\zeta \left(1 - \frac{R_c}{R} \right) \frac{1}{R} \left( \frac{1}{1 + R_\sigma/R} \right),$$ where we took into account Eqs. (\[R\_s\]) and (\[R\_c-Henry\]).

Each of the three co-factors dependent on $R$ emphasized in the right hand side of Eq. (\[Growth-Rate-Henry\]) describes its physically different contribution to the dynamics of the supercritical bubble growth process. Co-factor $1 - R_c/R$, increasing with $R$, corresponds to the fast (the scale of change of $R$ is $R_c$) increase of the driving force of the process (the value $n_0 - n_R$) with the growth of $R$. Co-factor $1/R$, decreasing with the growth of $R$, describes, as it is seen from Eq. (\[Flux\]), the contribution related to the decrease of the gradient of solution concentration near the bubble surface, which decreases the bubble growth rate with the growth of $R$. Finally, co-factor $1/(1 + R_\sigma/R)$, which increases with the growth of $R$, takes into account the counteraction of Laplace pressure to the bubble growth, i. e. the fact that the bubble growth is facilitated by the reduction of Laplace pressure with the growth of $R$, while other factors are equal (the scale of its change is $R_\sigma$). Notwithstanding the mentioned reduction of counteraction, the resulting contribution of the last 