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Induction heating is a highly efficient and fast method that uses a magnetic field to heat conductive materials, such as metals and semiconductors, without contact. This method has become increasingly popular for industrial, medical, and domestic applications due to its many advantages over traditional heating techniques, such as resistance, flame, and ovens/furnaces. Induction heating is beneficial for highly precise or repetitive operations, where consistent heating and temperature control are critical for the quality and repeatability of the end product.
In induction heating, an alternating current (AC) source is used to supply current to an induction heating coil. As a result, the coil generates an alternating magnetic field. When an object is placed in this field, two heating effects occur:
Both effects result in the heating of the treated object, but the second one is most commonly the main heat source in IH processes. Moreover, hysteresis is not observed in non-magnetic materials, and magnetic materials lose their magnetic specificities if heated above a specific temperature (the so-called Curie point).
Eddy currents also depend on the magnetic field frequency due to the skin effect at high frequencies, the currents flow close to the conductor surface. This specificity is used to control the penetration depth of the induction heating process. As a result, either the whole object or only a specific part of it (only the surface, for example) can be heated. Thus, induction heating can be used for different applications from metal melting to brazing and surface hardening.
Skin effect is also observed inside the induction coil conductor. Therefore, pipes can be used instead of solid wires. When the current flows through the inductor, similar resistive losses are observed due to the Joule effect. In order to prevent the coil from melting and damage, water cooling is often applied.
Compared to some of the classic heating techniques (resistance heating, flame heating, furnaces, etc.), induction heating has the following advantages:
Although induction heating systems have already reached maturity as a technology, the development of modern technologies continuously provides options for new research trends and industrial interest. In the coming years, the following topics are expected to be of significant interest:
Induction heating was first discovered by Michael Faraday as he studied the induction of currents in wires by a magnet. The fundamental principles of induction heating were later established and developed by James C. Maxwell in his unified theory of electromagnetism. James P. Joule was the first to describe the heating effect of a current flowing through a conductive material.
In , Sebastian Z. de Ferranti proposed induction heating for metal melting and filed the first patent on the industrial applications of induction heating. The first fully-functional induction furnace was presented in by F. A. Kjellin, and the first high-frequency furnace application of induction heating was implemented by Edwin F. Northrup in .
During the Second World War and afterward, the use of induction heating technology was boosted by the aircraft and automotive industries. Induction heating was not only used for metal melting but also for advanced material treatment, which significantly increased the range of induction heating applications.
The development of solid-state generators using new power semiconductor technologies provided the potential for IH beyond the industrial environment. Since the late s, different domestic applications have appeared. In recent years, a particular interest in induction heating for medical treatments has emerged, as this method provides precise and targeted local heating.
Today, induction heating technology provides highly efficient and reliable systems for a wide variety of applications.
UltraFlex Power offers a free induction heating calculator to help you estimate your heating process parameters quickly.
The company is the world’s best electromagnetic induction heater supplier. We are your one-stop shop for all needs. Our staff are highly-specialized and will help you find the product you need.
References
Lucia, O., P. Maussion, E. J. Dede, J. Burdio, Induction Heating Technology and Its Applications: Past Developments, Current Technology, and Future Challenges, () IEEE Transactions on Industrial Electronics, vol. 61 ( 5), pp. -.
Tudbury, C. A., Basics of Induction Heating, vol. 1, J. F. Rider, May , New York, US.
Magnet, Wikipedia article
https://en.wikipedia.org/wiki/Magnet#Magnetic_metallic_elementsJoule heating, Wikipedia article
https://en.wikipedia.org/wiki/Joule_heatingCurie temperature, Wikipedia article
https://en.wikipedia.org/wiki/Curie_temperatureInduction heating is a process for heating metals and other electrically-conductive materials that is precise, repeatable and a safe non-contact method. It involves a complex combination of electromagnetic energy and heat transfer that passes through an induction coil, creating an electromagnetic field within the coil to metal down materials. Materials such as Steel, Copper, Brass, Graphite, Gold, Silver, Aluminum, and Carbide can be heated for a range of applications, which include various heat treating applications such as hardening, annealing, tempering, brazing, soldering, shrink fitting, heat staking, bonding, curing, melting and many more.
Two key phenomena must be learned to understand the fundamentals of induction heating; Faradays Law of Induction and Skin Effect.
Faradays Law of Induction
When an electrically conducting material (such as a metal) is placed within a time-varying magnetic field, an electric current (called an eddy current) is induced in the part producing a second magnetic field which opposes the applied field (figure below). The reason behind this phenomenon is that a time-varying magnetic field disturbs the relaxed environmental condition of the electrically conducting material. In return, the material tries to oppose this change by producing another magnetic field to cancel the imposed field.
The induction phenomenon has two important consequences:
i. Induced force. An example is shown in the figure below, where a permanent magnet is dropped into a copper tube. The induced force according to the Faradays law tries to stop the magnets motion inside the tube.
ii. Induced heat. When an electrically conductive material is exposed to an alternating magnetic field, depending on the material, heat is induced by two mechanisms; Joule Heating and Magnetic Hysteresis. The latter occurs in the magnetic metals (such as Carbon Steel below Curie temperature) in which the rotation of the adjacent magnetic dipoles due to the direction change of the imposed magnetic field will lead into friction and heat. This effect increases by increasing the frequency of the imposed magnetic field.
Joule Heating is the main heating effect caused by induction phenomenon. Any current I, ac or dc, passing through an electrically conducting material causes voltage drop V resulting in energy conversion to heat. Heat power is defined by V.I=R.I^2, where R is the electrical resistance of the current path. The resistance of the current path is inversely proportional to the cross-section area in which the current is flowing.
If an electrically conducting material is exposed to a magnetic field, eddy currents are induced in the material. Special characteristics of such currents result in a phenomenon which we call Induction Heating. The eddy currents are concentrated at the surface of the material. The reason is that at high frequency, the imposed magnetic field changes its direction very fast. Therefore, the induced currents in one direction do not have enough time to penetrate into the depth of the metal before their time is up. The thickness of the current penetration in the material is called Skin Depth. Skin depth depends on the electromagnetic properties of the material and also is inversely proportional to frequency. Figure below shows the dependence of the skin depth to frequency. Here, δ is the skin depth, ρ is the electrical resistivity, ω is the angular frequency and μ is the magnetic permeability.
Using high frequencies in induction heating industry (Mainly 10kHz to 700kHz) implies very thin penetration depths in metals (typically less than 1mm). Passing high current density (big I) through that shallow depth (big R) results in high R.I^2. Consequently, high energy conversion from electrical to heat occurs.
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Video credits: https://www.youtube.com/watch?v=5BeFoz3Ypo4
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