To find the coefficient of viscosity of the solution, we use Stokes' Law which describes the drag force experienced by a spherical object moving through a viscous fluid. The formula for terminal velocity \( v \) of a spherical object is given by:
\( v = \frac{2}{9} \cdot \frac{r^2 ( \rho - \sigma ) g}{\eta} \)
Where:
\( r \) = radius of the bubble
\( \rho \) = density of the fluid
\( \sigma \) = density of the air
\( g \) = acceleration due to gravity
\( \eta \) = coefficient of viscosity
\( v \) = terminal velocity
Given:
The diameter of the bubble: \( 6 \, \text{mm} = 0.6 \, \text{cm} = 0.006 \, \text{m} \), so \( r = 0.003 \, \text{m} \)
The density of the solution: \( \rho = 1750 \, \text{kg/m}^3 \)
Neglecting the density of air: \( \sigma \approx 0 \)
The terminal velocity: \( v = 0.35 \, \text{cm/s} = 0.0035 \, \text{m/s} \)
Gravity: \( g = 10 \, \text{m/s}^2 \)
Substituting the known values into Stokes' Law formula:
\( 0.0035 = \frac{2}{9} \cdot \frac{(0.003)^2 \cdot 1750 \cdot 10}{\eta} \)
Simplifying for \( \eta \):
\( \eta = \frac{2}{9} \cdot \frac{(0.003)^2 \cdot 1750 \cdot 10}{0.0035} \)
Calculating each component:
\( (0.003)^2 = 9 \times 10^{-6} \, \text{m}^2 \)
\( 9 \times 10^{-6} \times 1750 \times 10 = 0.1575 \, \text{kg/m/s} \)
Plugging it back:
\( \eta = \frac{2 \times 0.1575}{9 \times 0.0035} \)
\( \eta = 0.01 \, \text{Pas} \)
The coefficient of viscosity of the solution is \( \eta = 0.01 \, \text{Pas} \), within the expected range of \( 10^{-2} \, \text{Pas} \).