To solve the problem of determining the new terminal velocity of the larger droplet formed by the coalescence of 8 smaller droplets, we can use the physics of terminal velocity and volume conservation. First, consider that the terminal velocity \( v \) of a droplet can be expressed as \( v \propto r^2 \), where \( r \) is the radius of the droplet. When droplets coalesce, their combined volume equals the volume of the larger drop. Given the radius \( r_0 = 0.01 \) mm for each of the smaller droplets and their terminal velocity \( v_0 = 10 \) cm/s, we can calculate the new radius of the larger droplet. The volume of a sphere is given by \( V = \frac{4}{3} \pi r^3 \). Therefore, the total initial volume of 8 small droplets is \( 8 \times \frac{4}{3} \pi r_0^3 \) and the volume of the larger drop is \( \frac{4}{3} \pi R^3 \). Equating these, we get:
\( R^3 = 8r_0^3 \)
Solving for \( R \), we have:
\( R = 8^{1/3}r_0 = 2r_0 \)
Substituting \( r_0 = 0.01 \) mm, we find:
\( R = 2 \times 0.01 \text{ mm} = 0.02 \text{ mm} \)
Next, calculate the terminal velocity of the larger droplet, using \( v \propto r^2 \). The new terminal velocity \( V \) is given by:
\( \frac{V}{v_0} = \left(\frac{R}{r_0}\right)^2 \)
Substitute the values:
\( \frac{V}{10} = \left(\frac{0.02}{0.01}\right)^2 = 2^2 = 4 \)
Therefore, \( V = 4 \times 10 = 40 \text{ cm/s} \)
The calculated terminal velocity of the larger droplet is indeed 40 cm/s, which fits perfectly within the given range of 40 to 40 cm/s.
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:
\[ V_t^{\text{large}} = 4 \cdot 10 = 40 \, \text{cm/s}. \]
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,


What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)