Here's a case where a force of interest is perpendicular to an incline (today's mass-on-incline problem had the force pointing down-- but geometric arguments are very similar).
By the alternate angle theorem from geometry, we have
that the angle
is the same as the angle
. Since angles
and
are complementary to the same angle, they are
equal. So
,
and
are all the same angle.
Now look at the right triangle formed by the vector
and
,
with angle
between them. From this triangle you get that
and
.
We'll be seeing lots of examples like this, so it will be worth
your while to go through the geometry and trig carefully. Please ask
again if it's not clear.
This kind of thing will get much easier with practice.