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Q.The dimensions of (με)−1(\mu\varepsilon)^{-1}, where ε\varepsilon is the permittivity and μ\mu the permeability of a medium, are: (A) [M0L1T−1][\mathrm{M^{0}L^{1}T^{-1}}] (B) [M0L2T−2][\mathrm{M^{0}L^{2}T^{-2}}] (C) [M1L2T−2][\mathrm{M^{1}L^{2}T^{-2}}] (D) [M1L−1T1][\mathrm{M^{1}L^{-1}T^{1}}]

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The product με\mu\varepsilon has dimensions of [T2L−2][T^2 L^{-2}], so (με)−1(\mu\varepsilon)^{-1} has dimensions of velocity squared: [L2T−2][L^2 T^{-2}]. The answer is (B).

The key insight here is recognizing what μ\mu and ε\varepsilon represent physically and how they combine in electromagnetic theory. The speed of light (or electromagnetic waves) in a medium is given by c=1μεc = \frac{1}{\sqrt{\mu\varepsilon}}, which immediately tells us that με\mu\varepsilon must have dimensions of inverse velocity squared.

Let me work through the dimensional analysis systematically.

Finding the dimensions of permittivity ε\varepsilon:

Permittivity appears in Coulomb's law and the relation for electric field. From the capacitance of a parallel-plate capacitor:

C=εAdC = \frac{\varepsilon A}{d}

where CC is capacitance, AA is area, and dd is separation. Since capacitance has dimensions [Q2T2M−1L−2][Q^2 T^2 M^{-1} L^{-2}] (from C=Q/VC = Q/V and energy U=12CV2U = \frac{1}{2}CV^2), we get:

[ε]=[C][L][L2]=[M−1L−3T4A2][\varepsilon] = \frac{[C][L]}{[L^2]} = [M^{-1} L^{-3} T^4 A^2]

In SI base units with charge Q=ATQ = AT, this becomes [ε]=[M−1L−3T4A2][\varepsilon] = [M^{-1} L^{-3} T^4 A^2].

Finding the dimensions of permeability μ\mu:

Permeability appears in Ampère's law. The magnetic field around a wire is B=μI2πrB = \frac{\mu I}{2\pi r}, giving:

[μ]=[B][L][A][\mu] = \frac{[B][L]}{[A]} …

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