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Vibrations And their effect on electro-optical imaging spacecraft Steve Hearon Applied Math Seminar December 14, 2009 (to fullfill requirements of an optomechanics course)

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Page 1: Vibrations And their effect on electro-optical imaging spacecraft Steve Hearon Applied Math Seminar December 14, 2009 (to fullfill requirements of an optomechanics

VibrationsAnd their effect on electro-optical imaging spacecraft

Steve HearonApplied Math Seminar

December 14, 2009(to fullfill requirements of an optomechanics course)

Page 2: Vibrations And their effect on electro-optical imaging spacecraft Steve Hearon Applied Math Seminar December 14, 2009 (to fullfill requirements of an optomechanics

Outline

• Material Properties, Stress/Strain and Bending• Vibration Transfer Basics (from J. Burge, Univeristy of Arizona)• Electro-optical Spacecraft Examples• Types of Disturbances that cause vibration in optical path• FEA Models• Effects of Vibration on Imaging

– Boresight – Primary Mirror Distortion

• Conclusions

Page 3: Vibrations And their effect on electro-optical imaging spacecraft Steve Hearon Applied Math Seminar December 14, 2009 (to fullfill requirements of an optomechanics

Material Properties

• Materials will deform when subjected to a load• Stress-strain relationship is

– where ε is strain (normalized change in length); σ is stress (force/area); and E is Young’s modulus

– E = 70 x 10^9 N/m^2 for Aluminum

• For an aluminum bar, 1cm x 1cm x 10 cm, 1 Newton force, change of length is :

– Stiffness k = F/ΔL = 70,000 N/mm

E

nmmPaemNL 14)10970/()1.01( 24

Page 4: Vibrations And their effect on electro-optical imaging spacecraft Steve Hearon Applied Math Seminar December 14, 2009 (to fullfill requirements of an optomechanics

Bending example: Bar with force applied at end

F

Max deflection occurs at end. Max deflection for the Aluminum barAs before 1N force, 1cm x 1 cm x 10 cm:

mmPae

mN

EW

FL 1.2)01.0)(970(2

)1.0)(1(3

2

34

3

4

3

StiffnessmmN

L

EWk /467

3

23

4

Page 5: Vibrations And their effect on electro-optical imaging spacecraft Steve Hearon Applied Math Seminar December 14, 2009 (to fullfill requirements of an optomechanics

Natural Frequency of Vibration

• Natural Frequency of Vibration of a mode is

– where k is stiffness and m is mass of the moving structure

• For previous examples, assuming a 1-pound mass at the end of the aluminum bar:

• Bending direction is much more compliant than axial tension

m

kfN 2

1

Hzkg

mNef AXIAL 1880

5.0

/77

2

1

Hz

kg

mNefBENDING 154

5.0

/57.4

2

1

Page 6: Vibrations And their effect on electro-optical imaging spacecraft Steve Hearon Applied Math Seminar December 14, 2009 (to fullfill requirements of an optomechanics

Analysis of Vibrations (J. Burge, University of Arizona)

• Each degree of freedom can be represented as a simple mode that has mass, stiffness, and damping

• This can be modeled using a simple 2nd-order differential equation

• (Charts from J. Burge, University of Arizona)

Natural Frequency of Vibration

Disturbance

Page 7: Vibrations And their effect on electro-optical imaging spacecraft Steve Hearon Applied Math Seminar December 14, 2009 (to fullfill requirements of an optomechanics

Analysis of Vibrations (J. Burge, University of Arizona)

• Critical Damping Ratio is

)2/( NR mCC Critical Damping Ratio:

Page 8: Vibrations And their effect on electro-optical imaging spacecraft Steve Hearon Applied Math Seminar December 14, 2009 (to fullfill requirements of an optomechanics

(From J. Burge, University of Arizona)

Page 9: Vibrations And their effect on electro-optical imaging spacecraft Steve Hearon Applied Math Seminar December 14, 2009 (to fullfill requirements of an optomechanics

(From J. Burge, University of Arizona)

Page 10: Vibrations And their effect on electro-optical imaging spacecraft Steve Hearon Applied Math Seminar December 14, 2009 (to fullfill requirements of an optomechanics

Electro-optical Spacecraft Example - Hubble

•2.4m Primary Mirror

•Richey-Chretien (2-mirror)•SA and Coma corrected

•Staring Arrays

•24 arcminutes Full FOV for widest sensor

•Reaction Wheels for attitude control•Gyroscopes for stabilization

Page 11: Vibrations And their effect on electro-optical imaging spacecraft Steve Hearon Applied Math Seminar December 14, 2009 (to fullfill requirements of an optomechanics

Electro-optical Spacecraft Example -- IKONOS

•0.7m primary mirror•10m focal length

•Three-Mirror Anastigmat (TMA)•Controls SA, Coma, Astig, FC

•Attitude controlled by Reaction Wheels

•Pushbroom detector technology•6500 lines/sec, 12 um pixels PAN•48 um pixels MSI

•Fully steerable, swath 12 km•Resolution 0.8m PAN

Page 12: Vibrations And their effect on electro-optical imaging spacecraft Steve Hearon Applied Math Seminar December 14, 2009 (to fullfill requirements of an optomechanics

Types of Disturbances That Can Affect Optical Path (1)

• Reaction Wheel– Electric motor attached to a flywheel– Upon spinup, causes spacecraft to turn other way– Work around a nominal zero rotation rate– IKONOS and Hubble

• Control Moment Gyroscope (CMG)– Gyroscope that is always spinning during operation ~ 6000 rpm– Spacecraft attitude controlled by turning axes of CMG’s– S/C rotates in reaction to CMG rotation (ang. mom. conserved)– More energy efficient than Reaction Wheels– Used in WorldView Satellite, International Space Station

• Thrusters– Used for orbit adjusts

Page 13: Vibrations And their effect on electro-optical imaging spacecraft Steve Hearon Applied Math Seminar December 14, 2009 (to fullfill requirements of an optomechanics

Types of Disturbances That Can Affect Optical Path (2)

• Slewing to acquire a target– s/c decelerates after slewing to begin imaging– Vibration damps out before imaging can begin

• Motors– Solar array– Communications antenna– Cryocoolers

• Sudden temperature change; thermal snap– Spacecraft enters or exits umbra

Page 14: Vibrations And their effect on electro-optical imaging spacecraft Steve Hearon Applied Math Seminar December 14, 2009 (to fullfill requirements of an optomechanics

Finite Element Analysis•Describes material in terms of small elements connected by nodes• Each element models the compliance of the material

(J. Burge, University of Arizona)

Page 15: Vibrations And their effect on electro-optical imaging spacecraft Steve Hearon Applied Math Seminar December 14, 2009 (to fullfill requirements of an optomechanics

Using FEA Tools in Vibration Analysis (1)

• FEA Tools allow the natural frequencies of a complex structure to be obtained

• Additionally, the shape of the natural mode is obtained,• For a complete dynamical description, the damping ratio is

also needed– Damping ratio is difficult to model for space structures– Often a low value is assumed e.g. 0.005– It is possible to perform a factory test (“modal test”) to obtain this– However, difficult to transform measurements at std pressure and 1 g

to vacuum and no gravity

Page 16: Vibrations And their effect on electro-optical imaging spacecraft Steve Hearon Applied Math Seminar December 14, 2009 (to fullfill requirements of an optomechanics

Using FEA Tools in Vibration Analysis (2)

• With natural frequencies, mode shapes, damping, and the input disturbance, the time-varying motion of the structure can be obtained

• Effect on imaging obtained by importing structure into ASAP or another optical modeling tool

• Optionally, can perform an analysis based on analytical calculations

Page 17: Vibrations And their effect on electro-optical imaging spacecraft Steve Hearon Applied Math Seminar December 14, 2009 (to fullfill requirements of an optomechanics

FEA Results from a Study for an 8-Meter space telescope

• Shown on next slide is a table of natural modes from following report:– “HST Optics Enhancement, preliminary feasibility

study summary report”, 2000

• Note that mode shapes and frequencies have been calculated, and damping ratios have all been set to 0.005

Page 18: Vibrations And their effect on electro-optical imaging spacecraft Steve Hearon Applied Math Seminar December 14, 2009 (to fullfill requirements of an optomechanics

FEA Results from a Study for an 8-Meter space telescope

Page 19: Vibrations And their effect on electro-optical imaging spacecraft Steve Hearon Applied Math Seminar December 14, 2009 (to fullfill requirements of an optomechanics

Trussed Mirror Concept

• Following two slides show NASTRAN results for first natural frequency for a trussed-mirror concept

Page 20: Vibrations And their effect on electro-optical imaging spacecraft Steve Hearon Applied Math Seminar December 14, 2009 (to fullfill requirements of an optomechanics

Lockheed Martin

Strutted Mirror - 1st Natural Mode at 73.7 Hz

Page 21: Vibrations And their effect on electro-optical imaging spacecraft Steve Hearon Applied Math Seminar December 14, 2009 (to fullfill requirements of an optomechanics

Baseline Petal - 1st Natural Mode at 63.2 Hz

Lockheed Martin

Page 22: Vibrations And their effect on electro-optical imaging spacecraft Steve Hearon Applied Math Seminar December 14, 2009 (to fullfill requirements of an optomechanics

Effects of Vibration on Optical Path –Boresight Variation -- Jitter

• Vibrational Modes that affect telescope as a whole cause jitter• Jitter is often spec’d as a PSD in units of microrad^2/Hz

– On a per-axis basis

• Frequencies greater than line rate cause image blur• Frequencies less than line rate cause frame-to-frame jitter

(Line-to-line jitter)

Lockheed Martin

Frequency (Hz)

PSD (urad^2/Hz)

Jitter realization With programmedMotion added(pushbroom)

Page 23: Vibrations And their effect on electro-optical imaging spacecraft Steve Hearon Applied Math Seminar December 14, 2009 (to fullfill requirements of an optomechanics

Effects of Vibration on Optical Path –Primary Mirror distortions

• Distortions of the Mirrors (e.g. primary or secondary mirror) cause spreading of point-spread-function– Results in a decrease of Strehl Ratio

• Movie showing time-dependent PM distortions, and resulting variation in Point-Spread Function:

– X:\7\7CNO\Hearon\PSFvsTime_2kHz_04.avi

Lockheed Martin

Page 24: Vibrations And their effect on electro-optical imaging spacecraft Steve Hearon Applied Math Seminar December 14, 2009 (to fullfill requirements of an optomechanics

Conclusions

• Vibrations are an important consideration for EO spacecraft, across their entire lifecycle– Development, build, operation

• Vibration analysis tools help designers to understand and mitigate potential vibration issues early in the design process

Lockheed Martin