Series & Parallel Analysis#
The first simplification technique: reduce series and parallel combinations to equivalent single components. It’s the starting point for understanding most circuits and the first tool to reach for when making sense of a schematic.
Series Combinations#
Components in series carry the same current. Voltages add.
- Resistors: R_total = R1 + R2 + R3 + …
- Capacitors: 1/C_total = 1/C1 + 1/C2 + … (capacitance decreases — the smallest cap dominates)
- Inductors: L_total = L1 + L2 + … (assuming no mutual coupling)
Why Series Capacitors Seem Backwards#
The series capacitor formula confuses everyone at first. Think of it this way: series capacitors are like making the dielectric thicker. A thicker dielectric means less capacitance. The series combination is always less than the smallest individual capacitor.
For two caps in series: C_total = (C1 × C2) / (C1 + C2)
Parallel Combinations#
Components in parallel share the same voltage. Currents add.
- Resistors: 1/R_total = 1/R1 + 1/R2 + … (resistance decreases — the smallest R dominates)
- Capacitors: C_total = C1 + C2 + C3 + … (capacitance adds directly)
- Inductors: 1/L_total = 1/L1 + 1/L2 + … (assuming no mutual coupling)
For two resistors in parallel: R_total = (R1 × R2) / (R1 + R2)
Quick mental math: two equal resistors in parallel = half of one. A 10 kΩ in parallel with a 1 kΩ is approximately 0.9 kΩ — the smaller one dominates.
When Simplification Helps#
- Calculating total load resistance — What does the power supply see? Reduce parallel loads to one equivalent resistance
- Finding expected voltages — Combine resistors, then use Ohm’s law or voltage divider equations
- Estimating filter behavior — Equivalent RC or LC values determine cutoff frequencies
- Quick sanity checks — “Is this node about where expected?” often comes down to a quick series/parallel reduction
When Simplification Hides Problems#
- Component tolerances disappear — When R1 + R2 is combined, individual tolerances are lost. The worst-case equivalent resistance depends on which way each tolerance goes, and simplification sweeps this under the rug
- Power distribution is hidden — A single equivalent resistor doesn’t indicate how power is split among the actual components. Each real resistor has its own power dissipation and thermal limit
- Parasitic behavior doesn’t simplify cleanly — Two capacitors in parallel don’t just add capacitance — they also combine their ESR (in parallel, reducing it) and their ESL (in parallel, reducing it). The simplified model of “bigger C” misses the improved high-frequency behavior that was the whole reason for paralleling them
- Loading effects — Replacing a load with its equivalent resistance can mask the fact that adding another branch changes what the original components see. This is where voltage divider loading analysis takes over
Mixed Series-Parallel Networks#
Most circuits aren’t purely series or purely parallel. The approach:
- Identify the innermost series or parallel group
- Reduce it to a single equivalent element
- Repeat until simplification is no longer possible
- Apply KVL/KCL to whatever remains
Some networks (bridges, T-networks, pi-networks) can’t be fully reduced by series/parallel alone. These require node or loop analysis, or delta-wye transformations.
Tips#
- Start from the innermost combinations and work outward
- Two equal resistors in parallel = half the value of one — a useful mental shortcut
- For quick estimates, the parallel combination of two very different values is approximately the smaller one
Caveats#
- Series elements must carry the same current — If there’s a branch point between two elements, they’re not in series. This sounds obvious but causes errors in complex schematics
- Parallel elements must share the same two nodes — If two elements connect between the same pair of nodes, they’re in parallel. If they don’t share both nodes, they’re not parallel, even if they look close on the schematic
- Real components aren’t purely R, C, or L — A real capacitor in a series chain adds its ESR as a series resistance and its ESL as a series inductance. At some frequency, this changes the effective impedance significantly
- Don’t over-simplify for AC — At AC, impedances are needed, not just resistances. A 1 kΩ resistor in parallel with a 100 nF cap has different equivalent impedance at every frequency. Series/parallel reduction still works, but with complex numbers
In Practice#
- A measured resistance that doesn’t match the expected series/parallel combination suggests a component is out of tolerance, damaged, or there’s a parallel path not accounted for
- Unexpected voltage at a node often means the assumed series/parallel model is missing a load or leakage path
- Filter behavior that doesn’t match calculations may indicate parasitic elements (ESR, ESL, stray capacitance) that the simplified model ignores