Match the state instead of restarting the transient
A finite resistor limits current even when an ideal source changes abruptly. The same RC=1 s element starts at zero voltage, sees 6 V until time ts, and then sees −2 V. The resistor remains connected. Capacitor voltage is continuous because a finite current cannot transfer finite charge in zero time.
Learning outcome: Compare observations just before, exactly at and after a chosen switch. Retain which one-sided convention is used for current. Predict how delaying the switch changes the second initial state without changing the −2 V final asymptote.
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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Try
If ts=1 s, boundary voltage is 6(1−1/e)≈3.792723 V. Just before switching, current is 3/e mA≈1.103638 mA. Just after, it is −2.896362 mA. Their difference is −4 mA while capacitor voltage has not jumped.
Open the experimentPredict
What changes discontinuously at the ideal switch in this bounded model?
Experiment
Compare observations just before, exactly at and after a chosen switch. Retain which one-sided convention is used for current. Predict how delaying the switch changes the second initial state without changing the −2 V final asymptote.
Match capacitor state across a source change
Worked teaching model · synthetic values · Same 2000 ohm and 500 microfarad element, initially zero voltage. Source is 6 V before the switch and −2 V afterward; switch does not disconnect the resistor. At the exact switch instant display the right-hand source/current and continuous capacitor voltage. No impulsive capacitor voltage jump.
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Continuous state with a changed derivative
Unlike graph quantities rescale independently; read units and values, not screen angles. 1: piecewise analytic voltage (solid).2: actual switch coordinate (open-circle marked location). Joined curves show the supplied model, not additional observations.
Equivalent numerical coordinates for Continuous state with a changed derivative
piecewise analytic voltage
| time (s) | capacitor voltage (V) |
|---|---|
| 0 | 0 |
| 0.05 | 0.2926235 |
| 0.1 | 0.5709755 |
| 0.15 | 0.8357521 |
| 0.2 | 1.087615 |
| 0.25 | 1.327195 |
| 0.3 | 1.555091 |
| 0.35 | 1.771871 |
| 0.4 | 1.97808 |
| 0.45 | 2.174231 |
| 0.5 | 2.360816 |
| 0.55 | 2.538301 |
| 0.6 | 2.70713 |
| 0.65 | 2.867725 |
| 0.7 | 3.020488 |
| 0.75 | 3.165801 |
| 0.8 | 3.304026 |
| 0.85 | 3.43551 |
| 0.9 | 3.560582 |
| 0.95 | 3.679554 |
| 1 | 3.792723 |
| 1.05 | 3.510209 |
| 1.1 | 3.241473 |
| 1.15 | 2.985843 |
| 1.2 | 2.742681 |
| 1.25 | 2.511377 |
| 1.3 | 2.291355 |
| 1.35 | 2.082063 |
| 1.4 | 1.882979 |
| 1.45 | 1.693603 |
| 1.5 | 1.513464 |
| 1.55 | 1.342111 |
| 1.6 | 1.179114 |
| 1.65 | 1.024067 |
| 1.7 | 0.8765813 |
| 1.75 | 0.7362888 |
| 1.8 | 0.6028384 |
| 1.85 | 0.4758965 |
| 1.9 | 0.3551456 |
| 1.95 | 0.2402838 |
| 2 | 0.1310238 |
| 2.05 | 0.02709257 |
| 2.1 | -0.0717699 |
| 2.15 | -0.1658108 |
| 2.2 | -0.2552653 |
| 2.25 | -0.340357 |
| 2.3 | -0.4212987 |
| 2.35 | -0.4982929 |
| 2.4 | -0.571532 |
| 2.45 | -0.6411992 |
| 2.5 | -0.7074687 |
| 2.55 | -0.7705062 |
| 2.6 | -0.8304693 |
| 2.65 | -0.887508 |
| 2.7 | -0.9417649 |
| 2.75 | -0.9933756 |
| 2.8 | -1.042469 |
| 2.85 | -1.089169 |
| 2.9 | -1.13359 |
| 2.95 | -1.175846 |
| 3 | -1.21604 |
| 3.05 | -1.254274 |
| 3.1 | -1.290644 |
| 3.15 | -1.325239 |
| 3.2 | -1.358148 |
| 3.25 | -1.389451 |
| 3.3 | -1.419228 |
| 3.35 | -1.447553 |
| 3.4 | -1.474496 |
| 3.45 | -1.500125 |
| 3.5 | -1.524504 |
| 3.55 | -1.547695 |
| 3.6 | -1.569754 |
| 3.65 | -1.590737 |
| 3.7 | -1.610697 |
| 3.75 | -1.629684 |
| 3.8 | -1.647744 |
| 3.85 | -1.664924 |
| 3.9 | -1.681266 |
| 3.95 | -1.696811 |
| 4 | -1.711597 |
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.
actual switch coordinate
| time (s) | capacitor voltage (V) |
|---|---|
| 1 | 3.792723 |
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 |
|---|---|---|
| Voltage at switching boundary | 3.792723 | V |
| Observed capacitor voltage | 1.513464 | V |
| Right-hand selected source voltage | -2 | V |
| Observed signed current | -0.001756732 | A |
| Current immediately before switch | 0.001103638 | A |
| Current immediately after switch | -0.002896362 | A |
| Current jump | -0.004 | A |
Finite resistor current allows the derivative to jump, not the capacitor voltage itself.
The first interval ends at Vs=6(1−e^(−ts)). Use that voltage as the second initial condition: V=−2+(Vs+2)e^(−(t−ts)). The source changes by −8 V, so resistor current jumps by −8/2000 A. At the exact switch the display uses the right-hand current. Resetting the capacitor to zero or restarting the original formula discards stored charge.
Predict before inspecting the values. Save contrasting records with assumptions and one alternative explanation. This virtual display does not certify practical measurement technique.
Finite resistor current allows the derivative to jump, not the capacitor voltage itself.
The first interval ends at Vs=6(1−e^(−ts)). Use that voltage as the second initial condition: V=−2+(Vs+2)e^(−(t−ts)). The source changes by −8 V, so resistor current jumps by −8/2000 A. At the exact switch the display uses the right-hand current. Resetting the capacitor to zero or restarting the original formula discards stored charge.
Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.
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