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Joule's laws: electrical heating and the thermodynamics of ideal gases

Two laws formulated by James Prescott Joule: the electrical heating law (Q = I²Rt) and the thermodynamic result that an ideal gas's internal energy depends only on temperature; uses, limits, and history.

Author: Leandro Alegsa Creation date: November 13, 2022 Last updated: June 3, 2026

en.wikipedia.org · CC BY 2.5

Joule's laws refer to two distinct but historically connected results in physics, both associated with James Prescott Joule. The first describes how electrical heat is produced by a current; the second concerns the dependence of the internal energy of an ideal gas on its thermodynamic state. Together they link electrical phenomena and thermal behavior, and they played a key role in establishing the modern concept of energy.

Q=I^{2}\cdot R\cdot t

Joule's first law (electrical heating)

Often called the Joule–Lenz law, the first law quantifies the thermal energy generated by an electrical conductor carrying a steady electric current. In its usual form it gives the heat Q produced over time t as Q = I²·R·t, where I is current and R is resistance. Equivalently, the instantaneous power dissipated as heat is P = I²R, which can also be written P = VI = V²/R using Ohm's law (V = IR). This relation applies when resistance and current are well defined and heating is due to resistive (ohmic) dissipation.

Applications and practical considerations

Resistive heating elements (space heaters, toasters) rely directly on the I²R effect.
Electrical safety devices such as fuses exploit rapid heating from excessive current.
Power losses in transmission lines are commonly estimated with the I²R formula.

Limitations: the law assumes ohmic behavior and uniform current; for non-linear materials, high frequencies (skin effect), superconductors, or chemical energy conversion the simple form does not capture all effects. In alternating-current circuits the time-averaged power formula is used instead.

Joule's second law (ideal-gas internal energy)

Joule's second law states that the internal energy of an ideal gas depends only on its temperature, not on its pressure or volume. In practical terms, for an ideal monoatomic gas U = n·C_v·T (up to an additive constant), so any isothermal change in pressure or volume that does not change temperature leaves U unchanged. This result follows from the kinetic theory: in an ideal gas, internal energy is the sum of molecular kinetic energies, which depend solely on temperature.

Experiments such as the free expansion (Joule expansion) provided empirical support: when an ideal gas expands into a vacuum without doing work, its temperature remains essentially constant. Real gases deviate from this behavior because of intermolecular forces and finite molecular size; those deviations under throttling are measured by the Joule–Thomson coefficient, which can cause cooling or heating depending on conditions.

Historical significance and distinctions

Both laws originate with mid-19th century work by James Prescott Joule, whose careful measurements of mechanical work and heat helped establish conservation of energy and the concept of equivalence between heat and work. The electrical law is often associated with Heinrich Lenz (hence Joule–Lenz), while the gas law is a cornerstone of classical thermodynamics and kinetic theory. It is important to distinguish Joule's second law (internal energy of an ideal gas depends only on temperature) from the Joule–Thomson effect, which describes temperature change during throttling, and from more general statements about energy and energy transfer in thermodynamic processes.

For further reading on related topics see discussions of pressure (pressure), volume, and the behavior of non-ideal gases under real conditions. The two Joule laws remain fundamental: one governing how electrical currents produce heat, the other clarifying the thermal state variables that determine the microscopic energy content of ideal gases.

Heat of current in an electric line

Preferably, a current is conducted in an electrical line. In connection with heat generation, the electrical power is always an active power. It results from the existing current and the electrical voltage dropping along the conductor as a result of the conductor current (the formula symbols apply to direct variables as well as to the effective values of alternating variables).

$P=U\cdot I$

Since the voltage is due to the ohmic resistance of the conductor, ohm's law applies

$U=R\cdot I$

Thus, the heating (e.g. in an electric line, a transformer or a heating resistor) increases with the square of the current strength

$Q_{\mathrm {W} }=I^{2}\cdot R\cdot t={\frac {U^{2}}{R}}\cdot t\;.$

If the generation of the heat is desired, the heat is called electric heat, otherwise it is called current heat loss or ohmic loss.

The heat energy primarily leads to a heating of the conductor by a temperature difference of

$\Delta \vartheta ={\frac {Q_{\mathrm {W} }}{C_{\vartheta }}}$

with the heat capacity $C_{\vartheta }$ . At constant power, $Q_{\mathrm {W} }$ increases linearly with time. Thus, the temperature also increases linearly with time until another process is superimposed.

As the conductor becomes warmer than its surroundings, it transfers heat energy by conduction, radiation or convection. If the energy supply is continuously uniform, a state of equilibrium is established at an elevated temperature in which the heat flux given off ${\dot {Q}}_{W}$ (heat per time period, i.e., a thermal power) equals the absorbed electrical power:

${\dot {Q}}_{\mathrm {W} }={\frac {\Delta Q_{\mathrm {W} }}{\Delta t}}=P\,.$

With a surface involved in the heat transport and a heat transfer coefficient α a temperature difference arises $\alpha$

$\Delta \vartheta ={\frac {P}{\alpha \,A}}\,.$

In general, bodies have such a thermal inertia that the temperature difference is a constant at stationary current, even when heated by alternating current. Only in the case of a very small ratio of mass to surface, as in the case of the double helix shown, can a temperature or brightness fluctuation with twice the frequency of the alternating current be observed by metrological means.

Double helix heated to red heat as a result of a current flow

Heat of current in electric flow field

If a current flows through a conductive substance distributed over a larger volume, then $\mathrm {d} A$ a current of the strength

$\mathrm {d} I=J\;\mathrm {d} A$ ,

on whose path along a path element $\mathrm {d} s$ a voltage

$\mathrm {d} U=E\;\mathrm {d} s=\rho \,J\mathrm {d} s$

drops off, generating heat. In it, stands for the electric current density, for the electric field strength, for $E=\rho \;J$ Ohm's law, ρ $\rho$ for the specific electric resistance (reciprocal of the electric conductivity σ $\sigma$ ).

The loss of electric power results in the volume element $\mathrm {d} V=\mathrm {d} A\cdot \mathrm {d} s$ to

$\mathrm {d} P=\mathrm {d} U\cdot \mathrm {d} I=\rho \;J^{2}\mathrm {d} V$ .

Metallic conductors exhibit electrical resistivity that is largely independent of current (but temperature dependent). In semiconductors, ρ is $\rho$ not constant. In superconductors, ρ $\rho =0$ , no heat of current is generated there.

The total current heat loss in a current-carrying conductor is generally calculated from the volume integral

$P=\iiint _{V}\rho \ J^{2}\mathrm {d} V$ .

If ρ is $\rho$ constant, this factor can be pulled in front of the integral. In a homogeneous conductor, such as a long wire traversed by a direct current, the current distribution is independent of location, so that for such an object traversed by an integral current the power dissipation can be reduced to the macroscopic formula given above

$P=R\;I^{2}$

leads. In the case of more complicated geometric design with non-uniform current distribution, this must be calculated, e.g. using the finite element method, in order to be able to determine the power loss and the macroscopic resistance of the conductor.

In materials with non-constant resistivity, a current-dependent resistance can be R(I) found. The calculation of the current heat loss by $P=R(I)\cdot I^{2}$ is then valid this way.

Questions and Answers

Q: What are Joule's laws?

A: Joule's laws are two physical laws that describe the relation between heat generated by an electric current and how the energy of a gas relates to pressure and volume.

Q: What is Joule's first law?

A: Joule's first law shows the relation between heat generated by an electric current flowing through a conductor. It is shown as Q = I2Rt, where Q is the amount of heat, I is the electric current flowing through a conductor, R is the amount of electric resistance present in the conductor, and t is the amount of time that this happens for.

Q: What does Joule's second law say?

A: Joule's second law says that the internal energy of an ideal gas does not change if volume and pressure change, but does change if temperature changes.

Q: Who was James Prescott Joule?

A: James Prescott Joule was a physicist who developed both of these laws related to thermodynamics. His work on these two laws led to his name being associated with them.

Q: Why is it important to know about Joule's laws?

A: Knowing about Joule's laws helps us understand how energy works in different systems such as electrical circuits or gases under different conditions such as pressure or temperature changes. This understanding can help us design better systems for generating or using energy more efficiently.

Q: How can we calculate heat produced by an electric current according to Joules' first law?

A: According to Joulse' first law, we can calculate heat produced by an electric current using this equation - Q = I2Rt , where Q is the amount of heat, I is the electric current flowing through a conductor, R is the amount of electric resistance present in the conductor, and t is the amount of time that this happens for.

Author

AlegsaOnline.com - Joule's laws - Leandro Alegsa

Creation date: November 13, 2022
Last updated: June 3, 2026

URL: https://en.alegsaonline.com/art/51289