Related Formula
Let momentum be P$P$ ([P] = [M L T⁻¹]$[P] = [M L T^{-1}]$).
We assume:
P = q^x μ₀^y I^z$$P = q^x \mu_0^y I^z$$
Core Logic
Let's find the dimensional formulas of the individual variables:
- Charge (q$q$):
[q] = [A T]$[q] = [A T]$
- Current (I$I$):
[I] = [A]$[I] = [A]$
- Permeability of vacuum (μ₀$\mu_0$):
From Biot-Savart law or force between parallel wires: F = (μ₀ I² L)/(2π d)$F = \frac{\mu_0 I^2 L}{2\pi d}$:
[μ₀] = ([F])/([I]²) = [M L T⁻²][A]² = [M L T⁻² A⁻²]$$[\mu_0] = \frac{[F]}{[I]^2} = \frac{[M L T^{-2}]}{[A]^2} = [M L T^{-2} A^{-2}]$$
Step 1: Apply Dimensional Homogeneity
Substitute these into our assumed dimensional equation:
[M L T⁻¹] = [A T]^x [M L T⁻² A⁻²]^y [A]^z$$[M L T^{-1}] = [A T]^x [M L T^{-2} A^{-2}]^y [A]^z$$
[M L T⁻¹] = [M]^y [L]^y [T]x - 2y [A]x - 2y + z$$[M L T^{-1}] = [M]^y [L]^y [T]^{x - 2y} [A]^{x - 2y + z}$$
Comparing exponents on both sides:
- For [M]$[M]$:
y = 1$y = 1$
- For [L]$[L]$:
y = 1 (consistent)$$y = 1 \quad \text{(consistent)}$$
x - 2y = -1 x - 2(1) = -1 x = 1$$x - 2y = -1 \implies x - 2(1) = -1 \implies x = 1$$
x - 2y + z = 0 1 - 2(1) + z = 0 z = 1$$x - 2y + z = 0 \implies 1 - 2(1) + z = 0 \implies z = 1$$
Thus, x = 1, y = 1, z = 1$x = 1, y = 1, z = 1$.
Therefore, the required quantity is:
q¹ μ₀¹ I¹ = q μ₀ I$$q^1 \mu_0^1 I^1 = q \mu_0 I$$
Pattern Recognition
Sees: Permeability, charge, and current linked to momentum.
Trap: Deriving the dimensions of μ₀$\mu_0$ using complex magnetic formulas. Remember [μ₀] = [Force]/[Current]²$[\mu_0] = [\text{Force}]/[\text{Current}]^2$ is the quickest way to get its dimensions.
Shortcut: Since [q] = AT$[q] = AT$ and [I] = A$[I] = A$, [q μ₀ I] = [A T] [M L T⁻² A⁻²] [A] = [M L T⁻¹]$[q \mu_0 I] = [A T] [M L T^{-2} A^{-2}] [A] = [M L T^{-1}]$, which is exactly the dimensions of momentum. Hence, option (2) is correct.
Chapter Mix
Class 11 Physics: Units and Measurements
Class 12 Physics: Moving Charges and Magnetism