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ElectricalElectromagnetics Field Theory
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Two 300 ╬╝H coils in series without mutual coupling have a total inductance of

A

300┬а╬╝H300\ \mu H300┬а╬╝H

B

600┬а╬╝H600\ \mu H600┬а╬╝H

C

150┬а╬╝H150\ \mu H150┬а╬╝H

D

75┬а╬╝H75\ \mu H75┬а╬╝H

Correct Answer

тЪЩя╕П TE тАв Technical Concept & PrincipleElectricalElectromagnetics Field Theory
Option B

600┬а╬╝H600\ \mu H600┬а╬╝H

Quick Summary:

When two inductors are connected in series without any magnetic coupling, their equivalent inductance is simply the arithmetic sum of their individual inductances. For two identical inductors, this results in a total value double that of a single unit.

тЪЩя╕ПTETechnical SolutionConcept & Principle
ЁЯТб Explanation

When two inductors are connected in series without any magnetic coupling, their equivalent inductance is simply the arithmetic sum of their individual inductances. For two identical inductors, this results in a total value double that of a single unit.

ЁЯФв Key Formulas

Leq=L1+L2L_{eq} = L_1 + L_2LeqтАЛ=L1тАЛ+L2тАЛ тАФ Equivalent inductance for series connection without mutual coupling

тЪЩя╕П Working Principle

Inductors in series carry the same current III. The total voltage drop across the combination is V=Leqdidt=L1didt+L2didtV = L_{eq} \frac{di}{dt} = L_1 \frac{di}{dt} + L_2 \frac{di}{dt}V=LeqтАЛdtdiтАЛ=L1тАЛdtdiтАЛ+L2тАЛdtdiтАЛ. Since there is no mutual inductance MMM, the magnetic fields do not influence each other, leading to Leq=L1+L2L_{eq} = L_1 + L_2LeqтАЛ=L1тАЛ+L2тАЛ.

ЁЯУМ Key Points
  • тЦ╕

    The total inductance of series components is additive when magnetic coupling is absent.

  • тЦ╕

    If mutual inductance MMM existed, the formula would be Leq=L1+L2┬▒2ML_{eq} = L_1 + L_2 \pm 2MLeqтАЛ=L1тАЛ+L2тАЛ┬▒2M.

  • тЦ╕

    Units remain constant in addition; 300┬а╬╝H+300┬а╬╝H=600┬а╬╝H300\ \mu H + 300\ \mu H = 600\ \mu H300┬а╬╝H+300┬а╬╝H=600┬а╬╝H.

тЬЕ Advantages
  • тЦ╕

    Simple additive calculation for series circuits.

  • тЦ╕

    Easily configurable to reach higher inductance values using standard components.

тЭМ Disadvantages / Limitations
  • тЦ╕

    Increases physical space and potential for unintentional EMI if not shielded.

  • тЦ╕

    Series resistance of windings also adds up, increasing losses.

ЁЯЫая╕П Applications / Uses
  • тЦ╕

    Inductive filtering in power supplies.

  • тЦ╕

    Matching circuits in RF design.

ЁЯУД Additional Information
  • тЦ╕

    Inductance is defined by the property of a conductor where an electric current produces a magnetic field.

  • тЦ╕

    Option A (300 ╬╝H\mu H╬╝H) would be the result if they were in parallel.

  • тЦ╕

    Option C (150 ╬╝H\mu H╬╝H) is the result for identical inductors in parallel (L/2L/2L/2).

ЁЯУК Diagram / Illustration
Series Inductance Formula
Leq=L1+L2L_{eq} = L_1 + L_2LeqтАЛ=L1тАЛ+L2тАЛ
For L1=L2=300┬а╬╝HL_1 = L_2 = 300\ \mu HL1тАЛ=L2тАЛ=300┬а╬╝H
Leq=600┬а╬╝HL_{eq} = 600\ \mu HLeqтАЛ=600┬а╬╝H
тЬЕ

B is correct тАФ The total inductance is the sum of the individual inductances, 300┬а╬╝H+300┬а╬╝H=600┬а╬╝H300\ \mu H + 300\ \mu H = 600\ \mu H300┬а╬╝H+300┬а╬╝H=600┬а╬╝H.

Core Concepts Used
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Inductance in series Passive circuit elements Magnetic field independence
ЁЯТб EXAM TIP

Always check for 'mutual coupling' in exam questions; if specified, you must include the ┬▒2M\pm 2M┬▒2M term, but if explicitly stated as 'without mutual coupling', treat them as isolated components.

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