For counterclockwise uniform circular motion
in the x-y plane we found at page
5
an expression for the position vector
r(t)
and, moreover, at page
6
an expression for the velocity vector
v(t),
respectively given by
|
r(t) =
|
(
|
|
)
|
and
|
v(t) =
|
(
|
|
)
|
The vector product of
r(t)
and
v(t)
is given by
|
r(t) ×
v(t) =
|
(
|
|
0
|
|
0
|
|
ωR2
cos2(ωt)
+ ωR2
sin2(ωt)
|
|
)
|
=
|
(
|
|
)
|
Hence,
r(t) ×
v(t)
is independent of the instant of time t
and moreover proportional to ω:
r(t) ×
v(t)
= R2
ω
= |r(t)|2
ω
|
|