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Eddy Currents in Induction Heating

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The Role of Eddy Currents in Induction Heating

Eddy Currents in Induction Heating : Induction heating is a highly efficient method for heating conductive materials, widely used in industrial applications such as metal hardening, welding, brazing, and cooking. The primary mechanism driving induction heating is the generation of eddy currents, which produce localized heating within the material. This article explores the role of eddy currents in induction heating, their formation, governing equations, and industrial applications.

Formation of Eddy Currents

Eddy currents are circulating loops of electric current induced within a conductor when it is exposed to a changing magnetic field. These currents arise due to Faraday’s Law of Electromagnetic Induction, which states that a time-varying magnetic field induces an electromotive force (EMF) in a nearby conductor. Mathematically, the induced EMF ($\mathcal{E}$) is given by:

$$
\mathcal{E} = - \frac{d\Phi_B}{dt}
$$

where $\Phi_B$ is the magnetic flux through the conductor.

When an alternating current (AC) flows through an induction coil, it generates a changing magnetic field. This fluctuating field induces eddy currents within the conductive workpiece placed inside the coil. These circulating currents encounter electrical resistance in the material, which leads to Joule heating, given by:

$$
P = I^2 R
$$

where:

  • $P$ is the power dissipated as heat,
  • $I$ is the induced eddy current,
  • $R$ is the electrical resistance of the material.

Governing Equations

The intensity and distribution of eddy currents are governed by Maxwell’s Equations and the Lorentz force law. The key equations describing the behavior of eddy currents in induction heating are:

  1. Faraday's Law of Induction:
    $$
    \nabla \times \mathbf{E} = -\frac{\partial \mathbf{B}}{\partial t}
    $$
    This equation describes how a time-varying magnetic field induces an electric field.
  2. Ohm’s Law for Induced Currents:
    $$
    \mathbf{J} = \sigma \mathbf{E}
    $$
    where $\mathbf{J}$ is the induced current density, and $\sigma$ is the electrical conductivity of the material.
  3. Heat Generation by Joule Heating:
    $$
    q = \mathbf{J} \cdot \mathbf{E}
    $$
    where $q$ is the power density per unit volume.

These equations illustrate how an alternating magnetic field induces localized currents, which then generate heat within the material.

Skin Effect and Heating Efficiency

One critical phenomenon in induction heating is the skin effect, which refers to the tendency of eddy currents to concentrate near the surface of the conductor as the frequency of the applied AC increases. The penetration depth ($\delta$) of the eddy currents is given by:

$$
\delta = \sqrt{\frac{2}{\mu \sigma \omega}}
$$

where:

  • $\mu$ is the magnetic permeability,
  • $\sigma$ is the electrical conductivity,
  • $\omega$ is the angular frequency of the AC supply.

At high frequencies, the penetration depth decreases, meaning that most of the heat is generated near the surface of the material. This property is useful in surface-hardening applications, where only the outer layer of a workpiece needs to be heated and hardened.

Industrial Applications of Induction Heating

Eddy current-based induction heating is widely used in various industries due to its precise, rapid, and contactless heating capabilities. Some key applications include:

  1. Metal Hardening – Used in manufacturing processes to strengthen metal parts, such as gears and shafts.
  2. Brazing and Soldering – Provides controlled heat to join metal components efficiently.
  3. Melting and Forging – Utilized in metal casting industries for melting metals before shaping them.
  4. Cooking (Induction Stoves) – Induction cooktops use eddy currents to directly heat cookware, making them energy-efficient and safe.
  5. Magnetic Stirring and Sealing – Used in pharmaceutical and chemical industries for non-contact stirring and sealing of containers.

Advantages of Eddy Current Heating

The use of eddy currents in induction heating offers several advantages over conventional heating methods:

  • High Efficiency: Heat is generated within the material itself, reducing energy losses.
  • Rapid Heating: High-frequency eddy currents provide fast and localized heating.
  • Non-contact Process: Eliminates wear and contamination risks associated with direct heating methods.
  • Selective Heating: By adjusting the frequency, specific regions of a material can be heated while others remain unaffected.
  • Clean and Safe: No combustion or open flames, making it environmentally friendly and safer for operators.

An example simulation

Here I saw an interesting example that i tried to make myself to understand the phenomena. Basically, I have an isotropic magnet and a copper plate above it. And I have four probes that will measure the data on the copper plate.

A COMSOL simulation geometry

The above simulation is done with anisotropic magnet and. there is a copper plate above it with a gap and it is rotating. We are actually calculating the current density at 2 probe location.

The magnetic flux density of the magnet.
The electromagnetic force that is calculated due to the rotation of the magnet on the copper plate.

I hope you got some inspiration how you can actually dimension Device and check how to actually calculate electromagnetic force or current density due to combination of magnetic movement. The simulation is done using COMSOL Multiphysics® Software (official website HERE). There are some interesting blogs explaining the physics in there official website too.

Eddy currents play a fundamental role in induction heating, enabling efficient, precise, and localized heating for a wide range of industrial and domestic applications. By leveraging the principles of electromagnetic induction, industries can achieve energy-efficient heating solutions with superior control and reliability.

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