Laser archery distance device - Patent Review 4753528

Description Submit all comments and votes

BACKGROUND OF THE INVENTION

The invention relates to a method and apparatus for determining the distance to an archery target.

The use of bow and arrow for game hunting or target shooting is one of the most popular recreational activities throughout the world. Indeed, more than $1 billion is spent each year on purchases of bows alone. In shooting beyond distances of approximately 15 yards, which is almost always required in game hunting, the accuracy of the shot is dependent upon the ability of the archer to adjust the drop of the arrow due to gravity. A skilled archer can accurately hit target distances within approximately 50 yards.

Several techniques have been employed in the past for aiding in effecting the required compensation. The most popular technique employs pins which are spaced apart on the bow. In theory, for a particular type animal such as a deer, the bow angle will be correct when a particular set of two pins are exactly bracketed by the back and belly of the animal. This technique is, however, extremely rough since it presupposes that animals are of the same size and that the pull of each hunter on the string will be the same. Manual optical stereoscopic sights such as used for hunting with guns have also been employed. Such sights are in practice too slow and cumbersome to be of benefit in archery hunting.

The present invention relates to a unique apparatus adapted for mounting on the bow for providing accurate indication to the hunter of the distance to a target. Once the hunter knows the exact distance to the target, he can readily determine from experience or written instructions what angle to the horizontal should be employed for a given pull of the string.

This is achieved by directing a beam of collimated light, preferably coherent radiation from a small solid state laser, to the target so that, when the bow is aimed at a target, light reflected from the target is received by a linear photosensitive element which produces an output indicating the position of the incident radiation in a linear direction. The element and laser are mounted so that the position along the element indicates the distance to the target. Appropriate circuitry is further provided to determine that distance and preferably to digitally display the same to the hunter.

Other objects and purposes of the invention will be clear from the following detailed description of the drawings.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 shows a schematic view of the unique present invention illustrating the theory of operation thereof;

FIG. 2 shows a view of a linear photosensitive element;

FIG. 3 shows a perspective view of the present invention mounted in place on a compound bow;

FIGS. 4a and 4b show, respectively, the side and front of the housing of the present invention as mounted in FIG. 3;

FIG. 5 shows a detailed schematic of a circuit for producing a signal indicating the linear position of the incident beam and hence the target distance;

FIG. 6 shows a schematic view of another circuit for producing a digital display of the distance;

FIG. 7 shows a waveform diagram of the signals produced by the circuits of FIGS. 6 and 8;

FIG. 8 shows a schematic view of another circuit for producing a signal indicating the linear position of the incident beam and hence the target distance.

DETAILED DESCRIPTION OF THE DRAWINGS

Reference is now made to FIG. 1 which illustrates schematically the operation of the present invention. Collimated light, preferably from a laser 20, is directed by a lens 22 toward a target at which the bow is aimed. Three targets P.sub.1, P.sub.2 and P.sub.3 are shown in FIG. 1 at different distances from laser 20. Light reflected from a target at distance P.sub.1 is reflected back to a linear photosensitive element 24 at an angle so that it is incident on photodetector element 24 via lens 26 at a location P.sub.1 '. A target at P.sub.2 directs a reflection to element 24 via lens 26 to impinge at a different location P.sub.2 ', while reflected radiation distance P.sub.3 is received on photodetector element 24 at location P.sub.3 '. Therefore, the position, D, of the target can be determined from the position, X, of the incident reflected radiation on the photosensitive element 24.

In FIG. 1, the dimension A is the separation distance between the transmit lens and the receive lens, B is the focal length of the receive lens, X is the distance the received image moves on the photosensor with respect to the optical axis as the target distance varies, and D is the target distance. By similar triangles, then ##EQU1##

Referring to FIG. 2, the linear photosensitive element is illustrated for the purpose of explaining the manner in which the position of the incident radiation on element 24 is determined. Any suitable linear photosensitive element can be employed and several types are available as off-the-shelf items.

In such a photodiode, the current output is both a function of the intensity of the incident radiation and its position. Assuming in FIG. 2 I.sub.1 is the current through cathode K.sub.1, then such current is proportional to the distance x from the edge of the photodiode and to the intensity S of the received light. Similarly, I.sub.2 current through the other cathode K.sub.2 is proportional to the distance 2-x and also to the intensity S of the received light. Thus,

I.sub.1 .alpha.Sx (.alpha. means proportional to)

I.sub.2 .alpha.S(1+1-x)=2S-xS

I.sub.1 +I.sub.2 =Sx+2S-xS=2S

I.sub.1 -I.sub.2 =SX-2S+xS=2S(x-1)

so that ##EQU2##

Accordingly, the sum of the two currents is a function of the intensity of the received light and the ratio of the difference of the currents divided by the sum of the currents a function of the position x.

If a common amplifier is used for both currents so that the system gain, K, is the same for both signals, then an automatic gain control (AGC) is used to set I.sub.1 at unity. ##EQU3##

With appropriate offsets and scale factors then, ##EQU4##

The output current I.sub.2 " is then a direct linear function of the target distance when current I.sub.1 is held constant with an AGC.

Referring to FIGS. 3, and 4a and 4b laser 20, element 26 and the associated circuitry are mounted within a housing 40 which is attached to the bow 42 as shown in FIG. 3. As can be seen in FIG. 4a, the lenses 22 and 26 respectively transmitting and receiving the laser radiation are mounted in linear separation as described above. The housing 40 may be of any suitable material and fastened to the bow in any suitable fashion.

Referring now to FIG. 5, currents I.sub.1 and I.sub.2 are respectively amplified in transimpedance amplifiers 30 and 32 with the outputs of each amplifier being applied respectively to a conventional summing amplifier 34 and to conventional difference amplifier 36. The respective outputs of amplifiers 34 and 36 are applied to a conventional dividing circuit 38 so that, as indicated, the output reflects the ratio therebetween and, accordingly, the position x.

Reference is now made to FIG. 6 which illustrates another embodiment of the present invention. In this circuit, the sum of the amplitudes is used to control a gain control amplifier so that the sum is kept constant and, therefore, the difference directly indicates the position of the incident reflected radiation.

A conventional clock 50, generating a basic timing square wave, as shown in FIG. 7, drives a pulse generator 52 in this embodiment. Pulse generator 52 in turn triggers a conventional laser driver 54 to drive solid state laser 20 so that it produces a sequence of pulses of approximately one microsecond at 500 pulses repetition. These pulses are directed to the target at which the bow is aimed, as discussed above.

The returned pulses are received by photodiode element 24 and the two current signals produced at cathodes K.sub.1 and K.sub.2 respectively applied to amplifiers 30 and 32. These amplifiers respectively convert currents I.sub.1, I.sub.2 into amplitudes e.sub.1, e.sub.2 proportional to the currents. Switch circuit 62A alternatively applies the outputs e.sub.1, e.sub.2 of amplifier 30 and 32 to an automatic gain control (AGC) amplifier 64 in accordance with the output of pulse generator 52 and as shown in FIG. 7.

The automatic gain control amplifier 64 is controlled by the sum of the signals from the element 24 so that the signal representing the difference indicates the distance to the target. Circuit 64 also compensates for the wide range of beam intensity received resulting from different target reflectivities and distances.

The output of AGC amplifier 64 is applied to a hold amplifier 66 which, as shown in FIG. 7(h) alternatively provides an output indicating the amplitude of the two currents from element 24. The hold signals are synchronized to the peak output of the return pulses. The use of a single hold circuit improves the circuit accuracy over one in which separate hold circuits are provided since there is no requirement to match the two hold circuits. The pulses are converted to a composite rectangular wave at the hold amplifier 66 and the signal separated by switch circuit 62B into two rectangular waves proportional to the current signals from element 24. These two signals are then converted to d.c. levels at peak detectors 68 and 70 and the d.c. levels applied respectively to the sum and difference amplifiers 34 and 36. Since the d.c. level has a discontinuity at the sample gate, the d.c. outputs are also filtered by circuits 68 and 70. As noted above, the output of sum amplifier 34 is applied to a control amplifier 76 which in turn controls automatic gain control amplifier 64 so that the output of difference amplifier 36 indicates the distance to the target. The output of amplifier 36 is applied to an analog-to-digital conversion circuit 78 which converts the analog signal to a BCD output. The output of circuit 78 is applied to a conventional digital display 80 mounted on the unit and viewable to the archer to indicate precisely the distance to the target at which he has aimed. Any suitable display in that regard can be utilized.

Reference is now made to FIG. 8 which illustrates a further and preferred embodiment of the present invention. In this circuit, the current from one side of the photosensor is used to control an automatic gain control amplifier 64 so that the current is kept constant and, therefore, the current from the other side of the photosensor directly indicates the distance of the incident reflected radiation.

A conventional clock generating a basic timing square wave, as shown in FIG. 8, drives a pulse generator 52 which in turn triggers a conventional laser driver 54 so that the solid state laser 20 produces a sequence of pulses of approximately one microsecond at 500 pulses repetition. These pulses are directed to the target at which the bow is aimed as discussed above.

The returned pulses are received by photodiode element 24 and the two current signals produced at cathodes K.sub.1 and K.sub.2 respectively applied to amplifiers 30 and 32. Switch circuit 62A alternatively applies the outputs of amplifiers 30 and 32 to an automatic gain control amplifier 64 in accordance with the output of pulse generator 52 and as shown in FIG. 8.

The automatic gain control amplifier 64 is controlled by a signal produced from current I.sub.1 of element 24, so that the signal representing the current I.sub.2 indicates the distance to the target. AGC 64 also compensates for the wide range of beam intensities received resulting from different target reflectivities and distances.

The output of AGC amplifier 64 is applied to a hold amplifier 66 which as shown in FIG. 8 alternatively provides an output indicating the amplitude of the two currents from element 24. The hold signals are timed to the peak output of the return pulses. The use of a single hold circuit improves the circuit accuracy over one in which separate hold circuits are provided since there is no requirement to match the two hold circuits. The pulses are converted to a composite rectangular wave at the hold amplifier 66 and the signal separated by switch circuit 62 B into two rectangular waves proportional to the current signals from element 24. These two signals are then converted to d.c. levels at peak detectors 68 and 70. Since the d.c. level has a discontinuity at the sample gate, the d.c. outputs are also filtered by circuits 68 and 70. As noted above, the output of filter 68 is applied to control amplifer 76 which in turn controls automatic gain control amplifier 64 so that the output of filter 70 with appropriate offsets and scale factors indicates the distance to the target. The output of filter 70 is applied to an analog-to-digital conversion circuit 78 which converts the analog signal to a BCD output. The output of circuit 78 is applied to a conventional digital display 80 mounted on the unit and viewable to the archer to indicate precisely the distance to the targer at which he has aimed. Any suitable display in that regard can be utilized.

Many changes and modifications of the above-described embodiment of the invention can, of course, be carried out without departing from the scope thereof. Accordingly, that scope is intended to be limited only by the scope of the appended claims.

* * * * *