Title: Thesis Defense Presentation
1Improving the Accuracy of Target Engagement
Presented by Lane Carlson1 M. Tillack1, T.
Lorentz1, N. Alexander2, D. Goodin2, R.
Petzoldt2 (1UCSD, 2General Atomics) HAPL Project
Review Santa Fe, NM April 8-9, 2008
2Hit-on-the-fly experiment has demonstrated
improved engagement on moving targets
- Improvements in imaging and relaying the glint
return signal to the PSD give a more repeatable
dependable signal. - Improvements have yielded better engagement
- HAPL Oct 2007 - 150 µm (1?) for targets in 1.5
mm range. - 80 µm (1?) engagement for targets in 1.5 mm
range.
- Final Requirement
- 20 µm engagement accuracy in (x,y,z) at 20 m
(10-6)
3Surface issues have been resolved with glint
return imaging improvements
- Last time, concerned about surface roughness and
laser beam profile. - However, imaging system was looking at an
intermediate, incoherent field. - With simplified setup, found proper focusing
techniques that allow more precise imaging of the
glints true apparent source.
Surface finish issues are resolved with proper
focusing and aperture.
Proper focusing
Improper focusing
4Glint return provides a final reference point
5Systematic identification and reduction of errors
yields improved target engagement
- Error sources as of Oct 2007
- Relaying glint return....50 µm
- PSD accuracy limit..50 µm (spec)
- Target motion from
- glint to driver..24 µm (1?)
- PSD non-linearity..40 µm (1?)
- Verification camera7 µm
- Mirror pointing..6 µm
- Simplified setup helped identify four areas of
improvement related to relaying glint return - Proper focusing of the glint return on the PSD.
- Aperturing the glint return signal.
- Changing the systems magnification.
- Higher-order PSD calibration fit.
6Proper imaging of the glint return requires
focusing and aperturing
- The ideal glint return is an Airy disk with
apparent location displaced from the targets
center. - Previously, we were defocused due to saturation
concerns. - Proper focusing and aperturing of the glint
return minimizes coma, surface roughness speckle,
and wave aberrations.
Glint off target
Aperture
Intermediate field
At focus
Glint return relayed and Imaged onto sensor
Focus planes
(Not to scale)
7Improvements to imaging the glint return on the
PSD yield a more consistent return
Glint off target is imaged onto the PSD. How the
glint is imaged is very important.
8Magnification leverages target-PSD calibration
- PSD specified position accuracy is 50 µm.
- gt can correspond to a large target position
error. - By leveraging magnification ratio, we use more of
sensors area and reduce glint return positioning
error.
9Imaging improvements contribute to total
engagement improvement
- Cycle through improvements, then X, Y individual
10Imaging improvements contribute to total
engagement improvement
- Cycle through improvements, then X, Y individual
11Imaging improvements contribute to total
engagement improvement
- Cycle through improvements, then X, Y individual
12Imaging improvements contribute to total
engagement improvement
- Cycle through improvements, then X, Y individual
13Imaging improvements contribute to total
engagement improvement
- Cycle through improvements, then X, Y individual
14Improvements in relaying the glint return have
eliminated some errors
- Current error sources
- Relaying glint return....50 µm..eliminated
with improvements - PSD accuracy limit..50 µm (spec)
- Target motion from
- glint to driver..24 µm (1?)
- PSD non-linearity..40 µm (1?)reduced to 19
µm (1?) with higher - Verification camera7 µm order
calibration fit - Mirror pointing..6 µm
15PSD limit necessitates an alternative sensor
- PSD spec limits position accuracy to 50 µm.
- Deviation from improved PSD calibration 19 µm
(1?). - Using a camera will allow for direct geometric
position reporting of the glint centroid. - Camera accuracy and resolution lt 1 µm with energy
centroiding techniques.
6 x 4 mm camera image of glint return
Basler GigE camera
16Vacuum chamber design progresses to permit
engagement of lightweight targets
2 m tall
Dropping chamber
- Wake effects on target minimal for SS BBs but
substantial for a lightweight targets. - Better placement accuracy anticipated.
- Will permit dropping and engagement of
lightweight targets.
Crossing sensors
Engagement chamber
17We expect substantially reduced errors with
implementation of camera and vacuum chamber
- Predicted error sources
- Relaying glint return. --
- PSD accuracy limit..50 µm (spec)1 µm with
camera - Target motion from
- glint to driver..24 µm (1?).reduced to
5µm by vacuum - chamber
- PSD non-linearity..19 µm (1?)eliminated
with camera - Verification camera7 µm
- Mirror pointing..6 µm
- With full implementation of the camera and vacuum
chamber, we can reasonably expect to attain 20
µm engagement based on these numbers.
18Future effort focuses on completing demo and
achieving 20 µm engagement goal
- In summary
- We are continuing to use the glint return off a
falling target to engage targets to 80 µm (1?). - Next steps
- Construct a more rigorous 3D calibration.
- Replace PSD with camera to better resolve glint
return. - Long-term effort
- Mate with a prototypic injector in vacuum, engage
real targets.
19End of slideshow
20Our new imaging setup resolves surface issues
- In practice, engagement error was more than seen
with a stationary target. - Concerned that a falling, rotating target might
present a different surface to be imaged.
- With a simple camera setup, demonstrated that a
target rotated on a kinematic mount has a
position repeatability equivalent to a stationary
target.
Rotated target 5 µm
Stationary target 3 µm
Target rotation/different surface presentation is
not a concern.
21Imaging improvements contribute to total
engagement improvement
22Additional information
- Wake effects between glint and driver beam
location? Minimal for a steel BB in air,
substantial for a lightweight target. - Found that divergence is too great to adequately
homogenize glint laser beam. - Verified that glint lasers beam profile does not
affect glint return.