CRaTER Thermal Analysis C R T

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CRaTER Thermal Analysis
Bob Goeke for Huade Tan
Cosmic RAy Telescope for the Effects of Radiation
Contents
•
System Overview
– Design & Requirements
•
Inputs and Assumptions
– Power Dissipations
– Environment and Orbit
– Current Model
•
Results
– Instrument temperatures
– Orbital temperature ranges
•
Conclusions
– Uncertainties and Improvements
Cosmic RAy Telescope for the Effects of Radiation
July 15, 2016
Thermal Engineering
2
Design Approach & Requirements
• Design Approach
– Radiatively isolated with multi-layer thermal blanket over entire
surface.
– Single layer blanket covering 10cm2 telescope apertures nadir and
zenith
– Tight conductive coupling to spacecraft optical bench
• Interface Requirements at Instrument Mounting Surface
Survival
Operational
Rate-of-Change
Gradient
25 C
n/a
n/a
-40 C
-30 C
Thermal ICD para 6.1
Thermal ICD para 6.2
Thermal ICD para 6.3
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July 15, 2016
Thermal Engineering
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Model Requirements
•
The CRaTER thermal model is required to represent, with as much detail as
possible, the behavior of critical reference points in the CRaTER instrument
in a computer simulated mission orbit environment in order to anticipate and
correct for any possible hardware degradation or failure under similar
circumstances.
•
In order to ensure the survival of the CRaTER instrument, the thermal
model should account for the worst case scenarios in both hot and cold
temperature limits.
•
The model must adhere to all RGMM and RTMM requirements given in the
TICD.
Cosmic RAy Telescope for the Effects of Radiation
July 15, 2016
Thermal Engineering
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Instrument Power Consumption
•
Power dissipations in the instrument are modeled as heat loads. The relevant
values of such heat loads are given in the following table. Hot case numbers are
taken to be 120% of nominal and cold case numbers are assumed to be 80 % of
the nominal power consumption of each electrical component.
digital board
analog board
5V power supply
dual 5 V power supply
telescope
total power
Hot Case (W) Nominal (W)
Cold Case (W)
3.19
2.66
2.12
2.52
2.10
1.68
1.33
1.11
0.89
1.94
1.62
1.29
0.10
0.08
0.06
9.08
7.57
6.04
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July 15, 2016
Thermal Engineering
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MLI and Optical Bench
•
Surface finish properties:
Cold Case
Coating
Kapton 3mil
Black Kapton 3 mil
Germanium Black Kapton
Silver Teflon (5 mil)3,4
Silver Teflon (10 mil)4
•
Hot Case
Location
Absorptance
S
Emittance
H
Absorptance
S
Emittance
H
MLI Blanket
MLI Blanket
0.45
0.91
0.49
0.08
0.09
0.80
0.81
0.81
0.78
0.87
0.51
0.93
0.51
0.11
0.13
0.76
0.78
0.78
0.73
0.83
Effective emittance:
e* for MLI assumed to be .005 or .03 for best and worst cases.
• Modeled optical bench temperatures are +25 C hot case, –30 C cold case
and –40 C cold survival case.
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July 15, 2016
Thermal Engineering
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Environmental Parameters
•
Orbital Heat Rate Factors:
Solar Constant
Albedo Factor
Planetshine/Infrared Emission
Hot Case
Cold Case
Survival Case
1450 W/m2 1280 W/m2
1280 W/m2
0.13
0.06
0.06
--5.2 W/m2
5.2 W/m2
•
Lunar surface IR constants modeled after the characteristic Lambertian surface
having a subsolar temperature of 1420 w/m2 hot case and 1280 w/ m2 cold case to a
shadow IR emission of 5 w/m2 for both cases..
•
Surface IR emissions across the bright side are described in the General Thermal
Subsystem specification 431-SPEC-000091.
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July 15, 2016
Thermal Engineering
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Orbit
•
•
•
The current instrument model is
assumed to be in a basic polar orbit at
a hot case altitude of 30 km.
At a Beta angle of zero, the model
simulates the hot operational worst
case scenario where the instrument
cycles from one temperature extreme
to the other.
The total heat absorbed (solar, albedo
& IR) by the instrument through each
orbit is computed using the Radcad
Monte Carlo ray trace method.
Cosmic RAy Telescope for the Effects of Radiation
July 15, 2016
Thermal Engineering
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Orbit
•
•
•
This latest spacecraft geometric
model received from GSFS (as
seen to the left) corresponds to
the hot case solar array
orientation.
For the Beta 0 case, the solar
array articulates during the orbit.
Given the latest results of the
model, minor changes in heat
loads should not generate
significant changes in
temperature.
Cosmic RAy Telescope for the Effects of Radiation
July 15, 2016
Thermal Engineering
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Orbit
•
•
•
The current instrument model is
assumed to be in a basic polar orbit at
a cold case altitude of 70 km.
At a Beta angle of 90 degrees, the
model simulates the cold operational
worst case scenario where the
instrument never crosses the subsolar
point.
The total heat absorbed (solar, albedo
& IR) by the instrument through each
orbit is computed using the Radcad
Monte Carlo ray trace method.
Cosmic RAy Telescope for the Effects of Radiation
July 15, 2016
Thermal Engineering
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Orbit
•
•
•
This latest spacecraft geometric
model received from GSFS (as
seen to the left) corresponds to
the Beta 90 cold case solar array
orientation.
The solar array is stationary in
this case and faces the sun at all
points in the orbit.
Given the latest results of the
model, minor changes in heat
loads should not generate
significant changes in
temperature.
Cosmic RAy Telescope for the Effects of Radiation
July 15, 2016
Thermal Engineering
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Orbit
•
•
•
•
This latest spacecraft geometric
model received from GSFS (as
seen to the left) corresponds to
the Beta 90 cold survival case
solar array orientation.
The solar array is stationary in
this case and faces the sun at all
points in the orbit.
LRO is flying in a solar inertial
mode with the –Y pointing at the
sun at all times.
During this case, the instrument
will never be in direct sunlight
due to the placement of the solar
array.
Cosmic RAy Telescope for the Effects of Radiation
July 15, 2016
Thermal Engineering
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Current Instrument Model
•The coordinate system used in the
CRaTER model corresponds with
the reference coordinate system of
the spacecraft as outlined in the
TICD.
•The current instrument model
consists of 60 nodes and 52
surfaces.
Cosmic RAy Telescope for the Effects of Radiation
July 15, 2016
Thermal Engineering
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Current Instrument Schematic
•
Analog
Housing
•
Digital
Housing
Telescope
Housing
The CRaTER instrument is
divided into three distinct
radiatively coupled regions.
Each housing consists of an
isolated PCB or group of
PCBs and a specific power
dissipation as described in
the model inputs.
Cosmic RAy Telescope for the Effects of Radiation
July 15, 2016
Thermal Engineering
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Mounting Footprint
•
•
•
•
CRaTER’s current design mounts to
the spacecraft at six points located at
the base of the electronics box.
Each modeled mounting plate is
scaled to adjust for the true contact
surface area.
The model assumes a contact
conductance between the mounting
feet and the optical bench of 1.3 W/C
per mounting foot.
The surface finish of the instrument
panel directly facing the LRO is
assumed to be anodized aluminum
with an emissivity of 0.6.
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Thermal Engineering
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Results: Instrument
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Beta 00 Hot Temps
30
29
Temp (C)
28
27
26
25
24
0
5000
10000
15000
20000
25000
Time (s)
CR_EBOX.T101
CR_EBOX.T102
CR_EBOX.T103
CR_EBOX.T104
CR_EBOX.T105
CR_EBOX.T106
CR_EBOX.T201
CR_EBOX.T202
CR_EBOX.T301
CR_EBOX.T302
CR_EBOX.T303
CR_EBOX.T401
CR_EBOX.T402
CR_EBOX.T403
CR_EBOX.T501
CR_EBOX.T502
CR_EBOX.T601
CR_EBOX.T602
CR_EBOX.T603
CR_EBOX.T701
CR_EBOX.T702
CR_EBOX.T703
CR_EBOX.T704
CR_EBOX.T705
CR_EBOX.T706
CR_EBOX.T707
CR_EBOX.T708
CR_EBOX.T801
CR_EBOX.T802
CR_EBOX.T802
CR_EBOX.T803
CR_EBOX.T804
CR_EBOX.T805
CR_EBOX.T806
CR_EBOX.T807
CR_EBOX.T808
CR_EBOX.T809
CR_EBOX.T810
CR_EBOX.T811
CR_EBOX.T812
CR_SCOPE.T1
CR_SCOPE.T2
CR_SCOPE.T101
CR_SCOPE.T301
CR_SCOPE.T302
CR_SCOPE.T401
CR_SCOPE.T501
CR_SCOPE.T502
CR_SCOPE.T503
CR_SCOPE.T601
CR_SCOPE.T602
CR_SCOPE.T603
CR_SCOPE.T801
CR_SCOPE.T802
CR_IF.T401
CR_IF.T402
CR_IF.T403
CR_IF.T404
CR_IF.T405
CR_IF.T406
Cosmic RAy Telescope for the Effects of Radiation
July 15, 2016
Thermal Engineering
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Beta 90 Cold Case Temps
-25
0
5000
10000
15000
20000
25000
-26
Temp (C)
-27
-28
-29
-30
-31
Time (s)
CR_EBOX.T101
CR_EBOX.T102
CR_EBOX.T103
CR_EBOX.T104
CR_EBOX.T105
CR_EBOX.T106
CR_EBOX.T201
CR_EBOX.T202
CR_EBOX.T301
CR_EBOX.T302
CR_EBOX.T303
CR_EBOX.T401
CR_EBOX.T402
CR_EBOX.T403
CR_EBOX.T501
CR_EBOX.T502
CR_EBOX.T601
CR_EBOX.T602
CR_EBOX.T603
CR_EBOX.T701
CR_EBOX.T702
CR_EBOX.T703
CR_EBOX.T704
CR_EBOX.T705
CR_EBOX.T706
CR_EBOX.T707
CR_EBOX.T708
CR_EBOX.T801
CR_EBOX.T802
CR_EBOX.T802
CR_EBOX.T803
CR_EBOX.T804
CR_EBOX.T805
CR_EBOX.T806
CR_EBOX.T807
CR_EBOX.T808
CR_EBOX.T809
CR_EBOX.T810
CR_EBOX.T811
CR_EBOX.T812
CR_SCOPE.T1
CR_SCOPE.T2
CR_SCOPE.T101
CR_SCOPE.T301
CR_SCOPE.T302
CR_SCOPE.T401
CR_SCOPE.T501
CR_SCOPE.T502
CR_SCOPE.T503
CR_SCOPE.T601
CR_SCOPE.T602
CR_SCOPE.T603
CR_SCOPE.T801
CR_SCOPE.T802
CR_IF.T401
CR_IF.T402
CR_IF.T403
CR_IF.T404
CR_IF.T405
CR_IF.T406
Cosmic RAy Telescope for the Effects of Radiation
July 15, 2016
Thermal Engineering
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Beta 90 Cold Survival Case Temps
-35.5
-36
0
5000
10000
15000
20000
25000
-36.5
Temp (C)
-37
-37.5
-38
-38.5
-39
-39.5
-40
-40.5
Time (s)
CR_EBOX.T101
CR_EBOX.T102
CR_EBOX.T103
CR_EBOX.T104
CR_EBOX.T105
CR_EBOX.T106
CR_EBOX.T201
CR_EBOX.T202
CR_EBOX.T301
CR_EBOX.T302
CR_EBOX.T303
CR_EBOX.T401
CR_EBOX.T402
CR_EBOX.T403
CR_EBOX.T501
CR_EBOX.T502
CR_EBOX.T601
CR_EBOX.T602
CR_EBOX.T603
CR_EBOX.T701
CR_EBOX.T702
CR_EBOX.T703
CR_EBOX.T704
CR_EBOX.T705
CR_EBOX.T706
CR_EBOX.T707
CR_EBOX.T708
CR_EBOX.T801
CR_EBOX.T802
CR_EBOX.T802
CR_EBOX.T803
CR_EBOX.T804
CR_EBOX.T805
CR_EBOX.T806
CR_EBOX.T807
CR_EBOX.T808
CR_EBOX.T809
CR_EBOX.T810
CR_EBOX.T811
CR_EBOX.T812
CR_SCOPE.T1
CR_SCOPE.T2
CR_SCOPE.T101
CR_SCOPE.T301
CR_SCOPE.T302
CR_SCOPE.T401
CR_SCOPE.T501
CR_SCOPE.T502
CR_SCOPE.T503
CR_SCOPE.T601
CR_SCOPE.T602
CR_SCOPE.T603
CR_SCOPE.T801
CR_SCOPE.T802
CR_IF.T401
CR_IF.T402
CR_IF.T403
CR_IF.T404
CR_IF.T405
CR_IF.T406
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July 15, 2016
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Results Summary
•
CRaTER is driven by the temperature of the optical bench.
instrument interface
pcb's
nadir
scope
•
Hot Case Max Operating
Cold Case Min Operating
Cold Case Survival Min
Temperature [optical bench Temperature [optical bench Operating Temperature
at 25C]
at -30 C}
[optical bench at -40 C}
25 to 28C
-29 to -30C
-38 to -40C
27 to 30C
-26 to -27C
-37 to -39C
26 to 29C
-28C
-38C
26 to 29C
-28.5C
-37
Instrument Internal temperatures vary <5 C from the optical bench temperature
between extremes of hot and cold.
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July 15, 2016
Thermal Engineering
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Summary and Conclusions
•
Estimate of Internal Temperatures:
– Maximum internal temperatures are no more than 5 degrees C above the interface
temperature.
•
Uncertainties and Modeling Improvements:
– Temperature dependence of material properties: variations in thermal conductivity
can be neglected given an instrument temperature fluctuation of no more than a few
degrees C through the beta 0 orbit.
– Incorporating TEPs into the thermal model
– Incorporating actual circuitry details on the PCBs
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July 15, 2016
Thermal Engineering
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Electronic Component Temperatures
•
There are only 3 electrical components on the PC boards which draw more
than 100mw of power:
–
–
–
–
•
•
•
Part
1553 Interface
Actel FPGA
BAE SRAM
2.5 Linear Regulator
Typ. Pwr.
1100 mw
330 mw
100 mw
170 mw
Theta JC
7.6 C/W
2.0 C/W
11 C/W
2.3 C/W
Rise
8.4 C
0.7 C
1.1 C
0.4 C
The 1553 part has a surface area of 4 in2; if the only heat rejection path were
radiation from its top surface to the e-box walls, the junction temp would be
101C -- still below the required (derated) limit of 110C. Tests on the
engineering unit will guide us in adding some more margin to this component.
The other point sources of heat are the regulated power supplies; these are
mounted directly to the enclosure mid-plate with 3 #10-32 bolts each.
Both the 1553 Interface and the dual power supply are monitored in the
normal housekeeping stream.
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July 15, 2016
Thermal Engineering
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Cosmic RAy Telescope for the Effects of Radiation
July 15, 2016
Thermal Engineering
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Backup Slides
Cosmic RAy Telescope for the Effects of Radiation
Inputs
•
Thermal and Physical properties:
Material
Aluminum 6061
PCB
3mil Black Kapton Film
MLI
•
k (W/m/K)
Cp (J/kg/K) rho (kg/m^3) e*
180
869
2700
59.8
1003
2819
0
0
0
0
0
0
0.8
0.7
0.81
0.05
Optical Properties:
Material
Aluminum 6061
PCB
3mil Black Kapton Film
a
e
0.1
0.7
0.91
0.025
0.7
0.81
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July 15, 2016
Thermal Engineering
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Assumptions
•
Material properties:
– Thermophysical properties of Al-6061 were taken from Matweb databases
– Optical properties of Aluminum obtained from Cooling Techniques for Electronic
Equipment: Second Edition
•
MLI assumptions:
– Currently modeled using bulk properties
•
PCB assumptions:
– 2 ground and power layers (80% fill) and 4 signal layers (20% fill), 1 mm total thickness
– PCB properties determined at www.frigprim.com/online/cond_pcb.html
•
TEP assumptions:
– Currently not modeled
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July 15, 2016
Thermal Engineering
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Assumptions
•
Conductive Resistances:
– Interface characteristics between PCB and Aluminum are assumed to be of copper to
aluminum in vacuum at 30 C referred to in Heat Transfer. Holman, J.P
– Surfaces of the Ebox are assumed to behave under characteristic conduction of Al-6061
(assuming that the ebox is constructed out of a single block of aluminum)
– Conductive resistances are modeled between the top and bottom covers of the ebox, and the
interface between the ebox and the telescope assembly.
•
Internal Radiation:
– View factors between internal surfaces determined by Radcad using radk ray trace method
– Emissivity factors are calculated assuming either infinite parallel planes or general case for
two surfaces from PCBs to the interior walls.
•
Heat Flow to the Space Craft:
– Assuming interface temperatures of –40 -30 and 25 degrees C
– Contact conductance of mounting feet to LRO assumed to be 1.3 W/C per foot
– Radiative heat transfer to the LRO through 15 layer MLI
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July 15, 2016
Thermal Engineering
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