Vitreous frit

Abstract

A vitreous frit comprising the following by weight percentage ranges: TABLE-US-00001 SiO.sub.2 40-60 Al.sub.2O.sub.3 5-20 Na.sub.2O 10-35 Li.sub.2O 0-6 CaO 0-10 SrO 0-5 BaO 0-5 CeO.sub.2 0-5 TiO.sub.2 0-9.

Claims

1. A non-crystalline glass frit having a firing temperature in the range of about 1350-1800 F., having a coefficient of thermal expansion in the range of about 5.510.sup.6/ F.-8.010.sup.6/ F. from room temperature to about 1000 F., and consisting essentially of the following constituents and weight percentages: TABLE-US-00004 SiO.sub.2 40-60 Al.sub.2O.sub.3 5-20 Na.sub.2O 10-35 Li.sub.2O 0-6 CaO 0-10 SrO 0-5 BaO 0-5 CeO.sub.2 0-5 TiO.sub.2 0-9.

2. The glass frit as set forth in claim 1 wherein the percent by weight is as follows: TABLE-US-00005 SiO.sub.2 49 Al.sub.2O.sub.3 12 Na.sub.2O 15 Li.sub.2O 4 CaO 10 SrO 2 BaO 3 CeO.sub.2 5.

Description

BEST MODE FOR CARRYING OUT THE INVENTION

(1) Manufacture of electromagnetic radiation (EMR) absorbers has typically, for temperatures above about 500 F., included ferromagnetic conductive material uniformly dispersed in a vitreous matrix. Such EMR absorbers are often applied in the form of coatings to substrates whose EMR cross section is advantageously minimized. Electromagnetic radiation impinging on such absorber coatings induce eddy currents in the dispersed particles causing dissipation of the EMR energy. The vitreous matrix constitutes a dielectric which surrounds and separates the individual, electrically conducting particles and, thus, minimizes the electromagnetic (radar) cross section of the substrate underlying the coating by preventing the individual particles from cooperatively establishing eddy currents over a substantial area and reflecting impinging electromagnetic radiation.

(2) EMR absorption is often advantageously used in applications whose temperature is in excess of 1100 F. The manufacture and application of a coating for EMR absorption at lower, as well as higher, application temperatures is described hereinafter.

(3) A vitreous frit having the following range of constituents is wet milled (preferably in methanol) until an average frit particle size of <2-6 microns is preferably obtained:

(4) TABLE-US-00002 Constituent Weight Percent SiO.sub.2 40-60 Al.sub.2O.sub.3 5-20 Na.sub.2O 10-35 Li.sub.2O 0-6 CaO 0-10 SrO 0-5 BaO 0-5 CeO.sub.2 0-5 TiO.sub.2 0-9
The frit material has a coefficient of thermal expansion between about 5.510.sup.6/ F. and 8.010.sup.6/ F. from room temperature to 1000 F. depending largely upon the Na.sub.2O content with greater Na.sub.2O percentages providing higher thermal expansion.

(5) While the above illustrates a preferred set of weight ranges for the frit constituents, the preferred frit (by weight percentage) constitutes the following:

(6) TABLE-US-00003 Constituent Weight Percent SiO.sub.2 49 Al.sub.2O.sub.3 12 Na.sub.2O 15 Li.sub.2O 4 CaO 10 SrO 2 BaO 3 CeO.sub.2 5
A preliminary slip which results from wet milling the above described frit in methanol has a preferred constituent composition of 1000 grams of frit and 500 milliliters of methanol.

(7) The antiferromagnetic or conductive phase of the EMR absorber coating is preferably selected from NiO, CoO.sub.x (where 1x1.33), FeO, Fe.sub.2O.sub.3, and/or MnO.sub.x (where 1x2) and is milled into particles whose average size falls between 2 and 18 microns. There is no precise correlation between the preferred particle sizes of the frit and conducting phase particles except that for each conducting phase particle to be advantageously surrounded and isolated from other conducting phase particles, the frit particles must be smaller than the conducting phase particles. The preferred antiferromagnetic materials are NiO, CoO.sub.x, and Fe.sub.2O.sub.3. NiO and CoO.sub.x are virtually equivalent in their EMR absorption characteristics and coefficients of thermal expansion (7.610.sup.6/ F.). Fe.sub.2O.sub.3 with or without doping with 0.1-0.5 mole percent TiO.sub.2 is also a good EMR absorber when dispersed in the vitreous phase. NiO and CoO.sub.x have relatively higher EMR absorption characteristics at low temperatures (less than about 1000 F.) while Fe.sub.2O.sub.3 has a higher EMR absorption capability at higher temperatures (over about 1000 F.).

(8) A slip is formed by combining the preliminary slip and the conducting phase described hereinbefore, mixing them thoroughly and adding a volatile vehicle such as methanol to enable the slip to be sprayed on a desired substrate or dipped therein without agglomeration of the vitreous/conducting phase mixture. While the final coating advantageously has a high volume percentage of the conducting phase, preferably in the range of 40-70 volume percent, the EMR absorber coating of interest has about 54 volume percent of conducting phase. 350 grams of the milled conducting phase is mixed with 100 milliliters of the hereinbefore described preliminary slip and methanol is added until the resulting slip's viscosity approximates that of an enameling slip. No precise quantity of added methanol can be suggested since it is a function of the slip's average particle size with more methanol being required for smaller average particle size. Additionally, a commercial suspending agent up to 1% may be advantageously used to minimize slip settling. Use of methanol permits application of the slip by spraying to the substrate without wetting and/or causing flotation separation during application and drying for coating thicknesses in the 0.015-0.025 inch range.

(9) Subsequent to applying the slip to the substrate, the substrate/coating is air fired at a temperature of about 1600 F. Judicious selection of slip constituent percentage compositions (including other frit compositions which are not described in detail herein but which are known to those skilled in the art) permit the coating's firing temperature to be adjusted within the range of 1100 to 2100 F. Additional layers of the slip mixture may be applied and then fired until the total EMR absorber coating's thickness is obtained which provides optimum EMR absorption for the EMR frequency of interestfrom 0.04-0.1 inches but typically 0.060-0.085 inches.

(10) The electrical conductivity of the antiferromagnetic material is adjusted (doped) to provide the desired performance characteristics by reacting same with a monovalent doping oxide such as Li.sub.2O or a tetravalent doping oxide such as TiO.sub.2depending on the material to-be-doped. The monovalent oxide is preferably included in the vitreous frit to cause the doping to occur during firing of the EMR absorber coating on the substrate. Alternatively, such doping oxide may be reacted directly with the antiferromagnetic material in quantities of 0.005 to 0.5 mole percent of the antiferromagnetic material, depending upon the desired electrical conductivity of the antiferromagnetic material.

INDUSTRIAL APPLICABILITY

(11) An electromagnetic radiation coating made in accordance with the present disclosure will provide effective electromagnetic radiation absorption up to about 1800 F., will closely match the thermal expansivity of the underlying substrate, will be chemically stable, and will not significantly oxidize upon exposure thereof to high temperatures. The high volume percentage of the conducting phase in the EMR absorber is desired to counteract the typically lower coefficient of thermal expansion exhibited by the vitreous phase and thus provides a composite coefficient of thermal expansion for the EMR coating which approximately matches that of nickel base alloys such as Hastelloy X. Such thermal expansion match of the conducting phase coupled with the high volume fraction thereof: (1) minimizes thermal stresses induced by differences in coefficients of thermal expansion between the coating and the substrate; and (2) prevents increases in the radar cross section of the substrate resulting from fracture and spalling of the coating from the substrate.