Derive network capacitance from a floating-node inventory
Capacitors in parallel share voltage, and their plate charges add: Ceq = C1 + C2.
Learning outcome: Predict series voltage division for unequal capacitances, compare the equivalent against the smaller component, and sum energies. Then solve the supplied precharged-node counterexample to identify exactly why the equal-charge shortcut needs an initial inventory assumption.
Starting recap
Integrate current or resistance, preserve node topology and derive transient state with a signed energy account.
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For C1 = 2 and C2 = 3 microfarad, Cs = 1.2 microfarad and Ct = 3.2 microfarad. The series charge is 14.4 microcoulomb, with voltage drops 7.2 and 4.8 V. Total final stored energy is 230.4 microjoule.
Open the experimentPredict
What condition supports equal charge magnitudes in this ideal series pair?
Experiment
Predict series voltage division for unequal capacitances, compare the equivalent against the smaller component, and sum energies. Then solve the supplied precharged-node counterexample to identify exactly why the equal-charge shortcut needs an initial inventory assumption.
Track floating-node charge in a capacitor network
Worked teaching model · synthetic values · 12 V ideal source across a selected two-capacitor series branch in parallel with a fixed 2 microfarad capacitor. Initial floating middle-node net charge is zero. Final static endpoint only; ideal-source switching transient is not modeled.
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Read the node connections before calculating
M is an initially neutral floating node. The fixed capacitor connects directly between T and B, not through M. Source fixes the two labeled boundary potentials. Component orientation and drawing lengths are schematic; source polarities are specified in the caption and node labels.
| First node | Second node | Element |
|---|---|---|
| T: 12 V | M | 2 μF |
| M | B: 0 V | 3 μF |
| T: 12 V | B: 0 V | 2 μF parallel |
Common schematic symbols and conventions
The symbol key is not a wiring recommendation. An open switch removes a conducting path; an ideal closed switch supplies a zero-drop connection. A current arrow is a chosen conventional-charge reference, not electron drift. A junction dot signifies connection; a crossing without a dot need not connect.
Potential through the series capacitor branch
Axes rescale independently. Curves join sampled coordinates; a joining segment is not additional measured evidence. Read physical units rather than screen angles or apparent slopes.
Potential through the series capacitor branch: numerical coordinates
| ordered node index | potential (V) |
|---|---|
| 0 | 12 |
| 1 | 4.8 |
| 2 | 0 |
| Quantity | Value | Unit |
|---|---|---|
| Series equivalent capacitance | 1.2 | microfarad |
| Total equivalent capacitance | 3.2 | microfarad |
| Charge magnitude on each series capacitor | 14.4 | microcoulomb |
| First capacitor voltage | 7.2 | V |
| Second capacitor voltage | 4.8 | V |
| Parallel capacitor charge | 24 | microcoulomb |
| Total source-delivered charge | 38.4 | microcoulomb |
| Sum of stored energies | 230.4 | microjoule |
| Equivalent final-state energy | 230.4 | microjoule |
Equal series charge follows from the initially neutral isolated middle node; parallel branches instead share voltage.
With zero net charge initially on the floating middle node, the adjacent plate charges sum to zero. Thus Q/C1 + Q/C2 = 12 V and reciprocal capacitances add. If that node initially carried a nonzero charge, the simple equal-magnitude statement would require modification. The final energy is not a claim about dissipation during ideal-source switching.
Derive before checking. Retain contrasting captures and explain one assumption that could fail; calculated evidence is not actual laboratory work.
Equal series charge follows from the initially neutral isolated middle node; parallel branches instead share voltage.
With zero net charge initially on the floating middle node, the adjacent plate charges sum to zero. Thus Q/C1 + Q/C2 = 12 V and reciprocal capacitances add. If that node initially carried a nonzero charge, the simple equal-magnitude statement would require modification. The final energy is not a claim about dissipation during ideal-source switching.
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Which source, topology, initial condition or instrument assumption would invalidate this inference?
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