Ch1. Periodical Motions

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Spring 2016

Ch1. Periodical Motions

1. Useful Notions and Mathematics

2. Simple Harmonic Oscillators (SHOs)

3. Energy Conservation

4. SHOs and Near-Equilibrium Potential Energy

5. The superposition of SHOs

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0 th : Notions and Some Mathematics

Friction less

Friction

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Euler’s Complex Analysis

Complex number definition: x

2 i

2 i

 

1 And also satisfied by -i z

ˆ  x

 iy x & y : real numbers

Euler’s formula: e i

  cos

  i sin

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Leonhard Euler (1707-1783)

Euler’s Formula

Let’s define

Then z

   i

 dz

ˆ

ˆ

Therefore

Integrating

z

 i

"our jewel…one of the most remarkable, almost astounding, formulas in all of mathematics.“ Richard Feynman

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Complex Conjugate

Define z

ˆ  x

 iy z

ˆ  r (cos

  i

The conjugate z

ˆ

*

 x

 iy z

ˆ*  r (cos

  i

  e

 i

Phasor Presentation

Rotating Arrow + Phase Angle

 t

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Representation of a complex number in terms of real and imaginary components

   t

Complex Representation

Phasor form:

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 t

Simple Harmonic Oscillator

use physics/mechanics to write equation of motion for system restoring force

F s

  s x ( t )

Inertial force F i d

2

 m dt

2 x ( t )

 m  x  ( t ) equation of motion m  x  ( t )

 sx ( t )

0 insert generic trial form of solution find parameter values for which trial form is a solution

 t

 x  ( t )

 

2 x ( t )

0

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  s m

Solution: Complex Representation

 x  ( t )

 

0

2 x ( t )

0 

0

 s m

Phasor form:

Real Part:

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Simple Harmonic Oscillators (SHOs)

X=0

X=A; v=0; a=-a max

X=0; v=-v max

; a=0

X=-A; v=0; a=a max

X=0; v=v max

; a=0

X=A; v=0; a=-a max

X=-A X=A

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Linearly Polarized Light as Phasors

E ( t )

E

0 e

 i

 t

 i

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Phase matters!!!

Linearly Polarized Light as Phasors

E ( t )

E

0 e

 i

 t

 i

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Phase matters!!!

Gravitational wave detected. Or not?

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The Laser Interferometer Gravitational-

Wave Observatory ( LIGO )

Other Model Systems Using SHOs

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Energy conservation of SHOs

Mechanical & Electrical Oscillator

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SHOs & Near-Equilibrium-Potential

Simple Pendulum

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SHOs & Near-Equilibrium-Potential

L-J potential for interaction between a pair of neutral atoms or molecules

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Taylor Expansion Series

Arbitrary potentials V(x) can be well approximated by the power series near x

0 by Taylor expansion

Example: a Taylor series of a function f(x)

Near x

0

=0

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Adding Two Vibrations of Same Amplitudes

(I) Equal Frequencies

Two Parallel SHOs

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Additions of Two Parallel SHOs

(I) Equal Frequencies

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Additions of Two SHOs

Equal Frequencies

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[ + ]

22

Adding Vibrations of Equal Frequency

Examples

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Superposition of Many SHOs

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