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Journal articles on the topic 'Hysteresis – Measurement'

Author: Grafiati

Published: 4 June 2021

Last updated: 9 February 2022

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1

Kuczmann, Miklós, Péter Kis, Amália Iványi, and János Füzi. "Vector hysteresis measurement." Physica B: Condensed Matter 343, no. 1-4 (January 2004): 390–94. http://dx.doi.org/10.1016/j.physb.2003.08.075.

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2

Garshelis, Ivan J., and Guillaume Crevecoeur. "A Simple Magnetostatic Sensing Method for Assessing the Local Hysteresis Properties in Ferromagnetic Sheet Materials." Journal of Sensors 2012 (2012): 1–7. http://dx.doi.org/10.1155/2012/870916.

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Global hysteretic properties of electrical steels can be measured using ring or strip samples, while the assessment of the local hysteretic properties is a much more difficult task since the measurement method needs to be very sensitive. This paper presents a new method wherein the intensity and spatial distribution of the magnetic field, arising from large gradients in the local magnetization, are measured. These large gradients are induced by the passage of a test sample through the steep gradient field of a small, proximate permanent magnet. Magnetic field measurements during both directions of motion provide information indicative of the hysteresis properties. We theoretically analyze these measurements and show experimentally that the measurements correlate well with all the significant aspects of conventional hysteresis loops. The results given in this paper are qualitative, and the method is both by its simplicity and its sensitivity to important hysteresis features a powerful means of magnetic nondestructive evaluation.

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3

Kis, Péter, Miklós Kuczmann, János Füzi, and Amália Iványi. "Hysteresis measurement in LabView." Physica B: Condensed Matter 343, no. 1-4 (January 2004): 357–63. http://dx.doi.org/10.1016/j.physb.2003.08.069.

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4

Filippi, Sergio, Adnan Akay, and Muzio M. Gola. "Measurement of Tangential Contact Hysteresis During Microslip." Journal of Tribology 126, no. 3 (June 28, 2004): 482–89. http://dx.doi.org/10.1115/1.1692030.

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This paper describes a measurement system designed to determine the hysteresis that develops between two surfaces as a result of small-amplitude tangential relative motion. Hysteresis is determined by measuring the tangential force and relative displacement of the contacting surfaces as they oscillate. These measurements also produce values of contact parameters such as friction coefficient and tangential contact stiffness. Although these parameters depend on the tribological properties, most of them also exhibit strong sensitivity to measurement errors. The measurement system described here avoids or at least reduces many of the measurement artifacts. This paper validates the measurement system by analyzing and estimating potential errors and describes corrections to systematic errors where possible.

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5

Disselnkötter, Rolf. "Automized magnetic hysteresis measurement system." Journal of Applied Physics 79, no. 8 (1996): 5208. http://dx.doi.org/10.1063/1.361342.

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6

Ran, H. J., X. W. Luo, Y. L. Chen, H. Y. Xu, and M. Farhat. "Hysteresis phenomena in hydraulic measurement." IOP Conference Series: Earth and Environmental Science 15, no. 6 (November 26, 2012): 062048. http://dx.doi.org/10.1088/1755-1315/15/6/062048.

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7

Diaz, M. Elena, Javier Fuentes, Ramon L. Cerro, and Michael D. Savage. "Hysteresis during contact angles measurement." Journal of Colloid and Interface Science 343, no. 2 (March 2010): 574–83. http://dx.doi.org/10.1016/j.jcis.2009.11.055.

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8

Wang, Qi, Tong Li, Lan Luo, Yu He, Xiong Liu, Zhaoxue Li, Zhiyou Zhang, and Jinglei Du. "Measurement of hysteresis loop based on weak measurement." Optics Letters 45, no. 5 (February 18, 2020): 1075. http://dx.doi.org/10.1364/ol.383764.

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9

Park, Jae-Hwan, Byung-Kook Kim, Jae-Gwan Park, In-Tae Kim, Hae-June Je, Yoonho Klm, and Soon Ja Park. "Dielectric hysteresis measurement in lossy ferroelectrics." Ferroelectrics 230, no. 1 (May 1999): 151–56. http://dx.doi.org/10.1080/00150199908214911.

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10

Turvey, K., and T. Turvey. "Measurement of Magnetically Induced Stress as a Means of Determining Magnetization Characteristics of Mild Steel." International Journal of Electrical Engineering & Education 29, no. 4 (October 1992): 339–53. http://dx.doi.org/10.1177/002072099202900410.

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Measurement of magnetically induced stress as a means of determining magnetization characteristics of mild steel The magnetic major hysteresis loop and the initial magnetization curve are obtained for mild steel from measurements of the attractive force between magnetized semi-rings. A check determination of the hysteresis loop using a standard method yields good agreement.

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11

Ghafarirad, H., SM Rezaei, M. Zareinejad, and NA Mardi. "Charge-based hysteresis compensation in low impedance piezoelectric actuators by a modified Prandtl–Ishlinskii model." Proceedings of the Institution of Mechanical Engineers, Part E: Journal of Process Mechanical Engineering 233, no. 1 (November 24, 2017): 83–93. http://dx.doi.org/10.1177/0954408917743391.

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Piezoelectric actuators are one of the most popular actuators in micro- and nano-applications. The main deficiency of these actuators is the hysteretic behavior. Hysteresis not only can destroy the positioning accuracy, but also may lead to instability. In previous researches, hysteresis in the mechanical domain (voltage–position) has been modeled and compensated by several approaches. The limiting condition has been position measurement by a high cost, fine resolution sensor. So, an alternative idea can be compensation in the electrical domain (voltage–charge). In fact, it can be demonstrated that hysteresis compensation in the electrical domain can simultaneously compensate the mechanical one. But, experimental results depict that voltage–charge relation may be time dependent due to low internal impedances. It would lead to “time-dependent hysteresis”. As a result, conventional models cannot be applied for hysteresis identification. In this paper, a modified time-dependent Prandtl–Ishlinskii model is proposed to identify the time-dependent hysteresis in low impedance actuators. Utilizing the proposed model, experimental results validate that the mechanical hysteresis would be appropriately compensated as a result of compensation in the electrical domain.

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12

Pólik, Zoltán, and Miklós Kuczmann. "Measurement and control of scalar hysteresis characteristics." Pollack Periodica 2, no. 2 (August 2007): 27–37. http://dx.doi.org/10.1556/pollack.2.2007.2.3.

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13

Schneider, Carl S., Stephen D. Gedney, Sean M. Joyce, Todd W. Fulton, and Mark A. Travers. "Measurement and exponential model of ferromagnetic hysteresis." Physica B: Condensed Matter 570 (October 2019): 259–65. http://dx.doi.org/10.1016/j.physb.2019.06.041.

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14

Tučková, Michaela, Radoslav Harman, Pavel Tuček, and Jiří Tuček. "Design of experiment for hysteresis loops measurement." Journal of Magnetism and Magnetic Materials 368 (November 2014): 64–69. http://dx.doi.org/10.1016/j.jmmm.2014.05.012.

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15

Kuczmann, M. "Measurement and Simulation of Vector Hysteresis Characteristics." IEEE Transactions on Magnetics 45, no. 11 (November 2009): 5188–91. http://dx.doi.org/10.1109/tmag.2009.2031072.

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16

Ueda, F., K. Takeda, and T. Yamaguchi. "Automatic Hysteresis Measurement System with High Accuracy." IEEE Translation Journal on Magnetics in Japan 1, no. 7 (October 1985): 883–84. http://dx.doi.org/10.1109/tjmj.1985.4549001.

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17

Shin, Hyunjung, Jung Kyu Shin, Seungbum Hong, Jong Up Jeon, Han Wook Song, Jong In Hong, and Kwangsoo No. "Piezoelectric hysteresis measurement using atomic force microscopy." Integrated Ferroelectrics 38, no. 1-4 (January 2001): 31–38. http://dx.doi.org/10.1080/10584580108016915.

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18

Wang, Le, Xiaoli Wang, and Jing Shi. "Measurement and Estimation of Ferroelectric Hysteresis Loops." Ferroelectrics 411, no. 1 (November 2, 2010): 86–92. http://dx.doi.org/10.1080/00150193.2010.493086.

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19

Palici, Alexandra, George Alexandru Nemnes, Cristina Besleaga, Lucian Pintilie, Dragos-Victor Anghel, Ioana Pintilie, and Andrei Manolescu. "The Influence of the Relaxation Time on the Dynamic Hysteresis in Perovskite Solar Cells." EPJ Web of Conferences 173 (2018): 03017. http://dx.doi.org/10.1051/epjconf/201817303017.

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We investigate the dynamic behavior of perovskite solar cells by focusing on the relaxation time τ, which corresponds to the slow de-polarization process from an initial bias pre-poled state. The dynamic electrical model (DEM) is employed for simulating the J-V characteristics for different bias scan rates and pre-poling conditions. Depending on the sign of the initial polarization normal or inverted hysteresis may be induced. For fixed pre-poling conditions, the relaxation time, in relation to the bias scan rate, governs the magnitude of the dynamic hysteresis. In the limit of large τ the hysteretic effects are vanishing for the typical range of bias scan rates considered, while for very small τ the hysteresis is significant only when it is comparable with the measurement time interval.

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20

Zhang, Guilin, Chengjin Zhang, and Chaoyang Wang. "Iterative Learning Control of Hysteresis in Piezoelectric Actuators." Mathematical Problems in Engineering 2014 (2014): 1–6. http://dx.doi.org/10.1155/2014/856706.

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We develop convergence criteria of an iterative learning control on the whole desired trajectory to obtain the hysteresis-compensating feedforward input in hysteretic systems. In the analysis, the Prandtl-Ishlinskii model is utilized to capture the nonlinear behavior in piezoelectric actuators. Finally, we apply the control algorithm to an experimental piezoelectric actuator and conclude that the tracking error is reduced to 0.15% of the total displacement, which is approximately the noise level of the sensor measurement.

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21

Vértesy, Gábor, Tetsuya Uchimoto, Toshiyuki Takagi, and Ivan Tomáš. "Nondestructive Inspection of Ductile Cast Iron by Measurement of Minor Magnetic Hysteresis Loops." Materials Science Forum 659 (September 2010): 355–60. http://dx.doi.org/10.4028/www.scientific.net/msf.659.355.

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Systematic measurement of minor magnetic hysteresis loops of traditional hysteresis tests requires substantially lower magnetization of samples and offers higher sensitivity of detection of changes in the ferromagnetic materials’ microstructure. The keynote idea of this method, called Magnetic Adaptive Testing (MAT) is utilization of sensitive correlations between the varied microstructure of the magnetized material and the corresponding, highly sensitive modifications of some of the minor hysteresis loops. The paper presents some of the recent results of the MAT measurement performed on specially prepared series of cast iron samples. Results of the non-destructive magnetic tests were compared with the destructive mechanical measurements of Brinell hardness and linear correlation was found between them. A very good correlation was also found between magnetic descriptors and conductivity and chill/ferrite area fraction. Based on these results, Magnetic Adaptive Testing is suggested as a highly promising non-destructive method for monitoring structural changes in different types of ferromagnetic materials.

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22

Taguchi, Ryo, Kohei Kuwahara, Norihisa Akamatsu, and Atsushi Shishido. "Quantitative analysis of bending hysteresis by real-time monitoring of curvature in flexible polymeric films." Soft Matter 17, no. 15 (2021): 4040–46. http://dx.doi.org/10.1039/d0sm02233k.

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The measurement of bending curvature of polymer films characterised the bending hysteresis as a precursor phenomenon of fracture and fatigue. The measurement also enables us to predict the occurrence of bending hysteresis.

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23

Shah, Syed Afaq Ali, Muhammad Hassan Sayyad, Jinghua Sun, and Zhongyi Guo. "Hysteresis Analysis of Hole-Transport-Material-Free Monolithic Perovskite Solar Cells with Carbon Counter Electrode by Current Density–Voltage and Impedance Spectra Measurements." Nanomaterials 11, no. 1 (December 27, 2020): 48. http://dx.doi.org/10.3390/nano11010048.

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Due to the tremendous increase in power conversion efficiency (PCE) of organic–inorganic perovskite solar cells (PSCs), this technology has attracted much attention. Despite being the fastest-growing photovoltaic technology to date, bottlenecks such as current density–voltage (J–V) hysteresis have significantly limited further development. Current density measurements performed with different sweep scan speeds exhibit hysteresis and the photovoltaic parameters extracted from the current density–voltage measurements for both scan directions become questionable. A current density–voltage measurement protocol needs to be established which can be used to achieve reproducible results and to compare devices made in different laboratories. In this work, we report a hysteresis analysis of a hole-transport-material-free (HTM-free) carbon-counter-electrode-based PSC conducted by current density–voltage and impedance spectra measurements. The effect of sweep scan direction and time delay was examined on the J–V characteristics of the device. The hysteresis was observed to be strongly sweep scan direction and time delay dependent and decreased as the delay increased. The J–V analysis conducted in the reverse sweep scan direction at a lower sweep time delay of 0.2 s revealed very large increases in the short circuit current density and the power conversion efficiency of 57.7% and 56.1%, respectively, compared with the values obtained during the forward scan under the same conditions. Impedance spectroscopy (IS) investigations were carried out and the effects of sweep scan speed, time delay, and frequency were analyzed. The hysteresis was observed to be strongly sweep scan direction, sweep time delay, and frequency dependent. The correlation between J–V and IS data is provided. The wealth of photovoltaic and impendence spectroscopic data reported in this work on the hysteresis study of the HTM-free PSC may help in establishing a current density–voltage measurement protocol, identifying components and interfaces causing the hysteresis, and modeling of PSCs, eventually benefiting device performance and long-term stability.

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24

Chen, Dong Xia, Ma Xiu Zhang, You Qiang Lin, and Jian Ni. "Measurement of SWCC of Xiamen Residual Soil by Filter Paper." Applied Mechanics and Materials 256-259 (December 2012): 1046–51. http://dx.doi.org/10.4028/www.scientific.net/amm.256-259.1046.

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Soil suction is one of the most important parameters for unsaturated soils. An experimental program was carried out to measure the maric suction of soil specimens of a residual soil in Xiamen by filter paper method. Initial water content, soil structure, and stress state were taken into account to investigate the hysteresis loop of SWCC. The air-entry value of test soil is about 140kPa and residual saturation is about 18%. The soil specimen at wet of optimum has the largest hysteresis loop for a relatively uniform pore-size distribution. However, the soil specimen at dry of optimum has the smallest hysteresis loop. The soil specimen at optimum lies between them. For specimens subjected to different stress states under various applied loads, the higher the applied load on the specimen, the smaller the size of hysteresis loop. In drying or wetting process, there is a significant difference in matric suction though soil specimens are at same water content. Therefore, for this kind of soil, it should be attention that the shear strength may be greatly reduced during rainstorms.

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25

Rojas, Juan D., Diego A. Arias, and Alvaro Mariño. "LEVITATION AND SUSPENSION FORCES MEASUREMENT SYSTEM FOR HIGH TC SUPERCONDUCTORS." MOMENTO, no. 60 (January 19, 2020): 55–66. http://dx.doi.org/10.15446/mo.n60.84228.

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The interaction forces, attraction (suspension) and repulsion (levitation) between a permanent magnet and diferent bulk Yttrium-based superconductors were carried out with an automatic system developed in our group, which is reproducible, reliable and low cost. Two superconducting samples of YBa2Cu3O7-δ (YBCO) prepared by solid-state reaction method (S) and by the melt-textured growth method (MTG) were used. Both samples were characterized by XRD technique and presented the characteristic peaks and intensity relations of the YBCO-123 superconducting phase. Oxygen deficiencies δ > 0,15 and δ < 0,10 for the S and MTG samples respectively, were observed. Both samples displayed diferent hysteresis behavior in the Force (F) vs. Distance (z) measurements when they were field cooled (FC) and zero field cooled (ZFC). This behavior agrees with hysteresis loops observed in magnetization measurements. Both levitation and suspension phenomena were observed in the MTG sample with large hysteresis loops of the force. On the contrary, the S sample with small hysteresis loops did not show a suspension force, only displayed a slight levitation force.

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26

Chady, Tomasz, and Ryszard Łukaszuk. "Examining Ferromagnetic Materials Subjected to a Static Stress Load Using the Magnetic Method." Materials 14, no. 13 (June 22, 2021): 3455. http://dx.doi.org/10.3390/ma14133455.

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This paper discusses the experimental examination of anisotropic steel-made samples subjected to a static stress load. A nondestructive testing (NDT) measurement system with a transducer, which enables observation of local hysteresis loops and detection of samples’ inhomogeneity, is proposed. Local hysteresis loops are measured on two perpendicular axes, including one parallel to the rolling direction of the samples. The results confirm that the selected features of the local hysteresis loops provide important information about the conditions of ferromagnetic materials. Furthermore, it is shown that the selected parameters of the statistical analysis of the achieved measurements are beneficial for evaluating stress and fatigue changes induced in the material.

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27

Sims, Joseph D., and Hugh W. Coleman. "Hysteresis Effects on Thrust Measurement and its Uncertainty." Journal of Propulsion and Power 19, no. 3 (May 2003): 506–13. http://dx.doi.org/10.2514/2.6135.

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28

Kuczmann, Miklós. "Arbitrary flux waveform generation in scalar hysteresis measurement." Pollack Periodica 2, no. 3 (December 2007): 3–14. http://dx.doi.org/10.1556/pollack.2.2007.3.1.

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29

Kuczmann, Miklós. "Vector Preisach hysteresis modeling: Measurement, identification and application." Physica B: Condensed Matter 406, no. 8 (April 2011): 1403–9. http://dx.doi.org/10.1016/j.physb.2011.01.037.

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30

MIZUNO, Takeshi, Takahiro ADACHI, Masaya TAKASAKI, and Yuji ISHINO. "Mass Measurement System Using Relay Feedback with Hysteresis." Journal of System Design and Dynamics 2, no. 1 (2008): 188–96. http://dx.doi.org/10.1299/jsdd.2.188.

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31

Sullivan-Mee, Michael, Suchitra Katiyar, Denise Pensyl, Kathy D. Halverson, and Clifford Qualls. "Relative Importance of Factors Affecting Corneal Hysteresis Measurement." Optometry and Vision Science 89, no. 5 (May 2012): E803—E811. http://dx.doi.org/10.1097/opx.0b013e3182504214.

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32

Nowicki, Michał, Roman Szewczyk, Tomasz Charubin, Andriy Marusenkov, Anton Nosenko, and Vasyl Kyrylchuk. "Modeling the Hysteresis Loop of Ultra-High Permeability Amorphous Alloy for Space Applications." Materials 11, no. 11 (October 24, 2018): 2079. http://dx.doi.org/10.3390/ma11112079.

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This paper presents investigation results regarding the Jiles-Atherton-based hysteresis loop modeling of ultra-high permeability amorphous alloy MELTA® MM-5Co. The measurement stand is capable of accurately measuring minor and major hysteresis loops for such a material together with exemplary measurement results. The main source of the measurement error is highlighted, which includes the Earth’s field influence. The results of hysteresis loop modeling with the original Jiles-Atherton model and with two of its modifications are given. In all cases, the parameters of the Jiles-Atherton model were identified in two-step identification on the basis of a differential evolution optimization algorithm. The results indicate that both the original and modified Jiles-Atherton models are suitable for modeling the ultra-soft amorphous alloy. However, the hysteresis model’s parameters vary significantly.

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33

Lange, Manfred, Dennis van Vörden, and Rolf Möller. "A measurement of the hysteresis loop in force-spectroscopy curves using a tuning-fork atomic force microscope." Beilstein Journal of Nanotechnology 3 (March 8, 2012): 207–12. http://dx.doi.org/10.3762/bjnano.3.23.

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Measurements of the frequency shift versus distance in noncontact atomic force microscopy (NC-AFM) allow measurements of the force gradient between the oscillating tip and a surface (force-spectroscopy measurements). When nonconservative forces act between the tip apex and the surface the oscillation amplitude is damped. The dissipation is caused by bistabilities in the potential energy surface of the tip–sample system, and the process can be understood as a hysteresis of forces between approach and retraction of the tip. In this paper, we present the direct measurement of the whole hysteresis loop in force-spectroscopy curves at 77 K on the PTCDA/Ag/Si(111) √3 × √3 surface by means of a tuning-fork-based NC-AFM with an oscillation amplitude smaller than the distance range of the hysteresis loop. The hysteresis effect is caused by the making and breaking of a bond between PTCDA molecules on the surface and a PTCDA molecule at the tip. The corresponding energy loss was determined to be 0.57 eV by evaluation of the force–distance curves upon approach and retraction. Furthermore, a second dissipation process was identified through the damping of the oscillation while the molecule on the tip is in contact with the surface. This dissipation process occurs mainly during the retraction of the tip. It reaches a maximum value of about 0.22 eV/cycle.

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34

Hamid, Youssef, David A. Hutt, David C. Whalley, and Russell Craddock. "Relative Contributions of Packaging Elements to the Thermal Hysteresis of a MEMS Pressure Sensor." Sensors 20, no. 6 (March 19, 2020): 1727. http://dx.doi.org/10.3390/s20061727.

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Piezoresistive silicon pressure sensor samples were thermally cycled after being consecutively packaged to three different levels. These started with the absolute minimum to allow measurement of the output and with each subsequent level incorporating additional packaging elements within the build. Fitting the data to a mathematical function was necessary both to correct for any testing uncertainties within the pressure and temperature controllers, and to enable the identification and quantification of any hysteresis. Without being subjected to any previous thermal preconditioning, the sensors were characterized over three different temperature ranges and for multiple cycles, in order to determine the relative contributions of each packaging level toward thermal hysteresis. After reaching a stabilised hysteretic behaviour, 88.5% of the thermal hysteresis was determined to be related to the bond pads and wire bonds, which is likely to be due to the large thermal mismatch between the silicon and bond pad metallisation. The fluid-fill and isolation membrane contributed just 7.2% of the total hysteresis and the remaining 4.3% was related to the adhesive used for attachment of the sensing element to the housing. This novel sequential packaging evaluation methodology is independent of sensor design and is useful in identifying those packaging elements contributing the most to hysteresis.

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35

Yamin, Sumera. "Development of measurement frame for detailed measurements of hysteresis cycles of ferromagnetic sheets." Measurement 60 (January 2015): 25–32. http://dx.doi.org/10.1016/j.measurement.2014.09.074.

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36

Hassani, Vahid, Tegoeh Tjahjowidodo, and Albert D. Soetarto. "Modeling Hysteresis with Inertial-Dependent Prandtl-Ishlinskii Model in Wide-Band Frequency-Operated Piezoelectric Actuator." Smart Materials Research 2012 (January 24, 2012): 1–15. http://dx.doi.org/10.1155/2012/164062.

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One of the major problems occurring in many technical applications is the presence of the hysteretic behavior in sensors and actuators, which causes a nonlinear relationship between input and output variables in such devices. Since the nonlinear phenomenon of hysteresis degrades the performance of the piezoelectric materials and piezoelectric drive mechanisms, for example, in positioning control framework, it has to be characterized in order to mitigate the effect of the nonlinearity in the devices. This paper is aimed to characterize and model the hysteresis in typical piezoelectric actuators under load-free and preloaded circumstances incorporating the inertial effect of the system. For this purpose, the piezoelectric actuator is modeled as a mass-spring-damper system, which is expressed in terms of a stop operator as one of the essential yet efficient hysteresis operators in the Prandtl-Ishlinskii (PI) model. The reason of utilizing the stop operator in this study is for the sake of control purposes, as the stop operator plays as the inverse of the play operator in the PI model and can be used in a feed-forward controller scheme to suppress the effect of hysteresis in general control framework. The results reveal that this model exhibits better correspondence to the measurement output compared to that of the classical PI model.

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37

Sergienko, N., and I. Shargorodskaya. "Intraocular pressure as a factor affecting corneal hysteresis measurement." Oftalmologicheskii Zhurnal 31, no. 3 (May 11, 2011): 13–15. http://dx.doi.org/10.31288/oftalmolzh201131315.

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38

Li, Z., Z. Y. Li, X. M. Cheng, F. Jin, and Z. X. Huang. "Measurement of MOKE Hysteresis Loop Using Non-uniform Sampling." Transactions of the Magnetics Society of Japan 4, no. 4-2 (2004): 301–3. http://dx.doi.org/10.3379/tmjpn2001.4.301.

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39

Kuczmann, Miklos. "Numerical analysis of a 2D vector hysteresis measurement system." Pollack Periodica 2, no. 1 (April 2007): 17–26. http://dx.doi.org/10.1556/pollack.2.2007.1.2.

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40

Mohammadi Fathabad, Sobhan, and Farzad Shahri. "BH hysteresis measurement system for thin soft magnetic materials." Measurement 172 (February 2021): 108896. http://dx.doi.org/10.1016/j.measurement.2020.108896.

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41

Bostanci, Umut, M. Kurtuluş Abak, O. Aktaş, and A. Dâna. "Nanoscale charging hysteresis measurement by multifrequency electrostatic force spectroscopy." Applied Physics Letters 92, no. 9 (March 3, 2008): 093108. http://dx.doi.org/10.1063/1.2888765.

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42

Laval, Jorge A. "Hysteresis in traffic flow revisited: An improved measurement method." Transportation Research Part B: Methodological 45, no. 2 (February 2011): 385–91. http://dx.doi.org/10.1016/j.trb.2010.07.006.

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43

Hauser, H., P. L. Fulmek, and R. Grössinger. "Hysteresis modeling and measurement for two-dimensional particle assemblies." Journal of Magnetism and Magnetic Materials 242-245 (April 2002): 1067–69. http://dx.doi.org/10.1016/s0304-8853(01)01351-8.

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44

Garshelis, Ivan J., Stijn P. L. Tollens, Ryan J. Kari, Lode P. Vandenbossche, and Luc R. Dupré. "Drag force measurement: A means for determining hysteresis loss." Journal of Applied Physics 99, no. 8 (April 15, 2006): 08D910. http://dx.doi.org/10.1063/1.2172583.

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45

Cheng, Xiangyang, Florian Weyland, Nikola Novak, and Yingwei Li. "Indirect Electrocaloric Evaluation: Influence of Polarization Hysteresis Measurement Frequency." physica status solidi (a) 216, no. 24 (November 19, 2019): 1900684. http://dx.doi.org/10.1002/pssa.201900684.

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46

Lenhard, R. J. "Measurement and modeling of three-phase saturation-pressure hysteresis." Journal of Contaminant Hydrology 9, no. 3 (March 1992): 243–69. http://dx.doi.org/10.1016/0169-7722(92)90007-2.

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47

Lee, Hye Jin, Nak Kyu Lee, Hyoung Wook Lee, Hoon Jae Park, and Tae Hoon Choi. "Nano Scale Material Property Measurement of MEMS Material Using Piezo Actuated Material Testing Machine." Materials Science Forum 510-511 (March 2006): 734–37. http://dx.doi.org/10.4028/www.scientific.net/msf.510-511.734.

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Abstract:

Many micro technology researches have been concentrated in the field of materials and a process field. But the properties of micro materials should be understood to give still more advanced results. Among the various material properties, mechanical material properties such as tensile strength, elastic modulus, etc., is the basic property. To measure mechanical properties in micro or nano scale, actuating must be very precise. Piezo is a famous actuator, frequently used to measure very precise mechanical properties in micro research field. But piezo has a nonlinearity called hysteresis. Not precision result is caused because of this hysteresis property in piezo actuator. Therefore feedback control method is used in many researches to prevent this hysteresis of piezo actuator. Feedback control method produces a good result in processing view, but causes a loss in a resolution view. In this paper, hysteresis is compensated by using an open loop control method. To apply the open loop control method to piezo actuated nano scale material testing machine, hysteresis property is modeled in a mathematical function, and a compensated control input is constructed using inverse function of original data. The reliability of this control method can be confirmed by testing nickel, aluminum, and copper micro thin foil that is used in MEMS material broadly. If these MEMS material properties are used in a MEMS research field, more economical and high performance MEMS materials can be obtained.

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Wang, Ding-Yeong, and Chun-Yen Chang. "Switching Current Study: Hysteresis Measurement of Ferroelectric Capacitors using Current–Voltage Measurement Method." Japanese Journal of Applied Physics 44, no. 4A (April 8, 2005): 1857–61. http://dx.doi.org/10.1143/jjap.44.1857.

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Huang, Dong Yan, Bing Han, Tian Li Hu, Zong Gang Wang, and Tao Zhang. "Measurement of Hysteresis Loop by Using Pulsed Magnetic Field in LabView Environment." Applied Mechanics and Materials 121-126 (October 2011): 4028–32. http://dx.doi.org/10.4028/www.scientific.net/amm.121-126.4028.

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Abstract:

An apparatus for in situ measuring the hysteresis of magnetic materials by using pulsed magnetic field is structured. The samples were locally magnetized to saturation by the pulsed magnetic field. The pulsed field is generated by the discharge of a capacitor over the magnetizing coil. The measurement has been developed in LabView environment using National Instrument Data Acquisition Cards. The hysteresis loops of Q235 steel samples under various compressive stresses are presented.

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Kuczmann, Miklós. "Simulation of a vector hysteresis measurement system taking hysteresis into account by the vector Preisach model." Physica B: Condensed Matter 403, no. 2-3 (February 2008): 433–36. http://dx.doi.org/10.1016/j.physb.2007.08.068.

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