Dennis C. Evans p1 SuperNova/Acceleration Probe 16 November 2001 Optical Analysis & Stray Light Evaluation Optical Analysis and Stray Light Evaluation.

Slides:



Advertisements
Similar presentations
Chapter 17 Geometrical Optics.
Advertisements

Chapter 23.
Rodger Farley p1 Super Nova/Acceleration Probe 16 November 2001 Mechanical Mechanical Overview Rodger Farley Mick Correia Judy Brannen 16 November 2001.
PACS IIDR 01/02 Mar 2001 Baffle and Straylight1 D. Kampf KAYSER-THREDE.
Chapter 31 Images.
SPHERICAL MIRRORS Free powerpoints at
Chapter 23 Mirrors and Lenses.
Chapter 23 Mirrors and Lenses.
Light: Geometric Optics
Chapter 33 Lenses and Optical Instruments Refraction: Snell’s Law Example 32-8: Refraction through flat glass. Light traveling in air strikes a.
Copyright © 2009 Pearson Education, Inc. Chapter 32 Light: Reflection and Refraction.
Reflection of Light. Slide 2 Luminous objects – generate their own light (the sun) Illuminated objects – reflect light (the moon) Line of Sight – a line.
Wide-field, triple spectrograph with R=5000 for a fast 22 m telescope Roger Angel, Steward Observatory 1 st draft, December 4, 2002 Summary This wide-field,
Fiber Optics Defining Characteristics: Numerical Aperture Spectral Transmission Diameter.
On-Orbit Adjustment Calculation for the Generation-X X-ray mirror Figure D. A. Schwartz, R. J. Brissenden, M. Elvis, G. Fabbiano, D. Jerius, M. Juda, P.
1.B – Solar Dynamo 1.C – Global Circulation 1.D – Irradiance Sources 1.H – Far-side Imaging 1.F – Solar Subsurface Weather 1.E – Coronal Magnetic Field.
COrE+ Optics options.
Chapter 23 Mirrors and Lenses.
Generation-X telescope: Measurement of On-Orbit Adjustment Data Dan Schwartz, R. J. Brissenden, M. Elvis, G. Fabbiano, T. Gaetz, D. Jerius, M. Juda, P.
Tibor Agócs Purpose of the talk  Wide-field spectroscopy/imaging is the driver  MOS  IFU  NB/WB imager  Current FOV is 40 arcmin – it’s.
Chapter 33 Lenses and Optical Instruments
Copyright © 2009 Pearson Education, Inc. Chapter 33 Lenses and Optical Instruments.
The Devil’s in the Details Transits in detail Telescopes.
A SEMINAR ON HUBBLE SPACE TELESCOPE PRESENTED BY: HARI OM ELECTRONICS & COMMUNICATION REG NO SECTION-C ROLL NO.– 123.
Light Waves Sec 1.
Optical Design Work for a Laser-Fiber Scanned
1 Reflection and Mirrors. 2 The Law of Reflection “ The angle of incidence equals the angle of reflection.”
 Mirrors that are formed from a section of a sphere.  Convex: The reflection takes place on the outer surface of the spherical shape  Concave: The.
Mirrors & Reflection.
Chapter 18: Ray Optics Lisa & Becky. Ray Model of Light  Light rays travel in straight lines  Light rays cross but do not interact  Light rays travel.
ZTFC 12-segment field flattener (and related) options R. Dekany 07 Aug 2012.
First-Order Opto-Mechanical Considerations in High Power Applications
Chapter 18-1 Mirrors. Plane Mirror a flat, smooth surface light is reflected by regular reflection rather than by diffuse reflection Light rays are reflected.
PACS IIDR 01/02 Mar 2001 FPFPU Alignment1 D. Kampf KAYSER-THREDE.
 When light strikes the surface of an object  Some light is reflected  The rest is absorbed (and transferred into thermal energy)  Shiny objects,
SNAP Integration Model V. S14 The SNAP Integration Model Mechanical [ SC4 Breakout ] Robin Lafever LBNL Engineering.
NORDFORSK Summer School, La Palma, June-July 2006 NOT: Telescope and Instrumentation Michal I. Andersen & Heidi Korhonen Astrophysikalisches Institut Potsdam.
The Hobby-Eberly Telescope Mirror Alignment Recovery System Marsha Wolf Graduate Student UT Astronomy Department.
Optical Subsystem Roy Esplin Dave McLain. Internal Optics Bench Subassembly 2 Gut Ray Dichroic Beamsplitter (MWIR reflected, LWIR transmitted) LWIR Lens.
Introduction to the Principles of Aerial Photography
SAM PDR1 S OAR Adaptive Module LGS LGSsystem Andrei Tokovinin SAM LGS Preliminary Design Review September 2007, La Serena.
ZTF Optics Design P. Jelinsky ZTF Technical Meeting 1.
Progress Report Geo-CAPE Coastal Ecosystem Dynamics Imager (CEDI) IRAD Repackaging Study Jason Budinoff / GSFC Cathy Marx / GSFC May 12, 2011.
Tolerancing in Zemax OPTI 521 Tutorial By Stacie Hvisc December 5, 2006.
The Active Optics System S. Thomas and the AO team.
March Chuck DiMarzio, Northeastern University ECE-1466 Modern Optics Course Notes Part 2 Prof. Charles A. DiMarzio Northeastern University.
Delta II 7925H - 10L Baseline workup Launch Vehicle TheirsOurs Delta II 7925H Launch Vehicle 10L Composite Fairing 10L Stretch Composite Payload Fairing.
Improved Annular-Field Three-Mirror Anastigmat? M.Lampton UCB SSL Previous AFTMAs have pri-sec separation 2.4m Can pri-sec separation be reduced? –Support.
Low Polarization Optical System Design Anna-Britt Mahler Polarization Laboratory Group College of Optical Sciences.
1 Shield and Fold Mirror Dimensions Michael Sholl 3 February 2005 MODIFIED by Robin Lafever 23 Feb 2005.
N A S A G O D D A R D S P A C E F L I G H T C E N T E R I n t e g r a t e d D e s i g n C a p a b i l i t y / I n s t r u m e n t S y n t h e s i s & A.
Solar orbiter_______________________________________________.
SuperNova / Acceleration Probe System Engineering Mike Roberto and Mike Amato November 16, 2001.
ZTF Optics Design ZTF Technical Meeting 1.
Mirror vs Optical lens + LED lighting test M Fitton, P Loveridge, J O’Dell RAL.
Reflection of Light. Reflectance u Light passing through transparent medium is transmitted, absorbed, or scattered u When striking a media boundary, light.
The High Altitude Observatory (HAO) at the National Center for Atmospheric Research (NCAR) The National Center for Atmospheric Research is sponsored by.
N A S A G O D D A R D S P A C E F L I G H T C E N T E R I n s t r u m e n t S y n t h e s i s a n d A n a l y s i s L a b o r a t o r y APS Formation Sensor.
N A S A G O D D A R D S P A C E F L I G H T C E N T E R I n t e g r a t e d D e s i g n C a p a b i l i t y / I n s t r u m e n t S y n t h e s i s & A.
PACS IIDR 01/02 Mar 2001 Optical System Design1 N. Geis MPE.
Astronomical Spectroscopic Techniques. Contents 1.Optics (1): Stops, Pupils, Field Optics and Cameras 2.Basic Electromagnetics –Math –Maxwell's equations.
N A S A G O D D A R D S P A C E F L I G H T C E N T E R I n s t r u m e n t S y n t h e s i s a n d A n a l y s i s L a b o r a t o r y Super Star Tracker.
Lab 2 Alignment.
Rose Navarro HMI Lead Thermal Engineer
Astronomical Spectroscopic Techniques
Point Source Transmission Simulations on the COROT baffle
Intra-pixel Sensitivity Testing Preliminary Design Review
First Assessments of EUVI Performance on STEREO SECCHI
Observational Astronomy
Optics Alan Title, HMI-LMSAL Lead,
Presentation transcript:

Dennis C. Evans p1 SuperNova/Acceleration Probe 16 November 2001 Optical Analysis & Stray Light Evaluation Optical Analysis and Stray Light Evaluation Dennis Charles Evans 16 November 2001

Dennis C. Evans p2 SuperNova/Acceleration Probe 16 November 2001 Optical Analysis & Stray Light Evaluation ZEMAX Optical Layout  ISAL prescription from TMA62 write-up  Checked against customer supplied ZEMAX Optical Sensitivities  Basic Sensitivity  Active Secondary (5-dof) Stray Light Baffle Layout Spectrograph Enclosure and Insertion Views from the Detector Solar Flux Open Items

Dennis C. Evans p3 SuperNova/Acceleration Probe 16 November 2001 Optical Analysis & Stray Light Evaluation ZEMAX Optical Layout  ISAL prescription from TMA62 write-up  Checked against customer supplied ZEMAX

Dennis C. Evans p4 SuperNova/Acceleration Probe 16 November 2001 Optical Analysis & Stray Light Evaluation

Dennis C. Evans p5 SuperNova/Acceleration Probe 16 November 2001 Optical Analysis & Stray Light Evaluation

Dennis C. Evans p6 SuperNova/Acceleration Probe 16 November 2001 Optical Analysis & Stray Light Evaluation

Dennis C. Evans p7 SuperNova/Acceleration Probe 16 November 2001 Optical Analysis & Stray Light Evaluation Optical Sensitivity Basic Sensitivity  Individual Element Increments of mm or degree to  MF Limit (RMS Spot Radius) ( ÷ )*2 = Active Secondary  Five degree-of-freedom —Dx, Dy, Dz, Tx, Ty  Limits on Secondary — ± 1 mm or degree  Limits on Elements — ± mm or degree

Dennis C. Evans p8 SuperNova/Acceleration Probe 16 November 2001 Optical Analysis & Stray Light Evaluation Basic LimitActive Secondary Limit Primary Tilt deg0.185 deg Primary- Secondary Space mm0.033 mm Tertiary Tilt0.016 deg0.055 deg Key Tolerance Comparison

Dennis C. Evans p9 SuperNova/Acceleration Probe 16 November 2001 Optical Analysis & Stray Light Evaluation Basic Sensitivity (limited to RMS Radius) TETX TETY Tilt about X & Y 5=Primary deg ×3600 arc-sec/deg = arc-sec TTHI Thickness 4-6; mm TRAD Radius of Curvature mm (= same effect as thickness change) TIRX TIRY Sag (Tilt) Across Lens mm TSDX TSDY Surface Decenter mm TEDX TEDY Element Decenter mm TETX TETY Tilt about X & Y 8=Secondary deg ×3600 arc-sec/deg = arc-sec TTHI Thickness 7-9; mm TRAD Radius of Curvature mm TIRX TIRY Sag (Tilt) Across Lens mm TSDX TSDY Surface Decenter mm TEDX TEDY Element Decenter mm TETX Tilt about X & Y 17=Fold Flat deg ×3600 arc-sec/deg = arc-sec TETY Tilt about X & Y deg ×3600 arc-sec/deg = arc-sec TTHI Thickness 16-18; mm TRAD Radius of Curvature 17 insensitive at change TIRX Sag (Tilt) Across Lens mm TIRY Sag (Tilt) Across Lens mm TSDX TSDY Surface Decenter 17 insensitive at change ( ) TEDX TEDY Element Decenter 17 insensitive at change ( ) TETX TETY Tilt about X & Y 22=Tertiary deg ×3600 arc-sec/deg = arc-sec TTHI Thickness 21-23; mm TRAD Radius of Curvature mm TIRX TIRY Sag (Tilt) Across Lens mm TSDX TSDY Surface Decenter 22 insensitive at change ( ) TEDX TEDY Element Decenter 22 insensitive at change ( ) TETX TETY Tilt about X & Y 32-33=Filter insensitive at change ( ) TTHI Thickness 21-23; mm TRAD Radius of Curvature mm TIRX TIRY Sag (Tilt) Across Lens mm TSDX TSDY Surface Decenter 22 insensitive at change ( ) TEDX TEDY Element Decenter 22 insensitive at change ( ) TTHI Filter to Image mm (Image Plane is compensator for fast analysis)

Dennis C. Evans p10 SuperNova/Acceleration Probe 16 November 2001 Optical Analysis & Stray Light Evaluation | Minimum | | Maximum | Type Value MF Change Value MF Change (Primary Mirror) Thickness tolerance on surface 4 TTHI Thickness 8: E E+000 Radius tolerance on surface 5 TRAD Thickness 8: E E+000 Tilt X tolerance on surfaces 5 through 5 (degrees) TETX Parameter 2 on Surface 7: E E-002 Parameter 3 on Surface 7: E E-001 Tilt Y tolerance on surfaces 5 through 5 (degrees) TETY Parameter 1 on Surface 7: E E-002 Parameter 4 on Surface 7: E E-001 (Fold Flat) Thickness tolerance on surface 16 TTHI Thickness 8: E E-001 TIRX Parameter 1 on Surface 7: E E-001 TIR Y tolerance on surface 17 TIRY Parameter 2 on Surface 7: E E-001 Tilt X tolerance on surfaces 17 through 17 (degrees) TETX Parameter 2 on Surface 7: E E-001 Tilt Y tolerance on surfaces 17 through 17 (degrees) TETY (Tertiary Mirror) Tilt X tolerance on surfaces 22 through 22 (degrees) TETX Parameter 2 on Surface 7: E E+000 Tilt Y tolerance on surfaces 22 through 22 (degrees) TETY Parameter 1 on Surface 7: E E+000 Active Secondary Sensitivity

Dennis C. Evans p11 SuperNova/Acceleration Probe 16 November 2001 Optical Analysis & Stray Light Evaluation Stray Light Baffle Layout

Dennis C. Evans p12 SuperNova/Acceleration Probe 16 November 2001 Optical Analysis & Stray Light Evaluation

Dennis C. Evans p13 SuperNova/Acceleration Probe 16 November 2001 Optical Analysis & Stray Light Evaluation

Dennis C. Evans p14 SuperNova/Acceleration Probe 16 November 2001 Optical Analysis & Stray Light Evaluation

Dennis C. Evans p15 SuperNova/Acceleration Probe 16 November 2001 Optical Analysis & Stray Light Evaluation

Dennis C. Evans p16 SuperNova/Acceleration Probe 16 November 2001 Optical Analysis & Stray Light Evaluation

Dennis C. Evans p17 SuperNova/Acceleration Probe 16 November 2001 Optical Analysis & Stray Light Evaluation Spectrograph Enclosure and Insertion

Dennis C. Evans p18 SuperNova/Acceleration Probe 16 November 2001 Optical Analysis & Stray Light Evaluation

Dennis C. Evans p19 SuperNova/Acceleration Probe 16 November 2001 Optical Analysis & Stray Light Evaluation

Dennis C. Evans p20 SuperNova/Acceleration Probe 16 November 2001 Optical Analysis & Stray Light Evaluation

Dennis C. Evans p21 SuperNova/Acceleration Probe 16 November 2001 Optical Analysis & Stray Light Evaluation

Dennis C. Evans p22 SuperNova/Acceleration Probe 16 November 2001 Optical Analysis & Stray Light Evaluation Views from the Detector

Dennis C. Evans p23 SuperNova/Acceleration Probe 16 November 2001 Optical Analysis & Stray Light Evaluation

Dennis C. Evans p24 SuperNova/Acceleration Probe 16 November 2001 Optical Analysis & Stray Light Evaluation

Dennis C. Evans p25 SuperNova/Acceleration Probe 16 November 2001 Optical Analysis & Stray Light Evaluation Solar Flux Concentrations inside Instrument  Solar Flux = 1 SC =.1367 watt.cm -2 = 1367 watt.m -2 LocationImage Radius (mm) Flux (SC) Flux (watt.cm -2 ) Flux (watts) Entrance Aperture Secondary Mirror Prime Focus Ring Focal Plane Shutter Pupil FP 2 (CCD/Image)

Dennis C. Evans p26 SuperNova/Acceleration Probe 16 November 2001 Optical Analysis & Stray Light Evaluation Open Items & Concerns

Dennis C. Evans p27 SuperNova/Acceleration Probe 16 November 2001 Optical Analysis & Stray Light Evaluation Open Items  Shade angle (<30 o ?) and Barrel Baffle length  Baffle edge finish (Forward Ring)  Cleanliness, especially of Primary Mirror  Aft Optics Baffles (Mostly black paint)  MLI outer layer vs. mission length  Reverse views —AutoCAD Photo Ray Trace —reverse ray trace, TMA62  Focal plane —parfocalization (filter thickness)  S/G placement —behind focal plane? —center mounted  ASAP diffuse scatter model —(Friday PM – Next Week)

Dennis C. Evans p28 SuperNova/Acceleration Probe 16 November 2001 Optical Analysis & Stray Light Evaluation Mission Unique Concerns:  No mission unique concerns have been observed.  Stray light issues are manageable using proven baffling techniques that have been successfully demonstrated on flight missions.  Analysis done too early in the design cycle is likely to give false confidence (analytical design is better than real design).

Dennis C. Evans p29 SuperNova/Acceleration Probe 16 November 2001 Optical Analysis & Stray Light Evaluation Central Obscuration  Minimum possible - about 5% (Shadow of Secondary)  Current minimum design to keep direct light from Focal Surface 1 - about 15%  Maximum practical limit to keep direct light from inner baffle interior and front lip - slightly less than 25%

Dennis C. Evans p30 SuperNova/Acceleration Probe 16 November 2001 Optical Analysis & Stray Light Evaluation Stray Light Issues  Similarity to flight instruments shows successful design is possible —HST, FUSE, COBE-DIRBE, IUE, OAO  Similarity to flight instruments shows design flaws are possible that will not be detected by stray light analysis, but by careful design, inspection, and testing. —HST - Door reflections —DIRBE - Barrel Baffle side wall single bounces. —IUE/OAO - Pinhole leaks into aft optics assemblies; bolt head locations.  Design & Analysis Similarity —SIRTF - IRAC —WIRE (minor changes make orders of magnitude stray light differences) —GOES Earth Limb Sensor (light leaks around filters and side wall reflections) —MODIS - Stray light in calibrator designs, not instrument designs

Dennis C. Evans p31 SuperNova/Acceleration Probe 16 November 2001 Optical Analysis & Stray Light Evaluation Focus Drive Mechanism  Definition of acceptable image size needs to be reviewed.  RMS radius of mm may be to conservative for a pixel limited performance instrument.  Range of motions used were +/- 1 mm and degree.  The Displacement motions may be effectively increased to 5 or 10 mm for some corrections.  Tolerance analysis so far is only with two elements at a time and has not included Image Plane tilts.

Dennis C. Evans p32 SuperNova/Acceleration Probe 16 November 2001 Optical Analysis & Stray Light Evaluation View from the detector inspection is important.  Fold Flat throat can be illuminated by sky.  Fold flat throat design as in this study may not allow AFT star tracker AFT optics baffles and black surfaces  Baffles not designed yet  Black paint has been known to cause CTE changes in GFRP structures.