This invention relates generally to countermeasure decoys and, more specifically, to methods of producing pyrophoric countermeasure decoy flares.
Infrared (IR) decoy flares are used on many military aircraft to protect against attack by heat seeking missiles. They have also more recently been carried on some civilian aircraft operating in potentially hostile environments. One type of flare currently in use is made from a solid pyrotechnic composition of magnesium, TEFLON™ and VITON™. These are commonly called MTV flares and are ejected from an aircraft and simultaneously ignited by the action of a pyrotechnic squib. The use of pyrotechnic flares containing MTV is described in the article “Review on Pyrotechnic Aerial Infrared Decoys,” Propellants, Explosives, Pyrotechnics, v. 26, p. 3-11, Koch, E.-C. (2001). Burning MTV emits IR radiation that is essentially a spectral continuum attenuated by atmospheric absorption. It is intended that the falling flare will cause a missile seeker head to turn away from the target aircraft. The MTV flares are quite effective against older type missiles that seek heat in a single IR band. However, modern missiles employ counter-counter measures (CCM). Their seeker heads typically use more specific spectral bands in an attempt to distinguish between the flare and the aircraft.
Decoy flares containing pyrophoric materials have been developed in an attempt to produce flares with more specific spectral signatures that are effective against modern missiles with refined seeker heads. Pyrophoric flares are usually kept in an airtight storage compartment before deployment because pyrophoric materials ignite when they come in contact with air. Pyrophoric behavior has been observed in a number of metals, such as aluminum, silicon, phosphorus, iron, cobalt, nickel, copper, zinc, titanium, zirconium, hafnium, chromium, manganese, uranium, plutonium, alkali, alkaline earth, and lanthanide metals as described in Department of Energy Handbook 1081-94, “Primer on Spontaneous Heating and Pyrophoricity” (DOE-HDBK-1081-94, 1994). Generally, elements having Pauling electronegativities of 2 or less are sufficiently reactive with oxygen to be pyrophoric. Many alloys and compounds of these metals are also pyrophoric. For example, alloys of lithium, boron, and other alkali metals have been shown to ignite and burn spontaneously in air as described in U.S. Pat. No. 4,960,564 to Sutula et al., incorporated by reference.
Currently, pyrophoric metal containing flares are typically produced using methods such as those described in U.S. Pat. No. 4,895,609 to Baldi. The '609 patent to Baldi teaches a method to make metals pyrophoric by diffusing aluminum or zinc into the metal followed by leaching the aluminum or zinc out of the metal or, alternatively, by reacting the metal with aluminum followed by leaching the aluminum out of the metal to form porous nanostructures. Powdered aluminum and powdered nickel, iron, or cobalt is carried on an elongated support web and reacted by heating for a few seconds to a few minutes, followed by leaching to provide an elongated pyrophoric foil suitable for decoying some types of heat-seeking missiles. However, this process is labor intensive, difficult to control, uses hazardous chemicals such as acids and bases for leaching, and generates a large amount of environmental waste.
The present invention includes methods for producing pyrophoric countermeasure decoy flares that include depositing a sculptured thin film (STF) of a pyrophoric material onto a substrate using physical vapor deposition.
Generally, some example embodiments pertain to the production of infrared (IR) decoys with tunable IR emission signatures by physical vapor deposition of sculptured thin films of pyrophoric materials onto a substrate. In some examples, IR decoys are produced with a desired IR emission signature and/or temperature profile by controlling the mass, the thickness, the surface area-to-volume ratios, microstructures, and chemical compositions of STF films, and the thickness, chemical compositions, and surface roughness of substrates to meet specific requirements of an application.
In accordance with some examples of the invention, physical vapor deposition includes sputtering, thermal evaporation, e-beam evaporation, and pulsed laser deposition.
In accordance with other examples of the invention, depositing is conducted with a glove box integrated physical vapor deposition system.
In accordance with still further examples of the invention, depositing is performed with a continuous web coater.
In accordance with yet other examples of the invention, the pyrophoric material is selected from the elements in groups IA, IIA, IIIA, IVA, VA, VIA, VIIA, IB, IIB, IIIB, IVB, and VB of the periodic table of the elements.
In accordance with still another example of the invention, the pyrophoric material is selected from at least one of a mixture or an alloy of elements in groups IA, IIA, IIIA, IVA, VA, VIA, VIIA, VIIIA, IB, IIB, IIIB, IVB, and VB of the periodic table of the elements and depositing is performed using a pre-prepared pyrophoric material deposition source.
In accordance with still further examples of the invention, the substrate is a metal foil selected from at least one of an element, a mixture, or an alloy of elements from groups IA, IIA, IIIA, IVA, VA, VIA, VIIA, VIIIA, IB, IIB, IIIB, IVB, and VB of the periodic table of the elements.
In accordance with yet another example of the invention, the substrate is selected from carbon and a polymer.
In accordance with further examples of the invention, the substrate is selected from a cellulosic polymer and a paper sheet.
In accordance with still further examples of the invention, the substrate and the pyrophoric material are selected such that the flare will have a peak temperature in the range from approximately 400° C. to approximately 1500° C. upon exposure to air.
In accordance with additional examples of the invention, the substrate and the pyrophoric material are selected such that the flare will produce at least one of a visible glow or a flame upon exposure to air.
In accordance with yet other examples of the invention, the substrate and the pyrophoric material are selected such that the flare will not produce a visible glow or a flame upon exposure to air.
In accordance with other examples of the invention, the pyrophoric material is deposited on a single side of the substrate.
In accordance with still other examples of the invention, the pyrophoric material is deposited on both sides of the substrate.
In accordance with still further examples of the invention, the substrate has a thickness in the range from approximately 0.1 μm to approximately 1 mm.
In accordance with yet other examples of the invention, depositing includes depositing a sculptured thin film with a thickness in the range from approximately 1 μm to approximately 500 μm.
In accordance with additional examples of the invention, the substrate is in the shape of a circular disk having a diameter in the range from approximately 0.1″ to approximately 10″.
In accordance with further examples of the invention, the substrate has a rectangular surface having a length and a width in the range from approximately 0.1″ to approximately 10″.
In accordance with further examples of the invention, the substrate is a continuous foil having a width from 0.1″ to 200″, as in the case of web coater.
In accordance with other examples of the invention, the method further includes packaging the decoy flare into a container structured to contain multiple decoy flares.
In accordance with additional examples of the invention, the container is structured to contain between approximately 200 and approximately 5000 decoy flares.
In accordance with yet other examples of the invention, the method further includes pre-treating the substrate before conducting PVD of the STF.
In accordance with still further examples, the invention includes a pyrophoric countermeasure decoy flare that includes a substrate and a sculptured thin film of pyrophoric material deposited on the substrate by physical vapor deposition.
In accordance with other examples of the invention, physical vapor deposition includes sputtering, thermal evaporation, e-beam evaporation, and pulsed laser deposition.
These and other examples of the invention will be described in further detail below.
Preferred and alternative examples of the present invention are described in detail below with reference to the following drawings:
The deposition flux incident angles 46, 48, 50, 52 indicate a general path of travel of sputtered or deposited material from the target 34 toward the substrate 36. By using two targets trained angularly toward a central region between them, the two targets are able to coat both sides of the substrate at the same time. The particular angles of the path of travel with respect to the plane defined by the substrate results in a deposition pattern producing interstitial sites, pores, or gaps in the buildup of deposited material. Thus, by varying the angle of incidence the pores can be adjusted as desired. In turn, the resulting adjusted material will have a different thermal signature, as desired.
In this example system 20, the two sputtering guns 28, 32 allow deposition of a pyrophoric material on both sides of the substrate 36. Use of only one of the sputtering guns 28, 32, or a system containing only one sputtering gun would allow deposition of a pyrophoric material on a single side of the substrate 36.
STF films are highly porous, thin films and their nanostructures can be engineered to provide extremely high surface area-to-volume ratios, i.e., >500 cm2 per cm2 of covered substrate as described in Harris, K. D., et al (2001) “Porous thin films for thermal barrier coatings”, Surf. And Coat. Tech, 138, p. 185-191. STF films of pyrophoric materials with controlled chemical compositions and tailored surface area-to-volume ratios can be prepared by physical vapor deposition (PVD) techniques in a clean, one-step process. One mechanism behind porous STF formation during a PVD process is atomic self-shielding or atomic shadowing. The stronger atomic shadowing effect and the lower mobility of ad-atoms on the STF growing surfaces will lead to higher porosity. Generally, the high flux incident angle, low chamber pressure, and large substrate to source distance will enhance atomic shadowing effect, and the low substrate temperature and high deposition rate will lower the mobility of ad-atoms on the STF growing surfaces. Higher porosity and thicker STF films will leads to higher peak temperature of an IR signature. The described process can vary the porosity between 0% to 90% by changing substrate temperatures (<700oC), flux incident angle (30°to 90°), deposition rate (0.1 micron/h to 500 microns/h), substrate-to-source distance (>2 inches), chamber pressure (<1 atm), and substrate rotation (0-1000 rpm).
The pyrophoric nature of these materials allows the spontaneous heating of the deposited films, and subsequently, the substrates (e.g. metal and/or polymer foils) upon exposure to air to give specific IR signatures for decoying heat-seeking missiles.
Generally, pyrophoricity depends on the surface area and chemical composition of a pyrophoric material. Physical vapor deposition can deposit reproducible thin film coatings with closely controlled chemical compositions, microstructure, and morphologies and uniform thickness over extended surfaces on a variety of substrates. In some embodiments, PVD is used to deposit pyrophoric STF layers with controlled chemical compositions and tailored surface-to-volume ratios to allow spontaneous heating of the films, and subsequently, the substrates, to give a specific thermal signature. Examples of physical vapor deposition techniques in addition to sputtering include thermal evaporation, e-beam evaporation and pulse laser deposition. All these techniques have substantially similar process mechanisms. The main difference among these PVD techniques is the way to generate atomic flux of the deposited material from the solid targets/sources: thermal evaporation uses thermal heating, sputtering uses ion bombardment, e-beam evaporation uses electron bombardment, pulse laser deposition uses laser to generate atomic flux from the solid targets/sources. To form STF films, they all require common process parameters: vapor flux incident angle between 30° and 90°, substrate temperature less than 700oC, reduced pressure environment (1 atm<) to have vapor flux traveling in a line-of-sight, substrate-to-target distance greater than 2 inches, and substrate rotation from 0 rpm to 1000 rpm.
PVD can also be adapted to continuous web coaters to economically produce large quantities of the STF layers on a substrate. The process parameters will the same as those for a conventional PVD STF deposition except for the substrate will be moved at prescribed speeds during the deposition. Some example embodiments, include using a continuous web coater to apply the pyrophoric STF to a substrate.
Referring now to
The IR signature or time-temperature profile of an STF film IR decoy may be changed to match the required IR signatures for a given application. The IR signature of the STF film IR decoys is tailored to a particular application by controlling the chemical composition, the mass, the thickness, the surface area-to-volume ratios (porosity) of deposited STF films, and the thickness and chemical compositions of substrates to meet specific requirements of an application. The chemical composition, the mass, the thickness, and the surface area-to-volume ratios (porosity) of the STF films are controlled by controlling the deposition parameters during a physical vapor deposition process.
Typical process parameters are deposition flux incident angle, substrate temperature, deposition rate, deposition time, substrate-to-target distance, chamber pressure, substrate rotation, and deposition source materials. For example, the mass and thickness from 0.1 micron to 500 microns of the STF films are determined by deposition rate, which is in turn determined by deposition power and source material, and deposition time. Surface area-to-volume ratios (porosity) and nanostructures of the deposited STF films are determined by deposition flux incident angle (30°-90°), substrate temperature (<700° C.), deposition rate (0.1 micron/h to 500 microns/h), substrate-to-source distance (>2 inches), chamber pressure <1 atm), and substrate rotation (0-1000 rpm). The stronger atomic shadowing effect and the lower mobility of ad-atoms on the STF growing surfaces will lead to higher porosity. Generally, the high flux incident angle, low chamber pressure, and large substrate to source distance will enhance atomic shadowing effect, and the low substrate temperature and high deposition rate will lower the mobility of ad-atoms on the STF growing surfaces. Higher porosity and thicker STF films will leads to higher peak temperature of an IR signature.
As an example, Fe—Ti STF films reach higher peak temperatures (Tpeak) than Fe—Mn STF films. As the Ti concentration in the Fe—Ti source or in the STF film increases Tpeak increases. Pyrophoric STF films with high surface-area-to-volume ratio (high porosity) and large thicknesses favoring fast air diffusion on thin substrates will lead to high peak temperatures, Tpeak, and to short rise times, tpeak. The duration (tduration) is mainly determined by the mass and thickness of the STF films. Two more specific examples of methods of creating pyrophoric decoy flares using Fe—Mn and Fe—Ti as the pyrophoric material are discussed below, but the invention is not meant to be limited to the details described therein.
In a first example, Fe—Mn (87% wt. Fe-13% wt. Mn) STFs are deposited on 25 micron (0.025 mm) thick iron substrates from a source having the same chemical composition using a magnetron sputtering technique as schematically shown in
After loading the Fe substrates, the deposition chamber 22 is evacuated to a base pressure of ˜10−6 Torr and a 15 sccm Ar flow is intruduced into the chamber 22 followed by adjusting the chamber 22 pressure to be 10 mTorr. Under these conditions, 30 micron (0.03 mm) thick Fe:Mn STFs are deposited on the iron substrates. Upon completion of deposition, the deposition chamber 22 is filled with Ar to the atomsperic pressure. The completed STF decoys are then transferred to the glove box 24 through the loadlock door 26 in an Ar environment. Inside the glove box 26, the STF decoys are packaged into an air-tight container, such as the container 102 shown in
In a second example, Fe—Ti (60% wt. Fe—40% wt. Ti) STFs are deposited on 12 micron (0.012 mm) thick Aluminum substrate using a magnetron sputtering technique. The sputtering targets are manufactured from Fe—Ti alloy with a Ti composition of 40%. The process parameters are 450 Watt DC power to each gun, a 5.5″ substrate-to-gun distance, and a 70° deposition flux incident angle.
After loading the aluminum substrates, the deposition chamber 22 is evacuated to a base pressure of ˜10−6 Torr and a 15 sccm Ar flow is intruduced into the chamber 22 followed by adjusting the chamber pressure to be 10 mTorr. Under these conditions, 20 micron (0.02 mm) thick Fe—Ti STFs are deposited on the substrates. Upon completion of deposition, the deposition chamber 22 is filled with Ar to the atomsperic pressure. The completed STF decoys are then transferred to the glove box 24 through the loadlock door 26 in an Ar environment. Inside the glove box 26, the STF decoys are packaged in a air tight container, such as the container 102 shown in
The first and second examples described above produce the first and second time-temperature profiles illustrated in
While the preferred embodiment of the invention has been illustrated and described, as noted above, many changes can be made without departing from the spirit and scope of the invention. For example, other substrate materials or pyrophoric materials may be used in some embodiments. Also, some method steps may be performed in a different order than that described or concurrently with other steps. Accordingly, the scope of the invention is not limited by the disclosure of the preferred embodiment. Instead, the invention should be determined entirely by reference to the claims that follow.
The invention described herein was made in the performance of work under Naval Air Warfare Center, U.S. Government Contract No. N68335-06-C-0166. The Government may have rights to portions of this invention.