Sublevo
ISC 2027
All chaptersPhysics · Unit 2

Current Electricity

10 articles42 formulas58 ways the board asks it
PHYCells & Circuits

Series & Parallel Combinations

This subtopic is the algebra of combining resistors: series resistances add, while parallel resistances combine through reciprocals, and most circuits reduce by alternating these two rules. The core idea is that series elements share the same current and parallel elements share the same voltage.

ISC problems mix a parallel block in series with another resistor across a battery and ask for the main current and the branch currents.

Series combination
Rs=R1+R2+R3+⋯R_s = R_1 + R_2 + R_3 + \cdots
RsR_s equivalent series resistance (Ω\Omega). Same current flows through each; total PD is the sum of individual drops. RsR_s is larger than any single resistor.
Parallel combination
1Rp=1R1+1R2+1R3+⋯\dfrac{1}{R_p} = \dfrac{1}{R_1} + \dfrac{1}{R_2} + \dfrac{1}{R_3} + \cdots
RpR_p equivalent parallel resistance (Ω\Omega). Same PD across each; total current is the sum of branch currents. RpR_p is smaller than the smallest resistor.
Derivation
  1. Three resistors in parallel share the same potential difference VV across each (both ends tied to the same pair of nodes), while the source current II splits into the branch currents:
    I=I1+I2+I3I = I_1 + I_2 + I_3
  2. Ohm's law gives each branch current in terms of the common VV:
    I1=VR1,I2=VR2,I3=VR3I_1=\dfrac{V}{R_1}, \quad I_2=\dfrac{V}{R_2}, \quad I_3=\dfrac{V}{R_3}
  3. Substitute and factor out VV; the equivalent resistor RpR_p must carry the same total II for the same VV:
    I=VRp=V(1R1+1R2+1R3)  ⇒  1Rp=1R1+1R2+1R3I=\dfrac{V}{R_p} = V\left(\dfrac{1}{R_1}+\dfrac{1}{R_2}+\dfrac{1}{R_3}\right) \;\Rightarrow\; \dfrac{1}{R_p}=\dfrac{1}{R_1}+\dfrac{1}{R_2}+\dfrac{1}{R_3}
Two resistors in parallel (product over sum)
Rp=R1R2R1+R2R_p = \dfrac{R_1 R_2}{R_1 + R_2}
Handy shortcut for exactly two resistors. For 6 Ω6\,\Omega and 3 Ω3\,\Omega this gives 2 Ω2\,\Omega.
Current divider for branch currents
I1=I R2R1+R2,I2=I R1R1+R2I_1 = I \, \dfrac{R_2}{R_1 + R_2}, \qquad I_2 = I \, \dfrac{R_1}{R_1 + R_2}
II current entering a two-resistor parallel node, I1,I2I_1, I_2 branch currents. Each branch carries a fraction inversely proportional to its own resistance.
  • Series resistors carry identical current; parallel resistors share identical voltage — identify which is fixed before computing.
  • Equivalent series resistance exceeds the largest member; equivalent parallel resistance is below the smallest member — use this to sanity-check.
  • The product-over-sum shortcut applies only to two resistors at a time; for three or more use full reciprocals.
  • Find the main current from the battery using the total equivalent resistance, then redistribute into branches with the current divider.
  • Across a parallel block the voltage is common; branch currents follow Ii=V/RiI_i = V/R_i.
  • Include internal resistance rr in series with the external network when computing the main current if the battery is non-ideal.
  • In a current divider, the smaller-resistance branch carries the larger current (current prefers the easier path).
Where the marks go
  • Adding parallel resistances directly instead of adding their reciprocals (or using product-over-sum).
  • Forgetting to take the reciprocal of 1/Rp1/R_p at the end, reporting 1/Rp1/R_p as the resistance.
  • Assuming equal current in parallel branches when their resistances differ — current splits inversely with resistance.
  • Applying product-over-sum to three resistors at once instead of pairing or using full reciprocals.
How the board asks it
  • Numericaltotal equivalent resistance then current divider
    A battery of emf 6 V6\,V and internal resistance 0.5 Ω0.5\,\Omega is connected to a parallel combination of 3 Ω3\,\Omega and 6 Ω6\,\Omega, which is in series with a 1.5 Ω1.5\,\Omega resistor. Calculate the main current drawn from the battery and the current in each parallel branch.
  • Numericalparallel combination of three resistors
    Three resistors of 4 Ω4\,\Omega, 6 Ω6\,\Omega and 12 Ω12\,\Omega are connected in parallel across a 12 V12\,V source. Calculate the equivalent resistance of the combination and the total current supplied by the source.
  • Derive / proveparallel combination through reciprocals at common voltage
    Three resistors R1R_1, R2R_2 and R3R_3 are connected in parallel across a cell of potential difference VV. Obtain an expression for the equivalent resistance of the combination, stating clearly the quantity that is common to all three resistors.
  • Give reasonsequivalent resistance bounds as a sanity check
    Two resistors are connected in parallel. Give reasons why the equivalent resistance of the combination is always less than the smaller of the two individual resistances.
  • Applicationcurrent divider; current prefers the easier path
    A current of 9 A9\,A enters a junction and divides between two parallel resistors of 2 Ω2\,\Omega and 4 Ω4\,\Omega. State which branch carries the larger current, giving a reason, and calculate the current in each branch.

Practise this topic

Written for Sublevo. Question text quoted anywhere in these notes is the Council’s and carries its year and paper; the board’s own diagrams are not reproduced.