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 Reflective temperature compensating microwave susceptors

Details
Inventors: Lorence, Matthew W.; Rice, Michael J.; Lentz, Ronald R.; Pesheck, Peter S.; Perry, Michael R.;
Assignee: The Pillsbury Company (Minneapolis, MN)
Primary Examiner: Leung; Philip H.
Assistant Examiner:
Attorney, Agent or Firm: Arnold, White & Durkee

A reflective temperature compensating microwave susceptor is disclosed. The susceptor has a microwave interactive heating layer which may be characterized in various ways. In one aspect, the microwave interactive heating layer is operable to provide an increase in reflectance by several factors during heating from 23.degree. C. to 250.degree. C. The microwave interactive heating layer may have a surface resistance that decreases significantly from 23.degree. C. to 250.degree. C. In another aspect, the microwave interactive heating layer may have an electrical conductivity which increases significantly from 23.degree. to 250.degree. C. The microwave interactive heating layer is preferably formed as a thin film deposited upon a substrate, preferably a sheet of polyester. The coated polyester is adhesively bonded to a support member. The microwave interactive heating layer preferably comprises TiO.sub.x, where x has a value between two and one. Most preferably, the microwave interactive heating layer predominantly comprises Ti.sub.2 O.sub.3.

DETAILED DESCRIPTION OF A PREFERRED EMBODIMENT The ability of a susceptor to brown or crispen food is largely determined by the complex surface impedance of the susceptor and by changes in the surface impedance during cooking.
Most microwave ovens operate at a microwave frequency of 2.
45 GHz.
The surface impedance of the susceptor can be measured at the frequency of the microwave oven, e.
g.
, 2.
45 GHz, with a network analyzer.
The effect of susceptor breakup on surface impedance can be seen in Table 1, which shows surface impedances for conventional susceptors, measured with a network analyzer before and after microwaving each product according to package directions.
The data in Table 1 show that the dominant electrical effect of breakup is a large increase in the imaginary part of the surface impedance with a concomitant dramatic decrease in susceptor absorption and reflection, and increased microwave transmission.
While not intending to be bound by any particular theory, microscopic examination of conventional aluminized polyethylene terephthalate (PET) susceptors before and after cooking in the microwave shows that the observed electrical changes correlate with the appearance of microscopic and macroscopic cracks and other discontinuities in the conductive, microwave interactive layer of the susceptor.

TABLE 1
______________________________________
Surface Impedance
Product ohms/square % R % T % A
______________________________________
Totino's Micro-
wave Pizza
Before MW 73.
4 - j7.
8 51.
7 7.
9 40.
3
After MW 160.
6 - j1101.
6
2.
7 92.
8 4.
5
Van de Kamp's
Microwave Fish
Fillets
#1:
Before MW 84.
0 - j5.
5 47.
8 9.
6 42.
6
After MW 163.
0 - j602.
9
7.
3 80.
1 12.
6
#2:
Before MW 126.
2 - j13.
3 35.
8 16.
2 48.
0
After MW 163.
3 - j596.
3
7.
4 79.
7 12.
8
______________________________________
Highly significant in the above observations of the heating effects on a conventional susceptor is the substantial decrease in reflection (R) as a result of heating



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