Documents Found!
As seen in
Less Work, Better Grades
Join
Course Hero
Access
best resources
Ace
your classes
Ace your courses with Course Hero!

Submit your homework question or assignment here:
352 Tutors are online
 
We are so confident that you will love our service, we will answer your first homework question for FREE!
*  Attach Assignment (optional):
 
Study Smarter, Score Higher
 
Document Content (unformatted)
Course Hero has millions of student submitted documents similar to the one below including study guides, homework solutions, papers, exam answer keys and textbook solutions.
Testing Absolute Absolute measurement of flats Absolute measurement of flats Absolute measurement of spheres Absolute measurement of spheres Absolute measurement of surface roughness Absolute measurement of surface roughness James C. Wyant Absolute Surface Shape Measurement Removing system aberrations & Removing system aberrations & reference surface effects reference surface effects Improves measurement accuracy Improves measurement accuracy Tests for Tests for Flats Flats Spheres Spheres Surface roughness Surface roughness James C. Wyant ThreeFlatTest.nb James C. Wyant (2003) 1 Three-Flat Test If we have only two flats and we get straight line fringes when we compare the two flats we do not know they are flat because one could be concave and the second could be convex so the two surfaces match. If we have three flats and we get straight line fringes when we compare flat A with flat B and when we compare flat A with flat C and again when we compare flat B with flat C then the surfaces must all be flat. The following are the four measurements required to find an absolute measurement of the x and y profiles of the three flats. x B Inverted A x x C Inverted A x x C Inverted B x x x C Inverted B Rotated From the 4 measurements we obtain GAC @x_, y_D := fA @x, yD + fC @-x, yD GBC @x_, y_D := fB @x, yD + fC @-x, yD GAB @x_, y_D := fA @x, yD + fB @-x, yD Using the first, second, and third measurements we can solve for the y profiles. GBC' @x_, y_D := fB @-x, -yD + fC @-x, yD AB B B B B A AC C C C C A BC C C C C B ThreeFlatTest.nb GAB @0, yD + GAC @0, yD - GBC @0, yD 2 2 James C. Wyant (2003) 2 -GAB @0, yD + GAC @0, yD + GBC @0, yD 2 GAB @0, yD - GAC @0, yD + GBC @0, yD = fA @0, yD = fB @0, yD Using the first, second, and fourth measurements we can solve for the x profiles. = fC @0, yD AB B B B A AC C C C = fA @x, 0D 2 = fB @-x, 0D BC' A C C C B GAB @x, 0D - GAC @x, 0D + GBC' @x, 0D 2 2 We have obtained the x and y profiles of the three flats. The process can be repeated to obtain other profiles. -GAB @x, 0D + GAC @x, 0D + GBC' @x, 0D GAB @x, 0D + GAC @x, 0D - GBC' @x, 0D = fC @-x, 0D Absolute Sphere Testing.nb James C. Wyant (2003) 1 Absolute Sphere Testing Using the following procedure it is possible to separate interferometer errors from errors in the spherical mirror being tested. The technique will work with both the Twyman-Green interferometer and the laser-based Fizeau interferometer. Three measurements are required. W 0 W 180 W The focus three measurements give W180 @x_, y_D := 2 Wsurf @-x, -yD + Wref @x, yD + 2 Wdiv @x, yD Wfocus @x_, y_D := Wref @x, yD + Wdiv @x, yD + Wdiv @-x, -yD 1 4 HW0 @x, yD + W180 @-x, -yD - Wfocus @x, yD - Wfocus @-x, -yDL = Wsurf @x, yD W0 @x_, y_D := 2 Wsurf @x, yD + Wref @x, yD + 2 Wdiv @x, yD The mirror surface error is given by @-x.- yD in the last equation means we are rotating the data 180 in the computer. Single Measurement of Sphere TILT, POWER REMOVED INTERVAL = 0.025 RMS = 0.014 WAVES P-V = 0.121 WAVES FIZEAU INTERFEROMETER, F/1.1 REF. SPHERE James C. Wyant Flat at Focus f/1.1 Diverger TILT, POWER, COMA REMOVED INTERVAL = 0.05 RMS = 0.027 WAVES P-V = 0.243 WAVES James C. Wyant Absolute Reference TILT, POWER REMOVED INTERVAL = 0.025 RMS = 0.010 WAVES P-V = 0.084 WAVES James C. Wyant Absolute Measurement of Sphere TILT,POWER REMOVED INTERVAL = 0.025 RMS = 0.011 WAVES P-V = 0.081 WAVES James C. Wyant Absolute Surface Roughness Measurement Assumptions Surface height is random Surface height is random Statistics do not vary over surface Statistics do not vary over surface Each measurement = Test + Reference Each measurement = Test + Reference Test and reference uncorrelated Test and reference uncorrelated RMSmeas= James C. Wyant 2 2 + RMStest RMSref Effect of Reference Surface on Measurement Error in measured rms for 5 A rms reference surface 6 4 2 0 0 5 10 15 20 25 30 Rms roughness of test surface (A) James C. Wyant Subtraction of Errors due to Reference Surface Perfect mirror Perfect mirror Generate reference Generate reference Absolute rms measurement Absolute rms measurement James C. Wyant Generate Reference Average many measurements Average many measurements Move random surface > correlation Move random surface > correlation length between measurements length between measurements Effects of random surface reduce as Effects of random surface reduce as square root of number of measurements square root of number of measurements James C. Wyant Generate Reference and Subtract Surface + Reference Reference Surface (0.071 nm) James C. Wyant Absolute RMS Measurement Make 2 measurements where surface moved > correlation length between measurements Subtract measurements and divide by square root of 2 Reference cancels and obtain RMS of test surface Diff = Test1+ (-Test2 ) 1 RMSTest = 2 RMSDiff James C. Wyant Generate Reference and Absolute RMS Comparison Generate Reference Absolute RMS RMS = 0.071 nm RMS = 0.070 nm James C. Wyant
Find millions of documents here - Study Guides, Homework Solutions, Papers, Exam Answer Keys and more. Course Hero has millions of course related materials that will enable you to learn better, faster and get an A in all your courses.
Below is a small sample set of documents:

Arizona >> OPTICS >> 513 (Fall, 2009)
06SurfaceQuality.nb Optics 513 - James C. Wyant (2008) 1 Surface Quality SQ-1 a) How is surface profile data obtained using the FECO interferometer? Your explanation should include diagrams with the appropriate quantities defined. b) Can resolutio...
Arizona >> OPTICS >> 513 (Fall, 2009)
Optics 513L - James C. Wyant (2008) Optics 513 - Optical Testing and Testing Instrumentation Lab Lab #9 - Scatterplate Interferometer The purpose of this lab is to become familiar with the use of the scatterplate interferometer for the testing of mi...
Arizona >> OPTICS >> 513 (Fall, 2009)
Optics 513L - James C. Wyant (2008) Optics 513 - Optical Testing and Testing Instrumentation Lab Lab #8 Shack-Hartmann Test Smartt Point-Diffraction Interferometer The purpose of this lab is to Become familiar with the use of a Shack-Hartmann Test...
Arizona >> OPTICS >> 513 (Fall, 2009)
Optics 513L - James C. Wyant (2008) Optics 513 - Optical Testing and Testing Instrumentation Lab Lab #10 - Lateral Shearing Interferometry The purpose of this lab is \"to learn to appreciate the enjoyment of working with a lateral shear interferomete...
Arizona >> OPTICS >> 513 (Fall, 2009)
Optics 513L - James C. Wyant (2008) Optics 513L - Optical Testing and Testing Instrumentation Lab Lab #1 - Orientation Lab The purpose of this lab experiment is to become familiar with some elementary aspects of optical alignment and interferometry....
Arizona >> OPTICS >> 513 (Fall, 2009)
Optics 513L - James C. Wyant (2008) Optics 513 - Optical Testing and Testing Instrumentation Lab Lab #5 - Twyman-Green Interferometer The purpose of this lab is to Become familiar with the use of a Twyman-Green interferometer for the testing of sph...
Arizona >> OPTICS >> 513 (Fall, 2009)
Optics 513L - James C. Wyant (2008) Optics 513 - Optical Testing and Testing Instrumentation Lab Lab #3 - Refractive Index Measurement: Abbe Refractometer Goniometer Brewster\'s Angle The purpose of this lab is to become familiar with several method...
Arizona >> OPTICS >> 513 (Fall, 2009)
Optics 513L - James C. Wyant (2008) Optics 513 - Optical Testing and Testing Instrumentation Lab Lab #11 - Laser Based Fizeau Interferometer The purpose of this lab is to become familiar with the use of a laser based Fizeau interferometer for testi...
Arizona >> OPTICS >> 513 (Fall, 2009)
Optics 513L - James C. Wyant (2008) Optics 513 - Optical Testing and Testing Instrumentation Lab Lab #7 - Foucault, Wire, and Ronchi Tests The purpose of this lab is to obtain \"hands on\" experience with the Foucault (knife-edge), wire, and Ronchi te...
Arizona >> OPTICS >> 08 (Fall, 2008)
8.2.10) Star Test Ref: Chapter 11 of Malacara The careful visual examination of the image of a point source formed by a lens being evaluated is one of the most basic and important tests that can be performed. The interpretation of the image in terms ...
Arizona >> OPTICS >> 513 (Fall, 2009)
8.2.10) Star Test Ref: Chapter 11 of Malacara The careful visual examination of the image of a point source formed by a lens being evaluated is one of the most basic and important tests that can be performed. The interpretation of the image in terms ...
Arizona >> CHAPTER >> 513 (Fall, 2009)
8.2.10) Star Test Ref: Chapter 11 of Malacara The careful visual examination of the image of a point source formed by a lens being evaluated is one of the most basic and important tests that can be performed. The interpretation of the image in terms ...
Arizona >> OPTICS >> 08 (Fall, 2008)
NonInterferometric Testing.nb Optics 513 - James C. Wyant 1 Non-Interferometric Testing Introduction In these notes four non-interferometric tests are described: (1) the Shack-Hartmann test, (2) the Foucault test, (3) the wire test, and (4) the Ro...
Arizona >> OPTICS >> 513 (Fall, 2009)
NonInterferometric Testing.nb Optics 513 - James C. Wyant 1 Non-Interferometric Testing Introduction In these notes four non-interferometric tests are described: (1) the Shack-Hartmann test, (2) the Foucault test, (3) the wire test, and (4) the Ro...
Arizona >> CHAPTER >> 513 (Fall, 2009)
NonInterferometric Testing.nb Optics 513 - James C. Wyant 1 Non-Interferometric Testing Introduction In these notes four non-interferometric tests are described: (1) the Shack-Hartmann test, (2) the Foucault test, (3) the wire test, and (4) the Ro...
Arizona >> OPTICS >> 10 (Fall, 2009)
...
Arizona >> OPTICS >> 513 (Fall, 2009)
...
Arizona >> CHAPTER >> 513 (Fall, 2009)
...
Arizona >> OPTICS >> 513 (Fall, 2009)
LightDistributionNearFocus.nb 1 Light Distribution Near Focus Diagram showing notation for diffraction of a converging wave at a circular aperture y P 2a x z f Fresnel diffraction equation The amplitude can be written as u@x, yD = A kf Hx2 +y 2 ...
Arizona >> CHAPTER >> 513 (Fall, 2009)
LightDistributionNearFocus.nb 1 Light Distribution Near Focus Diagram showing notation for diffraction of a converging wave at a circular aperture y P 2a x z f Fresnel diffraction equation The amplitude can be written as u@x, yD = A kf Hx2 +y 2 ...
Arizona >> OPTICS >> 11 (Fall, 2009)
11. System Evaluation 11.1 Resolution Tests 11.2 Veiling Glare 11.3 Spread Function Measurement 11.4 Encircled Energy Measurement 11.5 Optical Transfer Function Measurement 11.5.1 Scanning Methods 11.5.2 Interferogram Analysis 11.5.3 Autocorrelation ...
Arizona >> OPTICS >> 513 (Fall, 2009)
11. System Evaluation 11.1 Resolution Tests 11.2 Veiling Glare 11.3 Spread Function Measurement 11.4 Encircled Energy Measurement 11.5 Optical Transfer Function Measurement 11.5.1 Scanning Methods 11.5.2 Interferogram Analysis 11.5.3 Autocorrelation ...
Arizona >> CHAPTER >> 513 (Fall, 2009)
11. System Evaluation 11.1 Resolution Tests 11.2 Veiling Glare 11.3 Spread Function Measurement 11.4 Encircled Energy Measurement 11.5 Optical Transfer Function Measurement 11.5.1 Scanning Methods 11.5.2 Interferogram Analysis 11.5.3 Autocorrelation ...
Arizona >> OPTICS >> 06 (Fall, 2009)
6. Measurement of Surface Quality 6.1 View transmitted or reflected light 6.2 Mechanical Probe 6.3 AFM 6.4 Lyot Test 6.5 FECO 6.6 Nomarski Interferometer 6.7 Sommargren Profiler 6.8 Interference Microscope Introduction Surface quality refers to surf...
Arizona >> OPTICS >> 513 (Fall, 2009)
6. Measurement of Surface Quality 6.1 View transmitted or reflected light 6.2 Mechanical Probe 6.3 AFM 6.4 Lyot Test 6.5 FECO 6.6 Nomarski Interferometer 6.7 Sommargren Profiler 6.8 Interference Microscope Introduction Surface quality refers to surf...
Arizona >> CHAPTER >> 513 (Fall, 2009)
6. Measurement of Surface Quality 6.1 View transmitted or reflected light 6.2 Mechanical Probe 6.3 AFM 6.4 Lyot Test 6.5 FECO 6.6 Nomarski Interferometer 6.7 Sommargren Profiler 6.8 Interference Microscope Introduction Surface quality refers to surf...
Arizona >> OPTICS >> 06 (Fall, 2009)
Invited Paper Comparison of surface roughness measured with an optical profiler and a scanning probe microscope Jay Jahanmir and James C. Wyant WYKO Corporation Tucson, Arizona 85706 ABSTRACT The surface topography of various samples has been mea...
Arizona >> OPTICS >> 513 (Fall, 2009)
Invited Paper Comparison of surface roughness measured with an optical profiler and a scanning probe microscope Jay Jahanmir and James C. Wyant WYKO Corporation Tucson, Arizona 85706 ABSTRACT The surface topography of various samples has been mea...
Arizona >> CHAPTER >> 513 (Fall, 2009)
Invited Paper Comparison of surface roughness measured with an optical profiler and a scanning probe microscope Jay Jahanmir and James C. Wyant WYKO Corporation Tucson, Arizona 85706 ABSTRACT The surface topography of various samples has been mea...
Arizona >> OPTICS >> 08 (Fall, 2008)
SpotSizes.nb Optics 513 - James C. Wyant (2003) 1 Spot Sizes Question I am using the star test to evaluate an optical system. How does the minimum blur diameter due to third-order spherical aberration compare to a) b) the blur diameter due to asti...
Arizona >> OPTICS >> 513 (Fall, 2009)
SpotSizes.nb Optics 513 - James C. Wyant (2003) 1 Spot Sizes Question I am using the star test to evaluate an optical system. How does the minimum blur diameter due to third-order spherical aberration compare to a) b) the blur diameter due to asti...
Arizona >> CHAPTER >> 513 (Fall, 2009)
SpotSizes.nb Optics 513 - James C. Wyant (2003) 1 Spot Sizes Question I am using the star test to evaluate an optical system. How does the minimum blur diameter due to third-order spherical aberration compare to a) b) the blur diameter due to asti...
Arizona >> OPTICS >> 05 (Fall, 2009)
GeometricPhaseShifter.nb James C. Wyant 1 Geometric Phase Shifter Initial Parameter Setup James C. Wyant Optical Sciences Center University of Arizona Tucson, AZ www.optics.arizona.edu/jcwyant Introduction There are polarization techniques for p...
Arizona >> OPTICS >> 513 (Fall, 2009)
GeometricPhaseShifter.nb James C. Wyant 1 Geometric Phase Shifter Initial Parameter Setup James C. Wyant Optical Sciences Center University of Arizona Tucson, AZ www.optics.arizona.edu/jcwyant Introduction There are polarization techniques for p...
Arizona >> CHAPTER >> 513 (Fall, 2009)
GeometricPhaseShifter.nb James C. Wyant 1 Geometric Phase Shifter Initial Parameter Setup James C. Wyant Optical Sciences Center University of Arizona Tucson, AZ www.optics.arizona.edu/jcwyant Introduction There are polarization techniques for p...
Arizona >> OPTICS >> 05 (Fall, 2009)
White Light Interferometry Eliminates ambiguities in heights present with monochromatic interferometry Techniques old, but use of modern electronics and computers enhance capabilities and applications 1998 - James C. Wyant Page 1 of 24 How High...
Arizona >> OPTICS >> 513 (Fall, 2009)
White Light Interferometry Eliminates ambiguities in heights present with monochromatic interferometry Techniques old, but use of modern electronics and computers enhance capabilities and applications 1998 - James C. Wyant Page 1 of 24 How High...
Arizona >> OPTICS >> 08 (Fall, 2008)
8. Testing of Curved Surfaces and/or Lenses 8.1 Radius of Curvature 8.1.1 Spherometer 8.1.2 Autostigmatic Measurement 8.1.3 Newton\'s Rings 8.1.4 Interferometer and Radius Slide 8.2 Surface Figure 8.2.1 Test Plate 8.2.2 Twyman-Green Interferometer (LU...
Arizona >> OPTICS >> 513 (Fall, 2009)
8. Testing of Curved Surfaces and/or Lenses 8.1 Radius of Curvature 8.1.1 Spherometer 8.1.2 Autostigmatic Measurement 8.1.3 Newton\'s Rings 8.1.4 Interferometer and Radius Slide 8.2 Surface Figure 8.2.1 Test Plate 8.2.2 Twyman-Green Interferometer (LU...
Arizona >> CHAPTER >> 513 (Fall, 2009)
8. Testing of Curved Surfaces and/or Lenses 8.1 Radius of Curvature 8.1.1 Spherometer 8.1.2 Autostigmatic Measurement 8.1.3 Newton\'s Rings 8.1.4 Interferometer and Radius Slide 8.2 Surface Figure 8.2.1 Test Plate 8.2.2 Twyman-Green Interferometer (LU...
Arizona >> OPTICS >> 04 (Fall, 2009)
Chapter 4 4. Basic Interferometry and Optical Testing 4.1 Two-Beam Interference 4.2 Fizeau Interferometer 4.3 Twyman-Green Interferometer 4.4 Laser-Based Fizeau Interferometer 4.5 Mach-Zehnder Interferometer 4.6 Typical Interferograms 4.7 Interferogr...
Arizona >> OPTICS >> 513 (Fall, 2009)
Chapter 4 4. Basic Interferometry and Optical Testing 4.1 Two-Beam Interference 4.2 Fizeau Interferometer 4.3 Twyman-Green Interferometer 4.4 Laser-Based Fizeau Interferometer 4.5 Mach-Zehnder Interferometer 4.6 Typical Interferograms 4.7 Interferogr...
Arizona >> CHAPTER >> 513 (Fall, 2009)
Chapter 4 4. Basic Interferometry and Optical Testing 4.1 Two-Beam Interference 4.2 Fizeau Interferometer 4.3 Twyman-Green Interferometer 4.4 Laser-Based Fizeau Interferometer 4.5 Mach-Zehnder Interferometer 4.6 Typical Interferograms 4.7 Interferogr...
Arizona >> OPTICS >> 05 (Fall, 2009)
JonesCalculus.nb Optics 513 - James C. Wyant 1 Jones Calculus Jones Vectors Linear Horizontal 1 lh = J N; 0 0 lv = J N; 1 Linear Vertical Linear at +45 degrees 1 1 lp45 = ! J N; 1 2 1 1 lm45 = ! J N; -1 2 1 1 rc = ! J N; - 2 1 1 lc = ! J N; 2 1...
Arizona >> OPTICS >> 513 (Fall, 2009)
JonesCalculus.nb Optics 513 - James C. Wyant 1 Jones Calculus Jones Vectors Linear Horizontal 1 lh = J N; 0 0 lv = J N; 1 Linear Vertical Linear at +45 degrees 1 1 lp45 = ! J N; 1 2 1 1 lm45 = ! J N; -1 2 1 1 rc = ! J N; - 2 1 1 lc = ! J N; 2 1...
Arizona >> CHAPTER >> 513 (Fall, 2009)
JonesCalculus.nb Optics 513 - James C. Wyant 1 Jones Calculus Jones Vectors Linear Horizontal 1 lh = J N; 0 0 lv = J N; 1 Linear Vertical Linear at +45 degrees 1 1 lp45 = ! J N; 1 2 1 1 lm45 = ! J N; -1 2 1 1 rc = ! J N; - 2 1 1 lc = ! J N; 2 1...
Arizona >> OPTICS >> 07 (Fall, 2009)
Simultaneous Phase-Shifting Fizeau Short Coherence Length Source Short coherence length source L L QWP PBS Imaging Lens Stop Reference Polarization Mask and Detector Test Surface Interference pattern resulting from long path length source bea...
Arizona >> OPTICS >> 513 (Fall, 2009)
Simultaneous Phase-Shifting Fizeau Short Coherence Length Source Short coherence length source L L QWP PBS Imaging Lens Stop Reference Polarization Mask and Detector Test Surface Interference pattern resulting from long path length source bea...
Arizona >> CHAPTER >> 513 (Fall, 2009)
Simultaneous Phase-Shifting Fizeau Short Coherence Length Source Short coherence length source L L QWP PBS Imaging Lens Stop Reference Polarization Mask and Detector Test Surface Interference pattern resulting from long path length source bea...
Arizona >> OPTICS >> 04 (Fall, 2009)
4.8 Classical Interferogram Analysis Elementary analysis of interferograms Elementary analysis of interferograms Computer analysis of interferograms Computer analysis of interferograms Typical Interferogram Surface Error = (/2) (/S) Classical...
Arizona >> OPTICS >> 513 (Fall, 2009)
4.8 Classical Interferogram Analysis Elementary analysis of interferograms Elementary analysis of interferograms Computer analysis of interferograms Computer analysis of interferograms Typical Interferogram Surface Error = (/2) (/S) Classical...
Arizona >> OPTICS >> 05 (Fall, 2009)
5. Direct-Phase Measurement Interferometry 5.1 Phase Shifters 5.2 Zero-Crossing Technique 5.3 Phase-Lock Interferometry 5.4 Up-Down Counters 5.5 Phase-Stepping and Phase-Shifting (Integrated Bucket) 5.5.1 Algorithms 5.5.1.1 Four Step 5.5.1.2 Integrat...
Arizona >> OPTICS >> 513 (Fall, 2009)
5. Direct-Phase Measurement Interferometry 5.1 Phase Shifters 5.2 Zero-Crossing Technique 5.3 Phase-Lock Interferometry 5.4 Up-Down Counters 5.5 Phase-Stepping and Phase-Shifting (Integrated Bucket) 5.5.1 Algorithms 5.5.1.1 Four Step 5.5.1.2 Integrat...
Arizona >> CHAPTER >> 513 (Fall, 2009)
5. Direct-Phase Measurement Interferometry 5.1 Phase Shifters 5.2 Zero-Crossing Technique 5.3 Phase-Lock Interferometry 5.4 Up-Down Counters 5.5 Phase-Stepping and Phase-Shifting (Integrated Bucket) 5.5.1 Algorithms 5.5.1.1 Four Step 5.5.1.2 Integrat...
Arizona >> OPTI >> 510 (Fall, 2009)
Fall 2008 OPTI 510L Fundamentals of Applied Optics Lab Instructor: Jim Burge Optical Sciences 733 (520) 621-8182 jburge@optics.arizona.edu Teaching Assistant: Rene Zehnder Optical Sciences 300 (520) 626-7302 rzehnder@optics.arizona.edu Class: Mein...
Arizona >> OPTI >> 510 (Fall, 2009)
Error Analysis Error analysis is an extremely important part of any measurement. All the uncertainties in a measurement conspire to give the incorrect result. It is important that you understand the limitations of your measurements and that you alway...
Arizona >> OPTI >> 510 (Fall, 2009)
510L LAB 7 Coma Set-up Equipment: o o o o o o Fiber Light Source (it\'s good to have a bright source when using small pinholes) 50 m Pinhole (or any small pinhole) Two slow, plano-convex lenses for collimating and focusing Two fast lenses of matchin...
Arizona >> HW >> 10 (Fall, 2009)
Two Part Epoxy Adhesives A Technical Memo Prepared for Opti 521 Introduction to Opto-Mechanical Engineering By Scott Gibb November 24, 2006 Description and Basic Characteristics Two-part epoxy adhesive is a type of thermosetting polymer. A thermoset,...
Arizona >> HW >> 521 (Fall, 2009)
Two Part Epoxy Adhesives A Technical Memo Prepared for Opti 521 Introduction to Opto-Mechanical Engineering By Scott Gibb November 24, 2006 Description and Basic Characteristics Two-part epoxy adhesive is a type of thermosetting polymer. A thermoset,...
Arizona >> HW >> 10 (Fall, 2009)
Optomechanical Epoxy Adhesives Mark T. Sullivan Lockheed Martin Space Systems Advanced Technology Center, 3251 Hanover Street, Palo Alto, CA 94304 mark.t.sullivan@lmco.com 650/424-2722 SUMMARY This report summarizes the basic characteristics and pro...
Arizona >> HW >> 521 (Fall, 2009)
Optomechanical Epoxy Adhesives Mark T. Sullivan Lockheed Martin Space Systems Advanced Technology Center, 3251 Hanover Street, Palo Alto, CA 94304 mark.t.sullivan@lmco.com 650/424-2722 SUMMARY This report summarizes the basic characteristics and pro...
Arizona >> HW >> 10 (Fall, 2009)
Manual Linear Stages Dathon Golish OPTI 521 HW #10b University of Arizona 520-626-9230 dgolish@u.arizona.edu November 29, 2006 This report will compare and contrast the characteristics of various manual linear stages of moderate travel distance (~10 ...
Arizona >> HW >> 521 (Fall, 2009)
Manual Linear Stages Dathon Golish OPTI 521 HW #10b University of Arizona 520-626-9230 dgolish@u.arizona.edu November 29, 2006 This report will compare and contrast the characteristics of various manual linear stages of moderate travel distance (~10 ...
Arizona >> HW >> 10 (Fall, 2009)
OPTI 521 HW 10 ADHESIVES TALIAFERRO Summers Optical Type RD3-74 2-Part Optical Epoxy with Plasticizer for Low Curing-Stress Applications http:/www.emsdiasum.com/summers/optical/cements/default.htm SUMMARY AND BASIC CHARACTERISTICS Summers Optical s...
Arizona >> HW >> 521 (Fall, 2009)
OPTI 521 HW 10 ADHESIVES TALIAFERRO Summers Optical Type RD3-74 2-Part Optical Epoxy with Plasticizer for Low Curing-Stress Applications http:/www.emsdiasum.com/summers/optical/cements/default.htm SUMMARY AND BASIC CHARACTERISTICS Summers Optical s...
Arizona >> HW >> 10 (Fall, 2009)
Milbond Structural Adhesive A Technical Memo for OPTI521 Tim Williams Nov. 30, 2006 Introduction and Basic Characteristics Basic characteristics, strengths, applications and usage information are given for Milbond Structural Adhesive. Milbond is a st...
Arizona >> HW >> 521 (Fall, 2009)
Milbond Structural Adhesive A Technical Memo for OPTI521 Tim Williams Nov. 30, 2006 Introduction and Basic Characteristics Basic characteristics, strengths, applications and usage information are given for Milbond Structural Adhesive. Milbond is a st...
Arizona >> HW >> 10 (Fall, 2009)
UV Curing Adhesives Jay Vizgaitis, Opti 521 Homework 10 Properties: UV curing adhesive are one part adhesives that cure within seconds when UV light is applied. They are used for bonding glasses to glass, metals, and plastics for applications such as...
Arizona >> HW >> 521 (Fall, 2009)
UV Curing Adhesives Jay Vizgaitis, Opti 521 Homework 10 Properties: UV curing adhesive are one part adhesives that cure within seconds when UV light is applied. They are used for bonding glasses to glass, metals, and plastics for applications such as...
Arizona >> WORKSHOP >> 2009 (Fall, 2009)
Co-Sponsor: http:/spie.org U of AZ College of Optical Sciences Computer Generated Holography (CGH) and Diffractive Optical Element (DOE) Workshop Introduction From the early work of Lohmann to present day, applications such as multi-spectral disper...
What are you waiting for?