A brief note on Combining Capacitors and Stored Energy . Read it before a test. Try each question at the end before you open its answer.
Series and parallel Parallel: the same V V V . The charges add, Q = Q 1 + Q 2 + … Q = Q_1 + Q_2 + \dots Q = Q 1 + Q 2 + … , and C = C 1 + C 2 + … C = C_1 + C_2 + \dots C = C 1 + C 2 + … Series: the same Q Q Q . The voltages add, and 1 C = 1 C 1 + 1 C 2 + … \dfrac{1}{C} = \dfrac{1}{C_1} + \dfrac{1}{C_2} + \dots C 1 = C 1 1 + C 2 1 + … Two in series: C = C 1 C 2 C 1 + C 2 C = \dfrac{C_1C_2}{C_1 + C_2} C = C 1 + C 2 C 1 C 2 and V 1 = V C 2 C 1 + C 2 V_1 = V\,\dfrac{C_2}{C_1 + C_2} V 1 = V C 1 + C 2 C 2 . The smaller capacitor has the larger voltage. Identical capacitors: n n n in series give C n \dfrac{C}{n} n C . n n n in parallel give n C nC n C . A network: replace plain series or parallel groups one at a time, then work back for the charge and voltage of each part. A rating: in a series chain, find the charge at which each capacitor reaches its limit. The smallest sets the limit. Energy Stored: U = 1 2 Q V = 1 2 C V 2 = Q 2 2 C U = \tfrac{1}{2}QV = \tfrac{1}{2}CV^2 = \dfrac{Q^2}{2C} U = 2 1 Q V = 2 1 C V 2 = 2 C Q 2 . A battery: it does work Q V QV Q V . Half is stored, and half is lost as heat in the resistance, whatever its value. In parallel: U ∝ C U \propto C U ∝ C . In series: U ∝ 1 C U \propto \dfrac{1}{C} U ∝ C 1 . Density of a field: u = 1 2 ε 0 E 2 u = \tfrac{1}{2}\varepsilon_0E^2 u = 2 1 ε 0 E 2 . Force between the plates: F = Q 2 2 ε 0 A = 1 2 Q E F = \dfrac{Q^2}{2\varepsilon_0A} = \tfrac{1}{2}QE F = 2 ε 0 A Q 2 = 2 1 QE . Joining and changing Common voltage: V ′ = C 1 V 1 + C 2 V 2 C 1 + C 2 V' = \dfrac{C_1V_1 + C_2V_2}{C_1 + C_2} V ′ = C 1 + C 2 C 1 V 1 + C 2 V 2 . Use a minus sign for a capacitor joined the wrong way round. Energy lost: C 1 C 2 2 ( C 1 + C 2 ) ( V 1 − V 2 ) 2 \dfrac{C_1C_2}{2(C_1 + C_2)}(V_1 - V_2)^2 2 ( C 1 + C 2 ) C 1 C 2 ( V 1 − V 2 ) 2 . It is zero only when V 1 = V 2 V_1 = V_2 V 1 = V 2 . If C → n C C \to nC C → n C : with the battery on, Q → n Q Q \to nQ Q → n Q and U → n U U \to nU U → n U . With the battery off, V → V n V \to \dfrac{V}{n} V → n V and U → U n U \to \dfrac{U}{n} U → n U . A worked example A 7.0 μ F 7.0\ \mu\text{F} 7.0 μ F capacitor is charged to 50 V 50\ \text{V} 50 V and joined to an uncharged 3.0 μ F 3.0\ \mu\text{F} 3.0 μ F capacitor. Find the common voltage and the fraction of the energy that is left.
The voltage. V ′ = 7.0 μ F × 50 V 7.0 μ F + 3.0 μ F = 35 V V' = \dfrac{7.0\ \mu\text{F} \times 50\ \text{V}}{7.0\ \mu\text{F} + 3.0\ \mu\text{F}} = 35\ \text{V} V ′ = 7.0 μ F + 3.0 μ F 7.0 μ F × 50 V = 35 V . The energy. The fraction left is C 1 C 1 + C 2 = 7.0 10 = 0.70 \dfrac{C_1}{C_1 + C_2} = \dfrac{7.0}{10} = 0.70 C 1 + C 2 C 1 = 10 7.0 = 0.70 . Practice with new numbers
A program to try The program finds the energy in a capacitor in three ways.
Run it. Compare the three lines.
1. Change V = 90.0 to V = 45.0. By what factor does the energy change?
Mistakes to avoid Mixing up the rules. Parallel capacitors share the voltage. Series capacitors share the charge. Writing U = Q V U = QV U = Q V . The energy stored is 1 2 Q V \tfrac{1}{2}QV 2 1 Q V . Averaging the voltages when capacitors are joined. Use the total charge over the total capacitance. Saying that energy is conserved on joining. It is lost unless the voltages are equal. Check yourself Capacitors of 1.5 μ F 1.5\ \mu\text{F} 1.5 μ F and 4.5 μ F 4.5\ \mu\text{F} 4.5 μ F are in series. What is the equivalent capacitance? Stuck? Show a hint Show the answerA 10 μ F 10\ \mu\text{F} 10 μ F capacitor stores 20 mJ 20\ \text{mJ} 20 mJ . What is its voltage? Stuck? Show a hint Show the answerTwo identical capacitors with equal and opposite charges are joined, plate to plate. How much energy remains? Stuck? Show a hint Show the answerA battery charges a capacitor and does 0.80 J 0.80\ \text{J} 0.80 J of work. How much heat is made? Stuck? Show a hint Show the answer