Skip to content
Dabour HubLEARN · PRACTICE · EXPLORESign inStudent

10.2.3Electricity and D.C. circuits

Resistors in Series

5 min read 6 parts Lesson 18 of 26 1 quiz

0%read
Lesson summary

10.2.3 Resistors in Series — AS PHYSICS 9702 notes: Derive and use R = R₁ + R₂ + … for resistors in series.Current — it is the same through all the resistors.Potential difference — it is shared between all the resistors.Combined resistance — it is the sum of the individual resist…

  • What the symbols mean
  • Separate p.d.s
  • Rearranging
  • Effect of adding resistors
  • Components
  • Reciprocal

Section 1 of 6Series circuit rules

Current
  • Current it is the same through all the resistors.
Potential difference
  • Potential difference it is shared between all the resistors.
Combined resistance
  • Combined resistance it is the sum of the individual resistances.

Section 2 of 6Derivation from Kirchhoff’s laws

1
The same current I flows through each resistor.
2
By Kirchhoff’s second law, the supply p.d. equals the sum of the p.d.s: V = V1 + V2.
3
Using V = IR for each, IR = IR1 + IR2.
4
Dividing by I gives R = R1 + R2.

Section 3 of 6The equation

1Equation
  • R = R1 + R2 + …
    What the symbols mean: RT = total resistance of resistors in series (Ω) · R1, R2 = the separate resistances (Ω)
2Separate p.d.s
  • Separate p.d.s each resistor connected in series has its own separate potential difference.
3Rearranging
  • Rearranging an unknown resistor is found from R2 = R − (R1 + R3).
4Effect of adding resistors
  • Effect of adding resistors the combined resistance increases.

Section 4 of 6More from the specification

More from the specification
Series resistor voltage and power
  • Series resistor voltage and power potential differences divide proportionally across series resistances, dissipating electrical power according to current squared times resistance.
Resistors in series and energy conservation
  • In a closed series circuit, the same current flows through all components,
  • and the total potential difference across the circuit equals the sum of individual p.d.s,
  • giving combined resistance R = R1 + R2 + R3.
Resistors in parallel rule
  • For parallel circuit branches connected across common junctions, the reciprocal of the total equivalent resistance equals the sum of the reciprocals of individual resistances: 1/Rp = 1/R1 + 1/R2 + 1/R3.
Kirchhoff's laws in problem solving
  • Kirchhoff's first law applies conservation of charge at any junction,
    • (sum of Iin = sum of Iout)
  • while Kirchhoff's second law applies conservation of energy around any closed loop.
    • (sum of EMF = sum of IR)
Potential divider circuits
  • When solving problems with series resistors, the potential difference across any individual resistor is proportional to its fraction of the total series resistance (Vout = Vin * (R2 / (R1 + R2))).
Resistors in series and energy conservation
  • In a closed series circuit, the same current flows through all components,
  • and the total potential difference across the circuit equals the sum of individual p.d.s,
  • giving combined resistance R = R1 + R2 + R3.
Resistors in parallel rule
  • For parallel circuit branches connected across common junctions, the reciprocal of the total equivalent resistance equals the sum of the reciprocals of individual resistances: 1/Rp = 1/R1 + 1/R2 + 1/R3.
Kirchhoff's laws in problem solving
  • Kirchhoff's first law applies conservation of charge at any junction,
    • (sum of Iin = sum of Iout)
  • while Kirchhoff's second law applies conservation of energy around any closed loop.
    • (sum of EMF = sum of IR)
Potential divider circuits
  • When solving problems with series resistors, the potential difference across any individual resistor is proportional to its fraction of the total series resistance (Vout = Vin * (R2 / (R1 + R2))).
Ammeter
  • Component that measures current.
Voltmeter
  • Instrument that measures p.d., connected in parallel.
Charge
  • Quantity of electricity in coulombs, Q = It.
    What the symbols mean: Q = charge (C) · I = current (A) · t = time (s)
Series circuit
  • Circuit with components connected one after another in a single loop.
Parallel circuit
  • Circuit with branches; same p.d. across each branch.
Closed circuit
  • Complete loop with a source in which current can flow
Energy transferred
  • W = V Q, in joules.
    What the symbols mean: E or W = energy transferred (J) · Q = charge (C) · V = potential difference (V) · I = current (A) · t = time (s)
Parallel
  • Components on separate branches, each with the full e.m.f.
Junction
  • Place where a pipe splits or joins; flow rates add.
Components
  • Perpendicular parts of a vector that add to give the vector.
Reciprocal
  • The value 1/x; the calculator button is x−1.

Section 5 of 6Key terms

TermMeaning
Series circuitComponents connected end to end so the same current passes through each.
Combined resistanceSingle resistance that could replace the network and draw the same current.
Kirchhoff’s second lawTotal e.m.f. equals the sum of the p.d.s across the components.
Potential differenceEnergy transferred per unit charge between two points.

Section 6 of 6Exam technique

1
Adding the reciprocals for resistors in series — only add the resistances.
2
Thinking the current is shared in series — the current is the same.
3
Forgetting that the combined resistance is larger than any single resistor.
4
Using the wrong resistor values when rearranging.
\n