Step 1: Understanding Terminal Velocity and Volume Conservation The terminal velocity \( v \) of a small drop is given by Stokes' law: \[ v \propto R^2 \] where \( R \) is the radius of the drop. When \( n \) small identical drops merge, the volume remains conserved: \[ n \times \frac{4}{3} \pi r^3 = \frac{4}{3} \pi R^3 \] where \( r \) is the radius of each small drop and \( R \) is the radius of the bigger drop.
Step 2: Finding the Radius of the Bigger Drop From volume conservation, \[ n r^3 = R^3 \] \[ R = n^{1/3} r \]
Step 3: Finding the Terminal Velocity of the Bigger Drop Since terminal velocity is proportional to the square of the radius, we can write: \[ V \propto R^2 \] \[ V \propto (n^{1/3} r)^2 \] \[ V \propto n^{2/3} r^2 \] Since the terminal velocity of the small drop is \( v \propto r^2 \), we can write: \[ V = n^{2/3} v \]
Thus, the terminal velocity of the bigger drop is \( n^{2/3} v \).
The shaft of a 6 m wide gate in the figure will fail at a moment of 3924 kN.m about the hinge P. The maximum value of water depth \( h \) (in m) that the gate can hold is ......... (round off to the nearest integer).
Consider steady flow of water in the series pipe system shown below, with specified discharge. The diameters of Pipes A and B are 2 m and 1 m, respectively. The lengths of pipes A and B are 100 m and 200 m, respectively. Assume the Darcy-Weisbach friction coefficient, \( f \), as 0.01 for both the pipes.
The ratio of head loss in Pipe-B to the head loss in Pipe-A is ___________ (round off to the nearest integer).
For the reaction:
\[ 2A + B \rightarrow 2C + D \]
The following kinetic data were obtained for three different experiments performed at the same temperature:
\[ \begin{array}{|c|c|c|c|} \hline \text{Experiment} & [A]_0 \, (\text{M}) & [B]_0 \, (\text{M}) & \text{Initial rate} \, (\text{M/s}) \\ \hline I & 0.10 & 0.10 & 0.10 \\ II & 0.20 & 0.10 & 0.40 \\ III & 0.20 & 0.20 & 0.40 \\ \hline \end{array} \]
The total order and order in [B] for the reaction are respectively: