Magnetic Sloshing Damping in Microgravity...Magnetic Sloshing Damping in Microgravity Álvaro...
Transcript of Magnetic Sloshing Damping in Microgravity...Magnetic Sloshing Damping in Microgravity Álvaro...
Magnetic Sloshing Damping in Microgravity
Álvaro Romero-Calvo
Gabriel Cano Gómez
Elena Castro-Hernández
Miguel Ángel Herrada Gutiérrez
Filippo Maggi
An alternative for small satellites
Index
1. Liquid sloshing
2. Magnetic liquid sloshing in microgravity
3. Qualitative and quantitative effects
4. Case of application
5. Conclusions & next steps
6. UNOOSA DropTES - StELIUM
8th iCubeSat Workshop 2019 2Image Credit: Isabel Romero Calvo
1. Liquid sloshing - g
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Physical Properties
Tank Geometry
Inviscid ModelMechnical Analogy
Implementation
Adapted from “Nonlinear dynamics and control of space vehicleswith multiple fuel slosh modes”, M. Reyhanoglu, J. Rubio Hervas
1. Liquid sloshing - g
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Physical Properties
Tank Geometry
Inviscid ModelMechnical Analogy
Implementation
1st modedominates
Excellent agreement
z
r
Experiment(𝒓𝒂𝒅/𝒔)
Model(𝒓𝒂𝒅/𝒔)
𝒘𝟏 18.65 18.46
𝒘2 35.37 33.14
𝒘𝟑 44.37 42.15
Analytical high-g sloshing models are reliable and widely used
Handpicking
1. Liquid sloshing - 𝝁𝒈
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Physical Properties
Tank Geometry
Inviscid ModelMechnical Analogy
Implementation
Surface Tension (𝜎)
Surface Tension (𝜎)
𝜎𝜎
“Experimental and Theoreticla Studies of Liquid Sloshing atSimulated Low Gravity”, F.T. Dodge, L.R. Garza
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So then, problem solved!
Telemetereing and Data Relay Satellite(TDRS) tanks with bladders. Extractedfrom “The New Dynamic Behavior ofLiquids in Moving Containers”, F.T. Dodge.
CFD simulation of liquid motion after a settlingacceleration of 3.27 X 10-6𝑔0. Extracted from “TheNew Dynamic Behavior of Liquids in MovingContainers”, F.T. Dodge.
Large amplitude sloshing analogy.Extracted from “The New DynamicBehavior of Liquids in MovingContainers”, F.T. Dodge.
Highly sensitive dynamics in 𝜇𝑔. CFD models are required
2. Magnetic liquid sloshing in microgravity
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Physical Properties
Tank Geometry
Inviscid ModelMechnical Analogy
Implementation
Surface Tension
Surface Tension
Magnetic Force
Coupled magnetofluidodynamic problem
Can be decoupled for small oscillations
Volume force density
being• 𝑴: Magnetization• 𝑀𝑛 : Normal surface component of M• 𝑯: Magnetic field
𝒇𝑲 = 𝜇0𝑴∇𝑯
Surface force density
+ 𝒇𝒔 =1
2𝜇0𝑀𝑛
2
3. Qualitative and quantitative effects
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Qualitative• Restoring force “equivalent” to gravity• Inhomogeneous magnetic acceleration• Short range of action, suitable for CubeSats• Modified free-surface shape
Quantitative• Shift of oscillation frequencies• Increase of damping ratios
Magnetic liquid sloshing can be predicted and quantified
“Experimental and Theoreticla Studies of Liquid Sloshing atSimulated Low Gravity”, F.T. Dodge, L.R. Garza
4. Case of Application
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Detumbling of a 3U CubeSat
1U cylindrical propellant tank (50% filling ratio)
Passive magnetic damping system(neodymium magnet magnetized at 1800 kA/m)
Control Law𝑴 = −𝑀0 · 𝑠𝑖𝑔𝑛 𝒘 −𝒘𝒅
Parameters
𝐼 = 1.09, 5, 5.5 · 10−2 𝑘𝑔𝑚2
𝒘𝟎 = 0 , 0,0.6 𝑟𝑎𝑑/𝑠𝒘𝒅 = 0 , 0,0.01 𝑟𝑎𝑑/𝑠𝑀0 = 5mNm
CubeSat STF-1. Adapted from NASA, West Virginia Space Grant Consortium (WVSGC), West Virginia’s University (WVU)
X
Z
Y
4. Case of Application
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h
Width
Ferrofluid1:10 vol EMG-700
Magnet
Curved Interface
𝑩𝒐𝒎𝒂𝒈
Magnet of 60 g -> 100% increase in fundamental frequency
4. Case of Application
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Equivalent spring-mass system
𝑇𝑅 =𝑋
𝑌
The magnet increases the natural frequencies and reduces the transmissiblity in the 0-2 rad/s band
1 2 3 4 5Mode
4. Case of Application
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Magnetic analogyFree sloshing analogy
Pendulum𝐶𝑦𝑧 = 0.5 𝑠−1, 𝐶𝑥 = 0.1 𝑠−1
(damping in terms of ang. mom.)
𝑚 = 0.4 𝑘𝑔, 𝑙 = 0.025 𝑚
𝒎𝒏 (Kg) 𝒌𝒏 (N/m) 𝒍𝒏 (m)
0 0.0735 - 0.0375
1 0.1572 1.1995 0.0373
2 0.0032 0.3296 0.0411
3 0.0009 0.3230 0.0444
Spring-MassDamping Coeff: 𝛾 = 0.15
VS
4. Case of Application
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No
n-m
agn
etic
Mag
net
icAngular Velocity (rad/s)
First 20 s First 1.5 h
4. Case of Application
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No
n-m
agn
etic
Mag
net
icSloshing disturbance (Nm)
First 20 s First 1.5 h
4. Case of Application
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No
n-m
agn
etic
Mag
net
icMechanical Displacement (m)
First 20 s First 1.5 h
5. Conclusions & next steps
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1. Magnetic fields can be used to position a magnetic liquid in microgravity
2. A significant increase in the sloshing frequencies of ferrofluid-based propellants can be achieved with low-mass magnets
3. Magnetic liquid sloshing can be predicted and quantified
4. The benefits for pointing angle accuracy have to be explored
5. The interaction with the spacecraft and the space environmenthas to be analysed
6. UNOOSA DropTES - StELIUM
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INGENIERÍA AEROESPACIAL Y MECÁNICA DE FLUIDOS
(TEP-956)
Validation of the magnetic sloshing model
Magnetic Sloshing Damping in Microgravity
Álvaro Romero-Calvo
Gabriel Cano Gómez
Elena Castro-Hernández
Miguel Ángel Herrada Gutiérrez
Filippo Maggi
Thank you for your attention!