Solve an RC initial-value problem with energy return
The common zero-charge formula is only one initial-value problem. Take a maintained 6 V source, resistance 2000 Ω and capacitance 500 µF, so RC=1 s. Initial voltage Vi can be below, equal to or above 6 V, including a negative polarity. Positive current enters the capacitor positive plate.
Learning outcome: Compare Vi=−2,6,10 V at the same time. Before revealing values, predict current sign, source-work sign and whether field energy rises or falls. Retain the full finite-time energy ledger rather than labeling every source as always delivering energy.
Starting recap
Review charge continuity, definite integrals, first-order differential equations, initial conditions and signed source work. Distinguish displayed time from physical time.
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With Vi=10 V at t=1 s, V=6+4/e≈7.471518 V and current is −2/e mA≈−0.735759 mA. Source work is about −0.00758545 J: energy has returned to the source. Resistor conversion remains positive, about 0.00345866 J, and the capacitor loses the sum of those two outgoing amounts.
Open the experimentPredict
For Vi=10 V at t=1 s, what is the signed current?
Experiment
Compare Vi=−2,6,10 V at the same time. Before revealing values, predict current sign, source-work sign and whether field energy rises or falls. Retain the full finite-time energy ledger rather than labeling every source as always delivering energy.
Solve RC relaxation from an arbitrary initial voltage
Worked teaching model · synthetic values · Ideal maintained 6 V source, 2000 ohm resistor and 500 microfarad capacitor, time constant 1 s. Signed current enters the capacitor positive plate. Initial voltage is prescribed, including opposite polarity or above-source states. No breakdown, parasitic, switching impulse or physical apparatus model.
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General initial-state relaxation
Unlike graph quantities rescale independently; read units and values, not screen angles. 1: analytic RC solution (solid). Joined curves show the supplied model, not additional observations.
Equivalent numerical coordinates for General initial-state relaxation
analytic RC solution
| time (s) | capacitor voltage (V) |
|---|---|
| 0 | 10 |
| 0.05 | 9.804918 |
| 0.1 | 9.61935 |
| 0.15 | 9.442832 |
| 0.2 | 9.274923 |
| 0.25 | 9.115203 |
| 0.3 | 8.963273 |
| 0.35 | 8.818752 |
| 0.4 | 8.68128 |
| 0.45 | 8.550513 |
| 0.5 | 8.426123 |
| 0.55 | 8.307799 |
| 0.6 | 8.195247 |
| 0.65 | 8.088183 |
| 0.7 | 7.986341 |
| 0.75 | 7.889466 |
| 0.8 | 7.797316 |
| 0.85 | 7.70966 |
| 0.9 | 7.626279 |
| 0.95 | 7.546964 |
| 1 | 7.471518 |
| 1.05 | 7.399751 |
| 1.1 | 7.331484 |
| 1.15 | 7.266547 |
| 1.2 | 7.204777 |
| 1.25 | 7.146019 |
| 1.3 | 7.090127 |
| 1.35 | 7.036961 |
| 1.4 | 6.986388 |
| 1.45 | 6.938281 |
| 1.5 | 6.892521 |
| 1.55 | 6.848992 |
| 1.6 | 6.807586 |
| 1.65 | 6.7682 |
| 1.7 | 6.730734 |
| 1.75 | 6.695096 |
| 1.8 | 6.661196 |
| 1.85 | 6.628949 |
| 1.9 | 6.598274 |
| 1.95 | 6.569096 |
| 2 | 6.541341 |
| 2.05 | 6.51494 |
| 2.1 | 6.489826 |
| 2.15 | 6.465937 |
| 2.2 | 6.443213 |
| 2.25 | 6.421597 |
| 2.3 | 6.401035 |
| 2.35 | 6.381477 |
| 2.4 | 6.362872 |
| 2.45 | 6.345174 |
| 2.5 | 6.32834 |
| 2.55 | 6.312327 |
| 2.6 | 6.297094 |
| 2.65 | 6.282605 |
| 2.7 | 6.268822 |
| 2.75 | 6.255711 |
| 2.8 | 6.24324 |
| 2.85 | 6.231377 |
| 2.9 | 6.220093 |
| 2.95 | 6.209359 |
| 3 | 6.199148 |
| 3.05 | 6.189436 |
| 3.1 | 6.180197 |
| 3.15 | 6.171409 |
| 3.2 | 6.163049 |
| 3.25 | 6.155097 |
| 3.3 | 6.147533 |
| 3.35 | 6.140337 |
| 3.4 | 6.133493 |
| 3.45 | 6.126983 |
| 3.5 | 6.12079 |
| 3.55 | 6.114899 |
| 3.6 | 6.109295 |
| 3.65 | 6.103965 |
| 3.7 | 6.098894 |
| 3.75 | 6.094071 |
| 3.8 | 6.089483 |
| 3.85 | 6.085119 |
| 3.9 | 6.080968 |
| 3.95 | 6.077019 |
| 4 | 6.073263 |
At most 82 representative computed coordinates including endpoints; the plotted curve can use a finer grid. A table of a revealed generator is not independent measurement evidence.
| Quantity | Value | Unit |
|---|---|---|
| Capacitor voltage | 7.471518 | V |
| Signed capacitor current | -0.0007357589 | A |
| Stored-energy change | -0.01104411 | J |
| Source work | -0.007585447 | J |
| Resistor conversion | 0.003458659 | J |
| Energy residual | -4.33681e-19 | J |
| Initial voltage slope | -4 | V/s |
The initial deviation from the final voltage, not the final voltage alone, decays exponentially.
Kirchhoff and I=C dV/dt give RC dV/dt+V=6. Since RC=1 s, V=6+(Vinitial−6)e^(−t). Integrating 6 I and I²R gives source work and nonnegative resistor conversion. An initially overcharged capacitor sends energy back into the maintained source while still dissipating heat. At Vinitial=6 there is no transient. Source work alone is not equal to stored-energy change.
Predict before inspecting the values. Save contrasting records with assumptions and one alternative explanation. This virtual display does not certify practical measurement technique.
The initial deviation from the final voltage, not the final voltage alone, decays exponentially.
Kirchhoff and I=C dV/dt give RC dV/dt+V=6. Since RC=1 s, V=6+(Vinitial−6)e^(−t). Integrating 6 I and I²R gives source work and nonnegative resistor conversion. An initially overcharged capacitor sends energy back into the maintained source while still dissipating heat. At Vinitial=6 there is no transient. Source work alone is not equal to stored-energy change.
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