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Journal articles on the topic 'Direct field'

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Author: Grafiati

Published: 10 December 2022

Last updated: 28 January 2023

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1

Peresada, S., S. Bozhko, S. Kovbasa, and Ye Nikonenko. "ROBUST DIRECT FIELD ORIENTED CONTROL OF INDUCTION GENERATOR." Tekhnichna Elektrodynamika 2021, no. 4 (June 17, 2021): 14–24. http://dx.doi.org/10.15407/techned2021.04.014.

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A novel and robust field oriented vector control method for standalone induction generators (IG) is presented. The proposed controller exploits the concept of direct field orientation and provides asymptotic rotor flux modulus and DC-link voltage regulations when a DC-load is constant or slowly varying. Flux subsystem, designed using Lyapunov’s second method, has, in contrast to standard structures, closed loop properties and therefore is robust with respect to rotor resistance variations. A decomposition approach on the base of the two-time scale separation of the voltage and torque current dynamics is used for design of the voltage subsystem. The feedback linearizing voltage controller is designed using a steady state IG power balance equation. The resulting quasi-linear dynamics of the voltage control loop allows use of simple controllers tuning procedure and provides an improved dynamic performance for variable speed and flux operation. Results of a comparative experimental study with standard indirect field oriented control are presented. In contrast to existing solutions, the designed controller provides system performances stabilization when speed and flux are varying. It is experimentally shown that a robust field oriented controller ensures robust flux regulation and robust stabilization of the torque current dynamics leading to improved energy efficiency of the electromechanical conversion process. The proposed controller is suitable for energy generation systems with variable speed operation. References 18, figures 8.

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2

PAN Sun-qiang, 潘孙强, 陈哲敏 CHEN Zhe-min, and 张建锋 ZHANG Jian-feng. "Direct measurement of sound field." Optics and Precision Engineering 23, no. 11 (2015): 3077–82. http://dx.doi.org/10.3788/ope.20152311.3077.

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3

Tai, C. T. "Direct Integration of Field Equations." Progress In Electromagnetics Research 28 (2000): 339–59. http://dx.doi.org/10.2528/pier99101401.

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4

Fan, H. f. "Direct methods outside traditional field." Acta Crystallographica Section A Foundations of Crystallography 43, a1 (August 12, 1987): C279. http://dx.doi.org/10.1107/s0108767387077997.

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5

Babakhani, Aydin, David B. Rutledge, and Ali Hajimiri. "Near-field direct antenna modulation." IEEE Microwave Magazine 10, no. 1 (February 2009): 36–46. http://dx.doi.org/10.1109/mmm.2008.930674.

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6

Borca, Bogdana, Tomasz Michnowicz, Rémi Pétuya, Marcel Pristl, Verena Schendel, Ivan Pentegov, Ulrike Kraft, et al. "Electric-Field-Driven Direct Desulfurization." ACS Nano 11, no. 5 (May 2017): 4703–9. http://dx.doi.org/10.1021/acsnano.7b00612.

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7

Gratwick, R., and M. A. Sychev. "Direct Methods in Variational Field Theory." Siberian Mathematical Journal 63, no. 5 (September 2022): 862–67. http://dx.doi.org/10.1134/s0037446622050056.

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8

Lindblad, Sven, and Karl‐Ola Lundberg. "The modulation direct field radius: Model." Journal of the Acoustical Society of America 105, no. 2 (February 1999): 1392. http://dx.doi.org/10.1121/1.426579.

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9

Lundberg, Karl‐Ola, and Sven Lindblad. "The modulation direct field radius: Experiments." Journal of the Acoustical Society of America 105, no. 2 (February 1999): 1393. http://dx.doi.org/10.1121/1.426584.

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10

Ávila, Francisco, María Victoria Collados, Jorge Ares, and Laura Remón. "Wide-field direct ocular straylight meter." Optics Express 28, no. 8 (April 1, 2020): 11237. http://dx.doi.org/10.1364/oe.387940.

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11

Tai, C. T. "Direct Integration of Field Equations - Abstract." Journal of Electromagnetic Waves and Applications 14, no. 6 (January 2000): 795–96. http://dx.doi.org/10.1163/156939300x01517.

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12

Costanzo, S., and G. Di Massa. "Direct Far-Field Computation from Bi-Polar Near-Field Samples." Journal of Electromagnetic Waves and Applications 20, no. 9 (January 2006): 1137–48. http://dx.doi.org/10.1163/156939306777442926.

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13

Hörchens, Lars. "Direct analysis of dispersive wave fields from near-field pressure measurements." Journal of the Acoustical Society of America 130, no. 4 (October 2011): 2035–42. http://dx.doi.org/10.1121/1.3626164.

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14

Tamao, Tsutomu. "Direct contribution of oblique field-aligned currents to ground magnetic fields." Journal of Geophysical Research 91, A1 (1986): 183. http://dx.doi.org/10.1029/ja091ia01p00183.

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15

Mitra, Dhrubaditya, Reza Tavakol, Axel Brandenburg, and Petri J. Käpylä. "Oscillatory migratory large-scale fields in mean-field and direct simulations." Proceedings of the International Astronomical Union 5, S264 (August 2009): 197–201. http://dx.doi.org/10.1017/s1743921309992626.

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AbstractWe summarise recent results form direct numerical simulations of both non-rotating helically forced and rotating convection driven MHD equations in spherical wedge-shape domains. In the former, using perfect-conductor boundary conditions along the latitudinal boundaries we observe oscillations, polarity reversals and equatorward migration of the large-scale magnetic fields. In the latter we obtain angular velocity with cylindrical contours and large-scale magnetic field which shows oscillations, polarity reversals but poleward migration. The occurrence of these behviours in direct numerical simulations is clearly of interest. However the present models as they stand are not directly applicable to the solar dynamo problem. Nevertheless, they provide general insights into the operation of turbulent dynamos.

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16

Kuang, Wenhuan, and Jie Zhang. "Direct stress field estimation through waveform matching." Geophysical Journal International 221, no. 2 (January 21, 2020): 843–56. http://dx.doi.org/10.1093/gji/ggaa034.

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SUMMARY Conventionally, the routine workflow of stress field estimation from seismic data consists of two steps: focal mechanism inversion and stress inversion. This two-step workflow suffers from the cumulative uncertainties of both the focal mechanism inversion process and the stress inversion process. To mitigate the cumulative errors, a few previous studies have put efforts to directly estimate the stress field using P-wave polarities. In this study, we develop a new approach to directly estimate tectonic stress fields with better accuracy through waveform matching. This new approach combines the two steps into a one-step workflow to mitigate the cumulative uncertainties through the physical relationship between a stress field and the recorded waveforms. This method assumes a homogeneous stress field in space in the local source region and that the fault slip occurs in the direction of the resolved shear stress acting on the fault plane. Under these assumptions, the stress pattern that generates the theoretical waveforms that best fit the waveforms observed is directly retrieved as the true stress field. The merits of the new approach include that this approach can mitigate the cumulative uncertainties suffered from the conventional two-step workflow and does not require determination of the focal mechanisms of each event; thus, this method is applicable to data sets with few stations. Synthetic tests with and without noise are conducted to demonstrate the performance and merits of this method. Then, the new approach is applied to a real data set from central Oklahoma between March 2013 and March 2016. The resulting stress pattern is consistent with that estimated from previous studies examining the same region. These applications show the benefits and validity of the new approach.

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17

Mao, Jin, Zhongming Xu, Si Chen, Shu Li, and Yansong He. "Direct extrapolation in near‐field acoustic holography." Electronics Letters 51, no. 18 (September 2015): 1388–90. http://dx.doi.org/10.1049/el.2015.0747.

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18

Stupakov, Oleksandr. "Barkhausen Noise Sensor with Direct Field Control." Sensor Letters 11, no. 1 (January 1, 2013): 209–12. http://dx.doi.org/10.1166/sl.2013.2819.

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19

Riek, C., D. V. Seletskiy, A. S. Moskalenko, J. F. Schmidt, P. Krauspe, S. Eckart, S. Eggert, G. Burkard, and A. Leitenstorfer. "Direct sampling of electric-field vacuum fluctuations." Science 350, no. 6259 (October 1, 2015): 420–23. http://dx.doi.org/10.1126/science.aac9788.

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20

D. Manjrekar, Thomas A. Lipo, Seo-G, Madhav. "Flux Tracking Methods for Direct Field Orientation." Electric Machines & Power Systems 27, no. 8 (July 1999): 905–20. http://dx.doi.org/10.1080/073135699268920.

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21

Vertesy, G., L. Pust, I. Tomas, and J. Paces. "Direct measurement of domain wall coercive field." Journal of Physics D: Applied Physics 24, no. 8 (August 14, 1991): 1482–85. http://dx.doi.org/10.1088/0022-3727/24/8/039.

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22

Matsuoka, Mamoru, Masanori Araki, and Makoto Mizuno†. "Beam Direct Converter with Varying Magnetic Field." Fusion Technology 26, no. 4 (December 1994): 1296–303. http://dx.doi.org/10.13182/fst94-a30314.

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23

Yu, Zhelin, Tengzhi Liu, Hanan Elajaili, George A. Rinard, Sandra S. Eaton, and Gareth R. Eaton. "Field-stepped direct detection electron paramagnetic resonance." Journal of Magnetic Resonance 258 (September 2015): 58–64. http://dx.doi.org/10.1016/j.jmr.2015.06.011.

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24

Gopaul, K. K., A. C. Dainty, J. K. Muchowski, C. E. Dawson, J. A. Stack, and A. M. Whatmore. "Direct molecular typing ofBrucellastrains in field material." Veterinary Record 175, no. 11 (July 30, 2014): 282.2–282. http://dx.doi.org/10.1136/vr.102674.

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25

Gadenne, Patrice, Xavier Quelin, Sebastien Ducourtieux, Samuel Gresillon, Lionel Aigouy, Jean-Claude Rivoal, Vladimir Shalaev, and Andrey Sarychev. "Direct observation of locally enhanced electromagnetic field." Physica B: Condensed Matter 279, no. 1-3 (April 2000): 52–55. http://dx.doi.org/10.1016/s0921-4526(99)00665-1.

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26

WEEKS, A. D. "Field Trial of TALC Direct Recording Scale." Journal of Tropical Pediatrics 35, no. 5 (October 1, 1989): 261–62. http://dx.doi.org/10.1093/tropej/35.5.261.

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27

Dereux, A., E. Devaux, J. C. Weeber, J. P. Goudonnet, and C. Girard. "Direct interpretation of near‐field optical images." Journal of Microscopy 202, no. 2 (May 2001): 320–31. http://dx.doi.org/10.1046/j.1365-2818.2001.00868.x.

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28

Han, Hui, Alexei V. Ouriadov, Edmund Fordham, and Bruce J. Balcom. "Direct measurement of magnetic field gradient waveforms." Concepts in Magnetic Resonance Part A 36A, no. 6 (November 2010): 349–60. http://dx.doi.org/10.1002/cmr.a.20194.

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29

Alexandrov, Anatoly Vitalievich, and Ludwig Waclawovich Dorodnicyn. "Direct tensor filter method for synthetic turbulent field generation." Keldysh Institute Preprints, no. 95 (2021): 1–15. http://dx.doi.org/10.20948/prepr-2021-95.

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A Direct Tensor Filter Method for synthetic turbulent field generation is proposed in this paper. The method is a generalization of the Direct Anisotropic Filter Method. The turbulent velocity fields built on the base of this method provides more properties corresponding to real physical turbulent fields in comparison to ones obtained with help of DAF method.

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30

Rouse, Jerry, Mikhail Mesh, and Eric Stasiunas. "Analytical Modeling of the Acoustic Field during a Direct Field Acoustic Test." Journal of the IEST 54, no. 2 (October 1, 2011): 1–53. http://dx.doi.org/10.17764/jiet.54.2.j23pv04t1808316u.

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The acoustic field generated during a Direct Field Acoustic Test (DFAT) has been analytically modeled in two space dimensions using a properly phased distribution of propagating plane waves. Both the pure-tone and broadband acoustic field were qualitatively and quantitatively compared to a diffuse acoustic field. The modeling indicates significant non-uniformity of sound pressure level for an empty (no test article) DFAT, specifically a center peak and concentric maxima/minima rings. This spatial variation is due to the equivalent phase among all propagating plane waves at each frequency. The excitation of a simply supported slender beam immersed within the acoustic fields was also analytically modeled. Results indicate that mid-span response is dependent upon location and orientation of the beam relative to the center of the DFAT acoustic field. For a diffuse acoustic field, due to its spatial uniformity, mid-span response sensitivity to location and orientation is nonexistent.

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31

Zhyltsov, A. V., and V. V. Lyktei. "MAGNETIC FIELD CALCULATION OF BRUSHLESS DIRECT CURRENT MOTOR WITH SMOOTH STATOR BY SECONDARY SOURCES METHOD." Tekhnichna Elektrodynamika 2018, no. 5 (August 9, 2018): 7–10. http://dx.doi.org/10.15407/techned2018.05.007.

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32

Jung, Guo-Bin, Ay Su, Cheng-Hsin Tu, Fang-Bor Weng, and Shih-Hung Chan. "Innovative Flow-Field Combination Design on Direct Methanol Fuel Cell Performance." Journal of Fuel Cell Science and Technology 4, no. 3 (May 23, 2006): 365–68. http://dx.doi.org/10.1115/1.2744056.

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The flow-field design of direct methanol fuel cells (DMFCs) is an important subject about DMFC performance. Flow fields play an important role in the ability to transport fuel and drive out the products (H2O,CO2). In general, most fuel cells utilize the same structure of flow field for both anode and cathode. The popular flow fields used for DMFCs are parallel and grid designs. Nevertheless, the characteristics of reactants and products are entirely different in anode and cathode of DMFCs. Therefore, the influences of flow fields design on cell performance were investigated based on the same logic with respect to the catalyst used for cathode and anode nonsymmetrically. To get a better and more stable performance of DMFCs, three flow fields (parallel, grid, and serpentine) utilized with different combinations were studied in this research. As a consequence, by using parallel flow field in the anode side and serpentine flow-field in the cathode, the highest power output was obtained.

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33

Rouse, Jerry W., Eric C. Stasiunas, and Mikhail Mesh. "Analytical modeling of the acoustic field during a Direct Field Acoustic Test." Journal of the Acoustical Society of America 129, no. 4 (April 2011): 2449. http://dx.doi.org/10.1121/1.3588026.

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34

Yang, Shang-Da, Chen-Shao Hsu, Shih-Lun Lin, You-Sheng Lin, Carsten Langrock, and M. M. Fejer. "Ultrasensitive direct-field retrieval of femtosecond pulses by modified interferometric field autocorrelation." Optics Letters 34, no. 20 (October 5, 2009): 3065. http://dx.doi.org/10.1364/ol.34.003065.

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35

D’Agostino, Francesco, Flaminio Ferrara, Claudio Gennarelli, Rocco Guerriero, and Massimo Migliozzi. "An Innovative Direct NF-FF Transformation Technique with Helicoidal Scanning." International Journal of Antennas and Propagation 2012 (2012): 1–9. http://dx.doi.org/10.1155/2012/912948.

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A direct near-field-far-field transformation with helicoidal scanning is developed. It is based on the nonredundant sampling representation of electromagnetic fields and uses a spherical antenna modelling to determine the number of helix turns. Moreover, the number of voltage samples on each of them is fixed by the maximum transverse dimension of the antenna, both to simplify the mechanical scanning and to reduce the computational effort. This technique allows the evaluation of the antenna far field directly from a minimum set of near-field data without interpolating them. Although the number of near-field data employed by the developed technique is slightly increased with respect to that required by rigorously applying the nonredundant sampling representation on the helix, it is still remarkably smaller than that needed by the standard near-field-far-field transformation with cylindrical scanning. The effectiveness of the technique is assessed by numerical and experimental results.

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36

ISHIKAWA, Ryo, Naoya SHIBATA, and Yuichi IKUHARA. "Direct Electric Field Imaging of Atomistic Graphene Defects." Nihon Kessho Gakkaishi 61, no. 4 (December 15, 2019): 231–36. http://dx.doi.org/10.5940/jcrsj.61.231.

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37

Grossnickle, Steven, and Vladan Ivetić. "Direct Seeding in Reforestation – A Field Performance Review." REFORESTA, no. 4 (December 30, 2017): 94–142. http://dx.doi.org/10.21750/refor.4.07.46.

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38

Passath, Helfried, Gerald Leber, Peter Hamberger, and Florian Bachinger. "Direct current compensation – field experience under service conditions." Journal of Energy - Energija 63, no. 1-4 (July 1, 2022): 3–12. http://dx.doi.org/10.37798/2014631-4158.

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Modern grain oriented core steel used in power transformers has a very high magnetic conductivity. This advanced material makes the transformer susceptible even for small direct current (DC) in the power grid. Already minor DC increases the no-load noise and no-load losses of the transformer considerably. This effect is known as half-cycle saturation. In order to overcome these parasitic DC an active compensation method called “DC compensation” (DCC) was recently developed by Siemens [1]. The question about the origin of the DC is not fully answered yet. However the following sources have been already identified: power electronics, renewable power generation (wind, solar), HVDC transmission lines and DC operated railroad or subway systems. The parasitic direct currents can flow over the power lines to ground or asymmetrically in the power line phases only. In this paper field data, a four-month DC load profile, of single-phase core type transformers, equipped with active DC compensation, are shown. The discussed unit, a bank of three single-phase autotransformers, is in service mainly exposed to DC flowing from the overhead lines through the windings to the common neutral. DC magnitude varies from 0.05 A to about 0.2 A DC per phase throughout the day. From factory tests we know that only 0.2 A DC causes a noise increase of 5.6 dB(A) compared to the noise level without any DC compensation. This might cause troubles at the substation when noise has to be below a guaranteed level. Data analysis of the field data shows that the DC throughout the day follows a clear profile with its highest level during midnight and lunch time. This might indicate a correlation to the load and / or switching operations in the grid to adjust to the actual needed load. However, the DC compensation equipment fully eliminates the direct flux in the core and thus the DC caused increase in noise.

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39

Ørskov., J. "SIMPLE METHOD FOR DIRECT »DARK-FIELD AGAR MICROSCOPY«." Acta Pathologica Microbiologica Scandinavica 27, no. 5 (August 18, 2009): 765–66. http://dx.doi.org/10.1111/j.1699-0463.1950.tb00079.x.

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40

Shimasaki, S., and A. Minagawa. "Direct chill casting with reversing rotational electromagnetic field." IOP Conference Series: Materials Science and Engineering 424 (October 13, 2018): 012055. http://dx.doi.org/10.1088/1757-899x/424/1/012055.

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41

Bandler, J. W., R. M. Biernacki, Shao Hua Chen, D. G. Swanson, and Shen Ye. "Microstrip filter design using direct EM field simulation." IEEE Transactions on Microwave Theory and Techniques 42, no. 7 (July 1994): 1353–59. http://dx.doi.org/10.1109/22.299729.

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42

Lin, J., X. C. Yuan, S. S. Kou, C. J. R. Sheppard, O. G. Rodríguez-Herrera, and J. C. Dainty. "Direct calculation of a three-dimensional diffracted field." Optics Letters 36, no. 8 (April 6, 2011): 1341. http://dx.doi.org/10.1364/ol.36.001341.

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43

Hou, Songming, Knut Solna, and Hongkai Zhao. "A direct imaging method using far-field data." Inverse Problems 23, no. 4 (June 25, 2007): 1533–46. http://dx.doi.org/10.1088/0266-5611/23/4/010.

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44

Stocklmayer, Susan. "Teaching Direct Current Theory Using a Field Model." International Journal of Science Education 32, no. 13 (April 12, 2010): 1801–28. http://dx.doi.org/10.1080/09500690903575748.

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45

Anco, Stephen C., and George Bluman. "Direct Construction of Conservation Laws from Field Equations." Physical Review Letters 78, no. 15 (April 14, 1997): 2869–73. http://dx.doi.org/10.1103/physrevlett.78.2869.

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46

Carpinelli, Joseph M., and B. S. Swartzentruber. "Direct measurement of field effects on surface diffusion." Physical Review B 58, no. 20 (November 15, 1998): R13423—R13425. http://dx.doi.org/10.1103/physrevb.58.r13423.

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47

Viskadouros, Georgios, Dimitrios Konios, Emmanuel Kymakis, and Emmanuel Stratakis. "Direct laser writing of flexible graphene field emitters." Applied Physics Letters 105, no. 20 (November 17, 2014): 203104. http://dx.doi.org/10.1063/1.4902130.

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48

Kantola, Anu M., Perttu Lantto, Ivo Heinmaa, Juha Vaara, and Jukka Jokisaari. "Direct magnetic-field dependence of NMR chemical shift." Physical Chemistry Chemical Physics 22, no. 16 (2020): 8485–90. http://dx.doi.org/10.1039/d0cp01372b.

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49

A. D. Rockwell and P. D. Ayers. "A Variable Rate, Direct Nozzle Injection Field Sprayer." Applied Engineering in Agriculture 12, no. 5 (1996): 531–38. http://dx.doi.org/10.13031/2013.25680.

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50

Loste, F., N. Eynard, and J. Teissié. "Direct monitoring of the field strength during electropulsation." Bioelectrochemistry and Bioenergetics 47, no. 1 (November 1998): 119–27. http://dx.doi.org/10.1016/s0302-4598(98)00183-4.

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