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MAXIM Periscope Module

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very low power dissipation within the optics module. infrequent operation of mirror actuators ... Varied the power dissipation on the optical bench by 5.6 uW / Hz ... – PowerPoint PPT presentation

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Title: MAXIM Periscope Module


1
MAXIM Periscope Module
  • Thermal
  • Rob Chalmers
  • 25 April 2003

2
Thermal Requirements
  • Temperature Stability (tens of mK)
  • Optical Bench
  • Mirrors
  • Temperature Gradients (TBD)
  • Mirrors
  • Optical Bench
  • Thermal Settling Time
  • Minimize recovery time following operation of
    Mirror Actuators

3
Materials
  • Requirements for extreme dimensional stability
    demand the use of materials with extremely low
    CTE. Some candidates
  • Material CTE
  • ULE (Corning 7972 premium grade) 0.0 0.10 x
    10-9/K
  • Zerodur 0.0 0.10 x 10-6/K
  • Invar 2.0 x 10-6/K

4
Thermal Design Concept
MAXIM Thermal Requirements appear similar to the
LISA Instrument, and the design approach is
similar
  • Passive design with multiple nested thermal
    regions
  • Optical bench highly isolated from instrument
    housing
  • Instrument housing highly isolated from
    spacecraft thermal influences
  • Low emittance (gold) thermal shields provide
    radiative isolation between regions
  • Exotic conductive isolation (Kevlar suspension or
    similar) may be required to achieve required
    thermal stability
  • Temperature-controlled thermal pre-collimators
    around entrance and exit apertures

5
Thermal Design Concept
Thermally-Isolating Kinematic Mounts
Thermal Pre-Collimators at Entrance and Exit
Apertures
6
Temperature Stability
  • MAXIM stability requirements and baseline
    thermal design approach are similar to LISA
  • (see backup charts)

7
Mirror Transient Response
  • 1.5 Watts applied to center of 5 x 20 x 2 cm ULE
    mirror for 10 seconds

8
Temperature GradientsThermal Influence of
Aperture on Mirror Gradients
0C aperture (assumed)
21C enclosure (assumed)
  • An aperture slit at 0C induces mirror
    temperature gradient of approx. 20 mK
  • Heated thermal pre-collimator reduces gradient
    to near zero.

9
Summary, Recommendations Future Work
  • Passive thermal design is a feasible approach
  • benign thermal environment
  • very low power dissipation within the optics
    module
  • infrequent operation of mirror actuators
  • Choice of materials for mirrors and optical bench
    greatly influences temperature stability and
    gradient requirements.
  • Need for extreme thermal isolation between the
    stable optics and the relatively unstable
    spacecraft will be a challenge to structural
    design.
  • Required analytical precision may test limits of
    existing thermal software. At these levels,
    machine-dependent round-off errors can be
    significant. Validation of analytical results by
    comparing different solution methods and
    convergence criteria is recommended.

10
Backup Charts
MAXIM Thermal Requirements appear similar to the
LISA Instrument. The following charts provided by
Hume Peabody are taken from a presentation of the
LISA thermal design.
11
LISA Thermal Design (1 of 5)
  • Overall philosophy
  • Minimize radiative and conductive heat transfer
    to the optical bench and gravitational reference
    sensor
  • Minimize temperature fluctuations across the
    optical bench and gravitational sensor
  • Extremely stable power system
  • Orbit provides a stable thermal environment
  • Two sources of heat solar input and electronics
  • Three zones of thermal isolation are used in
    series
  • Zone 1 Solar input ?SA ?Structure
  • Zone 2 Structure and electronics ? Y-Tube
  • Zone 3 Y-tube ? Optical bench and gravitational
    reference sensor

12
LISA Thermal Design (2 of 5)
  • Key design features
  • Solar cells are mounted on thin CFRP face sheets
    with insulating foam in between
  • Low conductance standoffs mount solar arrays to
    the Al honeycomb top plate
  • Top plate is gold-coated

Energy flow values represent steady-state
hot/cold cases (f1e-4)
Radiation Conduction
13
LISA Thermal Design (3 of 5)
  • Y- Tube constructed from CFRP
  • Electronics mounted with low conductance feet
  • Stable electronics power
  • Radiator rejects structure and electronics heat

146.2 W 142.7 W
SPACE
RADIATOR
116.4 W 113.7 W
27.2 W 26.3 W
24.3 W 23.5 W
13.6 W 14.8 W
ELECT. BOXES 154.2 W
STRUCTURE
INPUT FROM S/A 40.0 W 34.6 W
8.3 W 10.1 W
7.2 W 6.7 W
16.0 W 15.6 W
3.1 W 2.9 W
Y TUBE.
14
LISA Thermal Design (4 of 5)
RADIATOR
INPUT FROM STRUCTURE ELECT BOXES 26.3 W /
25.2 W
SPACE
42.3 W 41.4 W
  • Gold thermal shield between Y-Tube and optical
    bench
  • Optical bench made from ULE
  • Stable power dissipation

2.7 W 2.6 W
1.3 W 1.2 W
2.30 W 2.26 W
Y-TUBE 4.3 W INT. POWER
SHIELDS
15.8 W 15.8 W

INTERIOR
0.06 W 0.06 W
0.02 W 0.02 W
0.24 W 0.22 W
0.11 W 0.11 W
OPTICAL BENCH (2.9 W of internal power)
Interior includes everything except optical
bench and thermal shield
15
LISA Thermal Design (5 of 5)
  • Two driving thermal requirements
  • Stability of optical path of the cavity (30
    Hz/vHz) at 10-3 Hz
  • 60 x 10-6 K/vHz fluctuations across GRS housing
    at 10-4 Hz. (derived from radiometric effect,
    thermal radiation pressure)
  • RAL modeled the payload and spacecraft (Astrium)
  • Varied electronic power by 1 at 10 -4 Hz
  • Results showed that Optical Bench fluctuations
    are 6.5 x 10 -5 K
  • Assuming 3 x 10 -8 CTE and 0.3 meter Optical
    Bench ? 5.85 x 10 -13 change in length.
  • Varied the solar input by 0.3 at 10 -4 Hz
  • Results showed that fluctuations at the Optical
    Bench were 2.2 x 10 -6 K/vHz
  • Assuming 3 x 10 -8 CTE and 0.3 meter Optical
    Bench results in 1.98 x 10 -14/vHz
  • Varied the power dissipation on the optical bench
    by 5.6 uW / vHz
  • Results showed fluctuations were 2 x 10 -5 K/vHz
    at 1 x 10-3 Hz.
  • At 3 x 10 -3 Hz ? 4 x 10 -6 K/vHz (estimate)
  • (3 x 10-8/K) (4 x 10 -6 K/vHz) 1.2 x 10-13 /vHz
    x 2.8 x 10-14 Hz 34 Hz/vHz
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