Generators - Classical Mechanics - Lecture Slides, Slides of Classical Mechanics

These main points are discussed in these Lecture Slides : Generators, Phase Space, Contact Transformation, Hamiltonian, Harmonic Oscillator, Contact Transformation, Associated Momenta, Generator, Harmonic Oscillator, Simple Hamiltonian

Typology: Slides

2012/2013

Uploaded on 07/24/2013

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Generators

Phase

Space

A

contact

transformation

acts

on

a

Hamiltonian.^ –

Transform

on

T

*Q

The

function

does

not

always

give

a

point

transformation.^ –

Would

transform

only

on

Q

d

dt H H

qd p

dq p^

k k j j^

^

Cyclic

Variable

Write

one

system

in

terms

of

the

other.^ –

Find

the

new

Hamiltonian

The

new

generalized

position

is

cyclic.^ –

Simplified

Hamiltonian

-^

Frequency

dependence

is

explicit

q

p

q



1 2 sin      

q

p

p

 

1 2 cos   

  

^

p

H

H

q

p

H

2 2 (^2) 

Harmonic

Motion

The

equations

of

motion

follow

from

the

new

Hamiltonian

-^

Angular

momentum

and

angle

The

equations

of

motion

for

the

original

system

follow.

E 

p^

p

q

J =

2 

E/

 

t^0 t

q^

qd dt

H^ p

sin 2

0

2

t t

E

q^



t

^

cos 2

t^0 t

E

p^

Independent

Variables

Use

is

limited

when

new

coordinates

Q

are

functions

of

q

but

not

p

-^

dQ

k^ not

independent

of

dq

j

Transform

the

generator

to

new

independent

variables.

-^

“type

3”

transformation

j j

k j^

q p

t q q^

^

j j j j

k k j j

dp q

dq p

d

dt H H

qd p

dq p

) ( t q p d dt H H

qd p

dp q

k j

k k j j  

j

j

p

q^

k

k^

q

p^

Four

Generators

(^

t q q^

k j

^ j

j^

q

p^

^

k

k^

q

p^

j j

k j

k j^

q p t q p t q

q^

^

k

k^

q

p^

j

j

p

q^

j

j

p

q^

k

k

p

q^

j j j j k j k

j^

q p q p t p p t q

q^

^

  j j k j k

j^

q p t p q t q

q^

^

j

j^

q

p^

k

k

p

q^

Type 1 Type 2

Type 3 Type 4

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