Empirically, it was found that the energy of the gap between the silver layer and the glass is 100 N. It may follow from this that the sum of the rupture forces between the solder and the terminal, as well as between the solder and the silver layer, is less than this value, since if it were greater than or equal to this value, the terminal itself would have sufficient force to carry the entire system with it when it breaks. But it is also clear that for rupture, that is, for deformation by the elastic force (3.2.1), where stiffness is determined through the Youngs modulus (3.2.2), its energy is equal to the energy of destruction of the crystal lattice, that is, the product of the specific heat of melting and the amount of matter (3.2.3), is equal to the potential energy of deformation (3.2.4).
To determine the rupture force, which is already a priori the sum of the rupture forces between silver and solder, as well as between the terminal and solder, it is sufficient to use (3.2.5), where the distance is determined from the constancy of the area and the value of the volume change, which is calculated depending on the temperature (3.2.6), and from here the rupture force (3.2.7).
Now that the force of the rupture has been calculated, we can stop a little at the moment of pressing. From such a calculation, it became possible to determine that with a specific heat of 7.19 kJ/mol, with an amount of substance of the order of 0.0434 mol and 0.005149 grams and a density of the order of 7190 kg/m3, the area is 7.04424 *10-7 m2, with a side of 0.8393 mm, from which the temperature coefficient of 0.0042 K-1 is taken into account, with a resultant force of 99.99886267 N, that meets all the specified conditions.
Speaking of the pressing force, it can be noted that due to the attraction energy of the liquid flow of the alloy, it can be comparatively determined on the scale of the difference between the boundaries between the resulting force and the boundary force, from which a value of 0.001137328 N is obtained.
Used literature
1. Abdurakhmonov S. M., Sayitov S. S. Automated design for soldering the terminal of the rear window heating system of the car. Scientific-technical journal (STJ FerPI, FerPI ITJ, NTJ FerPI, 2021, Vol.23, special Issue No. 3), pp. 197-201.
2. Abdurakhmonov S. M., Sayitov G. S., Oshchepkova E. A., Rakhmonov D. H., Khuriboeva M. S. A new design for soldering the terminal of the rear window heating system the car. Current science. International Scientific Journal. Moscow, 2019 No. 9 (26), pp. 22-28.
3. Abdurakhmonov S. M., Sayitov S. S., Yuldasheva E. N. Automated soldering installation for terminal heating systems in auto-glass. Scientific-technical journal (STJ FerPI, FerPI ITJ, NTJ FerPI, 2021, Vol.25, No.6), pp. 256-259.
4. Abdurakhmonov S. M., Sayitov S. S. On the technology of soldering contact to heating systems of auto-glass // All sciences: international Scientific Journal. 2022. No.5, 2022. pp. 95-115.
5. Toyirov N. S., Kholikov A. A., Sayitov S. S. Energy saving when using hybrid solar power plants in the oil and gas industry // All sciences: International Scientific journal. 2022. 6, 2022. C. 253-260.
6. Akhmadzhonov A. E., Kholikov A. H., Sayitov S. S. Improving efficiency the use of thermal energy through the use of energy-efficient technologies at industrial enterprises // All Sciences: International Scientific Journal. 2022. 6, 2022. 387-396 S.
7. Abdurakhmonov S. M., Sayitov S. S. Avtovil oynalarini isitish tizimlariga terminal kavshirlash technologiyasi tugrisida //. All Sciences: International Scientific Journal. 2023. 2, 2023. C. 22-32.
8. Evgeny Konstantinov. Get out of the twilight // Science and Life. 2015. No. 11. pp. 112119.
GENERAL OVERVIEW OF THE DEVICE AND THE PHYSICAL COMPONENT OF A DC ELECTROMAGNET
UDC 621.318.3
Kholmatov Erkinjon Salievich
Lecturer of the Department of "Electronics and Instrumentation" of the Faculty of Computer Design Systems of the Fergana Polytechnic Institute
Ferghana Polytechnic Institute, Ferghana, Uzbekistan
Annotation. The use of a powerful force, obedient, easy to handle, which is applicable in a variety of cases, which illuminates, heats, drives machines as forces of the most powerful attraction is a very topical issue that requires very detailed consideration. Of course, the image of such a performance is precisely the electromagnetic design, the physics of which is built from the initial ideas about electromagnetism. There is also a large number of phenomena of this kind, each of which requires its own analysis in all parameters. This paper is devoted to the description of the algorithm created at the moment for such cases.
Keywords: electromagnet, magnetic field, magnetic induction vector, magnetic field inductance, conductor, magnetic field strength, solenoid, Maxwell equations for electromagnetism, electromagnetic induction.
Аннотация. Использование могущественной силы, послушной, простой в обращении, которая применима в самых различных случаях, которая освещает, отапливает, приводит в движение машины в качестве сил мощнейшего притяжения весьма актуальный вопрос, который требует весьма подробного рассмотрение. Разумеется, образом такого исполнения является именно электромагнитная конструкция, физика которой строиться от первоначальных представлений об электромагнетизме. Существует также большое количество явлений подобного рода, каждая из которых требует наличие своего разбора по всем параметрам. Описанию созданного на данный момент алгоритма для таких случаем и посвящена настоящая работа.
Ключевые слова: электромагнит, магнитное поле, вектор магнитное индукции, индуктивность магнитного поля, проводник, напряжённость магнитного поля, соленоид, уравнения Максвелла для электромагнетизма, электромагнитная индукция.
Initially, it is worth noting that the design of the electromagnet itself consists of a core and, most often, a metal wire, due to good electrical conductivity. This design itself is also similar to an elementary resistor or load, the function of which it can also perform, due to the determined resistance according to the regularity (1).
If we analyze the physics of this process, it turns out that in this case the charges begin to move, provided that it is a direct current, attracted by an electric field, which is created due to the potential difference at the output and input of the electromagnet winding. And after its resistance has been determined, and also provided that the flowing amount of charge (2) is known, it is possible to determine the passing current (3), where the velocity of the flying particles due to a correspondingly small potential difference, otherwise it would cause too strong an increase in temperature, is equal to the thermal velocity (5) for of the classical form and in (6) for the relativistic formulation, calculated in terms of energy (4).
And, accordingly, after that, it will be possible to come to the regularity of determining this magnitude of the potential difference, through the data obtained thanks to (710).
However, when using such a design, not only the elementary function of the resistor comes into play, but also something else. Any charge has some parameters, namely the value in Coulombs, as well as the magnitude of the electric field that it creates around itself. By itself, a charge a priori cannot create such a substance as a magnetic field, the proof of which will be given below, but it can be generated by an electric field. In a stationary state, a charge also has this property, and when a large number of charges in a conductor begin to move, they, by definition, both create and are subject to this very electric field. As a result, a vortex magnetic field is created around this very conductor.