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Home » Eddy Currents (Foucault’s Currents)

Eddy Currents (Foucault’s Currents)

1851
  • Léon Foucault
Eddy current brake system in an industrial setting demonstrating electromagnetism applications.

(generated image for illustration only)

Eddy currents are loops of electrical current induced within bulk conductors by a changing magnetic field, in accordance with Faraday’s law. They flow in closed loops in planes perpendicular to the magnetic field. Following Lenz’s law, these currents create their own magnetic field that opposes the change in the external flux, causing a repulsive or drag force and resistive heating.

When a solid metallic conductor moves through a magnetic field or is exposed to a time-varying field, the free electrons within it experience a Lorentz force, causing them to circulate. These swirling currents are called eddy currents. Their magnitude is proportional to the magnetic field strength, the area of the loops, and the rate of flux change, and inversely proportional to the material’s resistivity. The power dissipated as heat (\(P = I^2R\)) can be substantial, an effect harnessed in induction heating.

In many applications, such as transformer and motor cores, eddy currents are undesirable as they represent a significant energy loss (core loss). To mitigate this, the cores are constructed from thin, laminated sheets of a ferromagnetic material like silicon steel, with each sheet electrically insulated from the next. This lamination breaks up the large conductive paths, forcing the eddy currents into much smaller, higher-resistance loops, thereby drastically reducing the energy lost to heat.

UNESCO Nomenclature: 2205
– Electricity and magnetism

Type

Physical Phenomenon

Disruption

Revolutionary

Usage

Widespread Use

Precursors

  • Faraday’s law of induction
  • Lenz’s law
  • Ohm’s law
  • Discovery of the Lorentz force

Applications

  • Eddy current brakes in trains and roller coasters
  • induction heating for furnaces and cooktops
  • metal detectors
  • non-destructive testing of materials
  • damping in mechanical gauges
  • proximity sensors

Patents:

NA

Potential Innovations Ideas

  • contactless viscosity measurement for industrial fluids
  • eddy current-based propulsion for small underwater vehicles
  • self-heating cookware with integrated eddy current patterns
  • magnetic levitation systems using controlled eddy current repulsion
  • non-invasive blood flow monitoring through induced currents
  • targeted hyperthermia cancer treatment using nanoparticles and eddy currents
  • active damping systems for precision machinery
  • eddy current-based systems for detecting counterfeit coins
  • material sorting systems that differentiate alloys based on conductivity
  • touchless, high-torque magnetic gears
Related to: Eddy currents, Foucault’s currents, induction heating, Eddy current brake, non-destructive testing, Lenz’s law, Faraday’s law, electromagnetism, resistive heating, Léon Foucault.

Historical Context

Chemist conducting experiments with catalysts in a vintage laboratory setting, 1850.

Catalyst on Chemical Equilibrium

A catalyst increases the rate of both the forward and reverse reactions equally by providing an alternative reaction pathway with a lower activation energy. While a catalyst allows a system to reach equilibrium much faster, it does not change the position of the equilibrium itself. The equilibrium concentrations of reactants and products, and the value of the equilibrium constant K, remain unchanged.
19th-century chemist measuring gas volumes illustrating the Ideal Gas Law in thermodynamics.

Ideal Gas Law (Molar Form)

The ideal gas law is the equation of state for a hypothetical ideal gas, approximating the behavior of many gases under various conditions. The molar form relates pressure (\(P\)), volume (\(V\)), amount of substance in moles (\(n\)), and absolute temperature (\(T\)) via the universal gas constant (\(R\)): \(PV = nRT\).
Laboratory apparatus for measuring vapor pressure and temperature in thermodynamics.

Clausius-Clapeyron Relation

The Clausius-Clapeyron relation describes the relationship between pressure and temperature for a substance at a phase transition, such as liquid and vapor. For water vapor, it shows that saturation vapor pressure increases exponentially with temperature. The approximate form is \(\frac{dp}{dT} = \frac{L}{T(V_v - V_l)} \approx \frac{L p}{R_v T^2}\), where L is latent heat.

Eddy Currents (Foucault’s Currents)

Thermodynamic laboratory with Peltier and Seebeck apparatus illustrating Kelvin relations.

Kelvin (Thomson) Relations

The Kelvin relations are two equations that thermodynamically link the three thermoelectric coefficients: the first relation connects the Peltier coefficient (\(\Pi\)) to the Seebeck coefficient (\(S\)) via absolute temperature (\(T\)): \(Pi = S \cdot T\). The second relates the Thomson coefficient (\(\mathcal{K}\)) to the temperature derivative of the Seebeck coefficient: \(\mathcal{K} = T \frac{dS}{dT}\).
Lead-acid battery with lead and lead dioxide electrodes in sulfuric acid electrolyte, electrochemistry.

Lead-Acid Battery

Lead-Acid battery type is the first rechargeable battery, invented by Gaston Planté in 1859. It operates using a lead (Pb) anode and a lead dioxide (PbO₂) cathode immersed in a sulfuric acid (H₂SO₄) electrolyte. During discharge, both electrodes convert to lead sulfate (PbSO₄), a process that is reversed during charging, allowing for energy storage and reuse.
Laboratory setup illustrating the Maxwell-Faraday Equation in electromagnetism.

Maxwell-Faraday Equation

This is the differential form of Faraday's law of induction, one of Maxwell's four equations. It states that a time-varying magnetic field (\(\mathbf{B}\)) always accompanies a spatially varying, non-conservative electric field (\(\mathbf{E}\)). The relationship is expressed as \(\nabla \times \mathbf{E} = -\frac{\partial \mathbf{B}}{\partial t}\). This equation governs how changing magnetic fields create electric fields at a specific point in space.
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Engineers designing an efficient heat engine in a laboratory, illustrating thermodynamics applications.

Second Law of Thermodynamics

The Second Law introduces the concept of entropy and defines the direction of spontaneous processes. It can be stated in several ways, but a key consequence is that the total entropy of an isolated system can never decrease over time. This law explains the 'arrow of time' and why processes are irreversible, such as heat spontaneously flowing from a hot body to a cold one.
Laboratory scene illustrating thermodynamic experiments on the Perfect Gas Model.

The Perfect Gas Model

A perfect gas is a theoretical model of a gas where intermolecular forces are neglected and specific heat capacities (\(C_P\) and \(C_V\)) are assumed to be constant with respect to temperature. This simplifies thermodynamic calculations significantly. It is a specific case of the ideal gas, where specific heats can vary with temperature, making it a more constrained model.
19th-century laboratory scene with Ludwig Boltzmann studying the Ideal Gas Law in statistical thermodynamics.

Ideal Gas Law (Statistical Form)

The statistical mechanics formulation of the ideal gas law expresses the relationship in terms of the microscopic properties of the gas. It relates pressure (\(P\)) and volume (\(V\)) to the total number of particles (\(N\)) and the absolute temperature (\(T\)) through the Boltzmann constant (\(k_B\)): \(PV = Nk_BT\).
Current-carrying conductor experiment demonstrating Thomson Effect in thermoelectricity.

Thomson Effect

The Thomson effect describes the heating or cooling of a current-carrying conductor when a temperature gradient exists along its length. Heat is produced or absorbed when current flows through a material with a temperature gradient. The rate of heat production per unit length is given by \(\frac{dQ}{dx} = -\mathcal{K} J \frac{dT}{dx}\), where \(\mathcal{K}\) is the Thomson coefficient.
Laboratory apparatus demonstrating the Joule-Thomson effect in thermodynamics.

Joule-Thomson Effect

The Joule-Thomson (or Joule-Kelvin) effect describes the temperature change of a real gas when it is forced through a valve or porous plug while kept insulated (an isenthalpic process). At a given pressure, a gas has an inversion temperature. If expanded below this temperature, it cools; if expanded above it, it heats up. This cooling effect is a cornerstone of modern refrigeration and liquefaction.
Lead-acid battery with lead anode and lead dioxide cathode in a historical lab setting.

Lead-Acid Battery Chemistry

The first commercially successful rechargeable battery. It uses a lead (Pb) anode, a lead dioxide (PbO₂) cathode, and a sulfuric acid (H₂SO₄) electrolyte. During discharge, both electrodes are converted into lead sulfate (PbSO₄), and the sulfuric acid is consumed. This process is chemically reversible by applying an external current, making it a practical and robust energy storage system.
Laboratory setup for measuring molar volume of gas in physical chemistry experiments.

Molar Volume of a Gas

A direct consequence of Avogadro's law is the concept of molar volume: one mole of any ideal gas at a specified temperature and pressure occupies a fixed volume. At Standard Temperature and Pressure (STP), defined as 273.15 K (0 °C) and 1 atm, this volume is approximately 22.4 liters. This principle simplifies stoichiometry by allowing direct conversion between gas volume and moles.
Laboratory scene focused on electric motor design utilizing Gauss's Law for Magnetism.

Gauss’s Law for Magnetism

One of the four Maxwell's equations, Gauss's law for magnetism states that the net magnetic flux out of any closed surface is zero. This is expressed mathematically as \(\oint_S \vec{B} \cdot d\vec{A} = 0\). This law is a statement of the experimental observation that magnetic monopoles (isolated north or south poles) have never been detected. Magnetic field lines always form closed loops.

(if date is unknown or not relevant, e.g. "fluid mechanics", a rounded estimation of its notable emergence is provided)

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