Apparatus and method for non-intrusive off-body measurements in hypersonic flight experiments

• US 10,060,777 B2
• Filed: 05/04/2016
• Issued: 08/28/2018
• Est. Priority Date: 05/05/2015
• Status: Active Grant

• Current Assignee: Alan B. Cain, Rennie R. Mark, Stanislav Gordeyev
• Original Assignee: Alan B. Cain, Rennie R. Mark, Stanislav Gordeyev
• Inventors: Cain, Alan B, Gordeyev, Stanislav, Rennie, R. Mark
• Primary Examiner(s): Gray, Francis
• Application Number:
  US15/146,805
• Publication Number:
  US 20160327448A1
• Time in Patent Office: 846 Days
• CPC Class Codes: G01F 1/661 using light
• CPC Class Codes: G01F 1/7086 using optical detecting arrangements
• CPC Class Codes: G01F 1/712 using auto-correlation or cross-correlation detection means
• CPC Class Codes: G01M 9/065 dealing with flow
• CPC Class Codes: G01M 9/067 visualisation
• CPC Class Codes: G01P 5/26 by measuring the direct influence of the streaming fluid on the properties of a detecting optical wave

Abstract

An “air-data probe” system measures at least one component of freestream velocity by tracking the motion of a laser-induced breakdown (“LIB”) spark created in a freestream flow. Neutral density filters are positioned or deployed so that the brightness of the initial LIB spark doesn'"'"'t over saturate the LIB sensor system. This allows for more consistent tracking of the LIB spark throughout the duration of the LIB spark, including the later stages where the LIB spark is not nearly as bright as the initial LIB spark, thereby allowing all or substantially all of the light generated by the LIB spark to reach the sensors. This provides for enhanced visibility and more accurate detection of the LIB spark over time and as air density changes.

Claims

1. A method of measuring at least one component of freestream velocity for a vehicle comprising the steps of:

providing at least one laser;

providing a plurality of cameras;

generating a laser-induced breakdown spark from the at least one laser at a point away from the vehicle;

positioning at least one neutral density filter between the cameras and the laser-induced breakdown spark;

using the plurality of cameras to monitor and capture a plurality of physical characteristics associated with the laser-induced breakdown spark over time; and

calculating at least one component of freestream velocity by using the monitored plurality of physical characteristics associated with the laser-induced breakdown spark.

2. The method of claim 1 wherein the step of positioning the at least one neutral density filter between the cameras and the laser-induced breakdown spark comprises the steps of:

positioning a plurality of neutral density filters between the cameras and the laser-induced breakdown spark; and

selectively altering which of the plurality of neutral density filters is positioned between the cameras and the laser-induced breakdown spark based on at least one of;

passage of time;

or changes in air density surrounding the laser-induced breakdown spark.

3. The method of claim 1 wherein the step of positioning the at least one neutral density filter between the cameras and the laser-induced breakdown spark comprises the steps of:

positioning at least one neutral density filter between the cameras and the laser-induced breakdown spark at a first point; and

moving the at least one neutral density filter to a second point based on the change in intensity of the laser-induced breakdown spark due to at least one of;

passage of time;

or

changes in air density surrounding the laser-induced breakdown spark.

4. The method of claim 1 wherein the at least one component of freestream velocity comprises a directional component for at least one of:

streamwise freestream velocity, transverse freestream velocity, and normal freestream velocity.

5. The method of claim 1 wherein the plurality of cameras comprises at least one charged coupled device camera.

6. The method of claim 1 wherein an intensity associated with the laser-induced breakdown spark is regulated by adjusting an energy output of the at least one laser using a feedback monitoring cycle to reduce or increase the energy output of the at least one laser.

7. The method of claim 1 wherein the vehicle comprises a hypersonic flight-test vehicle.

8. A system for measuring at least one component of freestream velocity comprising:

a vehicle;

at least one laser, the at least one laser producing a laser-induced breakdown spark at point away from the vehicle;

a plurality of cameras contained within the vehicle, the plurality of cameras being positioned to monitor and capture a plurality of physical characteristics associated with the laser-induced breakdown spark over time;

at least one neutral density filter positioned between the laser-induced breakdown spark and the plurality of cameras; and

at least one component of freestream velocity calculated from the plurality of physical characteristics associated with the laser-induced breakdown spark over time.

9. The system of claim 8 wherein the at least one neutral density filter positioned between the cameras and the laser-induced breakdown spark comprises a plurality of neutral density filters between the cameras and the laser-induced breakdown spark wherein at least one of the plurality of neutral density filters is selectively positioned between the cameras and the laser-induced breakdown spark.

10. The system of claim 8 wherein the at least one neutral density filter positioned between the cameras and the laser-induced breakdown spark comprises at least one neutral density filter between the cameras and the laser-induced breakdown spark at a first point wherein the at least one neutral density filter is positioned at a second point based on the change in intensity of the laser-induced breakdown spark over time.

11. The system of claim 8 wherein the at least one component of freestream velocity comprises a directional component for at least one of:

streamwise freestream velocity, transverse freestream velocity, and normal freestream velocity.

12. The method of claim 8 wherein the plurality of cameras comprises at least one charged coupled device camera.

13. The method of claim 8 wherein an intensity associated with the laser-induced breakdown spark is regulated by adjusting an energy output of the at least one laser using a feedback monitoring cycle to reduce or increase the energy output of the at least one laser.

14. The method of claim 8 wherein the vehicle comprises a hypersonic flight-test vehicle.

15. An aero-optical instrument comprising:

one or more pulsed lasers generating a laser-induced breakdown spark;

a plurality of optical components sufficient to collect light from the laser-induced breakdown spark after it passes through an aircraft boundary layer, the plurality of optical components conditioning and transmitting that light;

one or more wavefront sensors measuring a plurality of wavefronts through the aircraft boundary layer based on the light collected from the laser-induced breakdown spark; and

at least optical device positioned to capture and measure an amount of light produced by the laser-induced breakdown spark.

16. The aero-optical instrument of claim 15 further comprising at least one neutral density filter selectively and moveably positioned between the at least one optical device and the laser-induced breakdown spark, wherein the at least one neutral density filter is moved from a first position to a second position to control the intensity of the amount of light from the laser-induced breakdown spark reaching the at least one optical device.

17. The aero-optical instrument of claim 15 further comprising a plurality of neutral density filters between the at least one optical device and the laser-induced breakdown spark wherein at least one of the plurality of neutral density filters is selectively positioned between the and the laser-induced breakdown spark to control the intensity of the amount of light from the laser-induced breakdown spark reaching the at least one optical device.

18. The aero-optical instrument of claim 15 further comprising a feedback monitoring cycle used to regulated an energy output of the one or more pulsed lasers to reduce or increase the energy output of the at least one laser so as to control the intensity of the amount of light from the laser-induced breakdown spark reaching the at least one optical device.

19. The aero-optical instrument of claim 15 further comprising:

at least one neutral density filter selectively and moveably positioned between the at least one optical device and the laser-induced breakdown spark, wherein the at least one neutral density filter is moved from a first position to a second position to control the intensity of the amount of light from the laser-induced breakdown spark reaching the at least one optical device; and

a feedback monitoring cycle used to regulated an energy output of the one or more pulsed lasers to reduce or increase the energy output of the at least one laser so as to control the intensity of the amount of light from the laser-induced breakdown spark reaching the at least one optical device.

20. The aero-optical instrument of claim 15 further comprising:

a plurality of neutral density filters between the at least one optical device and the laser-induced breakdown spark wherein at least one of the plurality of neutral density filters is selectively positioned between the and the laser-induced breakdown spark to control the intensity of the amount of light from the laser-induced breakdown spark reaching the at least one optical device; and

a feedback monitoring cycle used to regulated an energy output of the one or more pulsed lasers to reduce or increase the energy output of the at least one laser so as to control the intensity of the amount of light from the laser-induced breakdown spark reaching the at least one optical device.

21. The aero-optical instrument of claim 15 wherein the at least one optical device is a photosensor.

22. The aero-optical instrument of claim 15 wherein the at least one optical device is a position sensing device.