5.3 Series/Parallel Networks & Supply Internal Resistance
Key Takeaways
- Series resistances add: R_T = R₁ + R₂ + …; same current through each; voltages divide in proportion to resistance
- Parallel conductances add: 1/R_T = 1/R₁ + 1/R₂ + …; same voltage across each; currents divide inversely with resistance
- Combination networks are reduced step-by-step—identify pure series or parallel groups, replace with equivalents, then expand currents and voltages
- A voltage divider produces V_out = V_in × R_bottom/(R_top + R_bottom) when unloaded (or when load ≫ divider resistance)
- Supply internal resistance r causes terminal voltage V_T = E − I r to fall as load current rises—open-circuit voltage is E; loaded voltage is always lower for a passive internal r
5.3 Series/Parallel Networks & Supply Internal Resistance
Quick Answer: Series: R_T = ΣR, same I, voltages share. Parallel: 1/R_T = Σ(1/R), same V, currents share. Reduce combinations group by group. An unloaded divider gives V_out = V_in × R₂/(R₁+R₂). With internal resistance r, V_terminal = E − I r, so heavier loads pull the terminals down.
Topic 3.6 finishes with the networks you actually meet on aircraft wiring and bench power supplies: strings, branches, dividers, and real sources that are not ideal voltage fonts.
Series Resistance Networks
For n resistances in series:
R_T = R₁ + R₂ + … + R_n
| Property | Series behaviour |
|---|---|
| Current | Same through every element |
| Voltage | Splits: V_k = I R_k |
| Total voltage | V_T = Σ V_k = I R_T |
Worked Series Example
R₁ = 10 Ω, R₂ = 22 Ω, R₃ = 8 Ω on E = 40 V (ideal).
- R_T = 10 + 22 + 8 = 40 Ω.
- I = 40/40 = 1 A.
- Drops: 10 V, 22 V, 8 V (sum 40 V).
Parallel Resistance Networks
1/R_T = 1/R₁ + 1/R₂ + … + 1/R_n
For two resistors: R_T = (R₁ R₂)/(R₁ + R₂).
| Property | Parallel behaviour |
|---|---|
| Voltage | Same across every branch |
| Current | Splits: I_k = V / R_k |
| Total current | I_T = Σ I_k = V / R_T |
R_T is always less than the smallest branch resistance.
Worked Parallel Example
R₁ = 6 Ω, R₂ = 12 Ω, R₃ = 4 Ω across 24 V.
- 1/R_T = 1/6 + 1/12 + 1/4 = 0.1667 + 0.0833 + 0.25 = 0.5 ⇒ R_T = 2 Ω.
- I_T = 24/2 = 12 A.
- Branch currents: 4 A, 2 A, 6 A (sum 12 A).
Combination (Series–Parallel) Reduction
Worked Combination Example
Circuit: R₁ = 5 Ω in series with a parallel pair R₂ = 20 Ω and R₃ = 30 Ω; supply E = 50 V ideal.
- Parallel pair: R₂₃ = (20 × 30)/(20 + 30) = 600/50 = 12 Ω.
- R_T = 5 + 12 = 17 Ω.
- I_total = 50/17 ≈ 2.941 A.
- Drop on R₁: V₁ = 2.941 × 5 ≈ 14.71 V.
- Parallel voltage: V₂₃ = 50 − 14.71 ≈ 35.29 V (also 2.941 × 12).
- I₂ = 35.29/20 ≈ 1.765 A, I₃ = 35.29/30 ≈ 1.176 A (sum ≈ 2.941 A).
Always reduce from the inside out: combine pure parallel or series islands, redraw, repeat.
Voltage Dividers
Two resistors in series across V_in form a divider. Taking the output across the bottom resistor R₂:
V_out = V_in × R₂ / (R₁ + R₂) (unloaded)
Worked Unloaded Divider
V_in = 28 V, R₁ = 3 kΩ, R₂ = 1 kΩ, output across R₂.
V_out = 28 × 1000/(3000+1000) = 28 × 0.25 = 7 V.
Loaded Divider Trap
If a load R_L = 1 kΩ connects across R₂, R₂ and R_L are in parallel first:
R₂∥L = (1×1)/(1+1) = 0.5 kΩ.
Then V_out = 28 × 0.5/(3 + 0.5) = 28 × 0.5/3.5 = 4 V.
Loading pulled the tap from 7 V down to 4 V. Exam stems that ignore the load after mentioning it are testing whether you rebuild the parallel equivalent.
Supply Internal Resistance and Terminal Voltage
A real DC source is modelled as an ideal EMF E in series with internal resistance r. External load R_L connects to the terminals.
I = E / (R_L + r)
V_terminal = I R_L = E − I r = E × R_L/(R_L + r)
| Condition | Terminal voltage |
|---|---|
| Open circuit (I = 0) | V_T = E |
| Loaded | V_T = E − I r < E |
| Short circuit (idealised) | I → E/r, V_T → 0 |
Worked Internal-r Example 1
Battery E = 24 V, r = 0.5 Ω, load R_L = 7.5 Ω.
- I = 24 / (7.5 + 0.5) = 24/8 = 3 A.
- V_T = 3 × 7.5 = 22.5 V.
- Internal drop: I r = 1.5 V; check 24 − 1.5 = 22.5 V.
Worked Internal-r Example 2 — Heavier Load
Same battery, now R_L = 1.5 Ω.
- I = 24 / (1.5 + 0.5) = 24/2 = 12 A.
- V_T = 12 × 1.5 = 18 V.
- Internal drop 6 V.
Terminal voltage fell from 22.5 V to 18 V as load current rose. That is why a weak battery (higher effective r) may show near-rated open-circuit voltage on a high-impedance meter yet collapse when a starter or pump demands high current.
Worked Internal-r Example 3 — Finding r from Measurements
Open-circuit voltage measured E = 28.0 V. Under a 10 A load, terminals read 26.5 V.
I r = E − V_T = 1.5 V ⇒ r = 1.5/10 = 0.15 Ω.
This measurement pattern appears in Module 3 reasoning even when the algebra is short: open-circuit ≈ EMF; loaded sag reveals r.
Linking Networks to Internal r
Suppose E = 30 V, r = 1 Ω, and the external network is 4 Ω in series with a parallel pair of 12 Ω and 6 Ω.
- Parallel: R_p = (12×6)/(12+6) = 4 Ω.
- External R_L = 4 + 4 = 8 Ω.
- I = 30/(8+1) = 3.333 A.
- V_T = 30 − 3.333×1 ≈ 26.67 V (also 3.333 × 8).
- Series 4 Ω drop ≈ 13.33 V; parallel voltage ≈ 13.33 V; currents 13.33/12 ≈ 1.11 A and 13.33/6 ≈ 2.22 A.
One problem used series/parallel reduction, Ohm’s law, KCL at the parallel node, and internal-resistance sag together—the full topic 3.6 skill set.
Exam Priority Checklist
- Label series vs parallel vs mixed; redraw after each reduction.
- For dividers, ask whether the output is loaded.
- Never treat battery terminal voltage as equal to EMF under load unless r = 0 or I ≈ 0.
- Sense-check: adding a parallel path always lowers R_T; adding series always raises R_T; loading a divider always lowers (or leaves equal) V_out compared with the unloaded tap.
Series/parallel arithmetic plus internal-r awareness turns Ohm and Kirchhoff from isolated laws into a complete DC-circuit toolkit for CAAS Module 3.
Three resistors 5 Ω, 10 Ω, and 15 Ω are connected in series across an ideal 60 V supply. What is the circuit current?
An unloaded voltage divider has R₁ = 9 kΩ (top) and R₂ = 3 kΩ (bottom) across 48 V. What is V_out across R₂?
A battery has EMF E = 12 V and internal resistance r = 0.4 Ω. What is the terminal voltage when it delivers 5 A to a load?
Two resistors of 8 Ω and 24 Ω are in parallel. What is their equivalent resistance?