For capacitors in parallel, total charge stored is the sum of individual charges. Substituting $Q = C V$ and canceling the common $V$ gives:
C_{eq, parallel} = C_1 + C_2 + ... + C_n
For capacitors in series, total potential difference across the combination is the sum of individual potential differences. Substituting $V = Q/C$ and canceling the common $Q$ gives:
Most practical capacitors use an insulating material called a dielectric between their plates. Dielectrics increase capacitance by a dimensionless factor called the dielectric constant $\kappa$, where $\kappa > 1$ for all insulating materials. Dielectrics polarize in the electric field between plates, reducing the net electric field for a given stored charge, which increases capacitance per the definition $C = Q/V$.
When a dielectric fills the entire gap between plates of a parallel-plate capacitor, the capacitance becomes:
C = \kappa \frac{\epsilon_0 A}{d}
Work done to separate charge on a capacitor is stored as electric potential energy. There are three equivalent forms for stored energy:
U = \frac{1}{2} Q V = \frac{1}{2} C V^2 = \frac{Q^2}{2 C}
The energy is stored in the electric field between the plates, with energy density (energy per unit volume):