Lesson 7 of 7
Energy stored in a capacitor
I can use the area under a potential-difference-versus-charge graph and all three equivalent linear-capacitor energy expressions.Syllabus
Syllabus 9478, 14(k). Use the area under a potential-difference-versus-charge graph and all three equivalent linear-capacitor energy expressions.
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A capacitor is charged to charge Q and p.d. V. Why is the energy stored 1/2 QV and not QV?
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Each added charge is pushed against a p.d. that rises from zero to V.
At the start the p.d. is zero, so the first charge needs almost no work. The p.d. rises steadily to V, so the average p.d. is V/2 and the work done is Q x V/2.
Separating charge requires work as the capacitor's potential difference grows. Its stored energy is the area under a potential-difference-against-charge graph.
Add the work of successive charge transfers
For a capacitor with plate-charge magnitude Q and potential difference V, transferring a small additional charge ΔQ requires work approximately VΔQ at that stage. Adding these small strips gives the energy stored in the ideal capacitor, with zero energy for the uncharged state.
The required graph has V vertically and Q horizontally. For a linear capacitor of constant C, V = Q/C is a straight line through the origin with gradient 1/C. The total area is a triangle:
Using V = Q/C: U = Q2/(2C)
Using Q = CV: U = (1/2)CV2
These are three equivalent expressions for the same stored energy under the constant-capacitance model. Choose the form suited to the known or fixed quantities.
For charge of order 100 microcoulomb and voltage of order 10 V, QV/2 is of order 10-3 J. One millijoule, mJ, is 10-3 J.
Worked energy area
Read the axes and convert the charge unit
For C = 10.0 microfarad, the V-against-Q model has points (0,0), (40 microcoulomb,4 V), (80 microcoulomb,8 V) and (120 microcoulomb,12 V).
V against Q makes the charging work an area
The axes are reversed from Q(V): V is now vertical and Q horizontal. For this constant-C capacitor, each small addition of plate charge requires work approximately VΔQ at the current p.d.; summing those contributions gives the complete area.
The base is 120 × 10-6 C, so the area is 720 µJ = 0.720 mJ. The same stored energy is QV/2, Q2/(2C) or CV2/2 under the stated constant-capacitance condition.
= 7.20 × 10-4 J = 0.720 mJ
The unconverted numerical area 720 has unit microcoulomb volt, or microjoule. It is not 720 J. The same result follows from (1/2)(10.0 × 10-6)(12.0)2.
State what stays fixed
For the same capacitor, doubling V doubles Q and quadruples U. The 10.0 microfarad device at 24.0 V therefore has Q = 240 microcoulombs and U = 2.88 mJ.
Comparing different capacitances requires a different decision. At fixed voltage U is proportional to C, whereas at fixed charge U is inversely proportional to C.
| Case | Charge and voltage | U / mJ |
|---|---|---|
| Reference: C = 10.0 microfarad | Q = 120 microcoulomb V = 12.0 V | 0.720 |
| C = 20.0 microfarad, same Q | Q = 120 microcoulomb V = 6.0 V | 0.360 |
| C = 20.0 microfarad, same V | Q = 240 microcoulomb V = 12.0 V | 1.44 |
A disconnected isolated capacitor retains Q only under the ideal no-leakage assumption. A connected ideal source can maintain V by exchanging charge. The fixed-Q and fixed-V rows are separate comparisons; they do not hold both quantities fixed while changing C.
Check your understanding
A 10.0 microfarad capacitor at 12.0 V stores 0.720 mJ and has plate-charge magnitude 120 microcoulomb. Compare a 20.0 microfarad capacitor, first at the same charge and separately at the same voltage.
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Its energy is 0.360 mJ at fixed charge and 1.44 mJ at fixed voltage.
At Q = 120 microcoulomb, U = Q2/(2C) halves. At V = 12.0 V, U = CV2/2 doubles. The two comparisons do not hold both Q and V fixed.
Distinguish source transfer from stored energy
For an initially uncharged linear capacitor charged through resistance from a constant-voltage source to its final voltage, the source transfers charge Q at source voltage Vs. Its energy transfer is VsQ.
For the 12.0 V, 120 microcoulomb final state, the source transfers 1.44 mJ, while the capacitor stores 0.720 mJ. In this stated resistive charging model, the remaining 0.720 mJ is transferred in the resistance. The capacitor's changing voltage explains why its stored-energy area is triangular even though the source voltage stays constant.
This account depends on the initially uncharged capacitor, constant source voltage and stated charging process. Do not identify every source energy transfer with the capacitor's final stored energy.
Practise an exam question
Write your answer first, then tick the mark points it makes.
Exam-style question
A graph of potential difference V against charge Q for a capacitor is a straight line from the origin to (6.0 mC, 12 V). Use the graph to find the capacitance and the energy stored when the p.d. is 12 V. [3]
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