Fig. 7.

Stationary droplet solution, 2nd order reaction case. Shown are the radial-coordinate dependences of the chemical potentials μ_i (i = 1, 2), concentrations n_i (i = 1, 2), and pressure p for a stationary, spherically symmetric cluster of radius R, as obtained by solving the reaction-diffusion scheme in Eq. (2). The inset shows the r-dependence of the total amount of the solute, $n\equiv n_1+2n_2$. The following parameter values are employed: ${\kappa }_1^{\left(\mathrm{d}\right)}={\kappa }_2^{\left(\mathrm{d}\right)}={\kappa }_1^{\left(\mathrm{m}\right)}={\kappa }_2^{\left(\mathrm{m}\right)}=40$, $m_1^{\left(\mathrm{d}\right)}=m_1^{\left(\mathrm{m}\right)}=52.36$, $m_2^{\left(\mathrm{d}\right)}=m_2^{\left(\mathrm{m}\right)}=500$, $n_1^{\left(\mathrm{d}\right)}=0.0095$, $n_2^{\left(\mathrm{d}\right)}=0.062$, $n_1^{\left(\mathrm{m}\right)}=0.019$, $n_2^{\left(\mathrm{m}\right)}=0.005$, $D_1^{\left(\mathrm{d}\right)}=0.33$, $D_2^{\left(\mathrm{d}\right)}=0.13$, $D_1^{\left(\mathrm{m}\right)}=1$, $D_2^{\left(\mathrm{m}\right)}=0.38$, $k_1^{\left(\mathrm{d}\right)}=0.026$, $k_2^{\left(\mathrm{d}\right)}=0.000019$, $k_1^{\left(\mathrm{m}\right)}=0.0005$, $k_2^{\left(\mathrm{m}\right)}=0.000019$, Δg = 0.01