\[[m] = [\text{kg} \cdot \text{m}^2/\text{s}^2]^a \cdot [\text{kg}/\text{m}^3]^b \cdot [\text{s}]^c \]
Each dimension gives us a linear equalitie:
\[1 = 2a - 3b\]\[0 = a + b\]\[0 = -2a + c\]In the end: \[a = \frac{1}{5}; \quad b = - \frac{1}{5} ; \quad c = \frac{2}{5} \]
\[R(t) = S \]
$t,~\text{ms}$ $R,~\text{m}$ 16 215 25 258 53 340 62 345 90 385
To check our simple theory we can plot $\ln R$ vs. $\ln t$.
The slope is $0.34$, which likely corresponds to $1/3$. However, it is also quite close to $2/5$.
The slope
\[k = S E_0^{1/5} \rho_0^{-1/5} =1.0 \cdot 10^3~\text{m} \cdot \text{s}^{-2/5},\]so the energy
\[E = \rho_0 \left( \frac{k}{S} \right)^5 = 50 ~\text{TJ}.\]