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Quantities & Units Beginner 9 min read Nov 2026

Voltage (Potential Difference)

Voltage is the electrical pressure that drives current. Learn what a volt means, how EMF differs from terminal voltage, and how to measure voltage safely.

Definition

Voltage, or potential difference, is the difference in electric potential between two points, equal to the work needed to move one unit of charge between them. It is measured in volts, where one volt is one joule per coulomb (1 V = 1 J/C).

Learning objectives

  • Define voltage and state the meaning of one volt.
  • Distinguish electromotive force from terminal voltage.
  • Apply Ohm’s law and Kirchhoff’s voltage law to simple circuits.
  • Measure voltage correctly with a voltmeter or multimeter.
Voltage (Potential Difference) diagram A closed electrical circuit electrical principle schematic — not to scale
Voltage (Potential Difference) — 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
Voltage is often described as electrical pressure. It is not something that flows; it is a difference between two points that pushes charge through a circuit. A 12 V battery maintains about 12 V between its terminals, so each coulomb of charge that moves from one terminal to the other gains or gives up about 12 joules of energy.

A useful comparison is a water circuit: voltage is like the height difference or pressure that drives the flow, current is the amount of water flowing per second, and resistance is the narrowness of the pipe. If the pressure difference is zero, no water flows; if the voltage difference is zero, no current flows.
Intermediate How it behaves in a circuit
Voltage is measured in volts and is always a difference between two points. In a resistive circuit at constant temperature, Ohm’s law relates voltage, current and resistance: V = I × R. The source’s electromotive force (EMF) is the voltage it would deliver with no current, while the terminal voltage is lower when current flows because of the source’s internal resistance: V_terminal = EMF − I × r.

In series circuits the voltage divides between elements, and in parallel circuits each branch sees the same voltage. Kirchhoff’s voltage law formalises this: around any closed loop, the algebraic sum of voltages is zero. Voltage can be measured with a voltmeter or a multimeter in voltage mode, connected in parallel across the points of interest.
Advanced Limits, assumptions, engineering detail
Voltage is the line integral of the electric field between two points, V = −∫E·dl, which is why the volt is equivalent to a joule per coulomb. In a circuit with time-varying magnetic flux, the electric field is not conservative and the concept of a single-valued potential between two nodes needs care; this is why induced EMF appears as a source distributed around a loop rather than as a voltage at one point.

Real sources have internal resistance and finite current capability, so loading matters: a high-impedance voltmeter reads close to the open-circuit EMF, while a low-impedance load pulls the terminal voltage down. Measurement leads also form loops that can pick up induced voltages in strong magnetic fields, which is one reason why twisted pairs and careful routing are used in precision measurements.

Formulas and variables

Voltage, current and resistance
V = I × R
V Voltage · V I Current · A R Resistance · Ω
A current of 0.50 A through 24 Ω produces 12 V.
Voltage as energy per charge
V = W / Q
V Voltage · V W Energy · J Q Charge · C
60 J transferred by 5 C corresponds to 12 V.
Terminal voltage of a real source
V_terminal = EMF − I × r
V_terminal Voltage at the terminals · V EMF Electromotive force · V I Current drawn · A r Internal resistance · Ω
A 12.6 V battery with 0.050 Ω internal resistance at 20 A gives 12.6 − 1.0 = 11.6 V.

Units of measurement

QuantitySymbolUnit
Voltage / potential difference V volt (V)
Electromotive force EMF volt (V)
Charge Q coulomb (C)
Energy W joule (J)

Worked examples

Worked example

Voltage across a resistor

Problem. A 24 Ω resistor carries 0.50 A. What is the voltage across it?

Solution. V = I × R = 0.50 A × 24 Ω = 12 V.

V = 12 V.
Worked example

Terminal voltage under load

Problem. A battery has an EMF of 12.6 V and an internal resistance of 0.050 Ω. What is its terminal voltage when it supplies 20 A?

Solution. Internal drop = I × r = 20 A × 0.050 Ω = 1.0 V. V_terminal = 12.6 V − 1.0 V = 11.6 V.

V_terminal = 11.6 V.

Practical applications

  • Automotive 12 V and 24 V systems
  • Mains distribution and appliance supply
  • Sensor and signal circuits
  • Battery and charging-system diagnostics

Automotive applications

A vehicle battery at rest typically shows an open-circuit voltage close to its nominal 12 V, and the charging system raises the voltage while the engine runs. Voltage-drop tests isolate high-resistance connections: measuring from the battery positive post to the load positive terminal while the load is on shows how much voltage is lost in the cable and connections, and the same test applies to the ground return path.

Industrial applications

Industrial distribution uses nominal voltages set by the installation standard in force, such as 230 V single-phase and 400 V three-phase in many European networks. Equipment ratings, insulation coordination, switching devices and protective devices are all selected for the system voltage and for the overvoltage category expected at that point of the installation.

Measurement procedure

  1. Connect the voltmeter in parallel across the two points; never connect a voltmeter in series with a load.
  2. Select the correct AC or DC mode and an appropriate range, starting high if the value is unknown.
  3. Use a meter and leads rated for the installation category and the voltage present.
  4. For voltage-drop tests, measure while the circuit is loaded; an unloaded measurement can hide a bad connection.

Common mistakes

  • Saying that voltage flows: voltage is a difference between points, while current is what flows.
  • Confusing EMF with terminal voltage: EMF is the ideal source value, terminal voltage falls as current rises.
  • Connecting a voltmeter in series: the high meter resistance almost stops the current and gives a meaningless reading.
  • Measuring resistance on a live circuit instead of voltage, which can damage the meter or give false readings.

Safety considerations

  • Respect the meter’s voltage and CAT rating; a meter that is not suitable for the installation can arc and injure the user.
  • Avoid touching the metal tips of the probes; use probes with finger guards and shrouded tips.
  • Verify the meter on a known source before and after testing a hazardous circuit.

Frequently asked questions

Is voltage the same as EMF?
EMF is the ideal voltage a source can provide; terminal voltage is what remains after the internal drop when current flows.
Why can a 12 V battery be dangerous?
A battery can supply very high current, and a short circuit can cause burns, fire or explosion. Voltage alone does not describe the hazard.
What does 0 V mean?
A reading of 0 V means no potential difference between the two points measured. It does not prove the conductor is safe or de-energised.
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