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SU24927A1 - Method for measuring magnetic field strength - Google Patents

Method for measuring magnetic field strength

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Publication number
SU24927A1
SU24927A1 SU60950A SU60950A SU24927A1 SU 24927 A1 SU24927 A1 SU 24927A1 SU 60950 A SU60950 A SU 60950A SU 60950 A SU60950 A SU 60950A SU 24927 A1 SU24927 A1 SU 24927A1
Authority
SU
USSR - Soviet Union
Prior art keywords
magnetic field
field strength
measuring magnetic
string
measuring
Prior art date
Application number
SU60950A
Other languages
Russian (ru)
Inventor
Г.В. Брауде
Original Assignee
Г.В. Брауде
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 Г.В. Брауде filed Critical Г.В. Брауде
Priority to SU60950A priority Critical patent/SU24927A1/en
Application granted granted Critical
Publication of SU24927A1 publication Critical patent/SU24927A1/en

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  • Measuring Magnetic Variables (AREA)

Description

где 4 - амплитуда переменного тока, - частота переменного тока, равна  собственной частоте струны, Н - сила магнитного пол , р - плотность струны, /-площадь поперечного сечени  струны, р - коэффициент затухани  струны. На пр жение на концах струны, помещенной в магнитное поле и колеблющейс  под вли нием проход щего через нее переменного тока, будет складыватьс  из падени  напр жени  на омическом сопротивлении струны и обратной электродвижущей силы индукции, возгде /-длина струны.where 4 is the amplitude of the alternating current, is the frequency of the alternating current, is equal to the natural frequency of the string, H is the strength of the magnetic field, p is the density of the string, / is the area of the cross section of the string, p is the damping factor of the string. A strand at the ends of a string, placed in a magnetic field and oscillating under the influence of an alternating current passing through it, will consist of the voltage drop across the ohmic resistance of the string and the reverse electromotive force of induction, which is the length of the string.

Подставл   в выражение дл  выраженир дл  у и дел  его на / , получим эффективное сопротивление струны при резонансеSubstituting in the expression for the expression for y and doing it by /, we obtain the effective resistance of the string at the resonance

4lff 4lff

//г« // g "

где /-длина струны, /-площадь поперечного сечени  струны, р - плотность струны, р - коэффициент затухани  струны , Н-сила магнитного пол .where / is the length of the string, / is the area of the cross section of the string, p is the density of the string, p is the damping factor of the string, H is the strength of the magnetic field.

SU60950A 1929-12-24 1929-12-24 Method for measuring magnetic field strength SU24927A1 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
SU60950A SU24927A1 (en) 1929-12-24 1929-12-24 Method for measuring magnetic field strength

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
SU60950A SU24927A1 (en) 1929-12-24 1929-12-24 Method for measuring magnetic field strength

Publications (1)

Publication Number Publication Date
SU24927A1 true SU24927A1 (en) 1932-01-31

Family

ID=48343153

Family Applications (1)

Application Number Title Priority Date Filing Date
SU60950A SU24927A1 (en) 1929-12-24 1929-12-24 Method for measuring magnetic field strength

Country Status (1)

Country Link
SU (1) SU24927A1 (en)

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