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Thermal Food Processing

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Radio Frequency Dielectric Heating 471<br />

TABLE 15.1<br />

Electromagnetic-Based Heating Methods<br />

Heating Method Key Parameter Frequency Range<br />

Ohmic<br />

(Lower f)<br />

(Electric field)<br />

Capacitive dielectric<br />

(Medium f )<br />

(Electric field)<br />

Radiative dielectric<br />

(Higher f )<br />

(Electric field)<br />

Inductive–ohmic<br />

combination<br />

(Lower f )<br />

(Magnetic field)<br />

Inductive<br />

(Medium f )<br />

(Magnetic field)<br />

Radiative magnetic<br />

(Higher f )<br />

(Magnetic field)<br />

Common<br />

Frequencies<br />

s, E > sample<br />

size<br />

f, e′′, E 100 MHz < f < 100<br />

GHz or wavelength <<br />

sample size<br />

Hysteresis losses<br />

ƒ(B-H curves, f)<br />

and eddy current<br />

losses ƒ(H, s)<br />

f, m′′, H 1 MHz < f < 100 MHz<br />

or wavelength >><br />

sample size<br />

f, m′′, H 100 MHz < f < 100<br />

GHz or wavelength <<br />

sample size<br />

10 MHz, 27 MHz,<br />

39 MHz, and others<br />

915 MHz, 2.45 GHz,<br />

5.8 GHz, 24.124<br />

GHz, and others<br />

50 Hz < f < 1 MHz 50 Hz, 60 Hz,<br />

1–50 kHz, 450 kHz,<br />

and others<br />

50 MHz and others<br />

915 MHz, 2.45 GHz,<br />

5.8 GHz, 24.124<br />

GHz, and others<br />

Note: s = Electrical conductivity (S/m); E = RMS electric field intensity (V/m); e′′ = electric<br />

permittivity (F/m); H = RMS magnetic field intensity (A/m); m′′ = magnetic permeability (H/m);<br />

B = magnetic flux density (W/m ; f = electric field frequency (Hz).<br />

2 )<br />

Source: from Zhao, Y. et al., J. <strong>Food</strong> Process. Eng., 23, 25–55, 2000. With permission.<br />

The frequency at which lattice limitations occur is called the Debye resonance. It<br />

is the frequency at which maximum energy can be imparted to a medium for a<br />

given electric field strength. Other higher-frequency limitations include the reduction<br />

of field penetration into a medium as frequency is increased in the presence<br />

of high electrical conductivity and high dielectric loss components. A typical existing<br />

design for a dielectric heating system is shown in Figure 15.2.<br />

RF dielectric heating differs from higher-frequency electromagnetic radiative<br />

dielectric heating (e.g., microwave ovens). With RF heating, the wavelength of<br />

the chosen frequency is large compared to the dimensions of the sample being<br />

heated. With electromagnetic radiative heating, the wavelength is comparable to

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