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Units and Measurements question

2025 · 7 Apr · Shift 2 · Q51
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Units and Measurements question

2025 · 7 Apr · Shift 2 · Q51

JEE MainPhysicsUnits and MeasurementsMCQ+4 / −1
The dimension of μ0ϵ0\sqrt{\frac{\mu_0}{\epsilon_0}}ϵ0​μ0​​​ is equal to that of: (μ0\mu_0μ0​ = Vacuum permeability and ϵ0\epsilon_0ϵ0​ = Vacuum permittivity)
  1. A
    Voltage
  2. B
    Inductance
  3. C
    Resistance
  4. D
    Capacitance
View written solutionFree

Correct answer: C

  1. We need the dimension of
μ0ϵ0\sqrt{\frac{\mu_0}{\epsilon_0}}ϵ0​μ0​​​

where μ0\mu_0μ0​ is vacuum permeability and ϵ0\epsilon_0ϵ0​ is vacuum permittivity.

  1. Use the electromagnetic relation:
c=1μ0ϵ0c=\frac{1}{\sqrt{\mu_0\epsilon_0}}c=μ0​ϵ0​​1​

So,

μ0ϵ0=1c2\mu_0\epsilon_0=\frac{1}{c^2}μ0​ϵ0​=c21​

Also, the quantity

μ0ϵ0\sqrt{\frac{\mu_0}{\epsilon_0}}ϵ0​μ0​​​

is known as the intrinsic impedance of free space.

  1. Let us verify its dimensions directly.
  • Permeability:
[μ0]=NA2[\mu_0]=\frac{\text{N}}{\text{A}^2}[μ0​]=A2N​

Since

[N]=MLT−2,[A]=I[\text{N}] = MLT^{-2}, \qquad [A]=I[N]=MLT−2,[A]=I

we get

[μ0]=MLT−2I−2[\mu_0]=MLT^{-2}I^{-2}[μ0​]=MLT−2I−2
  • Permittivity: from Coulomb's law,
14πϵ0q2r2=F\frac{1}{4\pi\epsilon_0}\frac{q^2}{r^2}=F4πϵ0​1​r2q2​=F

So,

[ϵ0]=q2Fr2[\epsilon_0]=\frac{q^2}{Fr^2}[ϵ0​]=Fr2q2​

Now,

[q]=IT,[F]=MLT−2,[r]=L[q]=IT, \qquad [F]=MLT^{-2}, \qquad [r]=L[q]=IT,[F]=MLT−2,[r]=L

Hence,

[ϵ0]=(IT)2(MLT−2)(L2)=M−1L−3T4I2[\epsilon_0]=\frac{(IT)^2}{(MLT^{-2})(L^2)} = M^{-1}L^{-3}T^4I^2[ϵ0​]=(MLT−2)(L2)(IT)2​=M−1L−3T4I2
  1. Therefore,
[μ0ϵ0]=MLT−2I−2M−1L−3T4I2=M2L4T−6I−4\left[\frac{\mu_0}{\epsilon_0}\right] =\frac{MLT^{-2}I^{-2}}{M^{-1}L^{-3}T^4I^2} = M^2L^4T^{-6}I^{-4}[ϵ0​μ0​​]=M−1L−3T4I2MLT−2I−2​=M2L4T−6I−4

Taking square root,

[μ0ϵ0]=ML2T−3I−2\left[\sqrt{\frac{\mu_0}{\epsilon_0}}\right] =ML^2T^{-3}I^{-2}[ϵ0​μ0​​​]=ML2T−3I−2
  1. Now compare with dimensions of the given options.
  • Voltage:
[V]=workcharge=ML2T−2IT=ML2T−3I−1[V]=\frac{\text{work}}{\text{charge}}=\frac{ML^2T^{-2}}{IT}=ML^2T^{-3}I^{-1}[V]=chargework​=ITML2T−2​=ML2T−3I−1

Not same.

  • Inductance: Using
Energy=12LI2\text{Energy}=\frac{1}{2}LI^2Energy=21​LI2 [L]=ML2T−2I2=ML2T−2I−2[L]=\frac{ML^2T^{-2}}{I^2}=ML^2T^{-2}I^{-2}[L]=I2ML2T−2​=ML2T−2I−2

Not same.

  • Resistance: Using Ohm's law R=V/IR=V/IR=V/I,
[R]=ML2T−3I−1I=ML2T−3I−2[R]=\frac{ML^2T^{-3}I^{-1}}{I}=ML^2T^{-3}I^{-2}[R]=IML2T−3I−1​=ML2T−3I−2

This matches.

  • Capacitance: Using C=q/VC=q/VC=q/V,
[C]=ITML2T−3I−1=M−1L−2T4I2[C]=\frac{IT}{ML^2T^{-3}I^{-1}}=M^{-1}L^{-2}T^4I^2[C]=ML2T−3I−1IT​=M−1L−2T4I2

Not same.

  1. Hence,
μ0ϵ0\sqrt{\frac{\mu_0}{\epsilon_0}}ϵ0​μ0​​​

has the dimensions of resistance.

Therefore, the correct option is C.

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