The terminal velocity (\(V_t\)) of a droplet is given by:
\[ V_t =\( \frac{2R^2 (\rho - \sigma) g}{9\eta}\), \]
where \(R\) is the radius of the droplet.
When 8 small droplets coalesce:
Mass of larger drop \(M \propto 8m\), \quad \(M = \(\frac{4}{3}\)\pi R^3 (\rho)\).
The radius of the larger drop is:
\[ R_{\text{large}}^3 = 8R_{\text{small}}^3 \implies R_{\text{large}} = 2R_{\text{small}}. \]
Since terminal velocity (\(V_t\)) is proportional to \(R^2\):
\[ V_t \propto R^2 \implies V_t^{\text{large}} = 4V_t^{\text{small}}. \]
For the smaller droplet:
\[ V_t^{\text{small}} = 10 \, \text{cm/s}. \]
Thus:
\[ V_t^{\text{large}} = 4 \cdot 10 = 40 \, \text{cm/s}. \]
For the thermal decomposition of \( N_2O_5(g) \) at constant volume, the following table can be formed, for the reaction mentioned below: \[ 2 N_2O_5(g) \rightarrow 2 N_2O_4(g) + O_2(g) \] Given: Rate constant for the reaction is \( 4.606 \times 10^{-2} \text{ s}^{-1} \).
Let \( T_r \) be the \( r^{\text{th}} \) term of an A.P. If for some \( m \), \( T_m = \dfrac{1}{25} \), \( T_{25} = \dfrac{1}{20} \), and \( \displaystyle\sum_{r=1}^{25} T_r = 13 \), then \( 5m \displaystyle\sum_{r=m}^{2m} T_r \) is equal to: