JEE PYQ: Units & Measurements - Question ID 0f37ea8dff55 (JEE Main 2025)

ID: 0f37ea8dff55JEE Main 2025Single Correct MCQ
If μ0\mu_0 and ϵ0\epsilon_0 are the permeability and permittivity of free space, respectively, then the dimension of (1μ0ϵ0)\left(\frac{1}{\mu_0 \epsilon_0}\right) is :

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Step-by-step Explanation

Core Formula & Concept:

In electromagnetism, the two fundamental constants of free space are:

  • Permeability of free space, μ0\mu_0, which relates magnetic flux density to magnetic field strength.
  • Permittivity of free space, ϵ0\epsilon_0, which relates electric displacement to electric field strength.

A key result from Maxwell’s equations is that electromagnetic waves propagate in free space with speed c=1μ0ϵ0.c = \frac{1}{\sqrt{\mu_0 \epsilon_0}}. This speed cc has the dimension of length per time, i.e. [c]=LT1[c] = \mathrm{L\,T^{-1}}.

Our goal is to find the dimension of the product μ0ϵ0\mu_0 \epsilon_0 and then invert it to obtain the dimension of 1μ0ϵ0\frac{1}{\mu_0 \epsilon_0}.

Step-by-Step Derivation:

Step 1 – Write down the dimensions of μ0\mu_0 and ϵ0\epsilon_0.

From the definitions:

  • μ0\mu_0 appears in the force law between two current-carrying wires: F=μ0I1I22πr.F = \frac{\mu_0 I_1 I_2 \ell}{2\pi r}. Force FF has dimension MLT2\mathrm{M\,L\,T^{-2}}, current II has I\mathrm{I}, length \ell and rr have L\mathrm{L}. Solving for μ0\mu_0 gives [μ0]=MLT2I2=MLT2I2.[\mu_0] = \frac{\mathrm{M\,L\,T^{-2}}}{\mathrm{I^2}} = \mathrm{M\,L\,T^{-2}\,I^{-2}}.
  • ϵ0\epsilon_0 appears in Coulomb’s law: F=14πϵ0q1q2r2.F = \frac{1}{4\pi\epsilon_0}\frac{q_1 q_2}{r^2}. Charge qq has dimension IT\mathrm{I\,T}, so [ϵ0]=I2T2ML3T2=M1L3T4I2.[\epsilon_0] = \frac{\mathrm{I^2\,T^2}}{\mathrm{M\,L^3\,T^{-2}}} = \mathrm{M^{-1}\,L^{-3}\,T^4\,I^2}.

Step 2 – Compute the dimension of the product μ0ϵ0\mu_0 \epsilon_0.

Multiply the two dimensions: [μ0ϵ0]=(MLT2I2)(M1L3T4I2)=M11L13T2+4I2+2=L2T2.[\mu_0 \epsilon_0] = \bigl(\mathrm{M\,L\,T^{-2}\,I^{-2}}\bigr) \bigl(\mathrm{M^{-1}\,L^{-3}\,T^4\,I^2}\bigr) = \mathrm{M^{1-1}\,L^{1-3}\,T^{-2+4}\,I^{-2+2}} = \mathrm{L^{-2}\,T^2}.

Step 3 – Invert the product to find 1μ0ϵ0\frac{1}{\mu_0 \epsilon_0}.

Taking the reciprocal of L2T2\mathrm{L^{-2}\,T^2} gives [1μ0ϵ0]=L2T2=L2T2.\left[\frac{1}{\mu_0 \epsilon_0}\right] = \mathrm{L^{2}\,T^{-2}} = \frac{\mathrm{L^2}}{\mathrm{T^2}}.

Step 4 – Match with the given options.

The dimension L2/T2\mathrm{L^2/T^2} corresponds exactly to option B.

Common Traps & Exam Tip:

Students often confuse the dimensions of μ0\mu_0 and ϵ0\epsilon_0, especially the signs of the exponents. A frequent mistake is to forget that μ0\mu_0 carries I2\mathrm{I^{-2}} while ϵ0\epsilon_0 carries I2\mathrm{I^2}, so the current dimensions cancel out in the product. Always double-check the exponent arithmetic when multiplying dimensions.

Quick sanity check: Since c2=1μ0ϵ0c^2 = \frac{1}{\mu_0 \epsilon_0}, and [c]=LT1[c] = \mathrm{L\,T^{-1}}, squaring gives [c2]=L2T2[c^2] = \mathrm{L^2\,T^{-2}}. This immediately confirms that 1μ0ϵ0\frac{1}{\mu_0 \epsilon_0} must have dimension L2/T2\mathrm{L^2/T^2}.

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