Structural metallic binders for reactive fragmentation weapons

Information

  • Patent Grant
  • 8746145
  • Patent Number
    8,746,145
  • Date Filed
    Monday, June 18, 2012
    12 years ago
  • Date Issued
    Tuesday, June 10, 2014
    10 years ago
Abstract
A munition is described including a reactive fragment having an energetic material dispersed in a metallic binder material. A method is also described including forming a energetic material; combining the energetic material with a metallic binder material to form a mixture; and shaping the mixture to form a reactive fragment. The munition may be in the form of a warhead, and the reactive fragment may be contained within a casing of the warhead.
Description
FIELD OF THE DISCLOSURE

The present disclosure relates to energetic compositions for reactive fragment munitions. More specifically, the present disclosure relates to reactive fragments based, at least in part, on reactive energetic materials dispersed in a metallic matrix.


BACKGROUND

In the discussion that follows, reference is made to certain structures and/or methods. However, the following references should not be construed as an admission that these structures and/or methods constitute prior art. Applicant expressly reserves the right to demonstrate that such structures and/or methods do not qualify as prior art.


A conventional munition includes a container housing a high explosive and, optionally, fragments. Upon detonation of the high explosive, the container is torn apart forming fragments that are accelerated outwardly. In addition, to the extent that fragments are located within the container, these internal fragments are also propelled outwardly. The “kill mechanism” of the conventional fragmentation warhead is the penetration of the fragments (usually steel) into the device or target, which is kinetic energy dependent.


Reactive fragments are used to enhance the lethality of such munitions. A reactive fragment enhances the lethality of the device by transferring additional energy into the target. Upon impact with the target reactive fragments release additional chemical or thermal energy thereby enhancing damage, and potentially improving the lethality of the munition. The reactive fragment employs both kinetic energy transfer of the accelerated fragment into the target as well as the release chemical energy stored by the fragment. Moreover, the released chemical energy can be transferred to the surroundings thermally through radiant, conductive, and/or convective heat transfer. Thus, unlike purely kinetic fragments, the effects of such reactive fragments extend beyond the trajectory thereof.


Some reactive fragments employ composite materials based on a mixture of reactive metal powders and an oxidizer suspended in an organic matrix. However, certain engineering challenges are often encountered in the development of such reactive fragments. For example, a minimum requisite amount of activation energy must be transferred to the reactive fragments in order to trigger the release of chemical energy. There has been a general lack of confidence in the ignition of such reactive fragments upon impact at velocities less than about 4000 ft/s. In addition, since the above-mentioned reactive fragments are based on organic or polymeric matrix materials, which have a density less than that of most targets, i.e., steel, difficulties may arise with respect to the penetration capabilities of the fragment. Finally, the reactive fragments must possess a certain amount of structural integrity in order to survive shocks encountered upon launch of the munition. Again, due to the lower density of the polymeric matrix material, the above-mentioned reactive fragments may not possess the desired degree of structural integrity.


Thus, it would be advantageous to provide an improved reactive fragment which may address one or more of the above-mentioned concerns. Related publications include U.S. Pat. Nos. 3,961,576; 4,996,922; 5,700,974; 5,912,069; 5,936,184; 6,627,013; and 6,679,960, the entire disclosure of each of these publications is incorporated herein by reference.


SUMMARY OF THE INVENTION

According to the present invention, there is provided a munition including a reactive fragment which possesses one or more of: improved control of ballistic, thermal, structural and density characteristics.


According to the present invention, there is provided a munition comprising: a reactive fragment comprising energetic material component or components dispersed in a metallic binder material.


According to the present invention, there is provided a munition comprising: a reactive fragment comprising an energetic material component or components dispersed in a metallic binder material.


According to another aspect, there is provided a method comprising: forming a reactive energetic material; combining the reactive energetic material with a metallic binder material to form a mixture; and shaping the mixture to form a reactive fragment.





BRIEF DESCRIPTION OF THE DRAWING FIGURES

The following detailed description of preferred embodiments can be read in connection with the accompanying drawings in which like numerals designate like elements and in which:



FIG. 1 is a perspective view of a reactive fragment formed according to the principles of the present invention.



FIG. 2 is a cross-section of the reactive fragment of FIG. 1 taken along line 2-2.



FIG. 3 is a schematic cross-section of a warhead formed according to the principles of the present invention.



FIG. 4 is a schematic cross-section of a thin-film reactive material formed according to the principles of the present invention.



FIG. 5 is a schematic cross-section of a thin-film reactive material formed according to an alternative embodiment of the present invention.



FIG. 6 is a schematic illustration of a mode of operation of an embodiment of the present invention, at a first stage.



FIG. 7 is a schematic illustration of a mode of operation of an embodiment of the present invention, at a second stage.



FIG. 8 is a schematic illustration of a mode of operation of an embodiment of the present invention, at a third stage.





DETAILED DESCRIPTION

One embodiment of a reactive fragment 10 formed according to the principles of the present invention is illustrated in FIG. 1. According to the illustrated embodiment, the fragment 10 has a generally cylindrical geometry. However, it should be understood that any suitable geometry is comprehended by the scope of the present invention. Thus, the fragment 10 could also be formed with a spherical, polygonal, or other suitable geometry which renders it effective for its intended purpose.


As illustrated in FIG. 2, the reactive fragment 10 generally comprises a metallic binder material 20 having a reactive energetic material 30 dispersed therein. The reactive fragment 10 may optionally include a structural case or jacketing 40 which may improve the ballistic, target penetration, launch survivability of the fragment 10. Such case hardening and jacketing procedures per se are conventional in the ammunition arts.


The binder material 20 can be formed from any suitable metal or combination of metals. According to one embodiment, the binder material 20 comprises a metal or alloy that when combined with the reactive component (or components), the pressure used to compact and densify the fragment is of magnitude below that causing autoignition of the reactive materials. According to a further embodiment, the binder material 20 comprises one or more of: bismuth, lead, tin, aluminum, magnesium, titanium, gallium, indium, and alloys thereof. By way of non-limiting example, suitable binder alloys include (percentages are by mass): 52.2% In/45% Sn/1.8% Zn; 58% Bi/42% Sn; 60% Sn/40% Bi; 95% Bi/5% Sn; 55% Ge; 45% Al; 88.3% Al/11.7% Si; 92.5% Al/7.5% Si; and 95% Al/5% Si.


In addition, the binder material 20 may optionally include one or more reinforcing elements or additives. Thus, the binder material 20 may optionally include one or more of: an organic material, an inorganic material, a metastable intermolecular compound, and/or a hydride. By way of non-limiting example, one suitable additive could be a polymeric material that releases a gas upon thermal decomposition. The binder material 20 of the present invention may be provided with any suitable density. For example, the binder material 20 of the present invention may be provided with the density of at least about 7.5 g/cm3. According to a further embodiment, the binder material 20 of the present invention is provided with a density of about 7.5 g/cm3 to about 10.5 g/cm3. Furthermore, the binder may be reinforced using organic or inorganic forms of continuous fibers, chopped fibers, a woven fibrous material, filaments, whiskers, or dispersed particulate.


Fragment 10 may contain any suitable reactive energetic material 30, which is dispersed within the metallic binder material 20. The volumetric proportion of metal binder with respect to reactive materials may be in the range of about 20 to about 80%, with the reminder of the fragment being comprised of reactive materials. The energetic material 30 may have any suitable morphology (i.e., powder, flake, crystal, etc.) or composition.


The energetic material 30 may comprise a material, or combination of materials, which upon reaction, release enthalpic or work-producing energy. One example of such a reaction is called a “thermite” reaction. Such reactions can be generally characterized as a reaction between a metal oxide and a reducing metal which upon reaction produces a metal, a different oxide, and heat. There are numerous possible metal oxide and reducing metals which can be utilized to form such reaction products. Suitable combinations include but are not limited to, mixtures of aluminum and copper oxide, aluminum and tungsten oxide, magnesium hydride and copper oxide, magnesium hydride and tungsten oxide, tantalum and copper oxide, titanium hydride and copper oxide, and thin films of aluminum and copper oxide. A generalized formula for the stoichiometry of this reaction can be represented as follows:

MxOy+Mz=Mx+MzOy+Energy

wherein MxOy is any of several possible metal oxides, Mz is any of several possible reducing metals, Mx is the metal liberated from the original metal oxide, and MzOy is a new metal oxide formed by the reaction. Thus, according to the principles of the present invention, the energetic material 30 may comprise any suitable combination of metal oxide and reducing metal which as described above produces a suitable quantity of energy spontaneously upon reaction. For purposes of illustration, suitable metal oxides include: La2O3, AgO, ThO2, SrO, ZrO2, UO2, BaO, CeO2, B2O3, SiO2, V2O5, Ta2O5, NiO, Ni2O3, Cr2O3, MoO3, P2O5, SnO2, WO2, WO3, Fe3O4, MoO3, NiO, CoO, Co3O4, Sb2O3, PbO, Fe2O3, Bi2O3, MnO2 Cu2O, and CuO. For purposes of illustration, suitable reducing metals include: Al, Zr, Th, Ca, Mg, U, B, Ce, Be, Ti, Ta, Hf, and La. The reducing metal may also be in the form of an alloy or intermetallic compound of the above. For purposes of illustration, the metal oxide is an oxide of a transition metal. According to another example, the metal oxide is a copper or tungsten oxide. According to another alternative example, the reducing metal comprises aluminum or an aluminum-containing compound.


As noted above, the energetic material components 30 may have any suitable morphology. Thus, the energetic material 30 may comprise a mixture of fine powders of one or more of the above-mentioned metal oxides and one or more of the reducing metals. This mixture of powders may be dispersed in the metal binder 20. According to certain embodiments, the metal binder 20 acts as a partial or complete source of metal fuel for the energetic, or thermite, reaction.


Alternatively, as schematically illustrated in FIG. 4, the energetic material 30 may be in the form of a thin film 32 having at least one layer of any of the aforementioned reducing metals 34 and at least one layer of the aforementioned metal oxides 36. The thickness T of the alternating layers can vary, and can be selected to impart desirable properties to the energetic material 30. For purposes of illustration, the thickness T of layers 34 and 36 can be about 10 to about 1000 nm. The layers 34 and 36 may be formed by any suitable technique, such as chemical or physical deposition, vacuum deposition, sputtering (e.g., magnetron sputtering), or any other suitable thin film deposition technique. Each layer of reducing metal 34 present in the thin-film can be formed from the same metal. Alternatively, the various layers of reducing metal 34 can be composed of different metals, thereby producing a multilayer structure having a plurality of different reducing metals contained therein. Similarly, each layer of metal oxide 36 can be formed from the same metal oxide. Alternatively, the various layers of metal oxide 36 can be composed of different oxides, thereby producing a multilayer structure having different metal oxides contained therein. The ability to vary the composition of the reducing metals and/or metal oxides contained in the thin-film structure advantageously increases the ability to tailor the properties of the energetic material 30, and thus the properties of the reactive fragment 10.


The reactive fragment 10 of the present invention can be formed according to any suitable method or technique.


Generally speaking, a suitable method for forming a reactive fragment includes forming an energetic material, combining the energetic material with a metallic binder material to form a mixture, and shaping the combined energetic material and metallic binder material mixture to form a reactive fragment.


The energetic material can be formed according to any suitable method or technique. For example, when the energetic material is in the form of a thin film, as mentioned above, the thin-film energetic material can be formed as follows. The alternating layers of oxide and reducing metal are deposited on a substrate using a suitable technique, such as vacuum vapor deposition or magnetron sputtering. Other techniques include mechanical rolling and ball milling to produce layered structures that are structurally similar to those produce in vacuum deposition. The deposition or fabrication processes are controlled to provide the desired layer thickness, typically on the order of about 10 to about 1000 nm. The thin-film comprising the above-mentioned alternating layers is then removed from the substrate. Removal can be accomplished by a number of suitable techniques such as photoresist coated substrate lift-off, preferential dissolution of coated substrates, and thermal shock of coating and substrate to cause film delamination. According to one embodiment, the inherent strain at the interface between the substrate and the deposited thin film is such that the thin-film will flake off the substrate with minimal or no intervention.


The removed layered material is then reduced in size; preferably, in a manner such that the pieces of thin-film having a reduced size are also substantially uniform. A number of suitable techniques can be utilized to accomplish this. For example, the pieces of thin-film removed from a substrate can be worked to pass them through a screen having a desired mesh size. By way of non-limiting example, the mesh size can be 25-60 mesh. This accomplishes both objectives of reducing the size of the pieces of thin-film removed from the substrate, and rendering the size of these pieces substantially uniform.


The above-mentioned reduced-size pieces of layered film are then combined with metallic matrix material to form a mixture. The metallic binder material can be selected from many of the above-mentioned binder materials. This combination can be accomplished by any suitable technique, such as mixing or blending. Optionally, the pieces of thin-film and/or the metallic binder material can be treated in a manner that functionalizes the surface(s) thereof, thereby promoting wetting of the pieces of thin-film in the matrix of metallic binder. Such treatments are per se known in the art. For example, the particles can be coated with a material that imparts a favorable surface energy thereto. Additives or additional components can be added to the mixture. As noted above, such additives or additional components may comprise one or more of: an organic material, an inorganic material, a metastable intermolecular compound, a hydride, and/or a reinforcing agent. Suitable reinforcing agents include fibers, filaments, dispersed particulates.


This mixture can then be shaped thereby forming a reactive fragment having a desired geometrical configuration. The fragment can be shaped by any suitable technique, such as casting, pressing, forging, cold isostatic pressing, hot isostatic pressing, etc. As noted above, the reactive fragment can be provided with any suitable geometry, such as cylindrical, spherical, polygonal, or variations thereof. Once shaped, the reactive fragment can be case hardened or jacketed in order to improve the ballistic capabilities thereof.


There are number of potential applications for a reactive fragment formed according to principles of the present invention. As depicted in FIG. 3, one illustrative, non-limiting, application is the inclusion of reactive fragment 10 within a warhead 50. The warhead 50 generally comprises a penetrator casing 60 which houses a conventional explosive charge 70 and one or more reactive fragments 10. According to the illustrated example, a plurality of reactive fragments 10 are included. Non-limiting exemplary penetrator configurations that may benefit from inclusion of reactive fragments formed according to the present invention include a BLU-109 warhead or other munition such as BLU-109/B, BLU-113, BLU-116, JASSM-1000, J-1000, and the JAST-1000.


Although in the illustrated example, the reactive fragments 10 in the explosive charge 70 are randomly combined within the warhead 50, it should be recognized at the reactive fragments 10 and the explosive charge 70 can be arranged in different ways. For example, reactive fragments and an explosive charge may be separated or segregated, and may have spacers or buffers placed between them. Such an arrangement may be advantageous when it is desired to lessen the sensitivity of the reactive fragments. That is, upon impact of the warhead 50 with an appropriate target, the energy imparted to the reactive fragments is delayed via the above noted physical separation and/or spacers or buffers. Thus, the chemical energy released upon activation of the reactive fragments can also be delayed, which may be desirable to maximize the destructive effects of the warhead upon a particular target or groups of targets.


One advantage of a reactive fragment formed according to principles of the present invention is that both the composition and/or morphology of the reactive material 30 can be used to tailor the sensitivity of the reactive fragment to impact forces. While the total chemical energy content of the reactive material is primarily a function of the quantity of the reducing metal and metal oxide constituents, the rate at which that energy is released is a function of the arrangement of the reducing metal and metal oxide relative to one another. For instance, the greater the degree of mixing between the reducing metal and metal oxide components of the energetic material, the quicker the reaction that releases thermal energy will proceed. Consider the embodiment of the thin-film 32′ depicted in FIG. 5 compared with the embodiment of the thin-film 32 depicted in FIG. 4. The layers of reducing metal 34′ and metal oxide 36′ contained in the thin-film 32′ have a thickness t which is less than that of the thickness T of the layers in thin-film 32 (T>t). Otherwise, the volume of the thin films 32 and 32′ are the same. Thus, the total mass of reducing metal and the total mass of metal oxide contained in the two thin films are likewise the same. As a result, the total thermal energy released by the two films should be approximately the same. However, it is evident that the reducing metal and metal oxide are intermixed to a greater degree in the thin-film 32′. The thermal energy released by the thin-film 32′ will proceed at a faster rate than the release of thermal energy from the thin-film 32. Thus, the timing of the release of thermal energy from a thin-film formed according to the principles of the present invention can be controlled to a certain extent by altering the thickness of the layers of reducing metal and metal oxide contained therein.


Similarly, the timing of the release of chemical energy from a thin-film formed according to the principles of the present invention can also be controlled, at least to some degree, by the selection of materials, and their location, within a thin-film. For example, in the thin-film 32′ depicted in FIG. 5, the rate at which thermal energy is released can be altered by placing layers of metal oxide and/or reducing metal which have a greater reactivity toward the interior of the thin film 32′, while positioning reducing metal and four/or metal oxide layers having a lower reactivity on the periphery (i.e. top and bottom). Since those layers located on the periphery of the thin-film 32′ are presumably more susceptible to ignition due to their proximity to outside forces, these layers will begin to release thermal energy prior to those layers contained on the interior. By placing less reactive materials on the periphery, the overall reaction rate of the thin-film 32 can be slowed.


The ability to tailor the rate of release of thermal energy from a reactive fragment can be advantageous in the design of certain munitions. For example, in the case of a penetrating warhead containing reactive fragments, it can be desirable to maximize the release of energy from the warhead after the target has been penetrated, thereby maximizing the destructive effects of the warhead. This behavior is schematically illustrated in FIGS. 6-8 as illustrated in FIG. 6, a warhead 50 containing reactive fragments 10 and an explosive charge 70 approaches a target 80. Upon collision (FIG. 7), the warhead 50 begins to penetrate the target 80 and an initial release of kinetic and thermal energy 90 occurs, primarily due to the kinetic impact of the warhead casing 60 and the initial release of thermal energy, mainly from the explosive charge 70. At this stage, the kinetic and thermal effects of the fragments on the target 90 are minimal. At a later stage, depicted in FIG. 8, the target has been fully penetrated and a subsequent release of kinetic and thermal energy is imparted to the target 80. As illustrated in FIG. 8, the casing 60 has broken apart releasing casing fragments 62 which kinetically impact the target 90. The fragments 10 also kinetically impact the target. At this point, a subsequent release of thermal energy also occurs, which is a combination of thermal energy released from the explosive charge 70, as well as the release of thermal energy from the energetic material 30 contained in the reactive fragments 10, which has been intentionally delayed so as to occur within the interior region of the target, thereby maximizing the destructive capabilities of the warhead 50.


One alternative munition in which the reactive fragments (10) of the present invention may be utilized (not shown) comprises a warhead designed to detonate prior to impacting the target, the reactive fragments (10) are propelled into the target and can then release the chemical energy stored therein.


Another advantage provided by the present invention is the ability to design reactive fragments which can react at lower impact velocities, for example, at impact velocities on the order of 2,000 ft/sec. or less. This is an improvement over the existing technology because: (1) it permits reduced launch velocity thereby improving the survivability of the fragment; (2) extends the reactive envelope of the fragment by allowing the fragment to travel further before it lacks the kinetic energy to ignite; and (3) opens the system design space by potentially reducing the size of the warhead.


Other advantages provided by the present invention can be attributed to the use of a metallic binder material 20, of the type described herein, in the formation of a reactive fragment. First, the reactive fragment with the metallic binder possesses a greater density relative to other reactive fragments which are formed utilizing a polymeric binder material. This increased density enhances the ballistic effects of the fragment on the target by imparting more kinetic energy thereto. The metallic binder material also increases the structural integrity of the fragment thereby enhancing the same ballistic effects. This increased structural integrity also enhances the ability of the fragments to withstand the shock loadings encountered during firing of the munition within which the fragments may be contained.


Still other advantages can be attained from the reactive fragments of the present invention. During the blast, particles of the metallic binder material will likely exhibit a desirable nonideal gas-like behavior due to its high density, large molecular weight and heat transfer rates. Namely, momentum effects of the blast likely result in the particles of the metallic binder material lagging in velocity behind the lighter weight gas explosive products such as CO, CO2, N2, and H2O vapor. Similarly, heat transfer effects on the particles of the metallic binder material also lag behind. This desirable non-ideal behavior suggests that the sharpness of an overpressure peak during the initial blast will be somewhat attenuated due to thermal and kinetic energy storage of released binder particles. As the blast progresses, release of the kinetic and thermal energy stored by the particles of the metallic binder material will ideally result in an extension of the time at overpressure, thereby enhancing damage to the target (e.g., FIGS. 7-8). Many metallic binder materials, such as those discussed above, have relatively strong thermodynamic tendencies to react with oxygen in air. Thus, particles of metallic binder material may impart a significant afterburning component to the blast, further extending the overpressure in the time domain and the release of energy into the target. Any metallic binder material which is not consumed by afterburning can be readily distributed into the target as a result of a successful reactive fragment impact, thus increasing the likelihood of electrical short-circuiting if electrical components are housed within the target.


All numbers expressing quantities of ingredients, constituents, reaction conditions, and so forth used in the specification are to be understood as being modified in all instances by the term “about”. Notwithstanding that the numerical ranges and parameters setting forth, the broad scope of the subject matter presented herein are approximations, the numerical values set forth are indicated as precisely as possible. Any numerical value, however, inherently contains certain errors necessarily resulting from the standard deviation found in their respective measurement techniques.


Although the present invention has been described in connection with preferred embodiments thereof, it will be appreciated by those skilled in the art that additions, deletions, modifications, and substitutions not specifically described may be made without department from the spirit and scope of the invention as defined in the appended claims.

Claims
  • 1. A method comprising: forming a plurality of discrete structures, each discrete structure comprising an energetic material, the energetic material including a first material that is a reducing metal or a metal hydride and a second material that is a metal oxide;combining the plurality of discrete structures with a metallic binder material to form a mixture; andshaping the mixture to form a reactive fragment.
  • 2. The method of claim 1, wherein shaping the mixture comprises imparting a cylindrical or polygonal or other shape to the reactive fragment.
  • 3. The method of claim 1, wherein each discrete structure comprises a thin film or thin layered structure, each discrete structure comprising at least a first layer comprising the reducing metal and at least a second layer comprising the metal oxide.
  • 4. The method of claim 3, wherein the layers have a thickness of about 10 to about 10000 nm.
  • 5. The method of claim 1, wherein the second material is an oxide of a transition metal element, and wherein the first material is aluminum or aluminum-based.
  • 6. The method of claim 1, further comprising subjecting the reactive fragment to at least one of case-hardening and jacketing.
  • 7. The method of claim 1, wherein the metallic binder material has a density of at least about 7.5 g/cm3.
  • 8. The method of claim 1, wherein the metallic binder material has a density within the range of 1.0 to 17.0 g/cm3.
  • 9. The method of claim 1, wherein the metallic binder material comprises one or more of bismuth, lead, tin, indium, and alloys thereof.
  • 10. The method of claim 1, further comprising adding one or more of the following to the mixture: an organic material, an inorganic material, a metastable intermolecular composite, or a hydride.
  • 11. The method of claim 1, further comprising treating the surface of at least one of the energetic material and the metallic binder material in order to promote wetting.
  • 12. The method of claim 1, further comprising adding one or more of fibers, filaments, dispersed particulates, and mixtures thereof to the metallic binder material.
  • 13. The method of claim 1, further comprising placing the reactive fragment within a casing of a warhead.
US Referenced Citations (141)
Number Name Date Kind
1367846 Washburn Feb 1921 A
1399953 Fulton Dec 1921 A
2200742 Hardy May 1940 A
2200743 Hardy May 1940 A
3056255 Thomsen Oct 1962 A
3254996 MacDonald Jun 1966 A
3261732 Eilo Jul 1966 A
3325316 MacDonald Jun 1967 A
3344210 Silvia Sep 1967 A
3362859 Sutton Jan 1968 A
3377955 Hodgson Apr 1968 A
3422880 Brown et al. Jan 1969 A
3433196 Sjoblom Mar 1969 A
3437534 McEwan et al. Apr 1969 A
3596602 Gey et al. Aug 1971 A
3632458 Filter et al. Jan 1972 A
3661083 Weinholt May 1972 A
3831520 Bowen et al. Aug 1974 A
3961576 Montgomery, Jr. Jun 1976 A
4112847 Thomanek Sep 1978 A
4129465 Johnson et al. Dec 1978 A
4357873 Jager Nov 1982 A
4703696 Böcker Nov 1987 A
4757764 Thureson et al. Jul 1988 A
4933241 Holt et al. Jun 1990 A
4982667 Weimann Jan 1991 A
4996922 Halcomb et al. Mar 1991 A
5000093 Rozner et al. Mar 1991 A
5090322 Allford Feb 1992 A
5243916 Freche et al. Sep 1993 A
5266132 Danen et al. Nov 1993 A
5392713 Brown et al. Feb 1995 A
5401340 Doll et al. Mar 1995 A
5429691 Hinshaw et al. Jul 1995 A
5439537 Hinshaw et al. Aug 1995 A
5505799 Makowiecki Apr 1996 A
5509357 Lawther Apr 1996 A
5538795 Barbee, Jr. et al. Jul 1996 A
5544589 Held Aug 1996 A
5547715 Barbee et al. Aug 1996 A
5567908 McCubbin et al. Oct 1996 A
5700974 Taylor Dec 1997 A
5717159 Dixon et al. Feb 1998 A
5732634 Flickinger et al. Mar 1998 A
5773748 Makowiecki et al. Jun 1998 A
5817970 Feierlein Oct 1998 A
5852256 Hornig Dec 1998 A
5859383 Davison et al. Jan 1999 A
5912069 Yializis et al. Jun 1999 A
5936184 Majerus et al. Aug 1999 A
5939662 Bootes et al. Aug 1999 A
5949016 Baroody et al. Sep 1999 A
6186072 Hickerson, Jr. et al. Feb 2001 B1
6220166 Cherry Apr 2001 B1
6276276 Erickson Aug 2001 B1
6276277 Schmacker Aug 2001 B1
6308607 Woodall et al. Oct 2001 B1
6321656 Johnson Nov 2001 B1
6382105 Jones May 2002 B1
6443789 Tominetti et al. Sep 2002 B2
6464019 Werner et al. Oct 2002 B1
6467416 Daniels et al. Oct 2002 B1
6494140 Webster Dec 2002 B1
6520258 Yang et al. Feb 2003 B1
6597850 Andrieu et al. Jul 2003 B2
6615737 Bonnel et al. Sep 2003 B2
6627013 Carter, Jr. et al. Sep 2003 B2
6666143 Collins Dec 2003 B1
6668726 Lussier Dec 2003 B2
6679960 Jones Jan 2004 B2
6682281 Larsen Jan 2004 B1
6682817 Della Porta et al. Jan 2004 B1
6713177 George et al. Mar 2004 B2
6720204 Sudijono et al. Apr 2004 B2
6736942 Weihs et al. May 2004 B2
6843868 Fawls et al. Jan 2005 B1
6846372 Guirguis Jan 2005 B1
6863992 Weihs et al. Mar 2005 B2
6955732 Chan et al. Oct 2005 B1
6962634 Nielson et al. Nov 2005 B2
6991860 Phillips et al. Jan 2006 B2
7191709 Nechitalio Mar 2007 B2
7231876 Kellner Jun 2007 B2
7278354 Langan et al. Oct 2007 B1
7282634 Kuklinski Oct 2007 B2
7383775 Mock et al. Jun 2008 B1
7513198 Zhang et al. Apr 2009 B2
7614348 Truitt et al. Nov 2009 B2
7658150 Rönn et al. Feb 2010 B2
7718016 Schild et al. May 2010 B2
7743707 Melin et al. Jun 2010 B1
7770521 Williams et al. Aug 2010 B2
7829157 Johnson et al. Nov 2010 B2
7845282 Sheridan et al. Dec 2010 B2
7886666 Williams et al. Feb 2011 B2
7886668 Hugus et al. Feb 2011 B2
7927437 Gangopadhyay et al. Apr 2011 B2
7955451 Hugus et al. Jun 2011 B2
7972453 Sheridan et al. Jul 2011 B2
7977420 Nielson et al. Jul 2011 B2
8033223 Sheridan et al. Oct 2011 B2
8075715 Ashcroft et al. Dec 2011 B2
8122833 Nielson et al. Feb 2012 B2
8250985 Hugus et al. Aug 2012 B2
8361258 Ashcroft et al. Jan 2013 B2
20010046597 Weihs et al. Nov 2001 A1
20020069944 Weihs et al. Jun 2002 A1
20030010246 Bonnel et al. Jan 2003 A1
20030037692 Liu Feb 2003 A1
20030097953 Serizawa et al. May 2003 A1
20030131749 Lussier Jul 2003 A1
20030164289 Weihs et al. Sep 2003 A1
20030167956 Kellner Sep 2003 A1
20030203105 Porta et al. Oct 2003 A1
20040060625 Barbee, Jr. et al. Apr 2004 A1
20040101686 Porta et al. May 2004 A1
20040151845 Nguyen et al. Aug 2004 A1
20040244889 Sailor et al. Dec 2004 A1
20050002856 Zaluska et al. Jan 2005 A1
20050011395 Langan et al. Jan 2005 A1
20050100756 Langan et al. May 2005 A1
20050126783 Grattan et al. Jun 2005 A1
20050142495 Van Heerden et al. Jun 2005 A1
20050183618 Nechitailo Aug 2005 A1
20050189050 Sheridan Sep 2005 A1
20050199323 Nielson et al. Sep 2005 A1
20050235862 Gousman et al. Oct 2005 A1
20070006766 Kellner Jan 2007 A1
20070169862 Hugus et al. Jul 2007 A1
20070272112 Nielson et al. Nov 2007 A1
20070277914 Hugus et al. Dec 2007 A1
20080035007 Nielson et al. Feb 2008 A1
20080092764 Renaud-Bezot et al. Apr 2008 A1
20080202373 Hugus et al. Aug 2008 A1
20090078146 Tepera et al. Mar 2009 A1
20090221135 Gangopadhyay et al. Sep 2009 A1
20090235836 Pratt et al. Sep 2009 A1
20090255433 Wang et al. Oct 2009 A1
20100024676 Hugus Feb 2010 A1
20100251694 Hugus et al. Oct 2010 A1
20100269723 Hugus et al. Oct 2010 A1
Foreign Referenced Citations (8)
Number Date Country
1 348 683 Oct 2003 EP
1 659 359 May 2006 EP
1 585 162 Jan 1970 FR
2 867 469 Sep 2005 FR
1 507 119 Apr 1978 GB
2 260 317 Apr 1993 GB
2 412 116 Sep 2005 GB
WO 0216128 Feb 2002 WO
Non-Patent Literature Citations (21)
Entry
Partial European Search Report issued in EP 07 10 9539, Oct. 23, 2007, 6 pages, European Patent Office, The Hague, NL.
Extended European Search Report issued in EP 07 10 9539, Jan. 16, 2008, 9 pages, European Patent Office, The Hague, NL.
Sheridan, Copending U.S. Appl. No. 10/923,865, filed Aug. 24, 2004 entitled “Energetic Material Composition”.
Johnson, et al., Copending U.S. Appl. No. 11/399,263, filed Apr. 7, 2006 entitled “Method of Making Multilayered, Hydrogen-Containing Thermite Structures”.
Schild, et al., Copending U.S. Appl. No. 11/399,392, filed Apr. 7, 2006 entitled “Methods of Making Multilayered, Hydrogen-Containing Intermetallic Structures”.
Hugus, et al., Copending U.S. Appl. No. 11/447,068, filed Jun. 6, 2006 entitled “Heat Matrix Composite Energetic Structures”.
Sheridan, et al., Copending U.S. Appl. No. 11/451,313, filed Jun. 13, 2006 entitled “Enhanced Blast Explosive”.
Hugus, et al., Copending U.S. Appl. No. 11/504,808, filed Aug. 16, 2006 entitled “Metal Binders for Thermobaric Weapons”.
Hugus, et al., Copending U.S. Appl. No. 11/649,818, filed Jan. 5, 2007 entitled “Solid Composite Propellants and Methods of Making Propellants”.
Hugus, et al., Copending U.S. Appl. No. 11/709,233, filed Feb. 22, 2007 entitled “Energetic Thin-Film Based Reactive Fragmentation Weapons”.
Sheridan, et al., Copending U.S. Appl. No. 11/806,221, filed May 30, 2007 entitled “Selectable Effect Warhead”.
McDonough, James Eric, “Thermodynamic and Kinetic Studies of Ligand Binding, Oxidative Addition, and Group/Atom Transfer in Group VI Metal Complexes” a Dissertation, pp. 108-149, Dec. 2005, Coral Gables, FL.
Fischer, S.H., et al., “A survey of combustible metals, thermites, and intermetallics for pyrotechnic applications,” AIAA Meeting Papers on Disc, Jul. 1996, pp. 1-13, American Institute of Aeronautics and Astronautics, Inc. , USA.
Shi, L.Q., et al., “Investigation of the hydrogenation properties of Zr films under unclean plasma conditions,” J. Vac. Sci. Tevhnol, A 20(6), Nov./Dec. 2002, pp. 1840-1845, American Vacuum Society, USA.
Seman, Michael et al., “Investigation of the role of plasma conditions on the deposition rate and electrochromic performance of tungsten oxide thin films”, J. Vac. Sci. Technol., A21(6), Nov./Dec. 2003, pp. 1927-1933, American Vacuum Society, USA.
Grant, J., editor, Hackh's Chemical Dictionary, Third Edition, 1944, 4 pp. (cover page, title page and excerpt pages 845-846), McGraw-Hill Book Company, Inc., New York, USA.
Lewis, Sr., R.J., editor, Hawley's Condensed Chemical Dictionary, 12th edition, 1993, 3 pp. (cover page, title page and excerpt page 1139), Van Nostrand Reinhold Co., New York, USA.
Bennett, H., editor, Concise Chemical Dictionary, Third Enlarged Edition, 1974, 3 pp. (cover page, title page and excerpt page 1037), Chemical Publishing Company, Inc., New York, NY , USA.
Webster's Ninth New Collegiate Dictionary, 1990, 3 pp. (cover, title page and excerpt page 1224), Merriam-Webster's Inc., Springfield, Massachusetts, USA.
Boyd, J.M., “Thin-Film Electric Initiator. III. Application of Explosives and Performance Tests”, U.S. Army Material Command, Report No. -HDL—TR-1414, Jan. 1969, 27 pages, Harry Diamond Laboratories, Washington, DC 20438.
Prakash, Anand, et al., “Synthesis and Reactivity of a Super-Reactive Metastable Intermolecular Composite Formulation of Al/KMnO4”, Advanced Materials, Apr. 2005, pp. 900-903, vol. 17, No. 7, WILEY-VCH Verlag Gmbh & Co. KGaA, Weinheim, DE.
Related Publications (1)
Number Date Country
20120255457 A1 Oct 2012 US
Divisions (1)
Number Date Country
Parent 11447069 Jun 2006 US
Child 13526170 US