After a long time in this ideal RC model, the capacitor reaches the source voltage and its final charge and stored energy follow from that voltage. The final 24 C and 72 J values are exact for the stated capacitance and source; real circuits have leakage, dielectric absorption, equivalent series resistance, voltage tolerance, and measurement uncertainty.

After a long time, the final capacitor charge and stored energy are exact static quantities. Exact arithmetic here means exact results for the stated model inputs; measured inputs still carry uncertainty and significant-figure limits.

highlighted = computed this step

After a long time the capacitor reaches the source

This exact final-state lesson uses the source voltage 6 volts; it does not claim an intermediate charging voltage.

Vfinal=6 VV_{\text{final}} = 6\ \text{V}
Final capacitor stateThe final state uses the checked source voltage.6 V3 ohm4 F

Final charge comes from C times V

With capacitance 4 farads and voltage 6 volts, the final charge is 24 coulombs.

Qfinal=CV=24 CQ_{\text{final}} = C V = 24\ \text{C}
Final capacitor stateThe final state uses the checked source voltage.6 V3 ohm4 F

Final stored energy is exact

The final stored energy is 72 joules.

Ufinal=12CV2=72 JU_{\text{final}} = \frac{1}{2} C V^{2} = 72\ \text{J}
Final capacitor stateThe final state uses the checked source voltage.6 V3 ohm4 F

Final charge and energy both depend on voltage

With resistance and capacitance fixed, final charge scales directly with voltage while final stored energy follows voltage squared.

RCVτQfUf3 ohm4 F3 V12 s12 C18 J3 ohm4 F6 V12 s24 C72 J3 ohm4 F9 V12 s36 C162 J\begin{array}{c|c|c|c|c|c}R&C&V&\tau&Q_f&U_f\\3\ \text{ohm}&4\ \text{F}&3\ \text{V}&12\ \text{s}&12\ \text{C}&18\ \text{J}\\3\ \text{ohm}&4\ \text{F}&6\ \text{V}&12\ \text{s}&24\ \text{C}&72\ \text{J}\\3\ \text{ohm}&4\ \text{F}&9\ \text{V}&12\ \text{s}&36\ \text{C}&162\ \text{J}\\\end{array}
Final capacitor stateThe middle table row is the checked final state.6 V3 ohm4 F