Constant rate of change of magnetization hysteresis loop tracer

1991 ◽  
Vol 69 (8) ◽  
pp. 5100-5102 ◽  
Author(s):  
R. Cammarano ◽  
R. Street ◽  
P. G. McCormick ◽  
M. E. Evans
Keyword(s):  
Hysteresis Loop ◽  
Rate Of Change ◽  
Magnetization Hysteresis ◽  
Constant Rate ◽  
Magnetization Hysteresis Loop

scholarly journals Distinction of Consciousness Fields According to Taheri from Other Conventional Physical Fields: Evaluating the Magnetic Properties of Materials

2021 ◽  
Author(s):  
Mohammad Ali Taheri ◽  
Firouz Payervand ◽  
Farzad Ahmadkhanlou ◽  
Sara Torabi ◽  
Farid Semsarha
Keyword(s):  
Magnetic Field ◽  
Magnetic Properties ◽  
Hysteresis Loop ◽  
Standard Laboratory ◽  
Laboratory Conditions ◽  
Magnetization Hysteresis ◽  
Magnetization Hysteresis Loop ◽  
Properties Of Materials ◽  
Physical Fields

Abstract Magnetization hysteresis loop provides important information about the magnetic properties of materials. In this study, by examining the magnetic properties of three paramagnetic and diamagnetic materials in the vicinity of the Consciousness Fields (three types 1,2 and 3), we have investigated the nature of the Consciousness Fields in comparison with magnetic field. The magnetic properties of the materials under the influence of three distinct Consciousness Fields have changed significantly. Furthermore, the Consciousness Field 1 of the present study (with originally named Consciousness Bond Field by Taheri) has changed the magnetic properties of materials toward their physically inherent state in standard laboratory conditions. Based on the conditions and the results of the present study, it can be concluded that the Consciousness Fields are inherently neither electric nor magnetite fields and have a completely different and distinct impact on materials and their properties.

scholarly journals Distinction of Consciousness Fields According to Taheri from Other Conventional Physical Fields: Evaluating the Magnetic Properties of Materials

2021 ◽  
Author(s):  
Mohammad Ali Taheri ◽  
Forouz Payervand ◽  
Farzad Ahmadkhanlou ◽  
Sara Torabi ◽  
Farid Semsarha
Keyword(s):  
Magnetic Field ◽  
Magnetic Properties ◽  
Hysteresis Loop ◽  
Standard Laboratory ◽  
Laboratory Conditions ◽  
Magnetization Hysteresis ◽  
Magnetization Hysteresis Loop ◽  
Properties Of Materials ◽  
Physical Fields

Abstract Magnetization hysteresis loop provides important information about the magnetic properties of materials. In this study, by examining the magnetic properties of three paramagnetic and diamagnetic materials in the vicinity of the Consciousness Fields (three types 1,2 and 3), we have investigated the nature of the Consciousness Fields in comparison with magnetic field. The magnetic properties of the materials under the influence of three distinct Consciousness Fields have changed significantly. Furthermore, the Consciousness Field 1 of the present study (with originally named Faradarmani by Taheri) has changed the magnetic properties of materials toward their physically inherent state in standard laboratory conditions. Based on the conditions and the results of the present study, it can be concluded that the Consciousness Fields are inherently neither electric nor magnetite fields and have a completely different and distinct impact on materials and their properties.

Origin of peak effect in the magnetization hysteresis loop of melt-processed REBa2Cu3Oy superconductors

1997 ◽  
Vol 71 (26) ◽  
pp. 3895-3897 ◽  
Author(s):  
N. V. N. Viswanath ◽  
T. Rajasekharan ◽  
Latika Menon ◽  
N. Harish Kumar ◽  
S. K. Malik ◽  
...  
Keyword(s):  
Hysteresis Loop ◽  
Peak Effect ◽  
Magnetization Hysteresis ◽  
Magnetization Hysteresis Loop

scholarly journals Distinction of Consciousness Fields According to Taheri from Other Conventional Physical Fields: Evaluating the Magnetic Properties of Materials

2021 ◽  
Author(s):  
Mohammad Taheri ◽  
Forouz Payervand ◽  
Farzad Ahmadkhanlou ◽  
Sara Torabi ◽  
Farid Semsarha
Keyword(s):  
Magnetic Field ◽  
Magnetic Properties ◽  
Hysteresis Loop ◽  
Standard Laboratory ◽  
Laboratory Conditions ◽  
Magnetization Hysteresis ◽  
Magnetization Hysteresis Loop ◽  
Properties Of Materials ◽  
Physical Fields

Abstract Magnetization hysteresis loop provides important information about the magnetic properties of materials. In this study, by examining the magnetic properties of three paramagnetic and diamagnetic materials in the vicinity of the Consciousness Fields (three types 1,2 and 3), we have investigated the nature of the Consciousness Fields in comparison with magnetic field. The magnetic properties of the materials under the influence of three distinct Consciousness Fields have changed significantly. Furthermore, the Consciousness Field 1 of the present study (with originally named Faradarmani by Taheri) has changed the magnetic properties of materials toward their physically inherent state in standard laboratory conditions. Based on the conditions and the results of the present study, it can be concluded that the Consciousness Fields are inherently neither electric nor magnetite fields and have a completely different and distinct impact on materials and their properties.

Fast-phase transvascular fluid flux and the Fahraeus effect

1987 ◽  
Vol 62 (4) ◽  
pp. 1513-1520 ◽  
Author(s):  
W. N. Richardson ◽  
D. Bilan ◽  
M. Hoppensack ◽  
L. Oppenheimer
Keyword(s):  
Mechanical Properties ◽  
Slow Rate ◽  
Time Course ◽  
Rate Of Change ◽  
Distributed Model ◽  
Slow Phase ◽  
Fluid Flux ◽  
Fast Phase ◽  
Constant Rate ◽  
Fahraeus Effect

Transvascular fluid flux was induced in six isolated blood-perfused canine lobes by increasing and decreasing hydrostatic inflow pressure (Pi). Fluid flux was followed against the change in concentration of an impermeable tracer (Blue Dextran) measured directly with a colorimetric device. The time course of fluid flux was biphasic with an initial fast transient followed by a slow phase. Hematocrit changes unrelated to fluid flux occurred due to the Fahraeus effect, and their contribution to the total color signal was subtracted to determine the rate of fast fluid flux (Qf). Qf was related to Pi to derive fast-phase conductance (Kf). Slow-phase Kf was calculated from the constant rate of change of lobe weight. For a mean change in Pi of 7 cmH2O, 40% of the color signal was due to fluid flux. Fast- and slow-phase Kf's were 0.86 +/- 0.15 and 0.27 +/- 0.05 ml X min-1. cmH2O–1 X 100 g dry wt-1. The fast-phase Kf is smaller than that reported for plasma-perfused lobes. Possible explanations discussed are the nature of the perfusate, the mechanical properties of the interstitium, and the slow rate of rise of the driving pressure at the filtration site on the basis of a distributed model of pulmonary vascular compliance.

Origin and Geomorphology

2006 ◽  
Author(s):  
Thomas S. Bianchi
Keyword(s):  
Sea Level ◽  
Rate Of Change ◽  
Interglacial Period ◽  
Continental Margins ◽  
Before Present ◽  
Sea Level Changes ◽  
The Past ◽  
Constant Rate ◽  
Geologic Record ◽  
The U.S

Geologically speaking, estuaries are ephemeral features of the coasts. Upon formation, most begin to fill in with sediments and, in the absence of sea level changes, would have life spans of only a few thousand to tens of thousands of years (Emery and Uchupi, 1972; Schubel, 1972; Schubel and Hirschberg, 1978). Estuaries have been part of the geologic record for at least the past 200 million years (My) BP (before present; Williams, 1960; Clauzon, 1973). However, modern estuaries are recent features that only formed over the past 5000 to 6000 years during the stable interglacial period of the middle to late Holocene epoch (0–10,000 y BP), which followed an extensive rise in sea level at the end of the Pleistocene epoch (1.8 My to 10,000 y BP; Nichols and Biggs, 1985). There is general agreement that four major glaciation to interglacial periods occurred during the Pleistocene. It has been suggested that sea level was reduced from a maximum of about 80 m above sea level during the Aftoninan interglacial to 100 m below sea level during the Wisconsin, some 15,000 to 18,000 y BP (figure 2.1; Fairbridge, 1961). This lowest sea level phase is referred to as low stand and is usually determined by uncovering the oldest drowned shorelines along continental margins (Davis, 1985, 1996); conversely, the highest sea level phase is referred to as high stand. It is generally accepted that low-stand depth is between 130 and 150 m below present sea level and that sea level rose at a fairly constant rate until about 6000 to 7000 y BP (Belknap and Kraft, 1977). A sea level rise of approximately 10 mm y−1 during this period resulted in many coastal plains being inundated with water and a displacement of the shoreline. The phenomenon of rising (transgression) and falling (regression) sea level over time is referred to as eustacy (Suess, 1906). When examining a simplified sea level curve, we find that the rate of change during the Holocene is fairly representative of the Gulf of Mexico and much of the U.S. Atlantic coastline (Curray, 1965).

Factors Influencing the Rate-of-Pickling Test on Tin-Plate Steel★

CORROSION ◽  
1959 ◽  
Vol 15 (3) ◽  
pp. 51-56 ◽  
Author(s):  
R. M. HUDSON ◽  
G. L. STRAGAND
Keyword(s):  
Weight Loss ◽  
Corrosion Resistance ◽  
Steel Surface ◽  
Lag Time ◽  
Rate Of Change ◽  
Surface Layers ◽  
Experimental Conditions ◽  
Constant Rate ◽  
High Concentrations ◽  
Future Work

Abstract “Lag time” is a measure of the time of pickling necessary to produce a constant rate of weight loss from steel immersed in acid. This measurement has been used as a guide for improving the corrosion resistance of commercial electrolytic tin plate. It is determined by measuring either the rate of change of weight loss, hydrogen evolution, or corroding potential of a specimen in 6N hydrochloric acid at 90 C (194 F.) The lag time depends on surface effects inasmuch as removing the surface layers of steel by abrasion or by pickling destroys the lag. The influence of box-annealing atmospheres, cleanliness of steel, and time-temperature cycles on lag time have been investigated, and the complexity of these effects has been demonstrated. Explanations in terms of oxidation or decarburization of the steel surface during annealing are not feasible for the development of lag time under all the experimental conditions studied. Preliminary data demonstrating the high concentrations of certain elements on the steel surface before annealing, and the enrichment of the surface layer by some of these elements during annealing, are suggested as particularly promising areas for future work. In this way lag time phenomena in tin-plate steels may be better understood and further improvement in tin-plate corrosion resistance can be made. 2.3.4

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