Topic 5 of 6
Reduce a network and work back
Find the equivalent resistance to obtain total current, then return to the original branches. A single equivalent resistor does not preserve every branch current or voltage.
Derive the two combination rules
In a series path, steady charge flow gives the same I through every resistor. The total p.d. is the sum of the individual drops:
Rseries = R1 + R2 + …
In parallel, each branch shares the same endpoints and therefore the same V. Total current is the sum of branch currents:
1/Rparallel = 1/R1 + 1/R2 + …
For exactly two parallel resistors, this rearranges to R1R2/(R1 + R2). Use the reciprocal sum for two or more: 3 Ω, 6 Ω and 6 Ω in parallel give 1/R = 1/3 + 1/6 + 1/6, hence R = 1.5 Ω.
Current conservation at a junction expresses conservation of charge; voltage drops along a path describe energy transferred per charge. Resistors transfer energy without consuming charge. A parallel equivalent must be smaller than the smallest positive branch resistance, while a series equivalent exceeds every individual positive resistance.
Worked network
Keep internal resistance in the complete path
A source has e.m.f. 9.0 V and internal resistance 1.0 Ω. The external circuit has R1 = 2.0 Ω on A/B, with R2 = 6.0 Ω and R3 = 3.0 Ω both on B/C.
Account for the whole circuit
The branch currents add to 1.8 A. Both parallel branches have 3.6 V across the same B/C endpoints.
Open only the three-ohm branch
The surviving branch receives 6.0 V and carries 1.0 A. Opening its parallel neighbour changes the whole circuit, including the internal drop.
Rexternal = 2.0 + 2.0 = 4.0 Ω
I = 9.0/(4.0 + 1.0) = 1.8 A
Now work back through the original network:
VAB = (1.8)(2.0) = 3.6 V
VBC = 7.2 - 3.6 = 3.6 V
I6 = 3.6/6.0 = 0.60 A
I3 = 3.6/3.0 = 1.20 A
The branch currents add to 1.8 A. Alternatively, the simultaneous relationships (6.0 Ω)I6 = (3.0 Ω)I3 and I6 + I3 = 1.8 A give the same two values.
With C chosen as 0 V, the model potentials are D = 9.0 V, A = 7.2 V and B = 3.6 V. The ideal source raises potential from C to D; internal resistance lowers it from D to A. This is why applying 9.0 V directly across the external network would be wrong.
Pinternal = (1.8)2(1.0) = 3.24 W
Psource = (9.0)(1.8) = 16.20 W
The two destinations add to the source power, providing an independent check on the calculation.
Opening a branch can increase another branch's current
Open only the 3.0 Ω branch. The external path is now 2.0 + 6.0 = 8.0 Ω, giving:
VAC = 9.0 - 1.0 = 8.0 V
VAB = (1.0)(2.0) = 2.0 V
VBC = 8.0 - 2.0 = 6.0 V
Total current falls from 1.8 to 1.0 A, yet current in the 6.0 Ω branch rises from 0.60 to 1.0 A. Its p.d. has increased from 3.6 to 6.0 V. The original branch voltage was not fixed independently of the rest of this circuit.
For another network, first establish what remains connected and which source model is supplied. Keep total, branch and component readings separate; a statement that one current falls does not determine every other current.