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Journal articles on the topic 'Transverse magnetic'

Author: Grafiati

Published: 3 June 2025

Last updated: 31 July 2025

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1

Fadeyeva, T. A. "Singular beams with transverse electric and transverse magnetic fields." Semiconductor Physics Quantum Electronics and Optoelectronics 16, no. 1 (2013): 55–58. http://dx.doi.org/10.15407/spqeo16.01.055.

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2

Songquan Li, Songquan Li, Laixu Gao Laixu Gao, Shugang Liu Shugang Liu, Chunyu Liu Chunyu Liu, Yan Huang Yan Huang, and Hongan Ye Hongan Ye. "Design of transverse magnetic-reflected polarizing film." Chinese Optics Letters 12, no. 5 (2014): 053102–53104. http://dx.doi.org/10.3788/col201412.053102.

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3

Hicks, T. J. "Transverse magnetic ordering." Physica B: Condensed Matter 300, no. 1-4 (2001): 91–104. http://dx.doi.org/10.1016/s0921-4526(01)00574-9.

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4

Lu, J., and X. R. Wang. "Motion of transverse domain walls in thin magnetic nanostripes under transverse magnetic fields." Journal of Applied Physics 107, no. 8 (2010): 083915. http://dx.doi.org/10.1063/1.3386468.

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5

Eiling, A., and R. Pott. "Transverse magnetic field stability of magnetic pigments." IEEE Transactions on Magnetics 21, no. 5 (1985): 1497–99. http://dx.doi.org/10.1109/tmag.1985.1064094.

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6

Urinov, Khudoyor Omonovich, Adkham Kamolovich Amonov, Xakberdi Akhmedovich Jumanov, and Ismet Shevkitovich Mujdibaev. "LARGE VALUES OF THE TRANSVERSE M UES OF THE TRANSVERSE MAGNETIC RESISTANCEOF SINGLE CRYSTAL NICKEL FILMS." Scientific Reports of Bukhara State University 4, no. 5 (2020): 12–20. http://dx.doi.org/10.52297/2181-1466/2020/4/5/3.

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Background. The anisotropy of the transverse magnetoresistance of single-crystal nickel films was studied in this work. The measurements were carried out on samples whose surface plane coincided with the [001] plane. Studies of the magnetoresistance in a single-crystal nickel film have shown the effect of tensile stresses acting on it from the side of magnesium oxide. The modification of the anisotropy of magnetoreflection of a film on a substrate as compared to a free sample is apparently associated with a change in the shape of the Fermi surface of carriers.

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7

Solomin, Vladimir A., Andrei V. Solomin, Victor V. Koledov, and Nadezda A. Trubitsina. "Multifunctional linear induction motor with longitudinal-transverce magnetic flux for magnetic-levitational transport." Transportation Systems and Technology 4, no. 2 (2018): 167–79. http://dx.doi.org/10.17816/transsyst201842167-179.

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Background: Traction linear induction motors (LIM) at the current stage of human society development are the most promising for high-speed magnetic-levitation transport (MLT) and are already used in a number of commercial projects. Linear induction motors can be executed with longitudinal, transverse and longitudinal-transverse magnetic flux and have a large number of design options. Aim: In addition to traction efforts, LIM develops the forces of magnetic-levitation and lateral stabilization (self-stabilization). The efforts of magnetic-levitation of linear induction motors with longitu

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8

BRADAMANTE, FRANCO. "TRANSVERSE SPIN AND TRANSVERSE MOMENTUM EFFECTS AT COMPASS." Modern Physics Letters A 24, no. 35n37 (2009): 3015–24. http://dx.doi.org/10.1142/s0217732309001224.

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The study of transverse spin and transverse momentum effects is part of the scientific program of COMPASS, a fixed target experiment at the CERN SPS. For these studies, a 160 GeV/c momentum muon beam is scattered on a transversely polarized nucleon target, and the scattered muon and the forward going hadrons produced in DIS processes are reconstructed and identified in a magnetic spectrometer. The measurements have been performed on a deuteron target in 2002, 2003 and 2004, and on a proton target in 2007. The main results obtained measuring single spin asymmetries are reviewed, with particular

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9

Lee, Sung Uk, Hyo Joon Eom, Jang Soo Ock, and Jong Hwa Kwon. "Higher-Order Transverse Electric and Transverse Magnetic Modes in Gigahertz Transverse Electromagnetic Cells." Electromagnetics 31, no. 7 (2011): 483–93. http://dx.doi.org/10.1080/02726343.2011.607104.

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10

Potanin, Andrei A., Suresh M. Shrauti, David W. Arnold, and Alan M. Lane. "Transverse susceptibility of magnetic inks." Journal of Applied Physics 81, no. 8 (1997): 3803–5. http://dx.doi.org/10.1063/1.364775.

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11

Foster, John E. "Transverse magnetic field propellant isolator." Review of Scientific Instruments 71, no. 10 (2000): 3684. http://dx.doi.org/10.1063/1.1290509.

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12

Hicks, T. J. "ChemInform Abstract: Transverse Magnetic Ordering." ChemInform 33, no. 10 (2010): no. http://dx.doi.org/10.1002/chin.200210228.

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13

Warber, C. R., and E. C. Field. "A long wave transverse electric-transverse magnetic noise prediction model." Radio Science 30, no. 3 (1995): 783–97. http://dx.doi.org/10.1029/94rs03181.

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14

Lin, Yuan-Yao, Ray-Kuang Lee, and Yuri S. Kivshar. "Transverse instability of transverse-magnetic solitons and nonlinear surface plasmons." Optics Letters 34, no. 19 (2009): 2982. http://dx.doi.org/10.1364/ol.34.002982.

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15

McCutcheon, Murray W., Parag B. Deotare, Yinan Zhang, and Marko Lončar. "High-Q transverse-electric/transverse-magnetic photonic crystal nanobeam cavities." Applied Physics Letters 98, no. 11 (2011): 111117. http://dx.doi.org/10.1063/1.3568897.

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16

Boardman, A. D., and T. Twardowski. "Transverse-electric and transverse-magnetic waves in nonlinear isotropic waveguides." Physical Review A 39, no. 5 (1989): 2481–92. http://dx.doi.org/10.1103/physreva.39.2481.

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17

Liu, Jian, Xin Wang, Shu Mao Wang, and Han Fu. "The Structure Design of Low Frequency Electromagnetic Induction Heating System Based on Analysis of Thermal Effect." Applied Mechanics and Materials 433-435 (October 2013): 1549–53. http://dx.doi.org/10.4028/www.scientific.net/amm.433-435.1549.

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The low frequency transverse magnetic electric induction heating system uses high penetration of low frequency electromagnetic induction heat objects, which is new and high efficient. Due to the magnetic fluxing through objects transversely, it is different with other electromagnetic induction heating methods and this makes it applied more widely. And in this paper, we present the application of low frequency transverse magnetic electric induction heating system in the technique of the lock temperature on seamless line. With the analysis of heating efficiency, it also combines the theory of ed

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18

Gevorkyan E. A. "Transverse components of the electromagnetic field in a waveguide with modulated in space and in time magnetodielectric filling." Optics and Spectroscopy 130, no. 10 (2022): 1293. http://dx.doi.org/10.21883/eos.2022.10.54865.3813-22.

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The propagation of transverse magnetic (TM) and transverse electric (TE) electromagnetic waves in a regular ideal waveguide of arbitrary cross section is considered. It is assumed that the permittivity and permeability of the magnetodielectric filling of the waveguide are functions that depend on the coordinate and time. Analytical expressions for the transverse components of the magnetic and electric vectors of the TM- and TE-fields in the waveguide are obtained from the system of Maxwell equations. They are expressed in terms of the longitudinal components of the electric and magnetic vector

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19

Liu, Zheng Jun, Duo Liu, and Chang Jun Liu. "Comparison of Microstructure and Properties of Ni-Based Overlay Deposit under Longitudinal Magnetic Field and Transverse Magnetic Field." Advanced Materials Research 557-559 (July 2012): 1742–46. http://dx.doi.org/10.4028/www.scientific.net/amr.557-559.1742.

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plasma arc sufacing； magnetic field style ；Ni-based alloy；microstructure and properties Abstract. The Ni60 alloy was overlaid on low carbon steel by plasma arc surfacing with Longitudinal magnetic field or transverse magnetic field. The magnetic field current and surfacing current could been changed during surfacing. After plasma arc surfacing with magnetic field, the XRD, wear loss tes, micro-hardness test were used to analyze the effect of magnetic field style on properties of overlay deposit. The acting mechanism of magnetic field style and parameters on properties and microstructure of ove

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20

Corte-Leon, P., V. Zhukova, J. M. Blanco, et al. "Domain wall propagation in Fe-rich magnetic microwires with graded magnetic anisotropy." AIP Advances 12, no. 3 (2022): 035228. http://dx.doi.org/10.1063/9.0000324.

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We observed that stress-annealing of Fe75B9Si12C4 magnetic microwire at variable annealing temperature allows to create graded magnetic anisotropy. We have found that single domain wall (DW) propagation in a media with graded magnetic anisotropy is essentially non-uniform: faster DW propagation is observed in the region with moderate stress-annealing induced magnetic anisotropy. Higher DW velocity in the region with induced magnetic anisotropy is explained by the transverse character of stress-annealing induced magnetic anisotropy which affects the travelling DW in a similar way as application

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21

Vašek, Petr. "Scaling of Resistivities in MgB₂." Advances in Science and Technology 47 (October 2006): 113–17. http://dx.doi.org/10.4028/www.scientific.net/ast.47.113.

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Longitudinal and transverse voltages have been measured on thin films of MgB2 with different width of superconducting transition range. The study has been performed in zero and nonzero external magnetic fields. The non-zero transverse voltage has been observed in close vicinity of the critical temperature in zero external magnetic field while far enough from Tc this voltage has been zero. In magnetic field it merges into transverse voltage which is an even function with respect to the direction of the field. Usual Hall voltage starts to appear with increasing magnetic field. At the highest fie

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22

Asma, Mohammed Elbashir Saad*1 Mubarak Dirar Abdallah2 &. Swsan Ahmed Elhouri Ahmed3. "TIME DEPENDENT SCHRÖDINGER EQUATION FOR TWO LEVEL SYSTEMS TO FIND TRAVERSE RELAXATION TIME." GLOBAL JOURNAL OF ENGINEERING SCIENCE AND RESEARCHES 6, no. 3 (2019): 251–62. https://doi.org/10.5281/zenodo.2616917.

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Transverse relaxation time is important in magnetic resonance imaging (MRI). It is important to construct new models to find new parameters that control imaging quality. In this work Schrodinger Equation in energy space for two level systems was used to find transverse relaxation time.  By suggesting sine and cosine beside complex solutions a useful expression for transverse relaxation time was found. When electric interaction dominate, i.e. for dielectric materials the transverse relaxation time depends on the electric dipole moment. However the magnetic materials having magnetic spin an

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23

Yu, Mingna, Mei Li, and Jie Lu. "Engineering Planar Transverse Domain Walls in Biaxial Magnetic Nanostrips by Tailoring Transverse Magnetic Fields with Uniform Orientation." Nanomaterials 9, no. 1 (2019): 128. http://dx.doi.org/10.3390/nano9010128.

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Designing and realizing various magnetization textures in magnetic nanostructures are essential for developing novel magnetic nanodevices in the modern information industry. Among all these textures, planar transverse domain walls (pTDWs) are the simplest and the most basic, which make them popular in device physics. In this work, we report the engineering of pTDWs with arbitrary tilting attitude in biaxial magnetic nanostrips by transverse magnetic field profiles with uniform orientation but tuneable strength distribution. Both statics and axial-field-driven dynamics of these pTDWs are analyt

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24

Sheppard, C. J. R., and S. Saghafi. "Transverse-electric and transverse-magnetic beam modes beyond the paraxial approximation." Optics Letters 24, no. 22 (1999): 1543. http://dx.doi.org/10.1364/ol.24.001543.

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25

MOHIUDDIN, TARIQ M. G., A. A. ZHUKOV, D. C. ELIAS, et al. "TRANSVERSE SPIN TRANSPORT IN GRAPHENE." International Journal of Modern Physics B 23, no. 12n13 (2009): 2641–46. http://dx.doi.org/10.1142/s0217979209062116.

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In this paper we report transverse spin transport properties of graphene in a device, where for the first time a mono-atomically thin atomic fabric was sandwiched between magnetic thin films. We found that a single layer graphene flake was sufficient to break the exchange coupling between magnetic films and also to enhance the magnetoresistance effect.

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26

Itoh, Naoki, and Takemi Kotouda. "Velocity-Magnetic Field Correlation of Pulsars." International Astronomical Union Colloquium 160 (1996): 49–50. http://dx.doi.org/10.1017/s0252921100040999.

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Monte Carlo simulations of the evolution of pulsars are carried out in order to compare with the recent measurement of the pulsar transverse velocity by Lyne &amp; Lorimer (1994). The new electron density distribution model of Taylor &amp; Cordes (1993) is adopted in the simulation. Accurate pulsar orbits in the Galactic gravitational field are calculated. It is found that the constant magnetic field model of pulsars can account for the new measurement of the pulsar transverse velocity and the apparent correlation between the strength of the magnetic field and the transverse velocity o

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27

Uchida, Ken-ichi, Weinan Zhou, and Yuya Sakuraba. "Transverse thermoelectric generation using magnetic materials." Applied Physics Letters 118, no. 14 (2021): 140504. http://dx.doi.org/10.1063/5.0046877.

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28

Loginov, D., V. P. Kochereshko, A. Litvinov, et al. "Excitonic Polaritons in Transverse Magnetic Fields." Acta Physica Polonica A 112, no. 2 (2007): 381–86. http://dx.doi.org/10.12693/aphyspola.112.381.

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29

Dunaevsky, A., Y. Raitses, and N. J. Fisch. "Ferroelectric cathodes in transverse magnetic fields." Journal of Applied Physics 93, no. 6 (2003): 3481–85. http://dx.doi.org/10.1063/1.1556568.

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30

Talim, S. L. "Transverse pattern in magnetic domain wall." Physics Letters A 146, no. 3 (1990): 119–21. http://dx.doi.org/10.1016/0375-9601(90)90648-8.

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31

Soliman, H. M., G. M. El-Kashaf, and M. M. Masoud. "Coaxial Discharge and Transverse Magnetic Field." Contributions to Plasma Physics 34, no. 4 (1994): 587–91. http://dx.doi.org/10.1002/ctpp.2150340406.

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32

Loginov, D. K., V. P. Kochereshko, R. T. Cox, et al. "Excitonic polaritons in transverse magnetic fields." physica status solidi (b) 247, no. 6 (2010): 1528–30. http://dx.doi.org/10.1002/pssb.200983188.

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33

Jacobs, Allan E., Tetsuro Nikuni, and Hiroyuki Shiba. "Theory of Magnetic Structures of CsCuCl3in Transverse Magnetic Field." Journal of the Physical Society of Japan 62, no. 11 (1993): 4066–80. http://dx.doi.org/10.1143/jpsj.62.4066.

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34

Ni, J. L., F. Hu, S. J. Feng, X. C. Kan, and X. S. Liu. "Magnetic Properties of FeSiAl Soft Magnetic Composites under Transverse Magnetic Field." Journal of Superconductivity and Novel Magnetism 34, no. 3 (2021): 883–87. http://dx.doi.org/10.1007/s10948-020-05798-3.

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35

Sun, Chenglong, Mengen Shi, Xinyu Wang, Daying Deng, and Weihuo Li. "Effects of Annealing Processes on Microstructure and Properties of FeNi-Based Amorphous Alloy." Materials 18, no. 13 (2025): 3172. https://doi.org/10.3390/ma18133172.

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The present experiment is aimed at investigating the changes in the properties of an FeNiCBCo amorphous alloy after different stress relief annealing. It was established that, under equivalent temperature and time conditions, the strip that underwent no magnetic field annealing exhibited the maximum Bs of 1.09 T. The soft magnetic properties were found to be marginally enhanced by the transverse magnetic treatment, and the coercivity was notably reduced from 10.15 to 0.27 A/m after the longitudinal magnetic treatment. Furthermore, it was determined that, subsequent to the longitudinal magnetic

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36

Chen, S. H., Y. S. Huang, Y. Chen, et al. "A toy Monte Carlo simulation for the transverse polarization of high-energy electron beams." Journal of Instrumentation 17, no. 08 (2022): P08005. http://dx.doi.org/10.1088/1748-0221/17/08/p08005.

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Abstract Transversely-polarized beams are heuristic to the mechanism of CP violation and explore new physics. Besides, the transverse-polarization monitoring is a key point for the beam energy calibration by the resonant depolarization technique. In the article, the transverse polarization measurement of a high-energy electron beam is performed by Monte Carlo simulation on the circular electron-positron collider. The principle based on the Compton back-scattering combining a deflection magnetic field is discussed in detail. The physical presentation of the analyzing power is used to fit the as

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37

Zhalniarovich, Y., A. Przeworski, J. Glodek, and Z. Adamiak. "Low-field magnetic resonance imaging of otitis media in two cats: a case report." Veterinární Medicína 62, No. 2 (2017): 111–15. http://dx.doi.org/10.17221/94/2016-vetmed.

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Otitis media is a common disease in clinical veterinary practice. Although low-field magnetic resonance imaging reports for otitis media in dogs exist, in cats detailed information is missing. Radiography is helpful in diagnosing chronic inflammation, but may be insufficient during the initial phase of inflammation. For this reason, this report describes the magnetic resonance findings in two cats with otitis media. In both cases, middle ear empyema was detected. Magnetic resonance imaging of middle ear disorders in cats should contain pre- and post-contrast T1-weighted sequences in the dorsal

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38

Meng, Jian Bing, Xiao Juan Dong, and Chang Ning Ma. "Effects of External Transverse Alternating Magnetic Field on the Oscillating Amplitude of Atmospheric Pressure Plasma Arc." Advanced Materials Research 129-131 (August 2010): 692–96. http://dx.doi.org/10.4028/www.scientific.net/amr.129-131.692.

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A mathematical model was developed to describe the oscillating amplitude of the plasma arc injected transverse to an external transverse alternating magnetic field. The characteristic of plasma arc under the external transverse alternating magnetic field imposed perpendicular to the plasma current was discussed. The effect of processing parameters, such as flow rate of working gas, arc current, magnetic flux density and the standoff from the nozzle to the workpiece, on the oscillation of plasma arc were also analyzed. The results show that it is feasible to adjust the shape of the plasma arc b

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39

HU, AI-YUAN, and YUAN CHEN. "TWO-DIMENSIONAL ANISOTROPIC HEISENBERG FERROMAGNET IN COEXISTING TRANSVERSE AND LONGITUDINAL MAGNETIC FIELDS." International Journal of Modern Physics B 21, no. 22 (2007): 3877–87. http://dx.doi.org/10.1142/s0217979207037879.

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The two-dimensional spin-1/2 anisotropic Heisenberg ferromagnet is investigated in coexisting transverse and longitudinal magnetic fields. Using the Green function treatment, the magnetization and susceptibility are studied as a function of temperature, anisotropy and magnetic fields. The effects of exchange anisotropy and transverse magnetic field on the magnetic properties of the system are discussed.

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40

Ergasheva, N. M., M. Kh Teshaev, Z. I. Boltaev, and M. Z. Sharipov. "Linear transverse vibrations of a viscous magnetoelastic plate." Современные инновации, системы и технологии - Modern Innovations, Systems and Technologies 5, no. 2 (2025): 2001–8. https://doi.org/10.47813/2782-2818-2025-5-2-2001-2008.

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In this paper, linear transverse vibrations of a magnetoelastic plate are considered. The problem of forced vibrations of a magnetoelastic plate in a magnetic field is solved. Asymptotic and empirical frequency densities of linear transverse oscillations of the plate under the action of a magnetic field are found. Using the asymptotic method, solutions of the dynamic edge effect in transverse and longitudinal magnetic fields were obtained. To compare asymptotic estimates, studies and calculations were carried out using numerical modeling methods.

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41

Ouchani, Noama, Driss Bria, Bahram Djafari-Rouhani, and Abdelkarim Nougaoui. "Transverse-electric/transverse-magnetic polarization converter using 1D finite biaxial photonic crystal." Journal of the Optical Society of America A 24, no. 9 (2007): 2710. http://dx.doi.org/10.1364/josaa.24.002710.

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42

Wang, Hong Mei, and Chang Jun Liu. "Research on the Microstructure and Performance of Co-Based Alloy Surfacing Layer." Advanced Materials Research 652-654 (January 2013): 1886–91. http://dx.doi.org/10.4028/www.scientific.net/amr.652-654.1886.

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With the help of applying the welding method of DC transverse magnetic field plasma arc surfacing, the powder of Co-based alloy is built up welding on surface of low carbon steel, the refinement effect of primary and secondary crystal structure inflicted by the magnetic field is confirmed through hardness test, wear resistance test, metallographic test and XRD analysis. And study systematically the law of DC transverse magnetic field influencing the surfacing layer metal hardness and wear resistance. The results show that the mechanical properties of surfacing layer achieve the best value when

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43

Günalp, Gülen Dilara, Cemal Baykara, and Uğur Güven. "Effect of magnetic field on viscoelastic wave characteristics." Proceedings of the Institution of Mechanical Engineers, Part C: Journal of Mechanical Engineering Science 232, no. 19 (2017): 3482–90. http://dx.doi.org/10.1177/0954406217737583.

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In this study, the longitudinal wave characteristics of magnetic field sensitive viscoelastic rods under the transverse magnetic field effect is addressed by including lateral inertia effect. The analysis is based on the Love rod theory. The polymeric rod is modeled as standard linear solid viscoelastic material. The obtained explicit solution is illustrated graphically. The comparative results of the analysis show that the transverse magnetic field has a remarkable effect on the wave phase velocity and attenuation coefficient. The transverse magnetic field especially leads to a significant re

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44

Schade, Nicholas B., David I. Schuster, and Sidney R. Nagel. "A nonlinear, geometric Hall effect without magnetic field." Proceedings of the National Academy of Sciences 116, no. 49 (2019): 24475–79. http://dx.doi.org/10.1073/pnas.1916406116.

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The classical Hall effect, the traditional means of determining charge-carrier sign and density in a conductor, requires a magnetic field to produce transverse voltages across a current-carrying wire. We demonstrate a use of geometry to create transverse potentials along curved paths without any magnetic field. These potentials also reflect the charge-carrier sign and density. We demonstrate this effect experimentally in curved wires where the transverse potentials are consistent with the doping and change polarity as we switch the carrier sign. In straight wires, we measure transverse potenti

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45

Epik, Hakan. "The bolus effect of magnetic fields in superficial skin tumor brachytherapy: a simulation approach." Journal of Instrumentation 20, no. 05 (2025): P05045. https://doi.org/10.1088/1748-0221/20/05/p05045.

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Abstract Skin cancers have become a serious public health issue and there is a need to enhance the effectiveness of existing treatment methods and to develop new prevention and treatment therapies. In recent years, superficial brachytherapy method have been developed as an alternative to such conventional treatments as external radiotherapy and surgery for treating superficial skin tumors. Integrating a magnetic field can make the superficial skin tumor brachytherapy more effective and safer. This study investigates the effects of longitudinal and transverse magnetic fields on the dose distrib

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46

Bryan, Matthew T., Thomas Schrefl, Del Atkinson, and Dan A. Allwood. "Magnetic domain wall propagation in nanowires under transverse magnetic fields." Journal of Applied Physics 103, no. 7 (2008): 073906. http://dx.doi.org/10.1063/1.2887918.

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47

Barbic, Mladen, and Axel Scherer. "Magnetic nanostructures as amplifiers of transverse fields in magnetic resonance." Solid State Nuclear Magnetic Resonance 28, no. 2-4 (2005): 91–105. http://dx.doi.org/10.1016/j.ssnmr.2005.06.002.

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48

Voloshin, I. F., A. V. Kalinov, L. M. Fisher, and V. A. Yampol’skiĭ. "Suppression of magnetic relaxation by a transverse alternating magnetic field." Journal of Experimental and Theoretical Physics 105, no. 1 (2007): 278–82. http://dx.doi.org/10.1134/s106377610707062x.

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49

Ghezali, S., and M. Slimani. "Transverse magnetic mode excitation in an atomic mirror." Physics & Astronomy International Journal 6, no. 4 (2022): 156–60. http://dx.doi.org/10.15406/paij.2022.06.00269.

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We present a study of a transverse magnetic mode excitation in a multi-layer atomic mirror. We give the continuity relationships at the interfaces of the setting.1 We deduce the transverse and parallel components of the electric field through the atomic mirror and then the total component. We show that there is no enhancement of the electric field in the vaccum contrarily to the transverse electric field excitation.2

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50

Pan, Jun-Hua, Nian-Mei Zhang, and Ming-Jiu Ni. "Wake structure of laminar flow past a sphere under the influence of a transverse magnetic field." Journal of Fluid Mechanics 873 (June 20, 2019): 151–73. http://dx.doi.org/10.1017/jfm.2019.423.

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The wake structure of an incompressible, conducting, viscous fluid past an electrically insulating sphere affected by a transverse magnetic field is investigated numerically over flow regimes including steady and unsteady laminar flows at Reynolds numbers up to 300. For a steady axisymmetric flow affected by a transverse magnetic field, the wake structure is deemed to be a double plane symmetric state. For a periodic flow, unsteady vortex shedding is first suppressed and transitions to a steady plane symmetric state and then to a double plane symmetric pattern. Wake structures in the range $21

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