This invention relates to optical weapon sights such as riflescopes, reflector sights and holographic sights which superimpose a reticle pattern on an image of the target.
A riflescope (also called a “scope” for short) is an optical weapon sight based on the Keplerian telescope. In its most basic form, a riflescope is a Keplerian telescope with a reticle or cross hairs added to mark the “point of aim”. A riflescope must be mounted on a rifle such that its aiming axis (optical axis) is aligned with the rifle's barrel axis as shown in
Early riflescopes were equipped with an external-adjustment system built into the mounts. Their point of aim was adjusted by mounts having micrometer windage and elevation mechanisms that moved the entire scope laterally and/or vertically. An advantage of external-adjustment scopes is that all the lens elements and the reticle remain centered on the same optical axis, providing highest image quality. The disadvantage of the external-adjustment mechanism is that the mounts must be able to support the entire weight of the riflescope under recoil. The external adjust mechanism is also bulky, heavy and susceptible to mud and dirt when used in the field.
Most modern riflescopes have an internal-adjustment mechanism using threaded screws mounted in turrets. The screws are connected to external knobs which are accessible by the shooter. Turning the knobs moves the reticle assembly inside the main tube against spring pressure. The knobs have clearly marked graduations around their circumference and many have a ball-detent system that clicks as the adjustment screws are turned. Each graduation or click represents a change in reticle position such that the point of aim is shifted by a small amount on the target. In modern riflescopes the graduations are commonly expressed as 1 cm at 100 m or 0.5 inch at 100 yards. The graduations may also be expressed in minutes of arc (MOA) or milliradians (mil). For the purpose of zeroing-in a rifle, 1 MOA is considered to be equal to 1 inch at 100 yards. Similarly, 0.1 mil corresponds to 1 cm at 100 m. These conventions are used in the present invention as well.
In recent years, several optical adjustment mechanisms have been invented by the present author to replace the mechanical adjustment mechanism described above. U.S. Pat. No. 8,749,887 issued on Jun. 10, 2014 describes a riflescope wherein a pair of movable wedge prisms are positioned between the objective lens and its focal plane. U.S. Pat. No. 9,164,269 issued on Oct. 20, 2015 and U.S. Pat. No. 9,644,620 issued on May 9, 2017 describe mechanisms that utilize tiltable and rotatable wedge prisms for adjusting the point of aim in a riflescope.
The present invention discloses a simpler design: the point of aim is adjusted by attaching one or more wedge prisms in front of the objective.
This invention introduces a method for zeroing-in an optical weapon sight by attaching one or more thin wedge prisms to the front of the sight. For brevity, the invention is described with reference to a riflescope but it can be adapted to any type of optical weapon sight such as a reflex sight, red-dot sight, or holographic sight.
The foregoing aspects and many of the attendant advantages of this invention will become more readily apparent with reference to the following detailed description of the invention, when taken in conjunction with the appended claims and accompanying drawings, wherein:
A. Principle of Operation
This invention uses the principle of light refraction by thin wedge prisms. According to Snell's Law when a ray of light enters a transparent material the ray's direction is deflected, based on both the entrance angle (typically measured relative to the normal to the surface) and the material's refractive index. A light beam passing through a wedge prism is deflected twice: once entering, and again when exiting. The sum of these two deflections is called the deviation angle (
It follows from Snell's law that the beam deviation of a wedge prism is governed by the following formula:
In the above formula α is the beam deviation angle, ξ is the apex angle of the prism, ϕ is the incidence angle of the incoming beam and n is the index of refraction of the glass material used for making the prism. When the incident light is close to normal to the prism surface (i.e. ϕ≈0) and for a thin prism (i.e. ξ≤60), the formula (1) reduces to
α≈(n−1)ξ. (2)
Therefore, for thin wedge prisms the deviation angle α is practically independent of the incidence angle and is solely determined by the prism's apex angle and glass type. In this invention, the deviation angle α is also called “deviation power” or “deviation magnitude” associated with a thin wedge prism. For the purposes of this invention, the wedge prisms will be designed such that their deviation powers αi will be a fraction of a degree. Example values are 1 MOA, 2 MOA, and 5 MOA.
A wedge prism deflects light towards its base. Therefore, we define a hypothetical axis which connects the apex of the prism to its base, as its “deviation axis”. The “deviation direction” or “deviation orientation” θ of the prism is defined as the angle between the prism's deviation axis and the vertical axis (x axis as shown in
If two or more thin wedge prisms are stacked together, their deviation powers will be additive.
In three dimensional space, it is possible to orient a thin wedge prism such that its deviation axis points to any direction in the x-y plane. In this case, the total deviation provided by the prisms will be the vector sum of the deviation provided by each individual prism. With reference to
a=a1+a2. (3)
Calculating the total deviation power a and the deviation direction θ strictly from the polar coordinates (α1, θ1) and (α1, θ1) requires solving complicated trigonometric formulas. However, this calculation is greatly simplified if the two wedge prisms are oriented such that their deviation axes are parallel, i.e θ1=θ2. In this case the deviation power of the prisms are simply added together:
α=α1+α2 (4)
θ=θ1=θ2 (5)
Another situation where it is relatively easy to calculate the total deviation power α and the deviation direction θ is when then two wedge prisms have equal deviation power, i.e. α1=α2. In this situation the resulting deviation direction will be along the bisector of the angle δ formed between the deviation axes of the prisms. The deviation power can range between 0 and 2α1 depending on the angle δ:
B. Method for Zeroing-in a Riflescope Using Attachable Wedge Prisms
To use the optical adjustment method disclosed in the present invention, the user should first mount the riflescope on his rifle. The riflescope should be mounted on top of the receiver (or barrel) such that its optical axis is in line with the axis of the barrel. Due to the dimensional variations in the mounts, the optical axis of the riflescope is rarely exactly in line with the barrel. The fact that the trajectory of a bullet does not coincide with the line of sight (which is always straight) necessitates additional corrections as well. Therefore, the user should determine if there is any correction required to align the “point of aim” shown by the riflescope with the actual “point of impact” of the rifle.
This misalignment between the point of aim and the point of impact (also called aiming error) can be determined by shooting a group of three shots at a test target located 100 m away (see
After attaching the wedge prisms, the user may fire another group of three shots at the test target to verify that his rifle shoots to the desired point of impact. If any fine tuning is needed, the user can add more corrector prisms or adjust the orientation of the attached prisms slightly. Once the rifle's zero is verified, the shooter can take his rifle to the field and use it for hunting or target shooting.
The examples below further illustrate the method of zeroing-in the riflescope according to the present invention. The first example shows how to correct the point of aim of the riflescope using just a single wedge prism:
Consider that a hunter purchases a riflescope and mounts it on his rifle. In a weekend, the hunter goes to the shooting range and test-fires his rifle at 100 m. He examines the point of impact on the target and determines that a correction of 15 cm along a direction of 30° measured clockwise from the vertical axis is required to zero-in the rifle (
The next example shows how the aiming correction can be performed using two corrector prisms oriented along x or y coordinates:
Assume that a hunter using the riflescope according to this invention determines the aiming error of his rifle in Cartesian coordinates as shown in
The hunter first selects a wedge prism with deviation power of 10 cm at 100 m (1 mil) and attaches it to the front (objective side) of the riflescope such that the deviation axis of the prism points in the x direction (vertical). He then chooses a wedge prisms with deviation power of 5 cm at 100 m (0.5 mil) and attaches it to the front of riflescope such that the deviation axis of the prism points in the y direction. The riflescope is now zeroed-in. The hunter can fire a second group of three shots to verify his zero. The bullets should now hit near the center of the target.
While it is easy to use Cartesian coordinates, it is usually more efficient to zero-in the riflescope in polar coordinates. The next example shows how to zero-in a riflescope using two corrector prisms whose deviation axes are kept aligned:
Assume that a hunter purchases the riflescope described in this invention and mounts it on his new high-quality hunting rifle. Next, he takes the rifle to the shooting range and using a steady bench rest fires three shots aiming at the center of a target located 100 m away. Upon examining the target, he determines that a hypothetical vector connecting his point of aim to the the centroid of the holes (which indicate the rifle's point of impact) is 15 cm long and has a 30 degree angle measured clockwise from the vertical axis. With reference to
Once the magnitude and the direction of required correction is determined the hunter selects two wedge prisms with deviation power of 0.5 mil (5 cm at 100 m) and 1 mil (10 cm at 100 m) from the collection of wedge prisms supplied with the riflescope. He stacks these prisms together making sure that their deviation axes are aligned. This way, the deviation power of the prisms will be simply added to create a total deviation power of 15 cm at 100 m (equal to the required correction magnitude). The hunter then attaches the two prisms to the front of his riflescope such that the deviation axis of the prisms is oriented at 30 degrees clockwise from the vertical axis as shown in
The riflescope is now zeroed-in! The hunter can fire another group of three shots to verify that his rifle's point of aim is aligned with point of impact.
In the final example, we consider a case where the magnitude of the required correction is not an exact sum of the magnitudes provided by the wedge prisms supplied with the riflescope:
Consider the scenario described in Example 3 but assume that the distance between the point of impact and the point of aim was slightly shorter. For example, let's assume α=18 cm and θ=30°. The hunter should use two wedge prisms with α1=10 cm and α2=10 cm (i.e. of equal power and whose sum being larger than the required correction magnitude). Next, he should orient the deviation axes of the prisms such that θ1 is slightly more than 30° and θ2 is slightly less than 30° as shown in
The hunter may use the formula (7) mentioned in Section VI-A to first calculate an acute angle δ such that the required deviation magnitude α=18 cm is produced:
Then, attach the wedge prisms to the front side of his riflescope such that the bisector of the angle between the prisms is aligned with the required correction orientation θ=30°. This is achieved when
Alternatively, the hunter can use trial and error and adjust θ1 and θ2 manually such that a total deviation of 18 cm in the direction of 30° from the vertical axis is achieved.
The examples above illustrate how the method disclosed in this invention can be used to zero-in a non-adjustable riflescope (or other optical sight) with as few as a single wedge prism. In most practical cases, a user should be able to zero-in the riflescope using one or two wedge prisms following the rules of vector addition as described in subsection VI-A.
It is preferred that the wedge prisms are mounted inside a housing so that they can be more conveniently attached to an optical weapon sight. It is also preferred that the deviation power and the deviation axis of each prism is marked on its housing as shown in
The method introduced in this invention has several significant advantages over the prior art, including but not limited to the following:
The foregoing disclosure is believed to be sufficient to enable an ordinary person skilled in the art to build and use the invention. In addition, the description of specific embodiments will so fully reveal the general nature of the invention that others can, by applying current knowledge, readily modify and/or adapt for various applications such specific embodiments without undue experimentation and without departing from the generic concept. For example, the steps required to perform the methods of zeroing-in a riflescope described in Section VI-B can be performed by a machine rather than a human user (a robotic device used in an assembly line can mount a telescopic sight on a rifle, measure the angular misalignment between the aiming axis and the barrel axis, and attach a required number of prisms to correct the riflescope's point of aim). Such adaptations and modifications should and are intended to be comprehended within the meaning and range of equivalents of the disclosed embodiments.
It is to be understood that the phraseology or terminology herein is for the purpose of description and not of limitation, such that the terminology or phraseology of the present specification is to be interpreted by the skilled artisan in light of the teachings and guidance presented herein, in combination with the knowledge of one of ordinary skill in the art. Thus, the scope of the invention should be determined by the appended claims and their legal equivalents, as opposed to the embodiments illustrated.
This is a divisional application carved out of application Ser. No. 15/990,815 filed on May 28, 2018 now U.S. Pat. No. 10,502,530. This application claims the benefit of the earlier filing date of said prior-filed application which is incorporated herein by reference in its entirety. Parts of the specification and the drawings that were not relevant to the claims presented herein have been omitted. Some editorial updates have been made to the remaining text to better illustrate the invention. No new material has been added.
Number | Name | Date | Kind |
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8749887 | Jahromi | Jun 2014 | B2 |
9164269 | Jahromi | Oct 2015 | B1 |
9644920 | Jahromi | May 2017 | B2 |
20050039370 | Strong | Feb 2005 | A1 |
20160266372 | Baker | Sep 2016 | A1 |
Number | Date | Country |
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1930760 | Jun 2008 | EP |
Number | Date | Country | |
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Parent | 15990815 | May 2018 | US |
Child | 16699589 | US |