AP Syllabus focus: 'When a charged capacitor discharges, charge, stored energy, potential difference, and branch current decrease until a steady state is reached.'
A discharging capacitor releases stored electric energy back into a circuit. As the discharge proceeds, the capacitor’s charge, potential difference, stored energy, and branch current all decrease toward zero.
What discharge means
A charged capacitor stores separated positive and negative charge on its plates. That separation creates an electric field and stores electric potential energy. If a conducting path is provided between the plates, charge can move through the external circuit, so the capacitor begins to discharge.
During discharge, the capacitor is no longer building up charge separation. Instead, the existing separation is reduced. This means the amount of charge on the plates gets smaller with time. As the charge separation weakens, the electric field between the plates also weakens, so the capacitor becomes less able to push charge through the circuit branch.
A capacitor does not release all of its stored energy in one instant in a typical circuit. The discharge is a process: the electrical quantities change continuously until the circuit reaches a final condition in which no further change occurs.
Quantities that decrease
The AP focus for this subsubtopic is the linked decrease of four quantities:
Charge on the capacitor
Stored electric potential energy
Potential difference across the capacitor
Branch current
As discharge continues, each of these becomes smaller. The branch current exists because the capacitor’s potential difference drives charge through the branch. When the potential difference becomes smaller, the current also becomes smaller. Eventually, the discharge ends.
Steady state: The condition in which circuit quantities no longer change with time; for an ideal fully discharged capacitor, the capacitor’s potential difference and the branch current are zero.
At steady state, an ideal discharging capacitor has no remaining charge separation to drive current through the branch. The current therefore falls to zero, and the capacitor no longer transfers energy to the rest of the circuit.
Why the decreases are linked
These decreases are not independent. For a given capacitor, the capacitance stays constant, so a smaller amount of stored charge means a smaller potential difference across the capacitor. That smaller potential difference means a weaker push on charges in the branch, so the current decreases as well.
The stored energy also decreases because the capacitor’s energy depends on how much charge separation and potential difference remain. As the capacitor loses charge, the electric field between its plates weakens, and the stored energy drops.
= charge on the capacitor, in coulombs
= capacitance, in farads
= potential difference across the capacitor, in volts
= electric potential energy stored in the capacitor, in joules
= capacitance, in farads
= potential difference across the capacitor, in volts
These relationships help explain the discharge qualitatively. If is fixed, then decreasing requires decreasing . Because the stored energy depends on , the energy falls as the capacitor discharges and reaches zero in the ideal fully discharged state.
Physical picture during discharge
At the instant discharge begins, the capacitor has its greatest charge, greatest potential difference, and greatest stored energy for that situation. Because the driving potential difference is initially largest, the branch current is also initially largest.

Textbook RC-discharge graphs showing , , and all decreasing in magnitude as the capacitor discharges through a resistor. The curves illustrate that the branch current starts at its maximum magnitude and then decays as the capacitor’s potential difference falls, approaching the steady-state condition of zero current. Source
As charge flows through the branch, the capacitor loses some of the charge separation that created its electric field. With a weaker electric field, the capacitor produces a smaller potential difference. Since the driving potential difference is smaller, the branch current decreases. This is why the current is not constant during discharge.
The discharge therefore slows down as it proceeds. Early in the process, the changes are larger because the capacitor still has a substantial potential difference. Later in the process, the remaining charge separation is small, so the current becomes very small as well.
Branch current and energy transfer
The branch current during discharge is the current in the part of the circuit through which the capacitor is releasing energy. That current is evidence that energy is being transferred from the capacitor to other circuit elements or to the surroundings.
As the current decreases, the rate of energy transfer also decreases. In many practical cases, the energy released by the capacitor is converted into thermal energy in the circuit. The key AP idea is not the detailed mechanism, but the overall trend: the capacitor’s stored energy steadily decreases until the discharge is complete.
A useful way to think about the process is that the capacitor gradually runs out of the electrical “push” that originally drove the current. When that push is gone, the current stops.
Qualitative graphs and endpoint
If you sketch the discharge qualitatively against time, the graphs of charge, potential difference, stored energy, and branch current all slope downward toward zero.

Charge/discharge curves for an RC circuit: during discharge, the capacitor’s voltage drops exponentially while the current magnitude also decays, approaching zero as time increases. The plot emphasizes the “fast at first, then slower” shape that matches how the electric “push” weakens as the capacitor discharges. Source
They are not flat lines during the discharge because the values are changing continuously.
Useful graph features to remember:
Charge vs. time: decreases toward zero
Potential difference vs. time: decreases toward zero
Branch current vs. time: decreases toward zero
Stored energy vs. time: decreases toward zero
All four graphs approach the final steady state. In an ideal circuit, that final state corresponds to a fully discharged capacitor.
Common misconceptions
A discharging capacitor does not keep the current constant. The current decreases as the capacitor’s potential difference decreases.
Zero current at the end of discharge does not mean charges in the wire have stopped existing. It means there is no longer a net current driven by the capacitor.
The capacitor’s stored energy does not remain in the capacitor once discharge is complete. In the ideal fully discharged state, the stored energy is zero.
A larger current at the start of discharge does not mean the capacitor is gaining charge. It means the capacitor is losing charge more rapidly at the beginning.
FAQ
In an ideal one-direction discharge path, the capacitor releases its stored energy and the current falls to zero before any reversal occurs.
Polarity reversal needs an additional effect, such as:
an inductor in the circuit
an alternating source
more complex circuit behavior
In a simple discharge branch, the capacitor just approaches zero potential difference.
Real capacitors are not perfectly ideal. Some show dielectric absorption, where charge redistribution inside the dielectric causes a small voltage to reappear after discharge.
This recovered voltage is usually much smaller than the original voltage, but it matters in precision circuits and safety procedures.
That is why technicians may discharge a capacitor more than once before handling it.
Not in a normal physical circuit. Instant discharge would require an extremely large current, and real wires and components limit current.
In practice, discharge can be very fast, but not truly instantaneous. The speed depends on the circuit path available for charge to move.
Even when discharge seems immediate to the eye, it still takes a finite amount of time.
The initial direction is set by the capacitor’s polarity at the moment discharge begins. The electric field between the plates drives charge through the external path in the direction that reduces the charge separation.
So the current direction is the direction that lowers the capacitor’s stored energy and moves the system toward equilibrium.
If the capacitor were charged with the opposite polarity, the initial current direction would also reverse.
A capacitor can release energy in a very short time, producing a large current briefly. That short burst can:
damage components
create sparks
heat wires
pose a shock risk
The danger depends on both voltage and stored energy, not just on charge alone.
Large capacitors in power supplies, camera flashes, and lab equipment deserve special care even after the source is removed.
Practice Questions
A charged capacitor is allowed to discharge through a circuit branch. State what happens to: (a) the potential difference across the capacitor (b) the branch current as time passes. [2 marks]
(a) Potential difference decreases toward zero. [1]
(b) Branch current decreases toward zero. [1]
A student charges a capacitor and then disconnects the battery so the capacitor discharges through a branch in a circuit. Explain how the discharge proceeds from the instant the branch is completed until steady state is reached. Your answer should refer to charge, potential difference, stored energy, and branch current. [5 marks]
The charge on the capacitor decreases. [1]
The potential difference across the capacitor decreases. [1]
The stored electric potential energy of the capacitor decreases. [1]
The branch current flows during discharge but decreases with time. [1]
At steady state, the ideal capacitor has no remaining driving potential difference, so the branch current is zero. [1]
