Stokes' law for the settling velocity of a spherical particle in a fluid is given by:
\[
v = \frac{2r^2 (\rho_p - \rho_f) g}{9 \eta}
\]
where:
- \( r \) is the radius of the particle,
- \( \rho_p \) is the density of the particle,
- \( \rho_f \) is the density of the fluid,
- \( g \) is the acceleration due to gravity,
- \( \eta \) is the dynamic viscosity of the fluid (water).
Since the settling velocities of both galena and quartz particles are the same, we can set up the following ratio for the diameters (and thus the radii) of the two particles:
\[
\frac{r_{{galena}}^2 (\rho_{{galena}} - \rho_{{water}})}{r_{{quartz}}^2 (\rho_{{quartz}} - \rho_{{water}})} = 1
\]
Using \( r = \frac{d}{2} \), we substitute the given values:
\[
\frac{\left( \frac{d_{{galena}}}{2} \right)^2 (7400 - 1000)}{\left( \frac{25}{2} \right)^2 (2600 - 1000)} = 1
\]
Simplifying and solving for \( d_{{galena}} \):
\[
\frac{d_{{galena}}^2 (6400)}{25^2 (1600)} = 1
\]
\[
d_{{galena}}^2 = \frac{25^2 (1600)}{6400} \approx 12.5^2
\]
Thus, the diameter of the galena particle is approximately:
\[
d_{{galena}} \approx 12.5 \, \mu{m}
\]