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ElectricalBasic Electrical
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A wire of resistance R has its length and cross section both doubled. Its resistance will become

A

4R4 R4R

B

2R2 R2R

C

RRR

D

R/4R/4R/4

Correct Answer

тЪЩя╕П TE тАв Technical Concept & PrincipleElectricalBasic Electrical
Option C

RRR

Quick Summary:

The resistance of a wire is given by R=╧БLAR = \rho \frac{L}{A}R=╧БALтАЛ. When the length LLL is doubled (LтА▓=2LL' = 2LLтА▓=2L) and the cross-sectional area AAA is also doubled (AтА▓=2AA' = 2AAтА▓=2A), the new resistance RтА▓R'RтА▓ becomes RтА▓=╧Б2L2A=╧БLA=RR' = \rho \frac{2L}{2A} = \rho \frac{L}{A} = RRтА▓=╧Б2A2LтАЛ=╧БALтАЛ=R.

тЪЩя╕ПTETechnical SolutionConcept & Principle
ЁЯТб Explanation

The resistance of a wire is given by R=╧БLAR = \rho \frac{L}{A}R=╧БALтАЛ. When the length LLL is doubled (LтА▓=2LL' = 2LLтА▓=2L) and the cross-sectional area AAA is also doubled (AтА▓=2AA' = 2AAтА▓=2A), the new resistance RтА▓R'RтА▓ becomes RтА▓=╧Б2L2A=╧БLA=RR' = \rho \frac{2L}{2A} = \rho \frac{L}{A} = RRтА▓=╧Б2A2LтАЛ=╧БALтАЛ=R.

ЁЯФв Key Formulas

R=╧БLAR = \rho \frac{L}{A}R=╧БALтАЛ тАФ Ohm's law for resistance based on geometry

RтА▓=╧БnLnA=RR' = \rho \frac{nL}{nA} = RRтА▓=╧БnAnLтАЛ=R тАФ Proof of invariance under proportional scaling

тЪЩя╕П Working Principle

The electrical resistance of a conductor is directly proportional to its length and inversely proportional to its cross-sectional area. By increasing both dimensions by the same factor (a scale factor of 2), the ratios cancel out, leaving the total resistance invariant.

ЁЯУМ Key Points
  • тЦ╕

    Resistance is a property of the conductor's geometry and material resistivity (╧Б\rho╧Б).

  • тЦ╕

    Scaling factor 'n' applied to both L and A results in no change to resistance.

  • тЦ╕

    If only length were doubled, resistance would increase by a factor of 4 (assuming volume conservation).

  • тЦ╕

    If only area were doubled, resistance would decrease by a factor of 4.

тЬЕ Advantages
  • тЦ╕

    Uniform scaling preserves electrical properties.

  • тЦ╕

    Easier to analyze using geometric scaling factors.

ЁЯЫая╕П Applications / Uses
  • тЦ╕

    Cable sizing in power distribution.

  • тЦ╕

    Design of heating elements and conductors.

ЁЯУД Additional Information
  • тЦ╕

    Resistivity (╧Б\rho╧Б) depends only on the material type and temperature, not dimensions.

  • тЦ╕

    Option A (4R) would occur if only length were doubled while maintaining volume (which would force the area to decrease).

ЁЯУК Diagram / Illustration
Resistance Scaling FormulaNew Resistance R' = ╧Б ├Ч (2L) / (2A)2L2AR' = R (Resistance remains constant)
тЬЕ

C is correct тАФ Since the length and cross-sectional area are both scaled by the same factor, the ratio remains unchanged, resulting in the same resistance RRR.

Core Concepts Used
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Electrical Resistivity Geometric Scaling Ohmic Resistance
ЁЯТб EXAM TIP

Always verify if the problem implies volume conservation. If volume is constant and you double length, area MUST decrease, leading to 4R4R4R. If physical dimensions are explicitly stated as doubled (as in this case), use the direct formula ratios.

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