Ax

max

max

max

Tf

1

CT

2 f 2

)()( tCxtax where C is some constant then

)sin()(

)cos()(

)sin()(

max

max

tata

tvtv

tAtx

x

x

BABABA sinsincoscos)cos(

)cos()(

)sin()(

)cos()(

max

max

tata

tvtv

tAtx

x

x

m

kCspring

If x(t=0) = A then = 0: If x(t=0) = 0 and vx(t=0) > 0 then = /2:

Page 5: R. Field 11/7/2013 University of Florida PHY 2053Page 1 Simple Harmonic Motion: SHM Energy Conservation: Linear Restoring Force: At x max = A v x = 0 hence

R. Field 11/7/2013 University of Florida

PHY 2053 Page 5

SHM: General Solution

)cos()(

)sin()(

)cos()(

max

max

tt

tt

tAt

If the angular acceleration (t) and the angular position (t) are related as follows:

C

CA

AC

A

max

max

max

Tf

1

CT

2 f 2

)()( tCt where C is some constant then

• Angular Oscillations SHM:

Page 6: R. Field 11/7/2013 University of Florida PHY 2053Page 1 Simple Harmonic Motion: SHM Energy Conservation: Linear Restoring Force: At x max = A v x = 0 hence

R. Field 11/7/2013 University of Florida

PHY 2053 Page 6

The Pendulum: Small Oscillations SHM

(t)

mg

L

m

axis • Simple Pendulum:Small pendulum bob with mass m on string of lengh L and negligible mass. Calculate the torque about the axis of rotation as follows:

2mLI sinmgLI

)()( tCt SHM with period T given by

g

L

CT

22

)()( tCt

• Physical Pendulum:

(simple pendulum)

Moment of inertia, I, Length L, mass m, distance from axis of rotation to the center-of-mass, dcm. Calculate the torque about the axis of rotation as follows:

I

mgdC cm 2

sinmgdI cm )(sin)(1

tI

mgd

I

mgdt cmcm

SHM with period T given bycmmgd

I

CT

22

(physical pendulum)

L

gC

)(sin)(12

tL

g

mL

mgLt

Page 7: R. Field 11/7/2013 University of Florida PHY 2053Page 1 Simple Harmonic Motion: SHM Energy Conservation: Linear Restoring Force: At x max = A v x = 0 hence

R. Field 11/7/2013 University of Florida

PHY 2053 Page 7

SHM: Example Problems• A simple harmonic oscillator consists of a block of mass 2 kg attached

to a spring of spring constant 200 N/m. If the speed of the block is 40 m/s when the displacement from equilibrium is 3 m, what is the amplitude of the oscillations? Answer: 5m

• A simple pendulum has a length L. If its period is T when it is on the surface of the Earth (gravitational acceleration g ), what is its period when it is on the surface of a planet with gravitational acceleration equal to g/4? Answer: 2T

2212

212

21 kxmvkAE x )()( 222 txtv

k

mA x

mmsmmN

kgtxtv

k

mA x 5)3()/40(

)/200(

)2()()( 2222

g

LT 2 T

g

L

g

LTnew 222

)4/(2

Page 8: R. Field 11/7/2013 University of Florida PHY 2053Page 1 Simple Harmonic Motion: SHM Energy Conservation: Linear Restoring Force: At x max = A v x = 0 hence

R. Field 11/7/2013 University of Florida

PHY 2053 Page 8

SHM: Example Problems• Two blocks (m = 5 kg and M = 15 kg) and a

spring (k = 196 N/m) are arranged on a horizontal frictionless surface. If the smaller block begins to slip when the amplitude of the simple harmonic motion is greater than 0.5 m, what is the coefficient of static friction between the two blocks? Answer: 0.5

mgmaf sxs ga smaxA

mM

kAa spring )(

2max

5.0)5.0()/8.9)(20(

/196

)(

m

smkg

mNA

gmM

ks