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Vol.:(0123456789)
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https://doi.org/10.1007/s12217-021-09894-4
ORIGINAL ARTICLE
Axisymmetric Ferrofluid Oscillations inaCylindrical Tank
inMicrogravity
ÁlvaroRomero‑Calvo1 · MiguelÁngelHerrada2· TimH.J.Hermans3· LidiaParrillaBenítez2·
GabrielCano‑Gómez4· ElenaCastro‑Hernández2
Received: 6 October 2020 / Accepted: 30 May 2021
© The Author(s), under exclusive licence to Springer Nature B.V. 2021
Abstract
The sloshing of liquids in low-gravity entails several technical challenges for spacecraft designers due to its effects on the
dynamics and operation of space vehicles. Magnetic settling forces may be employed to position a susceptible liquid and
address these issues. Although proposed in the early 1960s, this approach remains largely unexplored. In this paper, the
equilibrium meniscus and axisymmetric oscillations of a ferrofluid solution in a cylindrical tank are studied for the first time
while subject to a static inhomogeneous magnetic field in microgravity. Coupled fluid-magnetic simulations from a recently
developed inviscid magnetic sloshing model are compared with measurements collected at ZARM’s drop tower during the
ESA Drop Your Thesis! 2017 campaign. The importance of the fluid-magnetic interaction is explored by means of an alterna-
tive uncoupled framework for diluted magnetic solutions. The coupled model shows a better agreement with experimental
results in the determination of the magnetic deformation trend of the meniscus, but the uncoupled framework gives a better
prediction of the magnetic frequency response which finds no theoretical justification. Although larger datasets are required
to perform a robust point-by-point validation, these results hint at the existence of unmodeled physical effects in the system.
Keywords Liquid sloshing· Microgravity· Ferrofluids· Space propulsion· Magnetic Positive Positioning
Nomenclature
𝛼
Laser inclination
𝐀
Magnetic vector potential
𝐀d
Dipole term of the magnetic vector potential
a Container radius
𝛽
Tilting angle of the visual line with respect to
the axis of the camera
𝐁
Magnetic flux density
Bo Bond number
Bomag
Magnetic Bond number
𝜒
Magnetic susceptibility
C Dynamic contour
C′
Meniscus contour
Δ𝜔−3dB
Peak width at -3 dB in frequency spectrum
dp
In-plane laser displacement
dV
Vertical laser displacement
𝜂
Geometric variable for magnetic vector
potential
E(x) Elliptic integral of second kind
F Dimensionless f
f Relative height between meniscus and vertex
f′
Relative height between meniscus contour
and vertex
FOV Field Of View of the camera
Γ
Dimensionless
𝛾
𝛾
Surface hysteresis parameter
G Wall boundary condition function
g Inertial acceleration
g0
Gravity acceleration at ground level
H
Dimensionless h
𝐇
Magnetic field
𝐇0
Applied magnetic field
h Relative height between meniscus and
dynamic liquid surface
* Álvaro Romero-Calvo
alvaro.romerocalvo@colorado.edu
1 Department ofAerospace Engineering Sciences, University
ofColorado Boulder, CO, USA
2 Área de Mecánica de Fluidos, Dep. Ingeniería Aeroespacial y
Mecánica de Fluidos, Universidad de Sevilla, Avenida de los
Descubrimientos s/n, Sevilla41092, Spain
3 Astrodynamics andSpace Missions, Delft University
ofTechnology, Delft, TheNetherlands
4 Departamento de Física Aplicada III, Universidad de Sevilla,
Avenida de los Descubrimientos s/n, Sevilla41092, Spain
/ Published online: 23 July 2021
Microgravity Science and Technology (2021) 33: 50
Content courtesy of Springer Nature, terms of use apply. Rights reserved.