The present invention relates to a splatter indicator sight for firearms. More specifically, the present invention is concerned with an indicator device for processing data regarding variables affecting the bullet trajectory and creating a visual map of all of the probable hit zones after the user has aimed the firearm at the target, thereby allowing the user to evaluate the risk of hitting the wrong target before shooting.
Firearms, such as handguns (single-shot pistols, revolvers, and semi-automatic pistols), long guns (rifles, carbines or shotguns) and machine guns or the like are aimed at their targets with greater accuracy by using sights. Many sights can be mounted onto firearms, for example, telescopic sights (or scopes), iron sights, red dot sights, and laser sights.
Despite these existing sighting systems, aiming errors still occur. Those errors depend to some degree on the skill of shooter, but also the quality and caliber of the firearm and other exterior conditions such as the range to the target, the movement of the target, the ambient light, and the wind. The aiming error becomes a considerable issue when the firearm is used by security forces in civilian zones where there exists a risk of hitting an innocent bystander or other friendly by accident.
The prior art reveals processing of data affecting the bullet trajectory in order to correct the aim or provide warnings to the user (where data received from sensors mounted onto the firearm or entered by the user is processed and provides for the automatic adjustment of aim, stabilization as well as the display of data related to aiming error) these existing aids focus on perfecting the aim. Potential for error still exists, however, and a shot fired might fall within an area surrounding the point of aim. Therefore, there is a need for a device that will clearly and quickly indicate the probable hit zones around the aiming point to let the user better decide whether or not to shoot.
In order to address the above and other drawbacks there is provided a method for supporting a decision to fire a projectile from a firearm having a firearm accuracy and pointed towards an intended target and an unintended target. The method comprises pre-calculating as a function of the firearm accuracy a first region surrounding a point of aim within which a projectile issued from the firearm will strike with a known probability, aiming the firearm at the intended target, delineating the first region about the point of aim with a laser affixed to the firearm, and not firing when at least a portion of the unintended target is within the first region.
There is also provided a method of providing a visible gun sight for a firearm having an accuracy. The method comprises pre-determining as a function of the firearm accuracy a first region surrounding a point of aim within which a projectile issued from the firearm will strike with a known probability, aiming the firearm at the intended target, and outlining the first region about the point of aim with a laser affixed to the firearm.
Other objects, advantages and features of the present invention will become more apparent upon reading of the following non-restrictive description of specific embodiments thereof, given by way of example only with reference to the accompanying drawings.
In the appended drawings:
The present invention is illustrated in further details by the following non-limiting examples.
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A variety of approaches may be used for generating and projecting the risk zone map 20 on a target 26 using a laser 14.
For example, in a first illustrative embodiment of same, the actual lasing action can be used to set the desired beam divergence. In other configurations a laser will generate a beam with a given divergence (typically on the order of 0.5-10 mrad) and then the desired spread angle will be set with external collimating optics. Lasing action in the laser cavity can be controlled to some degree with the configuration of the laser cavity, adjusting parameters such as mirror curvature, spacing, selection of location of the beam waist, inter-cavity apertures, bore diameter, etc. Specifically, in semiconductor (diode) lasers, an apparent point source can be generated by ion milling (or similar) a convex high reflector mirror into the diode laser's cavity.
In a second illustrative embodiment divergence of the laser can be introduced using a collimating telescope. In this regard, a single, solid cone of light is generated from a single laser source and a Galilean or Keplerian telescope is placed in the beam to collimate, or decollimate, the emitted laser beam. These telescopes may use two or more optics. Adjustment between the separation distance of these two optics in either telescope (focus) can provide for a change in the divergence angle of the emitted beams.
In the above two embodiments, it may also be desirable to utilize a beam diffuser, of which a number of known types exist, to generate a more uniform beam profile (top hat), prior to adjusting the beam divergence. This provides for much more uniform laser spot illumination assisting visibility and more carefully defining the edge of the desired spot.
In a third illustrative embodiment a diffuser may be used in conjunction with the laser 14 to generate a cone angle. Rather than using a telescope to change the natural divergence of the generated beam, a diffuser may be designed and used to generate a cone of light of the desired angle. Although “opal glass” or rough surface glass diffusers are common and could potentially be used, a Holographic Optical Element (HOE) diffuser is preferable.
In a fourth illustrative embodiment, HOEs are designed and used to shape light to precise shapes and patterns as they provide a low cost and optically efficient means to make complex projection patterns. In particular, both binary and diffractive optics, which are closely related, are included here. Employment of a custom pattern/angle HOE or other phase mask may be used for some implementations.
In a fifth illustrative embodiment, rear illumination and subsequent collimation of a window or mask pattern can be used. This would typically be a glass or plastic window with a pattern applied opaquely, such as chrome on glass, a chemically etched or laser cut stainless steel stencil or similar. A lens or lens system is used downstream of the window to gather light and collimate to the desired angle of divergence. The pattern disc may be somewhat diffuse in nature.
In a sixth illustrative embodiment, the risk zone map 20 is the result of a vector scan which traces the desired image or pattern using a rapidly moving spot. Scanning of simple patterns such as circles can be achieved with a spinning off axis mirror, wedge cut refractive optic or the like. Complex patterns can be achieve by spinning HOE scanner optics, or more conventionally with XY galvanometer scanners. The same result might also be achieved with MEMs scanning devices such a DLPs, GLVs and related technologies.
In a seventh illustrative embodiment, areas can be delineated with the use of multiple static spots rather than full vector or filled patterns. This is discussed more below as an additional claim as a way to increase the image brightness.
The visibility of the laser light on a target is determined by the energy density at the target location reflected back to the viewer's location. Even low power laser light may be quite visible when viewed at a significant distance if it remains in a small spot. However, if the angle of divergence is significant, and/or the spot is large, as it may be at long distances, practical and/or safe levels of laser light may not be as visible as would be desirable when the spot spreads to a large diameter. In order to address this problem, one solution is to delineate the diameter of an imaginary circle or box with two or more individual low divergence (small diameter) beams to maintain brightness with low levels of power. These multiple beams could be generated with multiple lasers, or with discrete optics or HOE, diffractive or binary optics to generate multiple beams from a single input beam (single laser).
As discussed above, the effect of the offset and/or parallax between the path of the bullet and the path of the laser light can affect can vary from moderate to insignificant depending on the distance from the firearm to the target. Indeed, if the laser is simply a cone of light being emitted from a device mounted, for example, to the top of the barrel of the firearm, for example like a riffle scope, there is offset between the origin of the path of the laser light and the path of the projectile (bullet). If the natural fall of the bullet is not taken into account, both the laser light and the bullet will travel a straight path, separated by 1-2 inches. If the target is at a significant distance, this offset is likely insignificant due to the inherent spread pattern or error in the bullets flight path. However, if the target is close to the weapon there will be offset, or alternately parallax.
In order to address this problem, the end of the barrel can be fitted with a mechanism such that the beam or beams are emitted uniformly around or directly down the axis of the barrel. This can be achieved in a couple of different manners.
Firstly, a reflector can be placed at some angle at the end of the barrel (typically 45 degrees). This reflective optic, such as a flat mirror will have a hole in the center to allow the passage of the projectile, while still allowing reflection of the light in a path concentric with the projectile.
Secondly, an optic can be used to collimate the light around the path of the projectile which is not a planar (flat) mirror, but may be a concave optic such as an off axis parabola. These approaches would also have a hole in the center, through which the projectile can pass.
Thirdly, a diffractive, holographic, binary or phase grating can be used to shape the light into the desired collimated pattern without a concave shape/curved surface.
Depending on the use environment, front surface mirrors may be desired.
Alternatively, one beam could be emitted above or below the barrel and one to the right or left of the barrel. In this way, the user imagines the intersection of a horizontal and vertical line as the center of emission, and then uses the location of the two beam spots to construct a square or circle which represents the risk zone map.
Also, for special single use conditions, a pellicle beam splitter can be placed directly over the end of the barrel at some angle, typically 45 degrees. The pellicle beams splitter is made from a very thin optically reflective layer of cellulous, mylar or similar material. The thickness of this material can be just a few microns such that it is an extremely thin weak film which will be pierced with milligrams of force and thus not affect the projectile, thereby allowing the emitted laser light to be aligned precisely with the bore of the weapon with zero offset or parallax. It can be noted that the pellicle beam splitter is effectively a tympanic membrane and will respond to acoustic vibrations (sound), this may limit its use in some situations. Alternately, a solid but very thin glass beam splitter could be used and shatter upon use.
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Another parameter of interest (discussed briefly above) and which may also be used to determine the proportions of the risk zone map 20 is the MOA. MOA is a unit of angular measurement equal to one sixtieth ( 1/60) of one degree. One (1) MOA is one inch at 100 yards (91 meters). MOA is often used when characterizing the accuracy of rifles and indicates that, under ideal conditions, the firearm in question is capable of repeatedly producing a group of shots whose center points (center-to-center) fit within a circle, the diameter of which can be subtended by that amount of arc.
Although the present invention has been described hereinabove by way of specific embodiments thereof, it can be modified, without departing from the spirit and nature of the subject invention as defined in the appended claims.
This application is a divisional application of U.S. patent application Ser. No. 12/352,355, now pending, filed on Jan. 11, 2009, which itself claims benefit of U.S. provisional application Ser. No. 61/020,515, filed on Jan. 11, 2008. All documents above are incorporated herein in their entirety by reference.
Number | Date | Country | |
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61020515 | Jan 2008 | US |
Number | Date | Country | |
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Parent | 12352355 | Jan 2009 | US |
Child | 13554021 | US |