derive, using C = Q/V, formulae for the combined capacitance of capacitors in series and in parallel
understand that, for a point outside a spherical conductor, the charge on the sphere may be considered to be a point charge at its centre
derive, using C = Q/V, formulae for the combined capacitance of capacitors in series and in parallel
understand that, for a point outside a spherical conductor, the charge on the sphere may be considered to be a point charge at its centre