Rate of decrease of the magnetic fields

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SUMMARY

The discussion focuses on the mathematical derivation of the rate of decrease of magnetic fields, denoted as V_B, using Faraday's law of electromagnetic induction. The equation derived shows that the electromotive force (EMF) around a closed path is equal to the negative rate of change of magnetic flux, represented as \(\oint E\cdot ds = \pi V_B(R_1^2 - R_2^2)\). The magnetic flux \(\phi_B\) is expressed as a function of area and magnetic field strength, specifically \(\phi_B(t) = \pi R^2(B_0 - V_Bt)\), where B0 is the initial magnetic field strength. This derivation highlights the relationship between changing magnetic fields and induced electric fields in a defined area.

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  • Understanding of Faraday's law of electromagnetic induction
  • Familiarity with magnetic flux calculations
  • Knowledge of calculus, specifically differentiation
  • Basic concepts of electromotive force (EMF)
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  • Learn about the applications of magnetic flux in electrical engineering
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Physicists, electrical engineers, and students studying electromagnetism who seek to deepen their understanding of the relationship between changing magnetic fields and induced electric currents.

Oblakastouf
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Let V_B be the rate of decrease of the magnetic fields

\frac{dB}{dt}

For the 3rd path:
\oint E\cdot ds = -\frac{d\phi _B}{dt} = -\frac{{d\phi _B}_1 + {d\phi _B}_2}{dt}

\phi _B_{(t)} = A_{(t)}B_{(t)}
The area is constant, it's only the magnetic field that's changing:
\phi _B_{(t)} = \pi R^2(B_0 - V_Bt)

Since B1 and B2 are in opposite directions, give one of them a minus sign:
{\phi _B}_1 + {\phi _B}_2 = \pi R_1^2(B_0 - V_Bt) - \pi R_2^2(B_0 - V_Bt) = \pi (B_0 - V_Bt)(R_1^2 - R_2^2)
Take the derivative of that:
\frac{{d\phi _B}_1 + {d\phi _B}_2}{dt} = -\pi V_B(R_1^2 - R_2^2)

And therefore:
\oint E\cdot ds = \pi V_B(R_1^2 - R_2^2)
 
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We appreciate that you know latex, but the title is useless, and you didn't follow the template. You also don't describe the problem. Don't expect an answer.
 

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