Examples are:
Theorem: Physical equations must be homogenous in all units.
general differential equation for
, This means that if
is the same,
the solutions are the same.
for gravity.
Buckingham PI theorem.
Transform equation to
for
unitless (homogenous degree 0). If
contain
r independent dimensions let
. Set
. Take the derivative with respect
to
, then set
. You will get r equations with n unknowns. This means
there is an
which is dimensionless.
General case:
where
for u s.t. the
are dimensionless.
Examples: