Heating of foods in a microwave oven differs significantly from heating foods in a conventional oven. In a conventional oven, heat energy is applied to the exterior surface of the food and moves inward until the food is cooked. Thus, food cooked conventionally is typically hot on the outer surfaces and warm in the center.

Microwave cooking, on the other hand, involves absorption, by the food, of microwaves which characteristically penetrate far deeper into the food than does infrared (heat) . Also, in microwave cooking, the air temperature in the microwave oven may be relatively low. Therefore, it is not uncommon for food cooked in a microwave oven to be cool on the surfaces and much hotter in the center. This makes it difficult to brown food and make it crisp. Therefore, it is difficult to make some food cooked in a microwave oven aesthetically pleasing.

In order to facilitate browning and crisping of food in a microwave oven, devices known as susceptors have been developed. Susceptors are devices which, when exposed to microwave energy, become very hot. By placing a susceptor next to a food product in a microwave oven, the surface of the food product exposed to the susceptor is surface heated by the susceptor and thereby becomes crisp and brown.

Many conventional susceptor structures have included a thin metal film, typically 60 - IOOA of Aluminum, deposited on a substrate such as polyester. The metalized layer of polyester is typically bonded,

for support, to a support member such as a sheet of paper board or corrugated paper.

Conventional susceptors have certain drawbacks. They undergo a process called breakup in which the electrical continuity of the thin metal film is lost during cooking. This is described in more detail in the Wendt et al U.S. Patent No. 4,927,991. The result of the loss of electrical continuity is an irreversible loss in the susceptor's microwave responsiveness and a lower level of percent power absorption in the susceptor during cooking. Lower power absorption leads to lower susceptor cooking temperatures and a corresponding decrease in the susceptor's ability to crisp food.

In order to further discuss the relevance of this deterioration, some other relationships should be set forth. The complex dielectric constant ε of a material is defined as follows:

ε = ε ₀ ε _r = ε ₀ (ε _r ' - j ε _r ") Eq. 1

where ε ₀ is the permitivity of free space, 8.854 x lO ^~1 Farads/cm; ε _r is the complex relative dielectric constant of the susceptor, relative to free space; ε _r ' is the real part of the complex relative dielectric constant ε _r ; and ε _r " is the imaginary part of the complex relative dielectric constant ε _r . ε _r ' ^# is also known as the loss factor for the material.

As an example of conventional susceptor operation, a frozen food product could be placed on a susceptor. The susceptor and the food product could

then be subjected*to microwave energy. Since ε _r ' ' (the imaginary part of the complex relative dielectric constant) of ice is very low, the frozen food product is initially a poor absorber of microwave energy. Therefore, the susceptor absorbs an excessive amount of the microwave energy and begins to deteriorate. Meanwhile, the frozen food product absorbs very little energy. This is undesirable. As the frozen food product thaws and starts absorbing microwave energy, the ability of the susceptor to absorb energy, and thereby surface heat the frozen food product, has already been deteriorated. Since this deterioration (i.e., the change in the electrical continuity of the susceptor) is generally irreversible, the susceptor is incapable of properly browning and crisping the food product.

In addition, as the susceptor deteriorates, it heats in a non-uniform fashion resulting in hot spots distributed along the surface of the susceptor. This results in uneven surface heating of the food products. Further, as the susceptor deteriorates and the microwave transmissiveness of the susceptor increases, the food product may be subjected to an undesirable amount of dielectric heating. This can cause the food product to become tough or to attain other similarly unappealing qualities.

Therefore, there is a continuing need for the development of susceptor structures which are not plagued by the problems of thin metallic film-type susceptor structures.

SUMMARY OF THE INVENTION The present invention is a microwave susceptor structure having a thick metal layer and a matching layer coupled to the thick metal layer. The matching

layer couples a desired amount of power into the thick metal layer.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a drawing of the susceptor structure of the present invention.

FIG. 2 is a graph showing percent power absorbed plotted against dielectric thickness for dielectric material and metal of the susceptor shown in FIG. 1.

FIG. 3A shows a three dimensional plot of percent power absorbed by a first embodiment of a susceptor of the present invention.

FIG. 3B shows a three dimensional plot of percent power absorbed by a second embodiment of a susceptor of the present invention.

FIG. 4 is a graph showing percent power absorbed plotted against dielectric thickness.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

FIG. 1 shows a susceptor 20 of the present invention. The susceptor 20 includes an electrically thick (greater than approximately 3 skin depths thick) metal layer 22 and an impedance matching dielectric layer 24. The metal layer 22 is typically bonded to layer 24 such that food, when placed on the thick metal layer 22, is isolated from any chemicals or other materials in layer 24.

Until now, it has generally been thought that thick metals would not make good susceptor structures since they have high electrical conductivity. Indeed, the thick metal portion 22 of the invented susceptor 20 will not heat significantly without the impedance matching dielectric layer 24.

In the present invention, the interaction of the susceptor with the microwaves provided by the microwave oven is viewed as a transverse electromagnetic (TEM) plane wave which propagates within the microwave oven. Hence, by choosing the proper dielectric layer 24, a desired amount of power can be coupled into thick metal layer 22. In other words, dielectric layer 24 is used as a matching layer for matching the wave impedance of the plane wave, as defined by the medium of transmission, generated by the microwave oven to that of the thick metal layer 22. By "matching", it is meant that the overall reflection coefficient of the dielectric and thick metal composite is reduced or eliminated and the power absorbed by the thick metal layer 22 is increased.

The wave impedance (Z) of the microwave is related to the characteristics of the wave front and the medium of transmission by the following relationship: ' Eq. 2

Z- ε

Where the medium of transmission is air, the wave impedance (Z ₀ ) is substantially represented as:

Eq. 3

Zo - -J-L -377Ω

N ^ε o

By matching the impedance of the thick metal layer 22 with the wave impedance of the microwaves in the microwave oven, a desired amount of power is coupled

into the thick metal layer 22 and absorbed by susceptor 20. Thus, thick metal layer 22 heats when exposed to microwave energy.

To couple a maximum amount of power into the thick metal layer 22, quarter wave matching is used. In other words, for maximizing power transfer,

Eq. 4

^Z match " y ^O^ metal

where Z _match is the impedance of dielectric layer 24; Z ₀ is the characteristic impedance of free space, and ^z m _et ai i ^{s the} impedance of the thick metal layer 22. The thickness (d) of dielectric layer 22 is chosen as

Eq. 5 j _m match

where λ _match is the wavelength of the microwave in the matching layer 24. Thus, by choosing a dielectric layer 24 which has an appropriate relative dielectric constant e _r and an appropriate thickness (d) , the amount of power coupled into a metal layer 22 having a given electrical conductivity (σ) can be maximized.

It has been seen that, when metal layer 22 is formed of a thick metal such as aluminum foil, and when dielectric layer 24 is formed of a high dielectric material (e.g. a commercially available metal loaded

polymer similar to that disclosed in EPO Publication No. 242,952 to E.I. DuPont De Nemours & Co.) the amount of power absorbed during microwave heating is related to the thickness of the dielectric layer 24 as shown in FIG. 2. FIG. 2 shows a graph calculated from a computer model of the thickness of the dielectric material 24 plotted against the calculated percent absorbed power by susceptor 20 during microwave heating. FIG. 2 shows that a great percentage of the system power can be absorbed by susceptor 20 if metal layer 22 and dielectric layer 24 are chosen properly.

Computer simulations have been run in which the thickness of the dielectric layer 24 and the complex dielectric constant of the dielectric layer 24 were systematically varied. For example, in one case, the thickness of the dielectric layer 24 was varied from approximately 0.16 cm to 0.006 cm in approximately 50 steps. In addition, the complex relative dielectric constant of dielectric layer 24 was varied from 500-jo to 2000-jo in approximately 50 steps. It was assumed that metal layer 22 was aluminum with an electrical conductivity of 3.5 x 10 ⁵ / ohm cm. The maximum system power absorbed was 28.4%. A three dimensional plot of the percent power absorbed by susceptor 20 plotted against the dielectric thickness and the complex relative dielectric constant of dielectric layer 24 used in the computer simulations is shown in FIG. 3A.

Surprisingly, it has also been shown that, where the metal layer 22 is a poor conductor, more microwave power is absorbed by susceptor 20 than if the metal layer is a good conductor. For example, another computer simulation was run using a dielectric material having a complex relative dielectric constant varying

from 500-jO to 2000-jO in approximately 50 steps. In addition, the simulation included metal layer 22 comprising Nichrome, having an electrical conductivity of 10 /ohm cm. A three dimensional plot showing the percent power absorbed by susceptor 20 using Nichrome plotted against the dielectric thickness and the complex relative dielectric constant of dielectric layer 24 is shown in FIG. 3B. The maximum power absorbed by susceptor 20 in this second case was 91.8%.

Thus, by choosing the dielectric layer 24 with an appropriate thickness and complex relative dielectric constant so that the impedance of the thick metal layer 22 is sufficiently matched to the wave impedance of the microwave generated by the microwave oven, substantially any desired amount of power can be coupled into the thick metal layer 22. By using this impedance matching technique, the thick metal is heated and operates properly as a susceptor in a microwave oven.

It is worth noting that microwaves generated in microwave ovens may typically have a frequency of approximately 2,450 megahertz. Therefore, the desired amount of power can be coupled into the thick metal layer 22 by carefully choosing the impedance of susceptor 20 to match (or match sufficiently to couple the desired amount of power) , the wave impedance of a microwave (typically modeled as a plane wave) at a frequency of 2,450 megahertz to the impedance of the thick metal layer 22.

Also, although the value of the dielectric loss factor, ε _r ", of the dielectric layer 24 is not critical, it should generally be as small as possible. If ε _r " of the dielectric layer 24 is too large, the

dielectric layer 24 may heat excessively and, in certain cases, deteriorate.

It has also been noted that, in using susceptor structure 20 of the present invention, a certain amount of temperature control is possible. FIG. 4 shows a graph of dielectric thickness of dielectric layer 24 plotted against percent power absorption by susceptor 20. A dielectric material is chosen where the dielectric constant is temperature dependent. For example, as shown in FIG. 4, at a dielectric thickness of 0.092 cm, the real portion of the complex relative dielectric constant is 1000 when little or no microwave energy has been absorbed by susceptor 20 (i.e., when susceptor 20 is cold) . At that point, the percent absorption capability of susceptor 20 is 40%. However, as susceptor 20 absorbs microwave energy and heats, the dielectric constant drops to 800 and the percent of system power absorbed by susceptor 20 is reduced to approximately 5%.

In other words, FIG. 4 shows two graphs where the dielectric constant shifts as the dielectric layer 24 heats. Initially, dielectric layer 24 heats very rapidly (40% absorption) and when it reaches a given temperature, its percent absorption drops to approximately 5% (the heater turns off) . Thus, by using a proper dielectric material, one with a temperature dependent relative dielectric constant, temperature control can be achieved.

In one preferred embodiment, the high dielectric material layer 24 is Barium Titanate or Calcium Titanate. In another preferred embodiment, it is a metal flake artificial dielectric or any other high e material.

CONCLUSION

By using the susceptor structure of susceptor 20, a surface heating susceptor can be achieved which cooks, in essence, like a frying pan. The heating is accomplished by currents within the metal layer 22, and metal layer 22 is highly arc resistent.

Also, the metal layer 22 electrically isolates the food from the dielectric layer 24. Thus, the electric field standing wave pattern inside the food remains relatively constant, unaffected by changes in the susceptor 20. The isolation provided by metal layer 22 also prevents contamination of the food product by any chemicals in the dielectric layer.

Further, the dielectric layer 24 can be chosen with a dielectric constant which is temperature dependent. This allows temperature control to be achieved.

Although the present invention has been described with reference to preferred embodiments, workers skilled in the art will recognize that changes may be made in form and detail without departing from the spirit and scope of the invention.