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DC Electricity Beginner 9 min read Nov 2026

Series Circuits

In a series circuit, components form a single path so the same current flows through each. Learn series resistance, voltage division and troubleshooting open circuits.

Definition

A series circuit is a circuit in which components are connected end to end so that there is only one path for current. The same current flows through every element, and the source voltage divides among the elements in proportion to their resistances.

Learning objectives

  • Calculate the equivalent resistance of resistors in series.
  • Explain why the same current flows through every series element.
  • Calculate the voltage across each element and verify the voltage sum.
  • Recognise the effect of an open circuit in a series path.
Series Circuits diagram Resistors in series R₁ R₂ same current, voltages add
Series Circuits — schematic illustration
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Progressive explanation

Start with the plain-language idea, then move into the engineering detail. Each level stands on its own, so you can stop at the depth you need.

Beginner The core idea
A series circuit has one path from the source through every component and back. If you break the path anywhere, the whole circuit stops. A string of older fairy lights is a classic example: one failed bulb turns off the whole string because there is no alternative route.

The current is the same everywhere in the loop. What changes is the voltage: each component uses part of the source voltage, larger resistances taking a larger share. Add up the voltage across each component and you get back to the source voltage.
Intermediate How it behaves in a circuit
For ideal resistors in series, the equivalent resistance is the sum: R_eq = R₁ + R₂ + … + Rₙ. The current is I = V_source / R_eq and is identical through every element. The voltage across element n is Vₙ = I × Rₙ, which is the voltage-divider relationship. The sum of the voltage drops equals the source voltage, consistent with Kirchhoff’s voltage law.

A useful property is that the total resistance of a series combination is always larger than the largest individual resistance. Real components also have tolerances, so the calculated division is nominal; measured voltages can differ slightly. If one element opens, the current falls to zero and the full source voltage appears across the open point, which is why a voltmeter can locate a break.
Advanced Limits, assumptions, engineering detail
The series model assumes the components are ideal and that no current branches away; stray capacitance, leakage and meter loading can change the result. In high-voltage applications, series connection is used to share voltage between devices, but the devices must be matched or have voltage-grading networks so that uneven leakage or capacitance does not overstress one element.

At high frequency, the impedance of each element is complex and the voltage division becomes a phasor relationship. Series resonance occurs when inductive and capacitive reactances cancel, producing a minimum impedance and a large current at the resonant frequency. In machine windings, series and parallel groups of coils are combined to obtain the required voltage and current rating, and the mutual coupling between coils means simple resistance addition does not fully describe the behaviour.

Formulas and variables

Equivalent series resistance
R_eq = R₁ + R₂ + … + Rₙ
R_eq Equivalent resistance · Ω R₁, R₂ Individual resistances · Ω
10 Ω + 22 Ω + 68 Ω = 100 Ω.
Series current
I = V_source / R_eq
I Current through the series path · A V_source Source voltage · V R_eq Equivalent resistance · Ω
12 V across 100 Ω gives 0.120 A.
Voltage across one element
Vₙ = I × Rₙ
Vₙ Voltage across element n · V I Series current · A Rₙ Resistance of element n · Ω
0.120 A × 68 Ω = 8.16 V.

Units of measurement

QuantitySymbolUnit
Resistance R ohm (Ω)
Current I ampere (A)
Voltage V volt (V)
Power P watt (W)

Worked examples

Worked example

Three series resistors

Problem. A 12 V source feeds 10 Ω, 22 Ω and 68 Ω in series. Find the current and the voltage across each resistor.

Solution. R_eq = 10 + 22 + 68 = 100 Ω. I = 12/100 = 0.120 A. Voltages: V₁ = 0.120 × 10 = 1.20 V, V₂ = 0.120 × 22 = 2.64 V, V₃ = 0.120 × 68 = 8.16 V. Check: 1.20 + 2.64 + 8.16 = 12.00 V.

I = 0.120 A; V₁ = 1.20 V, V₂ = 2.64 V, V₃ = 8.16 V.
Worked example

Series circuit with kilohm resistors

Problem. A 12 V supply is connected across 1.0 kΩ, 2.0 kΩ and 3.0 kΩ in series. Find the current and the voltage across the 3.0 kΩ resistor.

Solution. R_eq = 1.0 + 2.0 + 3.0 = 6.0 kΩ. I = 12/6,000 = 2.0 mA. V = I × R = 2.0 mA × 3.0 kΩ = 6.0 V. The other drops are 2.0 V and 4.0 V, summing to 12 V.

I = 2.0 mA; V_3kΩ = 6.0 V.

Practical applications

  • Voltage division and reference setting
  • LED current limiting in a string
  • Safety and limit switches wired in series
  • Multi-cell battery strings

Automotive applications

Series connections appear in switch and sensor circuits: a brake light switch and a fuse are in series with the lamp, so either one can interrupt the circuit. A break anywhere stops the current, and a voltmeter can find it by measuring across each element while the circuit is supposed to be on. Series strings also appear in battery packs, where cell voltage adds and the weakest cell limits the string.

Industrial applications

Industrial control circuits often place emergency stops, limit switches and safety relays in series so that any one of them can drop the contactor coil. This is a fail-safe arrangement: an open contact removes the command to run. For higher voltages, series-connected devices require voltage grading, because unequal leakage currents or capacitances can put excessive voltage across one device.

Measurement procedure

  1. Measure the current at any point in the series path; it should be the same everywhere within meter accuracy.
  2. Measure the voltage across each element and add them; the sum should equal the source voltage in a simple series loop.
  3. To find an open element, measure voltage across each element with the circuit energised; the element with the full source voltage across it is the likely open one.
  4. De-energise the circuit before measuring resistance, and isolate elements so parallel paths do not affect the reading.

Common mistakes

  • Adding voltage drops as if the voltage were the same across every element.
  • Expecting the current to be different in different parts of a series path.
  • Forgetting that an open circuit in a series path stops current everywhere.
  • Adding resistors in parallel when they are actually connected end to end in series.

Safety considerations

  • A series circuit is not safer because it has one path; all elements may be at a high potential relative to earth.
  • When a series element opens, the full source voltage can appear across the break, which is a shock hazard.
  • Isolate and prove dead before working on a circuit, even when a switch appears to be open.

Frequently asked questions

Why is current the same everywhere in a series circuit?
There is only one path, and charge is conserved, so the same rate of charge must pass every point in the loop.
What happens if one resistor in series fails open?
The current becomes zero and the source voltage appears across the open element. The rest of the circuit is de-energised.
Does total resistance increase or decrease in series?
It increases: the equivalent resistance is the sum, so it is always larger than the largest individual resistance.
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