<Dl> <Dd> G t o t a l = G 1 + G 2 + ⋯ + G n (\ displaystyle G_ (\ mathrm (total)) = G_ (1) + G_ (2) + \ cdots + G_ (n)). </Dd> </Dl> <Dd> G t o t a l = G 1 + G 2 + ⋯ + G n (\ displaystyle G_ (\ mathrm (total)) = G_ (1) + G_ (2) + \ cdots + G_ (n)). </Dd> <P> The relations for total conductance and resistance stand in a complementary relationship: the expression for a series connection of resistances is the same as for parallel connection of conductances, and vice versa . </P> <P> Inductors follow the same law, in that the total inductance of non-coupled inductors in parallel is equal to the reciprocal of the sum of the reciprocals of their individual inductances: </P>

Distinguish between a series circuit and a parallel circuit