Step 1: In dimensional analysis, we need to match the dimensions of both sides of the equation. For the power \(P\), we consider its fundamental dimensions: \[ [P] = [ML^2T^{-3}] \] (where \(M\) is mass, \(L\) is length, and \(T\) is time).
Step 2: The dimensions of each variable in the equation \(P \propto \left( \frac{q a^m}{c^n} \right)\) are:
Step 3: By equating the dimensions of the two sides and solving for \(m\) and \(n\), we find that \(m = 2\) and \(n = 3\).
Dimensional Analysis of Power Radiated by Accelerated Charge
The power (P) radiated from an accelerated charged particle is given by $P \propto \frac{(qa)^m}{c^n}$, where q is the charge, a is the acceleration, and c is the speed of light in vacuum. We need to find the values of m and n using dimensional analysis.
The dimensions of the quantities involved are:
Power (P): $[P] = [ML^2T^{-3}]$
Charge (q): $[q] = [AT]$
Acceleration (a): $[a] = [LT^{-2}]$
Speed of light (c): $[c] = [LT^{-1}]$
Substituting these dimensions into the proportionality:
$[ML^2T^{-3}] \propto \frac{([AT] [LT^{-2}])^m}{[LT^{-1}]^n}$
$[ML^2T^{-3}] \propto \frac{[A^m L^m T^{-m-2m}]}{[L^n T^{-n}]} = \frac{[A^m L^m T^{-3m}]}{[L^n T^{-n}]}$
$[ML^2T^{-3}] \propto [A^m L^{m-n} T^{-3m+n}]$
Referring to the hint, which implicitly uses Larmor's formula $P = \frac{q^2 a^2}{6 \pi \epsilon_0 c^3}$ for comparison:
The term involving q and a is $(qa)^m$. Comparing with $q^2 a^2$, we can infer that $m = 2$.
Now, let's look at the powers of L and T after substituting $m=2$:
$[ML^2T^{-3}] \propto [A^2 L^{2-n} T^{-6+n}]$
From Larmor's formula, the power is inversely proportional to $c^3$. The term in our proportionality is $c^{-n}$. Therefore, $n = 3$.
Alternatively, using the hint's direct comparison:
$\frac{a^m}{c^n} \sim \frac{a^2}{c^3}$
By comparing the powers of 'a', we get $m = 2$.
By comparing the powers of 'c', we get $n = 3$.
Thus, the values of m and n are 2 and 3 respectively.
Final Answer: (B) m = 2, n = 3