Advanced Mirror Technology Development (AMTD) thermal ......• Larger aperture space telescopes are...
Transcript of Advanced Mirror Technology Development (AMTD) thermal ......• Larger aperture space telescopes are...
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Advanced Mirror Technology Development (AMTD) thermal trade studies
Thomas Brooks, Phil Stahl, Bill Arnold
NASA/MSFC
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• Efforts associated with this presentation are performed as part of the Advanced Mirror Technology Development (AMTD) program
• Larger aperture space telescopes are required to answer our most compelling science questions.
• AMTD’s objective is to mature to TRL-6 critical technologies needed to produce 4-m or larger flight-qualified UVOIR mirrors by 2018 so that a viable mission can be considered by the 2020 Decadal Review.
•To accomplish our objective, we: • Use a science-driven systems engineering approach.• Mature technologies required to enable highest priority science AND result in a high-performance
low-cost low-risk system.
What is AMTD?
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Description of Primary Mirror
• 4m Circular Monolith
• 0.152m depth front to back
• Light-weighted with a back sheet
• Areal Density is 146 kg/m2
• Optical face coated with εaluminum=0.03
• Fixed Mount
• Material Properties:
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MaterialConductivity[W/(m*K)]
Specific Heat[J/(kg*K)]
Density[kg/m3]
EmissivityCTE
[1/K]ULE 1.31 766 2210 0.82 30x10-9
Silicon Carbide 180 750 3100 0.9 2.2x10-6
Zerodur 1.46 800 2530 0.9 7x10-9
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Heat Flow Through Mirror
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• Most heat enters the mirror from the heated plate and exits through the optical surface
• Heat is transported by radiation (56%) and conduction (44%)
Not to scale
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Description of Telescope Architecture
• Cylindrical Shroud; 60˚ Scarf
• No secondary mirror or baffles
• MLI on outer surface of shroud & sides of mirror ε*MLI=0.03
• Inner surface of shroud painted black
• Heated plate behind mirror
• Placed at L2Mirror
Heated Plate
Shroud
Scarf
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279.925
279.950
279.975
280.000
280.025
280.050
280.075
0 10000 20000 30000 40000 50000
Shro
ud
Te
mp
era
ure
(K
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Time(s)
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WFE Contour Video
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WFE Visualization
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Sample WFE Contour Plot (50mK, 140s Period) Sample WFE with Focus, Tilts, and Astigmatisms Removed (50mK, 140s Period)
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WFE Stability versus Controllability
• Material: ULE
• Period of ACS: 5000s
• Controllability of ACS: Varied
• Density of Mirror: ULE Density
• Emissivity: 0.82
• Thicknesses: Baseline Design
• Conductivity: ULE Conductivity
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RM
S W
FE (
nm
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Time (s)
Control to 1mK Control to 5mK Control to 10mK Control to 50mK
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WFE Stability versus Controllability
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0
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RM
S W
FE -
Mea
n R
MS
WFE
(p
m)
Time (s)
Control to 1mK Control to 5mK Control to 10mK Control to 50mK
1.0, 10.4
5.0, 56.6
10.0, 113.4
50.0, 567.4
y = 11.359x - 0.462R² = 1
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100
200
300
400
500
600
0 10 20 30 40 50 60
RM
S W
FE R
ange
(p
m)
Shroud Controllability (mK)
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WFE Stability versus Period
• Material: ULE
• Period of ACS: Varied
• Controllability of ACS: 50mK
• Density of Mirror: ULE Density
• Emissivity: 0.82
• Thicknesses: Baseline Design
• Conductivity: ULE Conductivity
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140.0, 16.3
200.0, 23.8
600.0, 72.4
1,800.0, 208.4
3,600.0, 412.3
y = 0.1147x + 0.7095R² = 0.9999
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50
100
150
200
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300
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400
450
0 1000 2000 3000 4000
RM
S W
FE R
ange
(p
m)
Shroud Oscillation Period (s)
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WFE Stability versus Conductivity
• Material: ULE
• Period of ACS: 140s
• Controllability of ACS: 50mK
• Density of Mirror: ULE Density
• Emissivity: 0.82
• Thicknesses: Baseline Design
• Conductivity: Varied
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0.25, 17.40
0.5, 17.3
1.0, 17.0
2.0, 16.54.0, 15.2
8.0, 12.5
y = -0.6341x + 17.649R² = 0.9983
0
2
4
6
8
10
12
14
16
18
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0 2 4 6 8 10
RM
S W
FE R
ange
(p
m)
Normalized Conductivity (Conductivity / ULE Conductivity)
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WFE Stability versus Mass and Control
• Material: ULE
• Period of ACS: 140s
• Controllability of ACS: Varied
• Density of Mirror: Varied
• Emissivity: 0.82
• Thicknesses: Baseline Design
• Conductivity: ULE Conductivity
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20.00, 6.66
30.00, 9.90
40.00, 13.37
50.00, 16.77
60.00, 20.03
20.00, 2.3430.00, 3.37
40.00, 4.4050.00, 5.48
60.00, 6.61
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RM
S W
FE R
ange
(p
m)
Shroud Controllability (mK) @ Period of 140s
1x Mass
2x Mass
3x Mass
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WFE Stability versus Thicknesses
• Material: ULE
• Period of ACS: 140s
• Controllability of ACS: 50mK
• Density of Mirror: ULE Density
• Emissivity: 0.82
• Thicknesses: Varied
• Conductivity: ULE Conductivity
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0.5, 36.3
1.0, 17.3
2.0, 8.04.0, 3.5
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15
20
25
30
35
40
0 1 2 3 4 5
RM
S W
FE R
ange
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Normalized Rib Thickness (Simulated Rib Thickness/Design Rib Thickness)
y = 18.063/x - 0.31553xR2 = 0.9991
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WFE Stability versus Emissivity
• Material: ULE
• Period of ACS: 140s
• Controllability of ACS: 20mK
• Mirror Density: ULE Density
• Emissivity: Varied
• Thicknesses: Baseline Design
• Conductivity: ULE Conductivity
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y = -1.9733x + 8.4309R² = 0.9772
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7
8
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0 0.2 0.4 0.6 0.8 1
RM
S W
FE R
ange
(p
m)
Emissivity of Mirror Surfaces Except the Optical Face
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WFE Stability versus Material
• Material: Varied
• Period of ACS: 140s
• Controllability of ACS: 50mK
• Mirror Density: Material Based
• Emissivity: Material Based
• Thicknesses: Baseline Design
• Conductivity: Material Based
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Silicon Carbide, 850.79
ULE, 22.78 Zerodur, 5.01
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100
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Silicon Carbide ULE Zerodur
RM
S W
FE R
ange
(p
m)
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Quick Review
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• RMS WFE Range is directly proportional to the ACS’s controllability and period.
• RMS WFE Range is inversely proportional to the mirror’s heat capacity and has a weak, negative linear relationship with conductivity and emissivity.
• For the material properties used, Zerodur causes the easiest to meet requirements on an active control system, followed closely by ULE, and distantly by Silicon Carbide
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1-D Rod Closed-Form Model
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Rod with a mass, specific heat, thermal energy, temperature and coefficient of thermal expansion of m, cp, Q, T, and CTE respectfully
Length of rod, L
𝑑𝑄
𝑑𝑡= ρ𝑉𝑐𝑝
𝑑𝑇
𝑑𝑡Equation 1
CTE)𝐿𝛥𝑇 = 𝛥𝐿 Equation 2
𝑑𝑇
𝑑𝑡 CTE)𝐿 =
𝑑𝐿
𝑑𝑡Equation 3
𝑑𝐿
𝑑𝑡=
CTE)𝐿
𝜌𝑉𝑐𝑝
𝑑𝑄
𝑑𝑡Equation 4
• Equation 1 describes heat transfer in and out of the rod
• Equation 2 describes linear thermal expansion
• Algebra and calculus then Equation 5
• Equation 4 shows variables that affect thermal strain rate
– Geometry dependent: L, V, dQ/dt (surface area)
– Material dependent: CTE, ρ, cp, and dQ/dt(emissivity and absorptivity)
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Summary
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• Numerical and analytical models agree that heat capacity and CTE have very strong affects on thermal deformation rates.
• For an actively controlled substrate, the following figures of merit are proposed:
Massive Active Optothermal Stability,MAOS =𝜌𝑐𝑝𝐶𝑇𝐸
Active Optothermal Stability, AOS =𝑐𝑝
𝐶𝑇𝐸
𝑑𝐿
𝑑𝑡=
CTE)𝐿
𝜌𝑉𝑐𝑝
𝑑𝑄
𝑑𝑡
0.5, 36.3
1.0, 17.3
2.0, 8.04.0, 3.5
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10
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20
25
30
35
40
0 0.5 1 1.5 2 2.5 3 3.5 4 4.5
RM
S W
FE R
ange
(pm
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Normalized Rib Thickness (Simulated Rib Thickness/Design Rib Thickness)
y = 18.063/x - 0.31553x
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Summary Continued
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A data table of potential substrate materials is provided*
MaterialMassive Active Optothermal
Stability (TJ/m3)
Active Optothermal
Stability (GJ/kg)
Specific heat
(J/kg/K)
Density
(kg/m3)
Coefficient of thermal
expansion (1/K)
Fused silica 2.91 1.32 741 2202 5.60E-07
ULE 7971 112 51.1 766 2200 1.50E-08
Zerodur 83.1 32.8 821 2530 2.50E-08
Cer-Vit C-101 140 56.0 840 2500 1.50E-08
Beryllium I-70A 0.298 0.161 1820 1850 1.13E-05
Aluminum 6061-T6 0.113 0.042 960 2710 2.30E-05
Silicon Carbide CVD 0.936 0.292 700 3210 2.40E-06
Borosilicate crown E6 0.595 0.255 830 2330 3.25E-06
* Data in this table is compiled from Yoder, P.R., Opto-Mechanical Systems Design, 2nd ed., Marcel Dekker, New York, NY (1993).
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Any Questions?Contact Information
Email: [email protected]
Phone Number: (256) 544-5596
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mailto:[email protected]
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Methodology
Thermal Analysis done in Thermal
Desktop
Write NASTRAN input file
Run Thermal Deformation Analysis in
NASTRAN
Post Processes Data for Optical
Analysis
• Tasks boxed in red are handled entirely with a program written in Python.• Program saves weeks of work per analysis.• Program has been used to determine relationships between the telescope’s characteristics and
technical performance parameters like stability.
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0 10000 20000 30000 40000 50000
RM
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nm
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Time (s)
Wavefront Error
279.925
279.950
279.975
280.000
280.025
280.050
280.075
0 10000 20000 30000 40000 50000
Shro
ud
Te
mp
era
ure
(K
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Time(s)
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