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INSTRUMENT / OPTOMECHANICAL INFORMATION EXCHANGE
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March 2000; Volume 2, Number 3
Edited by Roger S. Reiss 
[EMAIL PROTECTED]


IN THIS ISSUE:
Instrumentation at Photonics East
Space Communication Receiver
Metal / Glass Bonding
Thin Wall Brazing
Micro Beam Deflector 
To subscribe or unsubscribe

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Instrumentation at Photonics East

At Photonics East, 5-8 November 2000, there will be numerous sessions of
interest to the instrumentation and optomechanical community. Please take a
look at the call for papers at http://spie.org/info/pe/ for more
information. Within the "Intelligent Systems for Advanced Manufacturing"
symposium you'll find the following conference. This is a great opportunity
for anyone involved in the field in the Northeast to participate in and
support our community in the region. If you live within a couple hours'
drive of Boston, please plan to attend. A good turnout (both in papers
submitted and people showing up) will help to establish this conference for
years to come. Abstract due date is 10 April 2000.

Optomechanical Engineering Northeast (RB14)

Conference Chair: Mark A. Kahan, Optical Research Associates 

Cochairs: Roger S. Reiss, R.S. Reiss Associates; Daniel Vukobratovich, 
Raytheon Systems Co.; Paul R. Yoder, Jr., Consultant in Optical Engineering 

This will be a two-day engineering conference on new models/methods,
enabling technology, and emerging hardware. Paper contributions are
solicited on, but not limited to, the following topics: 
  - modeling 
  - thermo-optical modeling 
  - structural modeling 
  - integrated optical and AO modeling 
  - contamination, radiation and spacecraft charging hardware 
  - optomechanics of photonic devices 
  - optomechanics of MEMS, problems and hardware 
  - OM of telecommunication systems 
  - aerospace updates 

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Title: Space Communication Receiver 
(Part Two; Part One appeared in last issue.) 

Key words  :  receiver   space   communication 

Source: "Receiver Front End (RFE) for Optical Free Space Communications" by
Ulrich Hildebrand, ANT Nachrichtenhnik GmbH, D 71522 Backnang, Germany;
SPIE Proceedings, Vol. 2210,  page 96. 

  
The RFE consists of a housing, an optical system, lens and the detector
circuit (and detector circuit mounting provisions).  The reference article
discusses the mechanical and thermal aspects of the design, necessary to
obtain and maintain the required angular stability. 

The lens mounting (a must see illustration in the reference article)
consists of lens (Fused Silica) and the lens barrel (Titanium).
Consideration was given to a bonding but was abandoned because of out
gassing and qualifications problems (Editors note:  I have been working
with JPL / NASA and have a recommended material, 'RTV 566 A / B'.  Any
questions on application of this material or any RTV or epoxy, please email
<[EMAIL PROTECTED]>).  The lens is held in the lens mount by two sets of
springs; axial and radial.  The radial springs keep the lens centered using
a concentric pre loading.  The axial springs keeps the lens against the
mounting shoulder using an axial pre load.  The spring pre loads forces are
determined by the acceleration of vibration testing and or lift of
acceleration. 

The RFE has an operational temperature range of 20 + / - 8 * C.  There is
good thermal conductive coupling to the optical bench of 1 W / K with an
RFE power dissipation of 1.3 W.  The thermal design is a compromise between
mechanical integrity (stiffness) with good thermal conductivity and a
lightweight design that relies on radiant space cooling.  The housing is
coated with a black oxide ceramic layer with a low out gassing property and
an emmisivity of 0.8 

The conductive thermal interface is concentrated at the rear mounting foot.
 A thermal path is required between the detector circuit and the rear foot
because the detector circuit dissipates the largest part of the dissipated
power (the conductivity of the Titanium housing is not adequate).  This
path consists of a thermal conductor plate made of MoCu with a copper foil
beneath this plate and the detector circuit.  MoCu has a CTE close to
Titanium with conductivity of Aluminum.  The rotary mounting joints used
during alignment are clamped after alignment procedure is complete in order
to minimize temperature differences at these locations. 
  
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Title: Metal / Glass Bonding

Key words:  glass   metal   bonding

Source:  Jet Propulsion Laboratory (NASA), Pasadena, CA

Jet Propulsion Laboratory (NASA), Pasadena , CA has designed and
developed a metal-organic film which can be thermally bonded to glass
pieces and then soldered or welded to form a hermetic seal.  The film is
applied as an ink which consists of silver neodecanoate in xylene.

The relative amounts of ingredients are selected to control the desired
viscosity (application is by a simple scribing pen).  The ink like
mixture is deposited in matching pattern on two pieces of flat glass.
The pattern on the lower glass peice is a slightly wider line than the
line on the lower glass.  The glass pieces are heated in air to 260 * C
to evaporate the xylene and decompose the silver neodecanoate, leaving
adherent patterns on the glass pieces.  Solder paste is deposited on the
wider line and air dried.  The upper glass is placed over the lower
glass with its silver metal pattern resting on the solder paste.  The
glass pieces are clamped together and soldered, using the standard
thermal cycle, specified for the solder.  If the seal location requires
minimum heating, the heat for decomposition and the soldering can be
supplied by a well controlled laser beam which will confine the high
temperatures to the sealing region.

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Title  :  Thin Wall Brazing

Key words  :  brazing   thin   wall

Source:  "Brazing Book" by Handy & Harman, http://www.brazingbook.com

For fabrication using 'thin wall brazing' consideration is given to:
-    metals being joined
-    design of the joint configuration
-    ambient operating environment
-    economics of the fiiler material

If the parts being brazed are dissimilar metals, a filler material
should be used that will 'wet' both metals.  The filler material chosen
should flow readily over both metal surfaces and securely bond to each
metal.  Molten filler material has  the capability to alloy with a base
metal.

Consideration should be given to the difference in thermal expansion of
the two dissimilar metals.  This difference will effect the initial
clearance chosen for assembly heating during brazing.  To compensate of
this mismatch, start with a loose fit, so that when the heated assembly
reaches brazing temperature, the the gap separation is close to what was
desired.  Ideal joint clearance for brazing ranges from .001" to .002".

For wider clearances, a filler material can be formulated to
specifically fill a loose fit.  A filler material with a narrow melting
range is extremely hard to find.  A filler material with a broad melting
range is slow and sluggish, enabling the filler material to fill the
wider gap.

For thin wall brazed assemblies consideration should be given to any
vibration environment since vibration will fracture a brazed joint and
cause elongation of a fracture.

For economic reasons (usually not a factor in precision instruments and
devices), selection of the filler material should be with the lowest
silver content that will achieve the requirements of the 'thin wall
brazing' joint.

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Title  :  Micro Beam Deflector 

Key words  :  micro   light   deflector 

Source  :  "Micro-opto-mechanical beam deflectors" by Steffen Glocker, Rolf
Goring, and Torsten Possner, Fraunhofer Institute for Applied Optics and
Precision Engineering Jena, Jena, Germany, gloeckne@iof,fhg.de, Opt. Eng.
36(5) 1339-1345 (May 1997). 

Abstract: "...(Since) the required displacement of the micro-optical
components for efficient beam manipulation is quite small, high-speed
actuators with small electrical power consumption can be used (for light
beam deflection and light beam modulation)...The combination of
micro-optical components already available and (the use of) semi classical
piezoelectric actuators (allows for) new types of switching and modulation
systems for a very broad spectrum of applications." 

In the reference paper, a number of micro-optical systems concepts are
presented; 
-   steering of coherent and incoherent beams 
-   general aspects of micro-optical beam steering 
-   beam scanning systems (especially with Gaussian distribution) 
-   deflecting incoherent beams (emitted by multimode fibers) 
-   systems integration and applications 
-   conclusions and proposed future work 
-   system requirements 
        light losses 
        resolution (number of resolvable beams, behind the scanner) 
        cross talk (between different steering positions) 
        steered beam quality 
        switching time 
        modulation rate 

The actuation system is a critical area for the micro-optical scanners.
Scanning is achieved by the mechanical movement of the optical elements.
The switching times are restricted by the mass of the optical elements and
the amount of the movement required.  The micro-optical components used are
from several tens of milligrams up to several grams in mass and many
actuators are too weak for load (electrostatic, thermal. or magnetic
(others) actuators).  Some applications require switching times of a few
milliseconds, which can utilize piezoelectric actuators (these are actually
stronger than required). 

Bimorph piezoelectric layers can achieve movements of 100 um and even more.
 The actuator consist of two connected piezoelectric layers acting like a
bimetalic strip operating in a bending mode.  Translation can be achieved,
instead of bending, in one direction, if two of the bimorph layers are
combined to form a parallelogram. This suppresses movement in the unwanted
direction.  A planar and cylinder arrangement of the parallelogram has the
capability of  two-dimensional translation.  Linear sensors can be used for
position detection and direction.  Displacement can be adjusted using
various lengths and material stiffness..  Maximum displacements of 20 to
200 um with resonant frequencies of 0.1 to 0.6 kHz and switching times of a
few milliseconds is achievable. 
  
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