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SU79651A1 - Differential electrodynamic system to determine the magnetic loss of ferromagnetic materials - Google Patents

Differential electrodynamic system to determine the magnetic loss of ferromagnetic materials

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Publication number
SU79651A1
SU79651A1 SU394449A SU394449A SU79651A1 SU 79651 A1 SU79651 A1 SU 79651A1 SU 394449 A SU394449 A SU 394449A SU 394449 A SU394449 A SU 394449A SU 79651 A1 SU79651 A1 SU 79651A1
Authority
SU
USSR - Soviet Union
Prior art keywords
differential
ferromagnetic materials
frame
magnetic loss
electrodynamic system
Prior art date
Application number
SU394449A
Other languages
Russian (ru)
Inventor
В.С. Дирацу
Т.В. Степнов
Original Assignee
В.С. Дирацу
Т.В. Степнов
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by В.С. Дирацу, Т.В. Степнов filed Critical В.С. Дирацу
Priority to SU394449A priority Critical patent/SU79651A1/en
Application granted granted Critical
Publication of SU79651A1 publication Critical patent/SU79651A1/en

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  • Measuring Magnetic Variables (AREA)
  • Investigating Or Analyzing Materials By The Use Of Magnetic Means (AREA)

Description

Известны дифференциальные приборы электродинамической системы дл  определени  магнитных лотерь ферромагнитных материалов нри перемагничивании.Differential electrodynamic system devices for determining magnetic lotteries of ferromagnetic materials during magnetic reversal are known.

Описываемый прибор отличаетс  от известных тем, что в нем подвижна  рамка образована из двух встречно включенных витков, внутрь одного из которых вкладываетс  эта.лонный образец, а внутрь др)того испытуемый.The described device differs from the known ones in that the movable frame is formed from two oppositely included turns, inside one of which is put this etalon sample, and the subject is inserted inside the other.

На фиг. 1 схематически изображен продольный разрез нрибора; на фиг. 2-три проекции подвижной рамки.FIG. 1 shows a schematic longitudinal section of the tool; in fig. 2-three projections of the moving frame.

Намагничивающа  катушка 1, расположенна  па эбонитовом каркасе , создает равномерное магнитное поле; катушка питаетс  переменным током 50 гц.The magnetizing coil 1, located on the ebony frame, creates a uniform magnetic field; the coil is powered by an alternating current of 50 Hz.

В поле катушки помеил,ены испытуемый образен. 2 и эталонный образец 3 из ферромагнитного .материа.ча, которые охватываютс  измериаельной рамкой 4.In the coil field, the subject is educated. 2 and reference sample 3 of ferromagnetic material. Which are covered by measuring frame 4.

Измерительна  рамка представл ет co6oii два удлиненных витка а и б, соединенные «восьмеркой, т. е. навстречу. «Восьмерка в месте скреншвани  витков согнута в виде 6yKiibi Y (в плане); место скрещивани  имеет изол цию. Испытуемый и эта.чониьп образцы проход т через соответствующие витки рамки. Рамка подвешена на металлической упругой нити 5 и экранирована от электростатического вли ни  намагничиваюн1ей катхшки 1 латунной тр бкой-экраном 6, снабженно продольным разрезом во избежание по влени  токов Фуко.The measuring frame represents co6oii two elongated turns a and b, connected by a figure eight, i.e. towards it. “The eight in the place of skrenshvani turns is bent in the form of 6yKiibi Y (in plan); the crossing point is insulated. The subject and this sample pass through the corresponding turns of the frame. The frame is suspended on a metal elastic filament 5 and is shielded from electrostatic influence on an magnetized tubule 1 with a brass truss-shield 6, equipped with a longitudinal slit to prevent the appearance of Foucault currents.

Если магнитный лоток в испытуемом образце отличен от магнитного потока в эталонном образце, то в рамке по витс  ток.If the magnetic tray in the test sample is different from the magnetic flux in the reference sample, then a current appears in the frame.

79651--2- 79651--2-

Как известно, напр женность магнитного пол  в воздухе у поверхностн ферромагнетика равна напр женности внутри его, так как тан1-енциальные составл ющие нанр женности магнитного пол  у новерхности раздела равны.,As is well known, the strength of the magnetic field in the air at a surface-ferromagnet is equal to the intensity inside it, since the tangential components of the magnetic field strength at the surface of the section are equal.

Взаимодействие тока в рамке с магнитным нолем у поверхности образцов вызовет отклонение рамки прибора. Угол отклонени  рамки будет иронорционален разности ма|нитных потерь при неремагничивании в испытуемом и эталонном образцах. Отсчет угла поворота рамки производитс  при помощи зеркальц.а 7.The interaction of the current in the frame with the magnetic zero at the surface of the samples will cause the deviation of the instrument frame. The angle of deviation of the frame will be ironically equivalent to the difference of the magnitude loss during non-magnetisation in the test and reference samples. The frame angle is counted using mirrors a. 7.

Предмет изобретени Subject invention

Дифференциальный прибор электродинамической системы дл  определени  магнитных потерь ферромагнитных материалов при перемагничпвании , о т л и ч а ю щ, и и с   тем, что, с целью оиределени  разности магнитиых нотерь у измер емого и эталонного образцов, нодвижна  рамка ирибора состоит из двух встречно соединенных витков, внутрь каждого из которых, соответственно, вставл ютс  эталонный и измер емый образцы.A differential electrodynamic device for determining the magnetic losses of ferromagnetic materials during remagnetization, which also means that, in order to determine the difference between the magnetic notes of the measured and reference samples, the moving frame of the iribor consists of two mutually connected turns, inside each of which, respectively, are inserted reference and measurable samples.

SU394449A 1949-03-29 1949-03-29 Differential electrodynamic system to determine the magnetic loss of ferromagnetic materials SU79651A1 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
SU394449A SU79651A1 (en) 1949-03-29 1949-03-29 Differential electrodynamic system to determine the magnetic loss of ferromagnetic materials

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
SU394449A SU79651A1 (en) 1949-03-29 1949-03-29 Differential electrodynamic system to determine the magnetic loss of ferromagnetic materials

Publications (1)

Publication Number Publication Date
SU79651A1 true SU79651A1 (en) 1949-11-30

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Family Applications (1)

Application Number Title Priority Date Filing Date
SU394449A SU79651A1 (en) 1949-03-29 1949-03-29 Differential electrodynamic system to determine the magnetic loss of ferromagnetic materials

Country Status (1)

Country Link
SU (1) SU79651A1 (en)

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