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Abstract

The practical applications of bacteriophages are associated with the problems related to the intensification, optimization of process production of this biomaterial and the search for new methods of production. The production of bacteriophages requires a fine balance between the dynamic growth of the bacteriophage and the host. The electromagnetic field (EMF) is a promising biotechnological method for the process production of bacteriophages. This study evaluates the use of various types of EMF to enhance the process. It was found that the process production of bacteriophages is divided into two stages. In the first stage, the influence of various types of EMF on the proliferation process of bacteria (host) was analyzed. Secondly, the process production of bacteriophage was implemented for the optimal infection conditions under the action of the various types of EMF. Moreover, the study demonstrated that the most effective bacteriophage production was the process with the application of the rotating magnetic field (RMF), pulsed magnetic field (PMF) and the static magnetic field (SMF) with negative polarity.
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Authors and Affiliations

Rafał Rakoczy
1
ORCID: ORCID
Maciej Konopacki
1 2
ORCID: ORCID
Marian Kordas
1
ORCID: ORCID
Bartłomiej Grygorcewicz
2
ORCID: ORCID

  1. West Pomeranian University of Technology in Szczecin, Faculty of Chemical Technology and Engineering, Department of Chemical and Process Engineering, al. Piastów 42,71-065 Szczecin, Poland
  2. Pomeranian Medical University in Szczecin, Chair of Microbiology, Immunology and Laboratory Medicine, Department of Laboratory Medicine, al. Powstanców Wielkopolskich 72, 70-111 Szczecin, Poland
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Abstract

This article deal with non-conventional methods to affect the crystallization of Al-alloys by the application of electromagnetic field. The application of electromagnetic field is not technically complicated, it does not require mechanical contact with the melt, and the scale of the crystallization influence is not dependent on the thickness of the casting. Two experimental materials were used: AlSi10MgMn and AlSi8Cu2Mn and two values of electromagnetic induction: B = 0.1 T a B = 0.2 T. The best results for alloy AlSi10MgMn were achieved by application of electromagnetic field with induction B = 0.2 T; during this experiment the best mechanical properties were achieved - the biggest increase of mechanical properties was recorded. The best results for alloy AlSi8Cu2Mn were achieved by combination of electromagnetic field with induction B = 0.1 T and modification by 0.05 wt. % Sr. In this case we don´t recommend to use electromagnetic field with induction B = 0.2 T; because of deposition of coarse grains and decreasing of mechanical properties.
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Authors and Affiliations

D. Bolibruchová
M. Brůna
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Abstract

The paper presents an analytical solution of levitation problem for conductive, dielectric and magnetically anisotropic ball. The levitation exerts either an AC or impulse magnetic field. Both the Lorentz and material electromagnetic forces (of magnetic matter) could lift the ball in a gravitational field. The electromagnetic field distribution is derived by means of variables separation method. The total force is evaluated by Maxwell stress tensor (generalized), co-energy and Lorentz methods. Additionally, power losses are calculated by means of Joule density and the Poynting vector surface integrals. High frequency asymptotic formulas for the Lorentz force and power losses are presented. All analytical solutions derived could be useful for rapid analysis and design of levitations systems. Finally, some remarks about considered levitations are formulated.
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Bibliography

  1.  K.J. Binns, P.J. Lawrenson, and C.W. Trowbridge, The analytical and numerical solution of electric and magnetic fields, John Wiley & Sons, 1992.
  2.  B.S. Guru and H.R. Hiziroglu, Electromagnetic field theory fundamentals, University Press, Cambridge, 2004.
  3.  V. Dolga and L. Dolga, “Modeling and simulation of a magnetic levitation system”, Annals of the Oradea University of Timisoara, Romania, VI (XVI) (2007).
  4.  H. Górecki and M. Zaczyk, “Determination of optimal controllers. Comparison of two methods for electric network chain”, Bull. Pol. Ac.: Tech.66 (3), 267–273 (2018).
  5.  E. Fromm and H. Jehn, “Electromagnetic forces and power absorption in levitation melting”, British Journal of Applied Physics, 16, 653–663 (1965).
  6.  M. Zdanowski and R. Barlik, “Analytical and experimental determination of the parasitic parameters in high-frequency inductor”, Bull. Pol. Ac.: Tech.65 (1), 107–112 (2017).
  7.  E.C. Okress, D.M. Wroughton, G. Comenetz, P.H. Brace, J.C.R. Kelly, “Electromagnetic levitation of solid and molten metals”, J. Appl. Phys. 23 (5), 545–552 (1952).
  8.  D. Spałek, “Theorem about electromagnetic force surface representation in anisotropic region”, J. Tech. Phys.XLVIII (3-4), 135–145 (2007).
  9.  W.R. Smythe, Static and dynamic electricity, McGraw–Hill Book Company, New York, 1950.
  10.  D. Spałek, “Electromagnetic torque components in synchronous salient-pole machine”, COMPEL. Int. J. Comput. . Math. Electr. Electron. Eng. 16 (3), 129–143 (1997).
  11.  D. Spałek, “Two theorems about surface-integral representation of electromagnetic force and torque”, IEEE Trans. Magn. 53 (7), 1–10 (2017).
  12.  W. He, J. Zhang, S. Yuan, A. Yang, and Ch. Qu, “Threedimensional magneto-electric vibration energy harvester based on magnetic levitation”, IEEE Magn. Lett. 8, 6104703 (2017).
  13.  L. Ułanowicz and G. Jastrze˛bski, “The analysis of working liquid flow in a hydrostatic line with the use of frequency characteristics”, Bull. Pol. Ac.: Tech. 68 (4), 949–956, (2020).
  14.  T. Kaczorek, “Stability analysis of positive linear systems by decomposition of the state matrices into symmetrical and antisymmetrical parts”, Bull. Pol. Ac.: Tech. 67 (4), 761–768 (2019).
  15.  B.P. Mann and N.D. Sims, “Energy Harvesting from the Nonlinear Oscillations of Magnetic Levitation”, Universities of Leeds, Sheffield and York (promoting access to White Rose research papers http://eprints.whiterose.ac.uk/), 2017.
  16.  D. Spałek, “Analytical electromagnetic field and forces calculation for linear, cylindrical and spherical electromechanical converters”, Bull. Pol. Ac.: Tech. 52 (3), 239–250 (2004).
  17.  D. Spałek, “Levitation of Conductive and Magnetically Anisotropic Ball”, IEEE Trans. Magn. 55 (3), 1000406 (2019).
  18.  D. Spałek, “Generalization of Maxwell Stress Tensor Method for Magnetically Anisotropic Regions”, IEEE Trans. Magn. 55 (12), 1000406 (2019).
  19.  J.R. Wait, “A conductive sphere in a time varying magnetic field”, Geophysics, 16 (4), 666–672 (1951).
  20.  K. Jayasekera and I. Ciric, “Benchmark Computations of the Fields, Losses, and Forces for Conducting Spheroids in the Proximity of Current- Carrying Turns”, IEEE Trans Magn. 42 (7), 1802–1811 (2006).
  21.  I.S. Gradshteyn and I.M. Ryzhik, Tables of Integrals, Series, and Products, Academic Press, 2015.
  22.  D. Spałek, “Fourth boundary condition for electromagnetic field problems”, J. Tech. Phys. XLI (2), 129–144 (2000).
  23.  D. Spałek, “Anisotropy component of electromagnetic force and torque”, Bull. Pol. Ac.: Tech. 58 (1), 107–117 (2010).
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Authors and Affiliations

Dariusz Spałek
1
ORCID: ORCID

  1. Silesian University of Technology, Electrical Engineering Faculty, ul. Akademicka 10, 44-100 Gliwice, Poland
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Abstract

The paper analyzes the operation of innovative composite measurement instrumentation for spontaneous electromagnetic emission. The designed receiver measures and records both components of the EM field emitted by rocks subjected to increased mechanical stress. The range of signals transmitted by the receiver system and its dynamics were determined. A receiver was used to observe electromagnetic signals generated during a hard coal sample crushing in laboratory conditions. Test results confirmed the high dynamic range of the system at 98 dB and the ability to observe signals over a range of frequencies up to 50 kHz. The experimental results confirm the signal bandwidth characteristic of coal mine EM field emission obtained in earlier studies. The constructed autonomous receiver can be used in mine workings as a complementary warning system for emerging mine hazards.
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Bibliography

  1.  M. Akgun, “Coal mine accidents,” Turk Thorac Journal, vol. 16, no. 1, pp. s1–s2, 2015, doi: 10.5152/ttd.2015.008.
  2.  A. Tubis, S. Werbińska-Wojciechowska, and A. Wróblewski, “Risk assessment methods in mining industry – A systematic review,” Appl. Sci., vol. 10, pp.1‒34, 2020, doi: 10.3390/app10155172.
  3.  J.L.X. Meng, Y. Wang, and Z. Yang, “Prediction of coal seam details and mining safety using multicomponent seismic data: A case history from China,” Geophysics, vol. 81, no. 5 (September – October), pp. 149–165, 2016, doi: 10.1190/GEO2016-0009.1.
  4.  Y. Wang, N. Fu, X. Lu, and Z. Fu, “Application of a new geophone and geometry in tunnel seismic detection,” Sensors, vol.  19, p. 1246, 2019, doi: 10.3390/s19051246.
  5.  R.M. Bhattacharjeeb, A.K. Dasha, and P.S. Paulb, “A root cause failure analysis of coal dust explosion disaster – Gaps and lessons learnt,” Eng. Fail. Anal., vol. 111, pp. 1‒17, 2020, doi: 10.1016/j.engfailanal.2019.104229.
  6.  M. Li et al., “Piezoelectric effect and ignition properties of coal mine roof sandstone deformation and fracture,” Fuel, vol. 290, pp. 1‒9, 2021, doi: 10.1016/j.fuel.2020.120007.
  7.  M. Hayakawa, “Earthquake precursor studies in Japan” in Pre‐Earthquake Processes, Wiley, pp.7‒18, 2018, doi: 10.1002/ 9781119156949.ch2.
  8.  B. Kunar, “Risk assessment for disaster management in underground coal mines,” Indian Miner. Ind. J., vol. 11, pp.  113‒119, 2015.
  9.  G.-J. Liu, C.-P. Lu, H.-Y. Wang, P.-F. Liu, and Y. Liu, “Warning method of coal bursting failure danger by electromagnetic radiation,” Shock Vib., vol. 2015, p. 583862, 2015, doi: 10.1155/2015/583862.
  10.  E. Wang, H. Jia, D. Song, N. Li, and W. Qian, “Use of ultra-low-frequency electromagnetic emission to monitor stress and failure in coal mines,” Int. J. Rock Mech. Min. Sci., vol. 70, pp. 16–25, 2014, doi: 10.1016/j.ijrmms.2014.02.004.
  11.  A.A. Panfilov, “The results of experimental studies of VLF–ULF electromagnetic emission by rock samples due to mechanical action,” Nat. Hazards Earth Syst. Sci. Discuss., vol. 1, pp. 7821–7842, 2013, doi: 10.5194/nhessd-1-7821-2013.
  12.  Z. Shijiea, S. Xiaoyuanc, L. Chengwub, X. Xiaoxuan, and X. Zhuang, “The analysis of coal or rock electromagnetic radiation (EMR) signals based on Hilbert-Huang transform (HHT),” First International Symposium on Mine Safety Science and Engineering, Procedia Engineering, vol. 26, pp. 689‒698, 2011.
  13.  R. Mydlikowski and K. Maniak, “Measurement of electromagnetic field component emission as a precursor of emerging hazard in coal mines,” J. Telecomm. Inf.Technol., vol. 4, pp. 30‒35, 2019, doi: 10.26636/jtit.2020.145320.
  14.  A. Prałat, K. Maniak, and I. Pompura, “Electromagnetic phenomena in landslides,” Acta Geodynamica and Geomaterialia, vol.  2, no. 3, pp. 131‒138, 2005.
  15.  V. Frid, “Calculation of electromagnetic radiation criterion of rockburst hazard forecast in coal mines,” Pure Appl. Geophys., vol. 158, pp. 931‒944, 2001, doi: 10.1007/PL00001214.
  16.  V. Frid and K. Vozoff, “Electromagnetic radiation induced by mining rock failure,” Int. J. Coal Geol., vol. 64, pp. 57‒65, 2005, doi: 10.1016/j.coal.2005.03.005.
  17.  D. Lin-ming, L. Cai-ping, M. Zong-long, and G. Ming-shi, “Prevention and forecasting of rock burst hazards in coal mines,” Min. Sci. Technol., vol. 19, pp. 585–591, 2009, doi: 10.1016/S1674-5264(09)60109-5.
  18.  S.G. O’Keefe and D.Thiel, “Electromagnetic emissions during rock blasting,” Geophys. Res. Lett., vol. 18, no. 5, pp.  889‒892, 1991, doi: 10.1029/91GL01076.
  19.  P. Xiong et al., “Identification of electromagnetic pre-earthquake perturbations from the DEMETER data by machine learning,” Remote Sens., vol. 12, pp. 1‒27, 2020, doi: 10.3390/rs12213643.
  20.  A. Erturk and D.J. Inman, Piezoelectric Energy Harvesting, First Edition, John Wiley & Sons, Ltd. Published 2011, pp. 343‒344.
  21.  M. Krumbholz, M. Bock, S. Burchardt, U. Kelka, and A. Vollbrecht, “A critical discussion of the electromagnetic radiation (EMR) method to determine stress orientations within the crust,” Solid Earth, vol. 3, pp. 401‒414, 2012, doi: 10.5194/sed-4-993-2012.
  22.  A. Rabinovitch, V. Frid, D. Bahat ,and J. Goldbaum, “Decay mechanism of fracture induced electromagnetic pulses,” J. Appl. Phys., vol. 93, no. 9, pp 5085–5090, 2003, doi: 10.1063/1.1562752.
  23.  A. Rabinovitch, V. Frid, and D. Bahat, “Surface oscillations. A possible source of fracture induced electromagnetic radiation,” Tectonophysics, vol. 431, pp 15‒21, 2007, doi: 10.1016/j.tecto.2006.05.027.
  24.  A. Takeuchi and H. Nagahama, “Electric dipoles perpendicular to a stick-slip plane,” Phys. Earth Planet. Inter., vol.  155, pp. 208–218, 2006, doi: 10.1016/j.pepi.2005.12.010.
  25.  P. Koktavy and J. Sikula, “Physical model of electromagnetic emission in solids,” Proc. 26th Eur. Conf. Acous. Emission Testing EWGAE 2004, Berlin, Germany, 2004, pp. 899‒904.
  26.  S.K. Sharma, R. Kiran, A. Kumar, V.S. Chauhan, and R. Kumar, “A theoretical model for the electromagnetic radiation emission from hydrated cylindrical cement paste under impact,” J. Phys. Commun., vol. 2, no. 3, pp. 1‒12, 2018,
  27.  D. Miedzińska, T. Niezgoda, E. Małek, and D. Zasada, “Study on coal microstructure for porosity levels assessment,” Bull. Pol. Acad. Sci. Tech. Sci., vol. 61, no. 2, pp. 409‒505, 2013, doi: 10.2478/bpasts-2013-0049.
  28.  F. Zhao, Y. Li, Z. Ye, Y. Fan, S. Zhang, H. Wang, and Y. Liu, “Research on acoustic emission and electromagnetic emission characteristics of rock fragmentation at different loading rates,” Shock Vib., vol. 2018, p. 4680879, 2018, doi: 10.1155/2018/4680879.
  29.  Z. Loni, H. Espinosa, and D. Thiel, “Insulated wire fed floating monopole antenna for coastal monitoring,” Radioengineering, vol. 27, no. 1, pp. 127–133, 2018, doi: 10.13164/re.2018.0127.
  30.  V. Dyo, T. Ajmal, B. Allen, D. Jazani, and I. Ivanov, “Design of a ferrite rod antenna for harvesting energy from medium wave broadcast signals,” J. Eng., vol. 2013, no. 12, pp. 89–96, 2013, doi: 10.1049/joe.2013.0126.
  31.  T. Bolton and M.B. Cohen, “Optimal design of electrically-small loop receiving antenna,” Prog. Electromagn. Res. C, vol. 98, pp. 155–169, 2020, doi: 10.2528/PIERC19090911.
  32.  U. Tietze, Ch. Schenk, and E. Gamm, Electronic Circuits–Handbook for Design and Application, 2nd Edition. Springer, 2011, pp. 787‒841.
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Authors and Affiliations

Remigiusz Mydlikowski
1
ORCID: ORCID
Krzysztof Maniak
2
ORCID: ORCID

  1. Wroclaw University of Science and Technology, Faculty of Electronics, Photonics and Microsystems, ul. Janiszewskiego 11/17, 50-372 Wrocław, Poland
  2. National Institute of Telecommunications, ul. Szachowa 1, 04-894 Warsaw, Poland
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Abstract

Worldwide Interoperability for Microwave Access (WiMAX), based on the IEEE 802.16 standards, is a technology that offers low cost mobile broadband access to multimedia and internet applications for operators and end-users. Similarly to cellular phone or other Radio Frequency devices, WiMAX has to be considered as a possible source of electromagnetic pollution and so monitoring its emission could be necessary to verify compliance with the applicable emission limits. Generally, the monitoring of the electromagnetic pollution is performed by means of a suitable measurement chain constituted by an antenna connected to a traditional spectrum analyzer. The use of this kind of device to measure the power of digital modulated noise-like signals, such as WiMAX, requires to use proper measurement methods and to carefully set many instrument parameters to obtain reliable measurement results, otherwise a significant underestimate or overestimate of the human exposure can be obtained.

In this framework, this paper investigates the feasibility of using the traditional spectrum analyzer to perform the electromagnetic pollution measurements due to WiMAX devices. A large experimental campaign is carried out to identify the most proper measurement method and spectrum analyzer settings able to warrant reliable measurements.

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Authors and Affiliations

Giovanni Betta
Domenico Capriglione
Gianfranco Miele
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Abstract

A probable risk for different diseases has been reported due to exposure of peoples living in the vicinity of electrical substations and electrical workers. The aim of this paper is to examine and reduce the induced current density due to the power system field acting on human beings in the working environment, by using the spheroidal calculation model. The results obtained by means of computer programs developed by the author in the MATLAB environment are compared with the limit values given by the International Committee on Non-Ionizing Radiation Protection (ICNIRP) for demonstrating the degree of danger due to the induced current and have a certain guidance function for worker’s health to ensure their safety.

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Authors and Affiliations

Manel Bidi
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Abstract

Production deviations have a remarkable effect on the radiated sound of electrical machines, introducing additional signal components besides the fundamental field waves which significantly change and enrich the subjectively perceived sound characteristic. In literature these harmonics are mainly traced back to dynamic eccentricity, which modulates the fundamental fieldwaves. In this paper a thorough mechanic and electromagnetic analysis of a modern, well-constructed traction drive (permanent magnet synchronous machine) is performed to showthat for this typical rotor configuration dynamic eccentricity is negligible. Instead, deviations in the rotor magnetization are shown to be the dominant cause for vibration harmonics.
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Bibliography

[1] Nahlaoui M.A., Steins H., Kulig S., Exnowski S., Comparison of numerically determined noise of a 290 kW induction motor using FEM and measured acoustic radiation, Archives of Electrical Engineering, vol. 62, pp. 195–207 (2013), DOI: 10.2478/aee-2013-0015.
[2] Gieras J.F., Wang C., Cho Lai J., Noise of polyphase electric motors, CRC Press Taylor and Francis Group (2006).
[3] Hu Y., Wei H., Chen H., Sun W., Zhao S., Li L., Vibration Study of Permanent Magnet Synchronous Motor Base on Static Eccentricity Model, 22nd International Conference on Electrical Machines and Systems (ICEMS), Harbin, China, pp. 1–5 (2019), DOI: 10.1109/ICEMS.2019.8922162.
[4] LiY.,Wu H.,Xu X., CaiY., Sun X., Analysis on electromechanical coupling vibration characteristics of in-wheel motor in electric vehicles considering air gap eccentricity, Archives of Electrical Engineering, vol. 5, pp. 851–862 (2019), DOI: 10.24425/bpasts.2019.130882.
[5] Lundin U., Wolfbrandt A., Method for Modeling Time-Dependent Nonuniform Rotor/Stator Configurations in Electrical Machines, IEEE Transactions on Magnetics, vol. 45, iss. 7, pp. 2976–2980 (2009), DOI: 10.1109/TMAG.2009.2015052.
[6] Zhang M., Macdonald A., Tseng K.-J., Burt G.M., Magnetic Equivalent Circuit Modeling for Interior Permanent Magnet Synchronous Machine under Eccentricity Fault, 48th International Universities’ Power Engineering Conference (UPEC), Dublin, Ireland, pp. 1–6 (2013), DOI: 10.1109/UPEC.2013.6715044.
[7] Ebrahimi B.M., Faiz J., Roshtkhari M.J., Static-, Dynamic-, and Mixed- Eccentricity Fault Diagnoses in Permanent-Magnet Synchronous Motors, IEEE Transactions on industrial electronics, vol. 56, no. 11, pp. 4727–4739 (2009), DOI: 10.1109/TIE.2009.2029577.
[8] Rosero J.A., Cusido J., Garcia A., Ortega J.A., Romeral L., Broken Bearings and Eccentricity Fault Detection for a Permanent Magnet Synchronous Motor, 32nd Annual Conference on IEEE Industrial Electronics (IECON), Paris, France, pp. 964–969 (2006), DOI: 10.1109/IECON.2006.347599.
[9] Ilamparithi T., Nandi S., Saturation independent detection of dynamic eccentricity fault in salient-pole synchronous machines, IEEE International Symposium on Diagnostics for Electric Machines, Power Electronics and Drives (SDEMPED), Valencia, Spain, pp. 336–341 (2013), DOI: 10.1109/DEMPED.2013.6645737. [10] Goktas T., Zafarani M., Akin B., Discernment of Broken Magnet and Static Eccentricity Faults in Permanent Magnet Synchronous Motors, IEEE Transactions on Energy Conversion, vol. 31, iss. 2, pp. 578–587 (2016).
[11] Coenen I., van der Giet M., Hameyer K., Manufacturing Tolerances: Estimation and Prediction of Cogging Torque Influenced by Magnetization Faults, IEEE Transactions on Magnetics, vol. 48, iss. 5, pp. 1932–1936 (2012), DOI: 10.1109/TMAG.2011.2178252.
[12] Gasparin L., Fiser R., Cogging torque sensitivity to permanent magnet tolerance combinations, Archives of Electrical Engineering, vol. 62, pp. 449–461 (2013), DOI: 10.2478/aee-2013-0036.
[13] International Organization for Standardization, ISO 1940-1: Mechanical vibration — Balance quality requirements for rotors in a constant (rigid) state, Geneva, Switzerland (2003).
[14] https://www.smalley.com/wave-springs/bearing-preload, accessed March 2020.
[15] Henrotte F., Felden M., van der Giet M., Hameyer K., Electromagnetic force computation with the Eggshell method, 14th International Symposium on Numerical Field Calculation in Electrical Engineering (IGTE), Graz, Austria (2010).
[16] Herold T., Franck D., Schröder M., Böhmer S., Hameyer K., Transientes Simulationsmodell für die akustische Bewertung elektrischer Antriebe, e & i Elektrotechnik und Informationstechnik, vol. 133, no. 2, pp. 55–64 (2016).

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Authors and Affiliations

Markus Jaeger
1
Pascal Drichel
2
Michael Schröder
1
Joerg Berroth
2
Georg Jacobs
2
Kay Hameyer
1
ORCID: ORCID

  1. Institute of Electrical Machines (IEM), RWTH Aachen University, Germany
  2. Institute of Systems Engineering and Machine Elements (MSE), RWTH Aachen University, Germany
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Abstract

This paper takes a 50 kW interior permanent magnet brushless DC motor as an example, and explores the influence of the degree of stator slot skew on the overall motor magnetic density and air gap magnetic density; then reveals the influences of stator slot skewed structure on a series of key electromagnetic properties like no-load back electromotive force (B-EMF), cogging torque, electromagnetic torque, torque fluctuation, electromagnetic loss, input power, output power and operating efficiency. On this basis, a relatively best range of the skew degrees is obtained. The research work in this paper has direct reference value for the further improvement of design and manufacture, operation and maintenance, control and protection of such motors.
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Bibliography

[1] Zhang Chen, Principle and Application of Brushless DC Motor, China Machinery Industry Press, Beijing (1996).
[2] Tang Renyuan, Modern Permanent Magnet Motor Theory and Design, Mechanical Industry Press, Beijing (2005).
[3] LiWeiqi, LinRongwen, Tao Tao, Optimized design based on the air gap length of the built-in permanent magnet brushless DC motor, Electric Switchgear, vol. 58, no. 05, pp. 58–63 (2020).
[4] Parsa L., Hao L., Interior Permanent Magnet Motors with Reduced Torque Pulsation, IEEE Transactions on Industrial Electronics, vol. 55, no. 2, pp. 602–609 (2008), DOI: 10.1109/TIE.2007.911953.
[5] Ren Dejiang, Huang Qu, Li Jianjun, Wu Ning, Cogging torque optimization analysis of built-in permanent magnet synchronous motor, Explosion-Proof Electric Machine, vol. 54, no. 4, pp. 4–7+43 (2019).
[6] Zhao W., Lipo T.A., Kwon B., Torque Pulsation Minimization in Spoke-type Interior Permanent Magnet Motors with Skewing and Sinusoidal Permanent Magnet Configurations, IEEE Transactions on Magnetics, vol. 51, no. 11, pp. 1–4 (2015), DOI: 10.1109/TMAG.2015.2442977.
[7] AimengW., Heming L.,Weifu L., Haisen Z., Influence of skewed and segmented magnet rotor on IPM machine performance and ripple torque for electric traction, IEEE International Electric Machines and Drives Conference, pp. 305–310 (2009), DOI: 10.1109/IEMDC.2009.5075222.
[8] Adrian Młot, Marcin Kowol, Janusz Kołodziej, Andrzej Lechowicz, Piotr Skrobotowicz, Analysis of IPM motor parameters in an 80-kW traction motor, Archives of Electrical Engineering, vol. 69, no. 2 (2020), DOI: 10.24425/aee.2020.133038.
[9] Yang Zhihao, Yang Mengxue, Wang Sinuo, Bao Xiaohua, The influence of stator skew on the performance of permanent magnet synchronous motors, Transactions of the Chinese Society of Electrical Engineering, vol. 14, no. 3, pp. 97–102 (2019).
[10] Wang Dongliang, Chen Wei, Discussion on the electromagnetic design of concentrated winding permanent magnet motor from the perspective of torque fluctuation, Electric Tool, vol. 4, pp. 15–17 (2017), DOI: 10.16629/j.cnki.1674-2796.2017.04.004.
[11] Xiaodong S., Zhou S., Long C., Zebin Y., Skew Angle Optimization Analysis of a Permanent Magnet Synchronous Motor for EVs, IEEE International Conference on Applied Superconductivity and Electromagnetic Devices (ASEMD), pp. 1–2 (2018), DOI: 10.1109/ASEMD.2018.8558826.
[12] Wang Changcheng, Guo Hui, Sun Pei, Liu Ningning,Wang Yansong, Qin Yifei, A method for reducing cogging torque of permanent magnet synchronous motors, Light Industry Machinery, vol. 36, no. 6, pp. 62–66 (2018).
[13] He Qiang, Magnetic field analysis and cogging torque study of brushless DC permanent magnet motors, Hefei University of Technology (2016).
[14] Hongwei Fang, Hongxu Chen, Analysis and reduction of the cogging torque of flux-modulated generator for wave energy conversion, Energy Procedia, vol. 158, pp. 327–332 (2019), DOI: 10.1016/j.egypro.2019.01.097.
[15] Fu Lixin et al., GB/T 1029-2005 Three-phase synchronous motor test method, China Standard Press, Beijing (2006).
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Authors and Affiliations

Xue-gui Gan
1
ORCID: ORCID
Zhen-nan Fan
1
ORCID: ORCID
Jing-can Li
2
ORCID: ORCID

  1. The Key Laboratory of Fluid and Power Machinery, Ministry of Education, Xihua University, Chengdu, China
  2. State Key Laboratory of Power Transmission Equipment & System Security and New Technology, Chongqing University, Chongqing, China
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Abstract

The uncontrolled rectifier and controlled rectifier which use fixed switching frequency control strategy are applied usually during the working of a high-power high- speed permanent magnet generator (HSPMG). Even for the controlled rectifier, it will generate harmonics. The electromagnetic performance of the HSPMG is also affected by these harmonics. In this paper, the influences of the fixed switching frequency control strategy on a HSPMG were studied. Based on the Fourier theory, the harmonic currents of the generator were analyzed, and the change of harmonic distribution range and current total harmonic distortion (THD) were obtained. By using an indirect field-circuit coupling method, the influences of the fixed switching frequency control strategy on the losses and torque of the generator were analyzed. The relations between the switching frequency and the losses and torque of the generator were obtained, and the change mechanism of the loss was revealed. The obtained conclusions can provide reference for the optimized choice of the switching frequency of the distributed generation system with the HSPMG. It can also provide support for the HSPMG electromagnetic structural optimization and the optimization of the loss and harmonic on the system level.

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Authors and Affiliations

Qiu Hongbo
Wei Yanqi
Yang Cunxiang
Hu Kaiqiang
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Abstract

Induction surface hardening means the hardening of a thin zone of the material only, while its core remains soft. The paper deals with the modelling of the Consecutive Dual Frequency Induction Hardening (CDFIH) of gear wheels and its validation. For gear wheels with modulus m smaller than 6 mm a contour profile of hardness distribution could be obtained. The investigated gear wheel is heated first by a medium frequency inductor to the temperature approximately equal to the modified lower temperature Ac1m. It means beginning of the austenite transformation. Then the gear wheel is heated by the high frequency inductor to the hardening temperature making it possible to complete the austenite transformation and immediately cooled. In order to design the process it is necessary to identify modified critical temperatures and to obtain expected temperature distribution within the whole tooth.

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Authors and Affiliations

Jerzy Barglik
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Abstract

In order to research the losses and heat of damper bars thoroughly, a multislice moving electromagnetic field-circuit coupling FE model of tubular hydro-generator and a 3D temperature field FE model of the rotor are built respectively. The factors such as rotor motion and non-linearity of the time-varying electromagnetic field, the stator slots skew, the anisotropic heat conduction of the rotor core lamination and different heat dissipation conditions on the windward and lee side of the poles are considered. Furthermore, according to the different operating conditions, different rotor structures and materials, compositive calculations about the losses and temperatures of the damper bars of a 36 MW generator are carried out, and the data are compared with the test. The results show that the computation precision is satisfied and the generator design is reasonable.

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Authors and Affiliations

Yong Liao
Zhen-Nan Fan
Li Han
Li-Dan Xie
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Abstract

This paper deals with some aspects of formulation and implementation of a broadband algorithm with build-in analysis of some dispersive media. The construction of the finite element method (FEM) based on direct integration of Maxwell’s equations and solution of some additional convolution integrals is presented. The broadband, fractional model of permittivity is approximated by a set of some relaxation sub-models. The properties of the 3D time-dependent formulation of the FEM algorithm are determined using a benchmark problem with the Cole-Cole and the Davidson-Cole models. Several issues associated with the implementation and some constraints of the broadband finite element algorithm are presented.

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Authors and Affiliations

Bogusław Butryło
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Abstract

To study the principle of loss and heat at the end region of large 4-poles nuclear power turbine generator, 3D transient electromagnetic field and 3D steady temperature field finite element (FE) models of the end region are established respectively. Considering the factors such as rotor motion, core non-linearity and time-varying of electromagnetic field, the anisotropic heat conductivity and different heat dissipation conditions of stator end region, a 50 Hz, 1150 MW, 4-poles nuclear power turbine generator is investigated. The loss and heat at the generator end region are calculated respectively at no-load and rated-load, and the calculation results are compared with the test data. The result shows that the calculation model is accurate and the generator design is suitable. The method is valuable for the research of loss and heat at the end region of large 4-poles nuclear power turbine generator and the improvement of the generator’s operation stability. The method has been applied successfully for the design of the larger nuclear power turbine generators.

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Authors and Affiliations

Guang-Hou Zhou
Li Han
Zhen-Nan Fan
Yong Liao
Song Huang
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Abstract

The problems connected to developing inductive power transfer IPT systems in aspects of high efficiency and suppression of electromagnetic field (EMF) emission are discussed. It is shown how important it is to compensate for large leakage impedance of IPT coils (air transformer) to improve efficiency of high power transfer. Such compensation circuits operating with resonant frequencies at soft switching conditions additionally allow for reduction of switching losses in power semiconductor devices of converters. The consideration has been illustrated and verified by experimental results measured on two different test stands (50 kW with planar coils and with two 12 kW receiver coils) built in a laboratory of the Łukasiewicz Research Network – Electrotechnical Institute.

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Authors and Affiliations

R.M. Miśkiewicz
P. Anczewski
A.J. Moradewicz

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