The drag force on the droplet is given by:
\[
F_{\text{drag}} = c v
\]
Where:
- \( c = 1.0 \, \mu\text{N·s/m} \) (drag coefficient),
- \( v \) is the velocity of the droplet.
The velocity decreases according to the following equation:
\[
v(t) = v_0 e^{-kt}
\]
Where:
- \( v_0 = 0.7 \, \text{m/s} \) (initial velocity),
- \( v(t) \) is the velocity at time \( t \),
- \( k \) is a constant related to the drag coefficient.
The velocity reduces to 10% of its initial velocity, i.e., \( v(t) = 0.1 v_0 \). Using this, we can solve for the time \( t \) it takes for this change:
\[
0.1 v_0 = v_0 e^{-kt} $\Rightarrow$ e^{-kt} = 0.1 $\Rightarrow$ t = \frac{\ln(10)}{k}
\]
Now, to calculate the distance traveled \( d \), we integrate the velocity:
\[
d = \int_0^t v_0 e^{-kt} dt = \frac{v_0}{k}
\]
Substituting the known values, we find that the distance traveled is approximately \( 0.01 \, \text{m} \).
Thus, the distance is approximately \( 0.01 \, \text{m} \).