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These main points are discussed in these Lecture Slides : Poisson Brackets, Matrix Form, Single Set, Hamilton’s Equations, Symplectic, Return the Lagrangian, Dynamical Variable, Angular Momentum, Two Dimensional Harmonic, Oscillator
Typology: Slides
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The
dynamic
variables
can
be
assigned
to
a
single
set.
q^1
,^ q
, …, 2
qn
,^ p
, 1 p
, …, 2
pn
z^1
,^ z
, …, 2
z
2 n
Hamilton’s
equations
can
be
written
in
terms
of
z
Symplectic
2
n^
x^
2 n
matrix
Return
the
Lagrangian
^
z
t z H
z^
j j
j j^
q p
d dt
t z H
q p
t z H z J z t z z L
Example •^
The
two
dimensional
harmonic
oscillator
can
be
put
in
normalized
coordinates.
m
=
k
=
1
Find
the
change
in
angular
momentum
l
It’s
conserved
(^21) 1 2
(^22)
(^21)
1 2
q
q
p
p
1 2
2 1
p q
p q l^
q q q q p p p p
dl dt
H q l p
H p l q
dl dt
H z
l z
dl dt
i
i
i
i
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The
time
‐independent
part
of
the
expansion
is
the
Poisson
bracket
of
with
This
can
be
generalized
for
any
two
dynamical
variables.
Hamilton’s
equations
are
the
Poisson
bracket
of
the
coordinates
with
the
Hamitonian.
(^1) S
^
H z
F z
^
B z
A z
i
i
i
i^
A q
B p
B p
A q
z
H z
z z
z^
^
In
addition
to
the
Lie
algebra
properties
there
are
two
other
properties.^ –
Product
rule
Chain
rule
The
Poisson
bracket
acts
like
a
derivative.
^
z z^
B z
A z
t
B t
A
B z J z A B A
Let
z
t )
describe
the
time
development
of
some
system.
This
is
generated
by
a
Hamiltonian
if
and
only
if
every
pair
of
dynamical
variables
satisfies
the
following
relation:
d dt
d dt
^
B^ t
A
B A t
t z
B
J A z
B z
J t z
A
B z
J A z
t
B A t
,
, ,
2
2