JEE PYQ: Units & Measurements - Question ID 152922fe2636 (JEE Main 2003)

ID: 152922fe2636JEE Main 2003Single Correct MCQ
Dimensions of 1μ0ε0{1 \over {{\mu _0}{\varepsilon _0}}}, where symbols have their usual meaning, are

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Step-by-step Explanation

Core Formula & Concept:

In electromagnetism, the two fundamental constants are:

  • μ0\mu_0 – the permeability of free space, whose SI unit is henry per metre (H/m).
  • ε0\varepsilon_0 – the permittivity of free space, whose SI unit is farad per metre (F/m).

From Maxwell’s equations we know that electromagnetic waves in vacuum travel at the speed of light cc, and this speed is related to μ0\mu_0 and ε0\varepsilon_0 by the identity c=1μ0ε0.c = \frac{1}{\sqrt{\mu_0\,\varepsilon_0}}. Consequently, 1μ0ε0=c2.\frac{1}{\mu_0\,\varepsilon_0} = c^2. Since the speed of light cc has dimensions of length per time, [c]=LT1[c] = \mathrm{L\,T^{-1}}, its square will have dimensions L2T2\mathrm{L^2\,T^{-2}}. This is the key to finding the dimensions of 1/(μ0ε0)1/(\mu_0\,\varepsilon_0).

Step-by-Step Derivation:

Step 1: Write down the SI units of μ0\mu_0 and ε0\varepsilon_0.

  • μ0\mu_0 has unit henry per metre (H/m).
  • ε0\varepsilon_0 has unit farad per metre (F/m).

Step 2: Express H and F in base SI units.

  • 1 henry (H) = 1 kgm2s2A2\mathrm{kg\,m^2\,s^{-2}\,A^{-2}}.
  • 1 farad (F) = 1 kg1m2s4A2\mathrm{kg^{-1}\,m^{-2}\,s^{4}\,A^{2}}.

Step 3: Compute the unit of μ0ε0\mu_0\,\varepsilon_0.

[μ0]=Hm=kgm2s2A2m=kgms2A2.[\mu_0] = \frac{\mathrm{H}}{\mathrm{m}} = \frac{\mathrm{kg\,m^2\,s^{-2}\,A^{-2}}}{\mathrm{m}} = \mathrm{kg\,m\,s^{-2}\,A^{-2}}. [ε0]=Fm=kg1m2s4A2m=kg1m3s4A2.[\varepsilon_0] = \frac{\mathrm{F}}{\mathrm{m}} = \frac{\mathrm{kg^{-1}\,m^{-2}\,s^{4}\,A^{2}}}{\mathrm{m}} = \mathrm{kg^{-1}\,m^{-3}\,s^{4}\,A^{2}}. Multiply them: [μ0ε0]=(kgms2A2)(kg1m3s4A2)=m2s2.[\mu_0\,\varepsilon_0] = \bigl(\mathrm{kg\,m\,s^{-2}\,A^{-2}}\bigr) \bigl(\mathrm{kg^{-1}\,m^{-3}\,s^{4}\,A^{2}}\bigr) = \mathrm{m^{-2}\,s^{2}}.

Step 4: Find the unit of 1/(μ0ε0)1/(\mu_0\,\varepsilon_0).

[1μ0ε0]=1[μ0ε0]=1m2s2=m2s2.\Bigl[\frac{1}{\mu_0\,\varepsilon_0}\Bigr] = \frac{1}{[\mu_0\,\varepsilon_0]} = \frac{1}{\mathrm{m^{-2}\,s^{2}}} = \mathrm{m^{2}\,s^{-2}}.

Step 5: Translate to dimensional notation.

The dimensions m2s2\mathrm{m^2\,s^{-2}} correspond exactly to L2T2\mathrm{L^2\,T^{-2}}.

Step 6: Match with the given options.

Option C is [L2T2][\mathrm{L^2\,T^{-2}}], which agrees with our result. Common Traps & Exam Tip:

Many students mistakenly try to recall the dimensions of μ0\mu_0 and ε0\varepsilon_0 separately and then multiply them. A frequent error is to confuse the dimensions of μ0\mu_0 (which are MLT2A2\mathrm{M\,L\,T^{-2}\,A^{-2}}) with those of ε0\varepsilon_0 (which are M1L3T4A2\mathrm{M^{-1}\,L^{-3}\,T^{4}\,A^{2}}), leading to incorrect cancellation. Instead, remember the identity 1μ0ε0=c2,\frac{1}{\mu_0\,\varepsilon_0} = c^2, and use the known dimensions of cc to arrive at the answer quickly and reliably.

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