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: