o-26: assembling and test of a halbach array magnet system ... · michael faraday georg simon ohm...

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Authors: O-26: Assembling and Test of a Halbach Array Magnet System for Lorentz Force Velocimetry in Electrolytes M. Werner* and B. Halbedel LFV: Background Optimization procedure Optimization results Result and Outlook Part B3 ( Electrolytes“) of the Research Training Group „Lorentz Force Velocimetry and Eddy Current Testing“ ( funded by the DFG GRK-1567) Dipl.-Ing. Michael Werner Department of Inorganic-Nonmetallic Materials Mail: [email protected] Phone: +49 3677 69 3347 Dr.-Ing. Bernd Halbedel Mail: [email protected] Phone: +49 3677 69 2784 Department of Inorganic-Nonmetallic Materials LFV: Novel „contactless“ measurement method in electrolytes to provide an in-line observation system for glass melts Vision : Improvement of the process efficiency in electrolytic processes (e.g. glass casting, salt melt cooling) by measuring the flow velocities in closed channels Research: - Experiments on salt water under laboratory conditions with high velocities (~ 5 m/s) - Later adaption and optimization to a robust system for the harsh boundary conditions of real glass melts at lower velocities Magnet Fluid Flow Channel Primary magnetic field Eddy currents Accelerating force Fluid breaking force Michael Faraday Isaac Newton Heinrich Friedrich Emil Lenz Georg Simon Ohm Hendrik Antoon Lorentz Challenge: Tiny forces (some μN) on magnet systems with masses around 1 kg must be detected with highest possible resolution Task: - Finding the most effective magnet system design - Optimization of the specific geometries of this magnet system for - Assembling and characterization of the optimized design highest forces within the limited mass, to increase load step amount on force measurement system - High Reynolds number (salt water at 5 m/s) - Low magnetic Reynolds number - Low Hartmann number and interaction parameter - Well defined test channel with plug profile at the inlet FEM simulation of moving solid bodies, having the same geometry like the channel cross section is possible in a first approximation Optimization can be performed in very short time by combination of COMSOL FEM and MATLAB Optimization Toolbox Reference design / experimental setup: - Inner cross section: a * b = 50 mm * 50 mm - Length: l = 1500 mm - Conductivity of the fluid: = 4 S/m - Flow velocity: v = 5 m/s - Minimum gap between poles: > 56 mm - Geometries of magnet system (here standard system): l, d, h optimization parameters - Magnet system mass limit: m < 1 kg B σ δ FEM Standard system (two single magnets with same magnetization direction): m = 950 g leads to with l = 38.4 mm, h = 51.9 mm, d = 31.8 mm F = 35 μN max opt opt opt Halbach array combination (without/with triangular shaped endmagnets) m = 950 g, ) F = 115 μN max Lorentz force can be increased by a factor of three, using Mallinsons method of one sided fluxes in the same way Halbach did in his arrays (1980). (1973) Next step: - Further experimental tests on the channel to prove all simulations, see also Poster P3-19 - Design of magnet systems based on high temperature superconductors 30 40 50 60 70 80 20 30 40 50 60 70 80 10 20 30 40 length l [mm] height h [mm] Force [μN] 14 16 18 20 22 24 26 28 30 32 34 (Nelder-Mead simplex algorithm in MATLAB) Principle and Response surface for 950 g magnet material (NdFeB of grade ) N52 -20 0 20 -60 -40 -20 0 20 40 -150 -100 -50 0 50 100 150 Length l [mm] / x-direction Height h [mm] / z-direction Magnetic field magnitude in y [mT] -100 -50 0 50 100 150 Halbach array system out of 5 single magnets on each side, assembled with a carbon fiber composite bracket. (950 g magnets and 50 g CFC) Magnetic field was measured and fits perfect to the numerical predictions. Numerical investigation of the influence of the fluid profiles on the arising forces by FLUENT simulation of the experimental test channel: Force decreases with fluid profile change within the channel.

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Authors:

O-26: Assembling and Test of a Halbach Array MagnetSystem for Lorentz Force Velocimetry in Electrolytes

M. Werner* and B. Halbedel

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Part B3 ( Electrolytes“) of the Research Training Group „Lorentz Force Velocimetry and Eddy Current Testing“ ( funded by the DFG„ GRK-1567)

Dipl.-Ing. Michael WernerDepartment of Inorganic-Nonmetallic MaterialsMail: [email protected]: +49 3677 69 3347

Dr.-Ing. Bernd Halbedel

Mail: [email protected]: +49 3677 69 2784

Department of Inorganic-Nonmetallic Materials

LFV: Novel „contactless“ measurement method in electrolytes to providean in-line observation system for glass melts

Vision : Improvement of the process efficiency in electrolytic processes (e.g.glass casting, salt melt cooling) by measuring the flow velocities inclosed channels

Research: - Experiments on salt water under laboratory conditions with highvelocities (~ 5 m/s)

- Later adaption and optimization to a robust system for the harshboundary conditions of real glass melts at lower velocities

Magnet

Fluid Flow

ChannelPrimary magneticfield Eddy currents

Acceleratingforce

Fluid breakingforce

Michael Faraday Isaac NewtonHeinrich Friedrich Emil LenzGeorg Simon Ohm Hendrik Antoon Lorentz

Challenge: Tiny forces (some µN) on magnet systems with masses around1 kg must be detected with highest possible resolution

Task: - Finding the most effective magnet system design- Optimization of the specific geometries of this magnet system

for

- Assembling and characterization of the optimized design

highest forces within the limited mass, to increase loadstep amount on force measurement system

- High Reynolds number (salt water at 5 m/s)- Low magnetic Reynolds number- Low Hartmann number and interactionparameter

- Well defined test channel with plug profileat the inlet

FEM simulation of moving solid bodies,having the same geometry like the channelcross section is possible in a firstapproximation

Optimization can be performed in very shorttime by combination of COMSOL FEM andMATLAB Optimization Toolbox

Reference design / experimental setup:

- Inner cross section: a * b = 50 mm * 50 mm- Length: l = 1500 mm

- Conductivity of the fluid: = 4 S/m- Flow velocity: v = 5 m/s- Minimum gap between poles: > 56 mm- Geometries of magnet system (here standard

system): l, d, h optimization parameters- Magnet system mass limit: m < 1 kg

B

σ

δ

FEM

Standard system(two single magnets with samemagnetization direction):m = 950 g leads to with

l = 38.4 mm, h = 51.9 mm,

d = 31.8 mm

F = 35 µNmax

opt opt

opt

Halbach array combination(without/with triangular shaped endmagnets) m = 950 g, )F = 115 µNmax

Lorentz force can be increased by a factor of three, using Mallinsons method of one sidedfluxes in the same way Halbach did in his arrays (1980).(1973)

Next step:- Further experimental

tests on the channelto prove allsimulations, see alsoPoster P3-19

- Design of magnetsystems based onhigh temperaturesuperconductors

30

40

50

60

70

80 20

30

40

50

60

70

8010

20

30

40

length l [mm]

height h [mm]

Fo

rce

N]

14

16

18

20

22

24

26

28

30

32

34

(Nelder-Mead simplex algorithm in MATLAB)

Principle and Response surface for 950 gmagnet material (NdFeB of grade )N52

-20

0

20-60

-40-20

020

40

-150

-100

-50

0

50

100

150

Length l [mm] / x-direction

Height h [mm] / z-direction

Ma

gn

etic f

ield

ma

gn

itu

de

in

y [

mT

]

-100

-50

0

50

100

150

Halbach array system out of 5 single magnets on each side,assembled with a carbon fiber composite bracket. (950 g magnetsand 50 g CFC)Magnetic field was measured and fits perfect to the numericalpredictions.

Numerical investigation of the influence of the fluid profiles on the arisingforces by FLUENT simulation of the experimental test channel:Force decreases with fluid profile change within the channel.