(
and
might describe a set of axes painted on a
flywheel which is rotating with respect to an inertial observer.)
NOTE: For the questions below, work in
basis,
where the position
is given by
soln
[0.25in] Constant force
![]()
YES V = -ax-by-cz [0.5in] The force
(for some function G)
YES V = -G(r) [0.5in] The force
(r,
are polar coordinates in the xy-plane)
NO work integral around closed circular loop
[0.5in] The force
![]()
NO
[0.2in]
-1.2in
and
appear in the Lagrangian only in the
kinetic energy term for
, which depends only on
. Thus E-L gives
the angular momentum l of
is conserved.
when
, thus
The frequency of radial oscillations is
. The denominator is
because that is the effective mass for radial oscillations; see
the left hand side of the radial equation of motion (c). Thus
so
For
,
so that the periods in
r and
are equal; the orbit closes on itself and repeats
when
.
for
(this includes all physical r when E;SPMlt;0)
for
for
for all r