Identify the charge and voltage constraints of capacitor networks
Capacitor combination rules follow different common quantities from resistor rules. Across parallel capacitors, the potential difference is the same and plate charges add: Qtotal=(C1+C2)V. In a series pair with an initially neutral isolated intermediate conductor, the two capacitor charge magnitudes are equal. Their voltage drops add, so V=Q/C1+Q/C2 and 1/Ceq=1/C1+1/C2.
Learning outcome: Compare equal and unequal capacitances in both topologies. Retain individual voltages, charges and energy before summing. Then describe what extra datum would be needed if the isolated midpoint began with nonzero net charge.
Starting recap
Use charge continuity, energy per charge, consistent SI units and an explicit circuit topology. Exponential responses are supplied algebraic models; initial state, source constraint and measurement loading must be declared.
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For C1=2 µF, C2=4 µF and source 6 V, series Ceq=4/3 µF and common plate charge is 8 µC. Voltages are 4 and 2 V; energies 16 and 8 µJ total 24 µJ. In parallel Ceq=6 µF, charges are 12 and 24 µC, and total energy is 108 µJ.
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The equal series-capacitor charge magnitudes rely here on:
Experiment
Compare equal and unequal capacitances in both topologies. Retain individual voltages, charges and energy before summing. Then describe what extra datum would be needed if the isolated midpoint began with nonzero net charge.
Compare series and parallel charge and energy
Worked teaching model · synthetic values · Two ideal linear capacitors across an ideal maintained 6 V source, compared in two distinct topologies. In series the isolated intermediate conductor initially has zero net charge. No leakage, breakdown, ESR or physical handling.
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Series equivalent capacitance versus second element
Unlike graph quantities rescale independently; read units and values, not screen angles. 1: isolated neutral midpoint (solid). Joined curves show the supplied model, not additional observations.
Equivalent numerical coordinates for Series equivalent capacitance versus second element
isolated neutral midpoint
| second capacitance (µF) | equivalent capacitance (µF) |
|---|---|
| 2 | 1 |
| 2.1 | 1.02439 |
| 2.2 | 1.04762 |
| 2.3 | 1.06977 |
| 2.4 | 1.09091 |
| 2.5 | 1.11111 |
| 2.6 | 1.13043 |
| 2.7 | 1.14894 |
| 2.8 | 1.16667 |
| 2.9 | 1.18367 |
| 3 | 1.2 |
| 3.1 | 1.21569 |
| 3.2 | 1.23077 |
| 3.3 | 1.24528 |
| 3.4 | 1.25926 |
| 3.5 | 1.27273 |
| 3.6 | 1.28571 |
| 3.7 | 1.29825 |
| 3.8 | 1.31034 |
| 3.9 | 1.32203 |
| 4 | 1.33333 |
| 4.1 | 1.34426 |
| 4.2 | 1.35484 |
| 4.3 | 1.36508 |
| 4.4 | 1.375 |
| 4.5 | 1.38462 |
| 4.6 | 1.39394 |
| 4.7 | 1.40299 |
| 4.8 | 1.41176 |
| 4.9 | 1.42029 |
| 5 | 1.42857 |
| 5.1 | 1.43662 |
| 5.2 | 1.44444 |
| 5.3 | 1.45205 |
| 5.4 | 1.45946 |
| 5.5 | 1.46667 |
| 5.6 | 1.47368 |
| 5.7 | 1.48052 |
| 5.8 | 1.48718 |
| 5.9 | 1.49367 |
| 6 | 1.5 |
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 |
|---|---|---|
| Series equivalent capacitance | 1.33333 | µF |
| Series plate-charge magnitude | 8 | µC |
| First series capacitor voltage | 4 | V |
| Second series capacitor voltage | 2 | V |
| Series total energy | 0.000024 | J |
| Parallel equivalent capacitance | 6 | µF |
| First parallel plate charge | 12 | µC |
| Second parallel plate charge | 24 | µC |
| Parallel total energy | 0.000108 | J |
| Series voltage residual | 0 | V |
Series capacitors share charge magnitude under the neutral-midpoint premise; parallel capacitors share voltage.
For series Q/C1+Q/C2=V, so 1/Ceq=1/C1+1/C2. For parallel Qtotal=(C1+C2)V. These rules contrast with resistor combinations because different conserved/common quantities enter. Preexisting net charge on the isolated midpoint changes the equal-charge premise. The comparison uses two separately charged configurations, not an unmodeled sudden reconnection with missing dissipated energy.
Predict before inspecting the values. Save contrasting records with assumptions and one alternative explanation. This virtual display does not certify practical measurement technique.
Series capacitors share charge magnitude under the neutral-midpoint premise; parallel capacitors share voltage.
For series Q/C1+Q/C2=V, so 1/Ceq=1/C1+1/C2. For parallel Qtotal=(C1+C2)V. These rules contrast with resistor combinations because different conserved/common quantities enter. Preexisting net charge on the isolated midpoint changes the equal-charge premise. The comparison uses two separately charged configurations, not an unmodeled sudden reconnection with missing dissipated energy.
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