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

Transcript of Advanced Mirror Technology Development (AMTD) thermal ......• Larger aperture space telescopes are...

  • Advanced Mirror Technology Development (AMTD) thermal trade studies

    Thomas Brooks, Phil Stahl, Bill Arnold

    NASA/MSFC

  • • 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?

  • 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

  • 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

  • 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

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    Time(s)

  • 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)

  • 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

  • WFE Stability versus Controllability

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    -500

    -400

    -300

    -200

    -100

    0

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    RM

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    FE -

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    n R

    MS

    WFE

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    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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    ange

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    Shroud Controllability (mK)

  • 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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    RM

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    Shroud Oscillation Period (s)

  • 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

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    0 2 4 6 8 10

    RM

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    ange

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    Normalized Conductivity (Conductivity / ULE Conductivity)

  • 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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    Shroud Controllability (mK) @ Period of 140s

    1x Mass

    2x Mass

    3x Mass

  • 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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    Normalized Rib Thickness (Simulated Rib Thickness/Design Rib Thickness)

    y = 18.063/x - 0.31553xR2 = 0.9991

  • 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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    0 0.2 0.4 0.6 0.8 1

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    Emissivity of Mirror Surfaces Except the Optical Face

  • 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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  • 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

  • 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)

  • 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

    0

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    ange

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    Normalized Rib Thickness (Simulated Rib Thickness/Design Rib Thickness)

    y = 18.063/x - 0.31553x

  • 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).

  • Any Questions?Contact Information

    Email: [email protected]

    Phone Number: (256) 544-5596

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    mailto:[email protected]

  • 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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