Modeling of strain kinetics of damping viscoelastic magnetically controlled materials in creep mode

2019 ◽  
Vol 31 (2) ◽  
pp. 243-252
Author(s):  
Evguenia V Korobko ◽  
Mikalai A Zhurauski ◽  
Buhe Bateer ◽  
Zoya A Novikova ◽  
Vladimir A Kuzmin

The results of experimental studies of strain kinetics of composite magnetically controlled materials in the creep mode with preliminary exposure and without exposure are described by the Burgers model with two elastic and two viscous parameters, which is a combination of viscoelastic Kelvin–Voigt and Maxwell models connected in series. The dependence of the model parameters on the magnetic field induction is determined. The values of elastic and viscous parameters increase with increasing magnetic field induction in the range up to 500 mT by one or two orders of magnitude. It was determined that the value of the viscous Maxwell parameter does not change after preliminary exposure in the field. The values of the other two elastic and viscous Kelvin–Voigt parameters increase with exposure in a magnetic field.

1996 ◽  
Vol 10 (23) ◽  
pp. 1141-1149 ◽  
Author(s):  
CHOON-LIN HO ◽  
V.R. KHALILOV ◽  
CHI YANG

We obtain the equations that define the equilibrium of a homogeneous relativistic gas of neutrons, protons and electrons in a constant magnetic field as applied to the conditions that probably occur near the center of neutron stars. We compute the relative densities of the particles at equilibrium and the Fermi momentum of electrons in the strong magnetic field as function of the density of neutrons and the magnetic field induction. Novel features are revealed as to the ratio of the number of protons to the number of neutrons at equilibrium in the presence of large magnetic fields.


Author(s):  
Александр Николаевич Болотов ◽  
Ольга Олеговна Новикова

Работа направлена на создание магнитометрического прибора для точного определения намагниченности насыщения магнитных наножидкостей и подобных по свойствам функциональных дисперсных материалов. В основе прибора лежит магнитометрический метод с холловскими преобразователями индукции, усовершенствованный с учетом особенностей физико-механических свойств жидкостей. Измерительная магнитная система прибора построена таким образом, чтобы с помощью постоянных магнитов можно было создавать однородное намагничивающее поле величиной до (2 ÷ 4)⋅10 А/м в рабочем зазоре, где установлена кювета с изучаемой магнитной наножидкостью. Под кюветой с магнитной наножидкостью в среднем ее сечении располагается преобразователь Холла, который служит для измерения напряженности намагничивающего магнитного поля. Второй преобразователь Холла, предназначенный для измерения индукции магнитного поля в веществе, установлен в канавке прямоугольного сечения и располагается по центру магнитной наножидкости в кювете. Относительная ошибка измерения намагниченности на приборе не превышала 2 % для магнитных наножидкостей с намагниченностью в диапазоне от 10 кА/м до 50 кА/м. Созданный прибор может использоваться для экспресс - измерений в лабораторных и промышленных условиях и не требует специальных профессиональных навыков. Показано, что аддитивная составляющая инструментальной погрешности измерений зависит от значений остаточного напряжения (ЭДС неэквипотенциальности), побочных гальваномагнитных эффектов и термо-ЭДС измерительного преобразователя. Мультипликативная составляющая связана с временной и температурной нестабильностью коэффициента преобразования и тока или напряжения питания. Методическая погрешность магнитометра вызвана тем, что для измерений индукции магнитного поля используется не полностью замкнутая магнитная цепь. Показано, что по своим метрологическим параметрам прибор отвечает международным стандартам на магнитные измерения магнитомягких материалов. Прибор позволил определить намагниченность коллоидных систем в магнитных полях начала парапроцессов, индивидуальную намагниченность наночастиц дисперсной фазы, агрегативную устойчивость коллоидов в магнитных и гравитационных полях, оценить размеры сольватной оболочки наночастиц. The work is aimed at creating a magnetometric device for accurate determining the saturation magnetization of magnetic nanofluids and similar properties of functional dispersed materials. The device is based on a magnetometric method with the Hall induction transducers, improved taking into account the peculiarities of the physical and mechanical properties of liquids. The measuring magnetic system of the device is designed in such a way that with the help of permanent magnets it is possible to create a uniform magnetizing field up to (2÷4)⋅10 A/m in a working gap where the cuvette with the studied magnetic nanofluid is installed. Under the cuvette with a magnetic nanofluid in its middle section is a Hall Converter, which serves to measure the strength of the magnetizing magnetic field. The second Hall Converter, designed to measure the magnetic field induction in a substance, is installed in a rectangular groove and is located in the center of the magnetic nanofluid in the cuvette. The relative error of measuring the magnetization on the device did not exceed 2% for magnetic nanofluids with a magnetization in the range from 10 kA/m to 50 kA/m. The created device can be used for Express measurements in laboratory and industrial conditions and does not require special professional skills. It is shown that the additive component of the instrumental measurement error depends on the values of the residual voltage (nonequipotential EMF), side galvanomagnetic effects and thermo - EMF of the measuring Converter. The multiplicative component is related to the time and temperature instability of the conversion coefficient and the current or voltage supply. The methodic error of the magnetometer is caused by the fact that not a fully closed magnetic circuit is used for measuring the magnetic field induction. It is shown that the device meets international standards for magnetic measurements of soft magnetic materials in terms of their metrological parameters. The device allowed us to determine the magnetization of colloidal systems in magnetic fields of a start paraprocess, individual magnetization of nanoparticles of the dispersed phase, the aggregative stability of colloids in magnetic and gravity fields to estimate the size of the solvation shell of the nanoparticles.


2017 ◽  
Vol 1143 ◽  
pp. 247-252 ◽  
Author(s):  
Petrica Eduard Chirila ◽  
Ionel Chirica ◽  
Elena Felicia Beznea

Magnetorheological elastomers (MREs) are a kind of smart materials, which change the mechanical properties (viscoelastic characteristics) under the magnetic field action. In the paper the determination of damping properties (reactive force) of specimens made out of magnetorheological elastomers is presented. The specimens made out of MREs have been fabricated as a composite with matrix made out of silicone rubber with certain contents of magnetisable particles (carbonyl iron powder). The cylindrical specimens have been tested in compression loading, controlled by an electro-mechanic system. The MRE characteristics of the specimens have been determined in the presence of a magnetic field produced with an electromagnet (coil device). The reactive force occurring in the MRE specimen has been determined on the basis of the measured data during loading. The variation curves of the reactive force versus magnetic field induction are drawn. As a conclusion, the rigidity of the MRE specimen is increasing since the magnitude of the magnetic field induction is increasing.


2006 ◽  
Vol 980 ◽  
Author(s):  
Tomoyuki Kakeshita ◽  
Takashi Fukuda

AbstractMagnetic field has been known to be effective in solidification processes. Recently, however, it has been revealed that the magnetic field is also effective for controlling the arrangement of variants, which are formed in association with a solid-solid transformation, in some ferromagnetic intermetallic-based alloys with a large magnetocrystalline anisotropy. In this presentation, we will show two of such cases: one is the rearrangement of martensite variants by magnetic field in intermetallic-based ferromagnetic shape memory alloys (Ni2MnGa and Fe3Pt), and the other is formation of mono-variant state by ordering heat-treatment under magnetic field in a L10-type CoPt. The former process is diffusionless and proceeds by the movement of twinning plane under a magnetic field. The latter is a diffusion controlled process. For both the cases, a large magnetocrystalline anisotropy is essentially important for controlling the arrangement of variants, although kinetics of the two processes is quite different each other.


Author(s):  
Igor V. Belitsyn

The article considers inductive interference components. A description of the induced voltage electromagnetic component is described in detail. The technique of the calculated wire suspension height determining based on the actual magnetic field distribution is presented. The technique for the number of power line spans determining is provided. Dependences of the magnetic field induction vector on the distance along one power line’s span are obtained. Relationships of the magnetic field induction determining error depending on the number of adjacent spans are obtained. Recommendations for the number of spans determining, which must be taken into account when evaluating the magnetic component of the power line electromagnetic field are given


2006 ◽  
Vol 15 (06) ◽  
pp. 1263-1271 ◽  
Author(s):  
A. SOYLU ◽  
O. BAYRAK ◽  
I. BOZTOSUN

In this paper, the energy eigenvalues of the two dimensional hydrogen atom are presented for the arbitrary Larmor frequencies by using the asymptotic iteration method. We first show the energy eigenvalues for the case with no magnetic field analytically, and then we obtain the energy eigenvalues for the strong and weak magnetic field cases within an iterative approach for n=2-10 and m=0-1 states for several different arbitrary Larmor frequencies. The effect of the magnetic field on the energy eigenvalues is determined precisely. The results are in excellent agreement with the findings of the other methods and our method works for the cases where the others fail.


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