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Dielectric heating

Heating using radio waves

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Through Radio wave, Microwave and Electromagnetic radiation

In modern application two classes of dielectric heating are in use. Radio frequency heating or high-frequency heating refers to the use of HF and VHF frequencies (3–300 MHz). Microwave heating works at the higher microwave frequencies (0.3–300 GHz). Both (mainly) work via molecular dipole rotation within the dielectric induced by an oscillating electromagnetic field; the difference is that RF/HF heating involves the antenna near field, while MW largely occurs in the far field, leading to differences in effective range, penetration, and heating uniformity.

Mechanism

Dipole rotation

Molecular rotation occurs in materials containing polar molecules having an electrical dipole moment, with the consequence that they will align themselves in an electromagnetic field. If the field is oscillating, as in an electromagnetic wave or a rapidly oscillating electric field, these molecules rotate continuously by aligning with it. This is called dipole rotation or dipolar polarisation. As the field alternates, the molecules reverse direction. Rotating molecules push, pull, and collide with other molecules (through electrical forces), distributing the energy to adjacent molecules and atoms in the material. The process of energy transfer from the source to the sample is a form of radiative heating.

Temperature is related to the average kinetic energy (energy of motion) of the atoms or molecules in a material, so agitating the molecules in this way increases the temperature of the material. Thus, dipole rotation is a mechanism by which energy in the form of electromagnetic radiation can raise the temperature of an object. There are also many other mechanisms by which this conversion occurs.

Dipole rotation is the mechanism normally referred to as dielectric heating, and is most widely observable in the microwave oven where it operates most effectively on liquid water, and also, but much less so, on fats and sugars. This is because fats and sugar molecules are far less polar than water molecules, and thus less affected by the forces generated by the alternating electromagnetic fields. Outside of cooking, the effect can be used generally to heat solids, liquids, or gases, provided they contain some electric dipoles.

Frequency regimes

Dielectric heating involves the heating of electrically insulating materials by dielectric loss. A changing electric field across the material causes energy to be dissipated as the molecules attempt to line up with the continuously changing electric field. This changing electric field may be caused by an electromagnetic wave propagating in free space (as in a microwave oven), or it may be caused by a rapidly alternating electric field inside a capacitor. In the latter case, there is no freely propagating electromagnetic wave, and the changing electric field may be seen as analogous to the electric component of an antenna near field. In this case, although the heating is accomplished by changing the electric field inside the capacitive cavity at radio-frequency (RF) frequencies, no actual radio waves are generated or absorbed. In this sense, the effect is the direct electrical analog of magnetic induction heating, which is also near-field effect (thus not involving radio waves).

As mentioned above, practical dielectric heating runs in two ranges: HF/VHF, most commonly in the range of and microwave.

Near-field

RF heating generally uses 10–100 MHz. This kind of heating, as a near-field effect, requires a distance from electromagnetic radiator to absorber of less than ⁠𝜆/2π⁠ ≈ ⁠𝜆/6⁠ of a wavelength. It is thus a contact process or near-contact process, since it usually sandwiches the material to be heated (usually a non-metal) between metal plates taking the place of the dielectric in what is effectively a very large capacitor. However, actual electrical contact is not necessary for heating a dielectric inside a capacitor, as the electric fields that form inside a capacitor subjected to a voltage do not require electrical contact of the capacitor plates with the (non-conducting) dielectric material between the plates. Because lower frequency electrical fields penetrate non-conductive materials far more deeply than microwaves do, heating pockets of water and organisms deep inside dry materials like wood, it can be used to rapidly heat and prepare many non-electrically conducting food and agricultural items, so long as they fit between the capacitor plates.

Far field

At higher frequencies, the wavelength of the electromagnetic field becomes shorter than the distance between the metal walls of the heating cavity or than the dimensions of the walls themselves. This is the case inside a microwave oven. In such cases, conventional far-field electromagnetic waves form (the cavity no longer acts as a pure capacitor, but rather as an antenna), and are absorbed to cause heating. The dipole-rotation mechanism of heat deposition remains the same.

Ion drag

The lower end of HF (3–15 MHz) displays a special heating effect on conductive liquids. This is due to an additional mechanism caused ion-drag causes heating, where charged ions are slowly "dragged" back and forth in the liquid under influence of the electric field, striking liquid molecules in the process and transferring kinetic energy to them, which is eventually translated into molecular vibrations and thus into thermal energy. Higher frequencies vary too quickly for meaningful levels of this effect.

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