Solar Sail

63
Solar Sail Department of Aerospace Engineering and Mechanics AEM 4332W – Spacecraft Design Spring 2007

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Solar Sail. Department of Aerospace Engineering and Mechanics AEM 4332W – Spacecraft Design Spring 2007. Team Members. Solar Sailing:. Project Overview. Design Strategy. Trade Study Results. Orbit. Eric Blake Daniel Kaseforth Lucas Veverka. Eric Blake. - PowerPoint PPT Presentation

Transcript of Solar Sail

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Solar Sail

Department of Aerospace Engineering and Mechanics

AEM 4332W – Spacecraft Design

Spring 2007

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Team Members

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Solar Sailing:

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Project Overview

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Design Strategy

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Trade Study Results

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Orbit

Eric Blake

Daniel Kaseforth

Lucas Veverka

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Eric Blake

Optimal Trajectory of a Solar Sail: Derivation of Feedback Control Laws

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Recall Orbital Mechanics

• The state of a spacecraft can be described by a vector of 6 orbital elements.– Semi-major axis, a– Eccentricity, e– Inclination, i– Right ascension of the ascending node, Ω– Argument of perihelion, ω– True anomaly, f

• Equivalent to 6 Cartesian position and velocity components.

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Orbital Elements

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Equations of Motion

vr

nnrr

rr

v2^

2

^

2

^^^^

sinsincossincos rpprn

^

r

^

p

^^

rp

n

linesun

sail

= Sail Lightness Number = Gravitational Parameter

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Problem: Minimize Transfer Time

1),,(2^

2

^

2

nnr

rr

rvuxH vvr

^

r

^

p

^^

rp

n

linesun

sail

^^^

353)(2))((2)(3 rnrnnnr

rrr

rr vrvr rv

^^

}max{ vv nn

By Inspection:

Transversality:

fttv

ttv npnr

rnpnr

r

2

^

22

^

2)()(

0

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Solution

• Iterative methods are needed to calculate co-state boundary conditions.

• Initial guess of the co-states must be close to the true value, otherwise the solution will not converge.

• Difficult• Alternative: Parameter Optimization.

– For given state boundary conditions, maximize each element of the orbital state by an appropriate feedback law.

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Orbital Equations of Motion

r

pTfSe

e

pr

df

dasin

)1(

222

2

e

p

rTf

p

rTfS

r

df

decos1sin

2

Wfp

r

df

di)cos(

3

Wfip

r

df

d)sin(

sin

3

f

p

rTfS

e

ri

df

d

df

dsin1coscos

2

12

2sin1cos1

f

p

rTfS

e

r

r

p

dt

df

)1( 2eap fe

pr

cos1

32

cosr

S sinsincos22r

T cossincos22r

W

),,( xgx

= Sail Lightness Number = Gravitational Parameter

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Maximizing solar force in an arbitrary direction

^^^^

sinsincossincos rpprn ^^~~^~~^~

sinsincossincos rpprq

^

r

^

p

^^

rp

n

linesun

sail

Maximize:

qnnr

raq

2^

2

~

~

~2

tan4

tan893tan

Sail pointing for maximum acceleration in the q direction:

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Locally Optimal Trajectories• Example: Use parameter optimization method to derive

feedback controller for semi-major axis reduction.

• Equations of motion for a:

r

pTfSe

e

pr

df

dasin

)1(

222

2

3

2cos

rS

sinsincos22r

T

fe

fe

cos1

sintan

~

fe

pr

cos1 )1( 2eap

2

~

~2

tan4

tan893tan

Feedback Law:

Use this procedure for all orbital elements

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Method of patched local steering laws (LSL’s)

• Initial Conditions: Earth Orbit

• Final Conditions: semi-major axis: 0.48 AU inclination of 60 degrees

0

0

0

0

0

1

0tt

i

e

a

free

free

free

AU

i

e

a

tft

60

0~

48.0

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Trajectory of SPI using LSL’s

Time (years)

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Global Optimal Solution– Although the method of patched LSL’s is not ideal, it is a solution that is

close to the optimal solution.

– Example: SPI Comparison of LSL’s and Optimal control.

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Conclusion

• Continuous thrust problems are common in spacecraft trajectory planning.

• True global optimal solutions are difficult to calculate.

• Local steering laws can be used effectively to provide a transfer time near that of the global solution.

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Lucas Veverka

•Temperature

•Orbit Implementation

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Daniel Kaseforth

Control Law Inputs and Navigation System

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Structure

Jon T Braam

Kory Jenkins

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Jon T. BraamStructures Group:

• Primary Structural Materials

• Design Layout

•3-D Model

• Graphics

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Primary Structural Material

Weight and Volume Constraints• Delta II : 7400 Series • Launch into GEO

– 3.0 m Ferring» Maximum payload mass: 1073 kg» Maximum payload volume: 22.65 m3

– 2.9 m Ferring» Maximum payload mass: 1110 kg» Maximum payload volume: 16.14 m3

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Primary Structural Material

Aluminum Alloy Unistrut– 7075 T6 Aluminum

Alloy• Density

– 2700 kg/m3

– 168.55 lb/ft^3

• Melting Point– ? Kelvin

Picture of Unistrut

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Primary Structural Material

• Density

• Mechanical Properties– Allowing unistrut design

• Decreased volume

• Thermal Properties– Capible of taking thermal loads

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Design Layout

• Constraints– Volume– Service task– Thermal consideration– Magnetic consideration– Vibration– G loading

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Design Layout

• Unistrut Design– Allowing all inside surfaces to be bonded to

• Titanium hardware

– Organization• Allowing all the pointing requirements to be met with

minimal attitude adjustment

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Design Layout

• Large Picture of expanded module

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3-D Model

• Large picture

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3-D Model

• Blah blah blah (make something up)

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Graphics

• Kick ass picture

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Graphics

• Kick ass picture

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• The blanks will be filled in soon

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Trade Studies

• Blah blah blah

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Why I deserve an “A”

• Not really any reason but when has that stopped anyone!

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Kory Jenkins• Sail Support Structure• Anticipated Loading•Stress Analysis• Materials•Sail Deployment

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Attitude Determination and Control

Brian Miller

Alex Ordway

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Alex Ordway

•Sliding Mass vs. Tip Thrusters

•Component Selection

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Brian Miller

•Tip Thrusters vs. Slidnig Mass

•Attitude Control Simulation

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Attitude Control

• Conducted trade between tip thrusters and sliding mass as primary ACS

• Considerations– Power required– Torque produced– Weight– Misc. Factors

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Attitude Control

• Tip Thrusters (spt-50)– Pros

• High Torque Produced ~ 1.83 N-m• Low weight ~ 0.8 kg/thruster

– Cons• Large Power Requirement ~ 310 Watts• Lifetime of 2000 hrs• Requires a fuel, either a solid or gas

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Attitude Control

• Attitude Control System Characteristics– Rotational Rate– Transfer Time– Required Torque– Accuracy– Disturbance compensation

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Attitude Control

• Requirements– Orbit

• Make rotation rate as fast as possible

• Roll spacecraft as inclination changes

– Communications– Within Maximum Torque

• Pitch and Yaw Axis

~ 0.34 N-m

• Roll Axis

~ 0.2 N-m

M

mFzU

m – sliding massF – solar forcez – distance from cgM – spacecraft mass

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Attitude Control

• Pitch and Yaw Axis • Rotation Rate = 0.144 rad/hr

~ 8.25 deg.

• Transfer Time = 5300s ~ 1.47 hrs

• Required Torque = 0.32 N-m

~ 98.8% of maximum produced

• Converges to desired angle

Slope = 0.00004 rad/s

Torque Req.

Transfer Time

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Attitude Control

• Roll Axis • Rotation Rate = 0.072 rad/hr

~ 4.12 deg

• Transfer Time = 7000s ~ 1.94 hrs

• Required Torque = 0.15 N-m

~ 75% of maximum produced

• Converges to desired angle

Torque Req.

Slope = 0.00002 rad/s

Transfer Time

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Power, Thermal and Communications

Raymond Haremza

Michael HitiCasey Shockman

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Raymond HaremzaThermal Analysis

•Solar Intensity and Thermal Environment•Film material•Thermal Properties of Spacecraft Parts•Analysis of Payload Module•Future Work

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Casey ShockmanCommunications

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Michael HitiPower

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Demonstration of Success

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Future Work

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Acknowledgements

• Stephanie Thomas

• Professor Joseph Mueller

• Professor Jeff Hammer

• Dr. Williams Garrard

• Kit Ru….

• ?? Who else??