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If the Lagrangian of a system, closed or, Study notes of Physics

If the Lagrangian remains invariant under rotation about an axis, then the angular momentum of the system about this axis will remain constant in time.

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Hamiltonian Function: Conservation Laws
Closed System: No interaction with anything outside
the system.
Any closed system has: seven constants or integrals of
motion:
three components of the linear momentum
three components of angular momentum
the total energy
" Conservation of linear momentum:
Property of inertial frame:
o Space is homogeneous in an inertial system
or frame (a closed system is unaffected by a
translation of the system in space).
The Lagrangian of a closed system in an inertial
frame is invariant.
.const
q
L
qmp
k
kk =
==
2
In general:
If the Lagrangian of a system, closed or
otherwise, is invariant with respect to a
translation in a certain direction, then the
linear momentum of the system in that
direction is constant in time.
" Conservation of angular momentum:
Property of inertial frame:
o Space is isotropic in an inertial frame (a
closed system is unaffected by orientation or
rotation of the entire system).
The Lagrangian of a closed system remains
invariant if the system is rotated through an
infinitesimal angle.
rq
pp
constprJ
k
kG
G
G
G
G
=×= .
pf3

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1

Hamiltonian Function: Conservation LawsClosed System: No interaction with anything outside

the system.

Any closed system has:

seven constants

or

integrals of

motion:

-^

three components of the linear momentum

-^

three components of angular momentum

-^

the total energy

Conservation of linear momentum: •^

Property of inertial frame:

o^

Space is homogeneous in an inertial systemor frame

(a closed system is unaffected by a

translation of the system in space).

-^

The Lagrangian of a closed system in an inertialframe is invariant.

const L q

qm

p

k k

k^

=^

In general:

-^

If the Lagrangian of a system, closed orotherwise, is invariant with respect to atranslation in a certain direction, then thelinear momentum of the system in thatdirection is constant in time.

Conservation of angular momentum: •^

Property of inertial frame:

o^

Space is isotropic in an inertial frame

(a

closed system is unaffected by orientation orrotation of the entire system).

-^

The Lagrangian of a closed system remainsinvariant if the system is rotated through aninfinitesimal angle.

r q

p p

const p r J k k

G G

G

G

G

×

=^

3

In general:

•^

If the Lagrangian remains invariant underrotation about an axis, then the angularmomentum of the system about this axis willremain constant in time.

Conservation of Energy: •^

Property of inertial frame:

o^

The time is homogeneous within an inertialreference frame

-^

The Lagrangian of a closed system can not be anexplicit function of time.

o L^ ∂=t∂

=^

k

k k

k

k^

k^

qd dt L q

dqdt L q

Ld td

^

k k^

q qd (^) dt

^

from Lagrange equation:

k

k^

L q

L q d dt

∂^ ∂

(^

^

=^

k

k k

k

k^

k

q L q

q L q d td

Ld td

]

[^

∑k

k Lqqk

d td

Ld td

^ 

∑k^

k k^

L

L q q d dt

the quantity in parentheses must be constant in time.

const L q p

L

L q q

H^

k

k k

k^

k k^

^ 

=^

k qpk

H H

n

Hamiltonia the

called is

H^ =^ •

H^

is a constant of motion if

L

is not an explicit

function of time

-^

If the kinetic energy

T

is a homogeneous

quadratic function of the

q^ and the potentialk

energy

V

is a function of the

q^ alone, we willk

have:

const E V T V T T L T

H^