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Induction welding
Induction welding
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Induction welding is a form of welding that uses electromagnetic induction to heat the workpiece. The welding apparatus contains an induction coil that is energised with a radio-frequency electric current. This generates a high-frequency electromagnetic field that acts on either an electrically conductive or a ferromagnetic workpiece. In an electrically conductive workpiece, the main heating effect is resistive heating, which is due to induced currents called eddy currents. In a ferromagnetic workpiece, the heating is caused mainly by hysteresis, as the electromagnetic field repeatedly distorts the magnetic domains of the ferromagnetic material. In practice, most materials undergo a combination of these two effects.

Nonmagnetic materials and electrical insulators such as plastics can be induction-welded by implanting them with metallic or ferromagnetic compounds, called susceptors, that absorb the electromagnetic energy from the induction coil, become hot, and lose their heat to the surrounding material by thermal conduction.[1] Plastic can also be induction welded by embedding the plastic with electrically conductive fibers like metals or carbon fiber. Induced eddy currents resistively heat the embedded fibers which lose their heat to the surrounding plastic by conduction. Induction welding of carbon fiber reinforced plastics is commonly used in the aerospace industry.

Induction welding is used for long production runs and is a highly automated process, usually used for welding the seams of pipes. It can be a very fast process, as a lot of power can be transferred to a localised area, so the faying surfaces melt very quickly and can be pressed together to form a continuous rolling weld.

The depth that the currents, and therefore heating, penetrates from the surface is inversely proportional to the square root of the frequency. The temperature of the metals being welded and their composition will also affect the penetration depth. This process is very similar to resistance welding, except that in the case of resistance welding the current is delivered using contacts to the workpiece instead of using induction.

Induction welding was first discovered by Michael Faraday. The basics of induction welding explain that the magnetic field's direction is dependent on the direction of current flow. and the field's direction will change at the same rate as the current's frequency. For example, a 120 Hz AC current will cause the field to change directions 120 times a second. This concept is known as Faraday's Law.

When induction welding takes place, the work pieces heat up to under the melting temperature and the edges of the pieces are placed together impurities get forced out to give a solid forge weld.[2]

Induction welding is used for joining a multitude of thermoplastics and thermosetting matrix composites. The apparatus used for induction welding processes includes a radio frequency power generator, a heating station, the work piece material, and a cooling system.

The power generator comes in either the form of solid state or vacuum tube and is used to provide an alternating current of 230-340 V or a frequency of 50–60 Hz to the system. This value is determined by what induction coil is used with the piece.

The heat station utilizes a capacitor and a coil to heat the work pieces. The capacitor matches the power generators output and the induction coil transfers energy to the piece. When welding the coil needs to be close to the work piece to maximize the energy transfer and the work piece used during induction welding is an important key component of optimal efficiency.[3]

Some equations to consider for induction welding include:

Thermal calculation:

Where: is thermal mass

is resistivity

is efficiency

is surface density

Newton Cooling Equation:

Where: is heat flux density

h is the heat transfer coefficient

is the temperature of the work piece surface

is the temperature of the surrounding air[4]

See also

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References

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from Grokipedia
Induction welding is a process that uses to generate heat for joining materials, primarily metals in a solid-state manner and thermoplastics via implant fusion. For metals, it produces coalescence using heat from the resistance of the workpieces to induced high-frequency , typically without filler material or of the base metals. In metallic induction welding, a subset of high-frequency welding, an surrounding the workpiece generates eddy currents that cause rapid resistive heating in conductive materials like or aluminum at the interface. The process often involves feeding a flat metal strip—such as low-carbon or aluminum alloys—through forming rolls to create an open-seam tube, heating the abutting edges to (around 1000–1200°C for ), and applying with forging rolls to upset and bond the surfaces, forming a seamless longitudinal weld. Key parameters include current frequency (200–450 kHz for optimal and heating efficiency), line speed (up to 100 m/min), power input (50–500 kW depending on tube size), and impeder materials inside the tube to concentrate heating and prevent circumferential currents. Originating from early patents in the late and evolving with high-frequency generators in the for tube production, induction welding gained prominence in the post-World War II era for its potential, replacing slower furnace methods. Today, metallic induction welding is the dominant method for manufacturing welded steel tubes and pipes, with applications in oil and gas pipelines, automotive structural components (such as bumpers, subframes, and hydroformed parts), HVAC radiator tubing, and construction . variants use embedded susceptors for localized heating in applications like medical devices and automotive parts. Notable advantages for metallic welding include high production rates, a narrow heat-affected zone (typically 1–2 mm) that minimizes metallurgical degradation and distortion, and welds exhibiting higher hardness and strength than the base metal due to dynamic recrystallization during —often enabling post-weld forming without softening. The process supports a wide range of thicknesses (0.5–20 mm) and materials, though challenges like edge preparation and oxide expulsion require precise control to avoid defects such as lack of fusion or inclusions.

Fundamentals

Definition and overview

Induction welding is a non-contact welding process that employs to generate heat within the workpiece or an inserted implant, enabling the coalescence of materials without the use of flames, arcs, or direct physical contact between the heat source and the joint. This method relies on passed through an to create a rapidly changing , which induces heating through mechanisms such as eddy currents in conductive materials. The process is particularly valued for its precision, cleanliness, and ability to produce strong, consistent welds in both automated and high-volume production environments. The technique encompasses two primary categories: metallic induction welding and thermoplastic implant induction welding. In metallic induction welding, applicable to electrically conductive metals like , aluminum, and alloys, heat is generated directly within the base material near the interface, often using high-frequency currents to form continuous seams in applications such as pipe and tube . Conversely, thermoplastic induction welding targets non-conductive polymers and composites, where a susceptor —typically metal , fibers, or particles embedded at the —absorbs the induced to melt the surrounding matrix material, facilitating fusion under applied . This categorization allows induction welding to address diverse material classes, from metals to engineering plastics like and . Key characteristics of induction welding include its high-speed capability, with welding rates reaching up to several hundred meters per minute for thin-walled steel pipes, making it ideal for lines. It excels in creating uniform, hermetic seams without fillers, leveraging frequencies (typically 10-450 kHz) to induce currents for resistive heating in conductors or hysteresis losses in ferromagnetic susceptors. The process demands materials that are electrically conductive for direct heating or augmented with susceptors for non-conductive substrates, ensuring efficient energy transfer and minimizing distortion. These attributes contribute to its automation potential and suitability for industries requiring rapid, repeatable joins, such as automotive and manufacturing.

Physical principles

Induction welding operates on the principle of , where a time-varying induces an (EMF) in a nearby conductor, as described by . This law states that the magnitude of the induced EMF ϵ\epsilon is equal to the negative rate of change of ΦB\Phi_B through the conductor: ϵ=dΦBdt.\epsilon = -\frac{d\Phi_B}{dt}. Here, ΦB=BdA\Phi_B = \int \mathbf{B} \cdot d\mathbf{A} represents the , with B\mathbf{B} as the and dAd\mathbf{A} as the differential area element. In practice, an (AC) flowing through an generates an oscillating that links with the workpiece, inducing voltages that drive currents within it. This fundamental mechanism enables non-contact heating essential for welding both metals and thermoplastics. Heat generation in induction welding arises primarily from two mechanisms in conductive materials: eddy currents and, for ferromagnetics, hysteresis losses. Eddy currents are circulating loops of induced current within the conductor that encounter electrical resistance, leading to proportional to I2RI^2 R, where II is the current and RR is the resistance. These currents are confined near the surface due to the skin effect but effectively raise the temperature of metallic workpieces to forging temperatures required for solid-state bonding. In ferromagnetic materials, such as iron or , additional heating occurs through losses, where energy is dissipated as the magnetic domains repeatedly magnetize and demagnetize in response to the alternating field, with loss magnitude depending on the material's and the field's amplitude. For thermoplastic welding, non-conductive polymers incorporate a susceptor—a thin, conductive implant like metal mesh or particles—where induced eddy currents generate localized at the joint interface, melting the surrounding without broadly affecting the bulk material. The frequency of the AC supply plays a critical role in controlling the depth and efficiency of heating through the skin effect, which limits current penetration. Typical frequencies for induction welding range from 10 kHz to 450 kHz, allowing precise adjustment for material thickness and desired heat zone. The skin depth δ\delta, defined as the distance over which current density falls to 1/e1/e of its surface value, is given by δ=2ωμσ,\delta = \sqrt{\frac{2}{\omega \mu \sigma}},
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