Crosswind speed measurement by optical measurement of scintillation
The present disclosure describes methods and systems for measuring crosswind speed by optical measurement of laser scintillation. One method includes projecting radiation into a medium, receiving, over time, with a photodetector receiver, a plurality of scintillation patterns of scattered radiation, comparing cumulative a radiation intensity for each received scintillation pattern of the received plurality of scintillation patterns, and measuring a cumulative weighted average cross-movement within the medium using the compared cumulative radiation intensities.
1. A device for optically measuring crosswind, comprising:
a laser transmitter adapted to generate a laser to illuminate a path through an atmosphere;
a plurality of receivers, each receiver comprising a single-pixel photodiode coupled with distinct optics and adapted to analyze the path of the laser through the atmosphere, each receiver spaced apart from other receivers at a known particular distance, each receiver receiving a scintillation pattern created by atmospheric eddies diffracting and refracting scattered laser radiation, and, for each receiver, converting the received scintillation pattern into a single data point measuring cumulative light intensity; and
the device adapted to compare cumulative light intensities from each receiver and to generate a crosswind profile along the path of the laser.
2. The device of claim 1 , further comprising another receiver spaced apart from the plurality of receivers at a known particular distance and in a direction perpendicular to the plurality of receivers.
3. The device of claim 2 , wherein the device is adapted to provide multi-axis scintillation pattern movement determinations.
4. The device of claim 1 , wherein the optics further comprise micro optics coupled with diaphragms that selectively permit illumination of different parts of a particular single-pixel photodiode.
5. The device of claim 1 , wherein a particular single-pixel photodiode is a quadrant photodetector.
6. The device of claim 1 , wherein the receiver further comprises collection optics used to optically filter or isolate, using at least one of polarization or diffraction techniques, the scattered laser radiation in the atmosphere.
7. The device of claim 1 , wherein the laser transmitter is one of a light emitting diode (LED), a super-luminescent diode (SLED), a liquid laser, a gas laser, or a solid laser.
8. The device of claim 1 , wherein the laser transmitter is adapted to emit a laser of differing power, frequency, or optical property.
9. The device of claim 1 , further comprising:
a memory configured to hold the generated crosswind profile; and
a processor interoperably coupled to the memory and configured to calculate a ballistic solution using the generated crosswind profile.
10. The device of claim 9 , further comprising the processor configured to initiate transmission of data associated with the ballistic solution to a sighting device.
11. The device of claim 1 , wherein the laser illuminates a target that reflects laser radiation back to the plurality of receivers.
12. A device for optically measuring a cross-movement profile within a medium, comprising:
a plurality of receivers spaced apart from other receivers at a known particular distance, each receiver comprising a single-pixel photodiode coupled with distinct optics and adapted to analyze a path of a laser through a medium, each receiver adapted to receive from a substantially common direction and, over time, a plurality of snapshots of a moving scintillation pattern created by eddies in the medium due to temperature gradients diffracting and refracting scattered laser radiation, and for each receiver, converting each received snapshot into a single data point measuring cumulative light intensity; and
the device adapted to compare cumulative light intensities from each receiver and to generate a cross-movement profile within the medium, the generation of the cross-movement profile a function of the particular spacing between, and a size of, each of the plurality of receivers.
13. The device of claim 12 , wherein the medium is one of a liquid or a gas.
14. The device of claim 12 , further comprising a radiation emitter.
15. The device of claim 12 , further comprising:
a memory configured to hold the generated cross-movement profile within the medium; and
a processor interoperably coupled to the memory and configured to calculate a ballistic solution using the generated cross-movement profile within the medium.
16. The device of claim 12 , wherein the laser illuminates a target that reflects laser radiation back to the plurality of receivers.
17. A method for measuring cross-movement within a medium for medium-profiling purposes, comprising:
projecting radiation into a medium to illuminate a path through the medium;
receiving, over time, with a photodetector receiver of a plurality of photodetector receivers, a plurality of scintillation patterns, each scintillation pattern created by eddies in the medium diffracting and refracting scattered radiation, each photodetector receiver spaced apart from other photodetector receivers at a known particular distance, and each photodetector receiver comprising a single-pixel photodiode coupled with distinct optics;
for each photodetector receiver, converting each received scintillation pattern into a single data point measuring cumulative radiation intensity;
comparing the cumulative radiation intensity for each received scintillation pattern of the received plurality of scintillation patterns; and
calculating a cumulative weighted average cross-movement within the medium along the path using the compared cumulative radiation intensities.
18. The method of claim 17 , wherein the medium is one of a liquid or a gas.
19. The method of claim 17 , further comprising:
calculating a ballistic solution for a projectile using at least the calculated cumulative weighted average cross-movement within the medium; and
calculating a weapon aiming offset using the calculated ballistic solution.
20. The method of claim 17 , further comprising:
determining that a particular scintillation pattern is moving;
determining a direction-of-movement for the particular scintillation pattern; and
determining a speed-of-movement for the particular scintillation pattern.
21. The method of claim 20 , wherein the determination that the particular scintillation pattern is moving is performed by a cross-covariance computation between two or more scintillation patterns.
22. The method of claim 20 , further comprising providing a multi-axis scintillation pattern movement determination.
23. The method of claim 17 , wherein the laser illuminates a target that reflects radiation back to the plurality of receivers.