The present invention deals generally with firearms. More particularly, it deals with noise and flash suppressors for firearm muzzles.
Reducing muzzle noise and flash from military and security personnel firearms (e.g., long guns and pistols) provide a significant tactical advantage in the field. Existing suppression technology reduces noise and flash, but comparatively little science exists to explain how current designs can be modified or replaced to provide enhanced suppressor performance, including the useful life span of the suppressor. Furthermore, even less design guidance exists that can lead to integration of suppressors into a firearm's barrel assembly. Lessons learned as a result of the ongoing military and homeland security based conflicts have indicated that increased use of current suppressors, as part of everyday operations, have led to shortened life cycles of suppressors, increased maintenance (and sometimes damage) of weapons, and considerable variability in weapon accuracy.
To set the stage for developing improved suppressors, it is necessary first to identify the critical elements of the attendant flow fields as thoroughly documented in Klingenberg, Firearmter and Heimerl, Joseph M., Firearm Muzzle Blast and Flash, AIAA Progress in Astronautics and Aeronautics, Volume 139, 1992. See the copy of in Applicants' Information Disclosure Statement.
These characteristics can be broken down into three core elements. The first two core elements are: the precursor blast; and a main blast set up by the expanding gases. The precursor blast consists of mostly air with a small amount of propellant and the main blast is made up of spherical pressure waves that quickly overtake the fired projectile. Both of these blasts are sources of low frequency noise that carry very far distances. The third core element is the highly visible gas flash which follows the blast.
In general, a gas flash occurs because air mixes with the fuel rich propellants and the high temperatures from the blast waves. The result of this mixture forms a gas flash which is greatly increased in the secondary flow region that occurs away from the muzzle of a firearm.
When a gas flash forms, it occurs in three parts: primary, intermediate, and secondary flashes. The primary flash forms at the muzzle in the supersonic flow region and is very small. An intermediate flash occurs directly behind the projectile, but in front of the Mach disk leading any supersonic flow region. (Not all firearms have supersonic discharge flows.) The secondary flash is the most severe, and it occurs downstream of the firearm muzzle, and after the normal shock resulting from the muzzle gas over-expansion. The large flash seen when firing a projectile is actually the secondary flash.
With an understanding of the three core elements involved in the blast and flash from a projectile, the individual components can be analyzed to assess their critical components. Considering the principal characteristics of the blast wave, co-Applicants (from the Parent application) have found that it is essentially a spherical blast wave that travels rapidly but also decays rapidly both strength-wise and time/distance-wise. Relative to the flow-field attendant to the flash, it establishes after or behind the main blast wave with a structure very similar to that of a traditional under-expanded jet plume often seen in propulsion applications. The key elements of the post-blast wave flow field are the free jet boundary and the highly under-expanded jet flow region all flowing strongly in the downstream axial direction. The over-expanded gas results in the normal shock or Mach disk, which causes the secondary flash and a significant portion of the noise. The important point is that the key physics of this type of flow structure is common in propulsion aerodynamics, and can be used to generate performance correlations for use in developing more efficient suppressor designs.
There are a wide range of firearm suppressor designs. See, for example, the Prior Art shown in
An alternate means of controlling supersonic flows, originally developed for propulsion applications, involves the use of flow mixer-ejectors, as discussed in U.S. Pat. No. 5,884,472 to Walter M. Presz, Jr. and Gary Reynolds. Ejectors are well-known and documented fluid jet pumps that draw flow into a system and thereby increase the flow rate through that system. Mixer/ejectors are short compact versions of such jet pumps that are relatively insensitive to incoming flow conditions and have been used extensively in high-speed jet propulsion applications involving flow velocities near or above the speed of sound. See, for example, U.S. Pat. No. 5,761,900 to Walter M. Presz, Jr., which also uses a mixer downstream of a gas turbine nozzle to increase thrust while reducing noise from the discharge. Dr. Presz is a co-inventor in the present application. An ejector is a fluid dynamic pump with no moving parts.
Ejectors use viscous forces to lower the velocity and energy of a jet stream by ingesting lower energy flow which can lead to flow characteristics that may augment thrust, cool exhaust gases, suppress jet infrared signature, and importantly to ballistic applications, reduce attendant noise and flash. Mixers improve the performance characteristics of ejectors by inducing stiffing, or axial vortices, that promote rapid mixing of the high velocity primary jet with the cooler, and sometimes heavier, ingested gas; thus resulting in more compact devices. Numerous patented products have derived from this concept. The mixer/ejector concept is well accepted within the aviation and jet propulsion community as an extremely efficient solution to aircraft noise and exhaust temperature suppression.
Gas turbine technology has yet to be applied successfully to firearm muzzle suppressors. If one were to replace an under-expanded jet engine exhaust for a ballistic blast from a firearm, mixing and ejecting the hot gases expelled with the projectile over the length of the barrel, it may be seen that such a technology could significantly reduce noise, flash, and provide outside air to the barrel that could be employed to cool and clean the suppressor components.
Accordingly, it is a primary objective of the present invention to provide a firearm suppressor that employs advanced fluid dynamic ejector pump principles to consistently deliver levels of noise and flash suppressor equal to or better than current suppressors.
It is another primary objective to provide an improved firearm suppressor with significantly increased useful life span over that of current firearm suppressors.
It is another primary objective to provide a self-cleaning, self-cooling firearm suppressor using mixer/ejector technology.
It is another primary objective to provide an improved firearm suppressor using mixer/ejector technology to control the muzzle blast wave and overexpansion flow for better suppression.
It is another object, commensurate with the above-listed objects, to provide an improved suppressor which is durable and safe to use.
The Parent application dealt with pre-production embodiments shown herein as
Applicants have developed an improved firearm suppressor through the use of advanced mixer/ejector concepts. By recognizing and analyzing the blast and plume characteristics, inherent in ballistic discharges, Applicants have created a new two-step controlled unaided surge and purge system (nicknamed “CUSPS”) for firearm suppressors.
This new “CUSPS” approach attends to the blast surge effects by controlling the flow expansion into the suppressor, and attends to the flash effects by controlling inflow and outflow gas purging. The “CUSPS” rapidly reduces the pressure energy associated with a firearm muzzle blast before it exits the suppressor, thereby reducing noise and muzzle flash.
In the preferred C-I-P embodiment, the blast surge is mitigated via a rapid, divergent nozzle volume increase, created sequentially by: an inlet slotted mixer nozzle; a first expansion chamber; a blast baffle resembling a “wagon wheel”; a series of alternating baffles, with vent holes, strategically located along the suppressor's inner wall surface; and a second expansion chambers.
In the alternate C-I-P embodiment, a differently shaped blast baffle is angled or pitched forward.
Note that the two C-I-P embodiments contain no “outside” vent holes which extend through the suppressor housing's outer wall (i.e., throughbores). Instead of ingesting ambient air through such vent holes and mixing that air with the muzzle gases, as shown in the parent application, the C-I-P embodiments have different structures and work in a different manner. They too though can control or eliminate the Mach disk.
Based upon preliminary testing, Applicants believe that their C-I-P embodiments will generate the following benefits: lower noise; hide or eliminates flash; integrate cooling and self-cleaning; and maintain firearm accuracy at longer distances.
Referring to the drawings in detail,
This C-I-P application adds and discloses the near-production model shown in
In the prior embodiment 100 (see
The prior embodiment 100 (see
Though not shown, the vent holes 104 are preferably convergent. They narrow towards the outside of the suppressor.
While the depicted “CUSPS” suppressor 100 has lobed internal nozzles 116, it could instead have slotted rounded internal nozzles. Both types have divergent area distributions to minimize flow overexpansion and reduce noise and flash.
Tubular housing 102 need not be circular in cross section. Its major axis is preferably horizontal (i.e., co-axial with the firearm barrel 103; or, alternatively vertical (not shown) or in between (not shown).
Experimental and analytical analyses of the “CUSPS” embodiment 100 indicates: the “CUSPS” can reduce the noise induced by the firearm's muzzle blast wave, reduce the radiant flash caused by the propellant gases and ingest ambient air to both cool the suppressor and purge it of residual gases, thereby increasing its useful life span.
Based on their experimental and analytical results, and the observation that the vent holes permits easier flushing of the interior volume with cleaning fluids, the Applicants believe the “CUSPS” embodiment 100 will reduce the blast wave induced noise at three feet from the muzzle exit by 20 db or more, make the gas flash visually undetectable to an observer at any distance greater than 1000 muzzle diameters, and have an indefinite useful lifetime if properly maintained.
In the embodiment 100, the entrance and lobed nozzle 116 serve to control and reduce the static pressure of the gases exiting the muzzle while the vent holes 104 first dissipate the blast wave from the muzzle gases and thereafter ingest ambient air to purge, dilute and cool the residual gases. The ejector lobes assist and amplify the air ingestion process, stir the ingested air into the muzzle gases to enhancing their cooling and reduce the strength of the shock waves produced, which are further assisted by the convergent/divergent diffuser 127. Applicants believe the other disclosed embodiments will do the same.
The internal diameter of a suppressor housing 102 is between two and ten muzzle external diameters to accommodate the range of propellant gases used in the firearm. The “CUSPS” suppressor length is set between three and ten times its internal diameter to tailor its sound reduction to a desirable level.
The placement, number and size of the vent holes 104 are established to assure sufficient dilution of the muzzle gases to reduce flash and purging of the residual gases.
The entrance divergent nozzle's exit diameter and length are established using classic gas dynamic principals to produce isentropic, or near isentropic, expansion of the muzzle gases into the suppressor.
The exit nozzle diameter and length are established using classic gas dynamic principals to produce isentropic, or near isentropic, expansion of the muzzle gases out of the suppressor.
The mixer lobes, slots, tabs or swirl vanes have longitudinal, azimuthal and/or radial dimensions approximately equal to the radial dimensions of the entrance nozzle exit diameter and the suppressor internal diameter.
The ejector diameter is set between that of the entrance nozzle exit diameter and the suppressor internal diameter.
Each of the embodiments, from the Parent application, can be thought of as a firearm suppressor comprising:
Each of the “CUSPS” embodiments, from the Parent application, also can be though of in method terms. For example, a method for firearms, and other guns, comprising:
During the continued development of the “CUSPS” firearm suppressor identified in the Parent application, Applicants determined that certain modifications allowed a mixer/ejector to function effectively without outside vent holes. Their mixer nozzle in two new C-I-P embodiments (
Concept Development: Most suppressors function by manipulating the pressure energy generated in the discharge of a bullet. Typically suppressors are designed with multiple chambers that temporarily “trap” the energy, and release it at a slower rate or convert it to a different form. As the high pressure, high temperature gasses moving with tremendous velocity are suddenly stopped by a baffle with a single tight opening, much of the gas changes direction and bounces around the chamber. This sudden change of direction takes energy away from the flow, and converts that energy into heat and strain on the suppressor. It also causes a sudden increase in pressure, as the flow is instantly restricted. Such sudden increase in pressure causes a high pressure wave to propagate backwards up the barrel length and to interfere with the proper operation of the firearms loading and firing mechanisms.
Applicants' preferred approach for reducing the back pressure level and effect is to keep the flow in the suppressor moving forward purging chamber contaminants and not bottled-up in the suppressor. For practical reasons, a suppressor is limited in length and volumes. In order to keep the flow moving, an alternate flow path for the gases has been incorporated. In Applicants' preferred and enhanced C-I-P embodiment 1000 (see
As in the Parent application, the internal diameter of Applicants' preferred “CUSPS” suppressor housing 1001 (see
Unlike the embodiments disclosed in the Parent application, Applicants' preferred C-I-P embodiment 1000 does not interact with any “outside” vent holes (i.e., throughbores perpendicular to the suppressor centerline or longitudinal axis 1005) along the length of the suppressor. In fact, Applicants' C-I-P embodiment 1000 does not need to have such vent holes in its suppressor housing 1001 for the system to work effectively. Future versions of the C-I-P preferred embodiment could use such vent holes for different requirements.
The concept, as depicted in
A representative mixer nozzle 1002 (tested by Applicants) consists of three progressively increasing diameters of 0.230″, 0.300″, and 0.350″. The first two diameters have square corners, and the last diameter has a slow taper. It is on this taper that the three equally spaced slots are cut. These cuts are approximately 0.250″ wide and run about 0.750″ from the tip of the nozzle. As the supersonic flow approaches the square corners, it is refracted away from the centerline 1005.
A preferred alternative mixer nozzle 1002 ends abruptly a quarter inch into the second diameter, utilizing the inner diameter of the suppressor as the third diameter in the progression. This alteration is only useful when the barrel will only be used in the suppressed configuration, as it will not prevent flash without the rest of the suppressor.
Immediately following the mixer nozzle 1002 is an expansion chamber 1004. In order to allow the gaseous flow to separate into multiple paths, it is necessary to allow the flow to expand away from the centerline 1005 (i.e., the longitudinal axis of the suppressor). Since the flow has axial momentum in the same direction as the projectile (e.g., bullet not shown), it will tend to remain close to the centerline. The mixer nozzle 1002 and the expansion chamber 1004 are designed to generate ejector action that accelerates outward expansion of the muzzle gases in order for the muzzle gases to rapidly mix with the chamber gases and then have a viable, alternate flow path to the exit. At this point the core of this design is introduced.
After the flow has expanded to fill the expansion chamber 1004, the first obstacle is introduced: a generally “wagon wheel” shaped blast baffle 1006. Its purpose is to immediately disrupt the mixer nozzle exit flow, without creating excessive amounts of back pressure. Its secondary purpose is to encourage the gas to not flow along the centerline 1005. Both of these goals are important because immediately following the blast baffle 1006 is a stack of alternating baffles 1012A, 1012B, 1012C, 1012D, 1012E, 1012F. This is where the flow is now given two paths: the straight path of the bullet or projectile and a longer winding path through open, lower resistance flow paths set up by the baffle flat sections shown in
As best shown in
Dimensions of a representative blast baffle 1006, including its outer passageways (e.g., 1008A, 1008B) and central vent hole 1010, are as follows. The overall diameter of blast baffle 1006 is flush with the inner diameter of the suppressor; the blast baffle's center hole is 0.300″; and there are seven outer passageways, like 1008A and 1008B, which are evenly spaced trapezoids tangential to an inner diameter of 0.700″ and have outer diameters of 1.250″.
Following the blast baffle is a series of alternating, secondary baffles 1012A, 1012B, 1012C, 1012D, 1012E, 1012F. Looking at the cross-sectional side plan view of
Tested representative secondary baffles consist of circular disks approximately 0.092″ thick, with a 0.300″ center hole, and a flat horizontal cut 0.500″ from the center. They are spaced approximately 0.220″ apart.
Live round testing utilizing the Mk16 assault rifle and M855 ammunition has determined that for a 5.56 caliber assault rifle, 5-7 alternating baffles has excellent performance. This is significant because too few baffles will not be effective at slowing the flow, and the suppressor will not be effective at suppressing noise or flash. If more than seven baffles are used, the additional noise suppression is minimal compared to the added length and weight. It is anticipated that different caliber weapons will have an optimal baffle stack both in number and spacing.
Following the baffle stack, comprising the blast baffle 1006 and alternate baffles 1012A-F, is a second expansion chamber 1014. Testing indicates that an expansion chamber 1014 following the baffle stack significantly improves the suppression capabilities. It is believed that this may increase the interference between the two flow paths, or possibly allow for less restriction along the alternate path.
The final feature of this design is the exit orifice or suppressor discharge 1016. Although the exit geometry is relatively commonplace, it has proven to be quite effective. The simple cylindrical exit protrudes into the chamber a moderate amount to limit the amount of flow exiting the suppressor. High velocity flow that is not on centerline will miss the exit opening, flow past the cylindrical protrusion, hit the back wall of the suppressor and bounce around the final chamber before it escapes into the ambient air.
A representative exit orifice 1016 is described as follows: a flat plate with a 0.500″ diameter tube protruding 0.500″ from the center. This protrusion has a 0.300″ diameter hole through the center.
Both of these blast baffle configurations create an immediate disruption in the flow while allowing the gas to travel a path besides on centerline.
Field tests of the design shown in
As in the parent application, the entrance divergent nozzle's exit diameter and length (in the C-I-P embodiments) are established using classic gas dynamic principals to produce isentropic, or near isentropic, expansion of the muzzle gases into the suppressor.
The exit nozzle diameter and length are established using classic gas dynamic principals to produce isentropic, or near isentropic, expansion of the muzzle gases out of the suppressor.
The ejector diameter is set between that of the entrance nozzle exit diameter and the suppressor internal diameter.
Each of the C-I-P embodiments can be thought of as a firearm suppressor comprising:
Instead of ingesting ambient air through outer vent holes (in the suppressor's outer or longitudinal wall) and mixing that air with the muzzle gases, as shown in the parent application, the preferred C-I-P embodiment ingests and mixes chamber gases and contaminants with the muzzle gases, and allows fluid flow through and out the suppressor. It too though can control or eliminate the Mach disk.
Each of the C-I-P embodiments also can be though of in method terms. For example, a method for firearms, and other guns, comprising:
While all the embodiments (both the Parent and C-I-P) are detachable from a gun, they can be affixed, more permanently, to the barrel.
It should be understood by those skilled in the art that obvious structure modifications can be made about departing from the spirit or scope of the invention. For example, the same technique could be used for artillery or other guns.
This is a continuation-in-part (“C-I-P”) application of U.S. Utility patent application Ser. No. 12/212,166, filed Sep. 17, 2008 (“Parent application”), which was based upon a U.S. Provisional Patent Application Ser. No. 29/317,238, filed Sep. 17, 2007.
Number | Date | Country | |
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60994280 | Sep 2007 | US |
Number | Date | Country | |
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Parent | 12212166 | Sep 2008 | US |
Child | 12652287 | US |