Solute \(A\) is absorbed from a gas into water in a packed bed operating at steady state. The absorber operating pressure and temperature are 1 atm and 300 K, respectively. At the gas-liquid interface, \(y_i = 1.5 x_i\),
where \(y_i\) and \(x_i\) are the interfacial gas and liquid mole fractions of \(A\), respectively. At a particular location in the absorber, the mole fractions of \(A\) in the bulk gas and in the bulk water are 0.02 and 0.002, respectively. If the ratio of the local individual mass transfer coefficients for the transport of \(A\) on the gas-side (\(k_y\)) to that on the water-side (\(k_x\)), \(\frac{k_y}{k_x} = 2\), then \(y_i\) equals _________ (rounded off to 3 decimal places).
\[ y_i = 1.5 x_i \quad \text{(relation between interfacial gas and liquid mole fractions)} \] \[ y_{\text{bulk}} = 0.02 \quad \text{(mole fraction of \(A\) in the bulk gas)} \] \[ x_{\text{bulk}} = 0.002 \quad \text{(mole fraction of \(A\) in the bulk water)} \] \[ \frac{k_y}{k_x} = 2 \quad \text{(ratio of mass transfer coefficients)} \]
Step 2: Interfacial Composition Using Mass Transfer Coefficient Ratio.At steady state, the rate of mass transfer from gas to liquid is equal: \[ k_y (y_{\text{bulk}} - y_i) = k_x (x_i - x_{\text{bulk}}) \] Using the ratio: \[ \frac{k_y}{k_x} = 2 \Rightarrow k_y = 2k_x \] Substituting: \[ 2k_x (0.02 - y_i) = k_x (x_i - 0.002) \] Divide both sides by \(k_x\): \[ 2(0.02 - y_i) = x_i - 0.002 \tag{1} \]
Step 3: Use Interfacial Equilibrium Relation.From equilibrium: \[ y_i = 1.5 x_i \Rightarrow x_i = \frac{y_i}{1.5} \] Substituting into equation (1): \[ 2(0.02 - y_i) = \frac{y_i}{1.5} - 0.002 \] Multiply both sides by 1.5: \[ 3(0.02 - y_i) = y_i - 0.003 \] \[ 0.06 - 3y_i = y_i - 0.003 \] \[ 0.063 = 4y_i \Rightarrow y_i = \frac{0.063}{4} = 0.01575 \]
Final Answer: The interfacial mole fraction of A in the gas phase is \( \boxed{0.0158} \) (rounded to 4 decimal places).An ideal monoatomic gas is contained inside a cylinder-piston assembly connected to a Hookean spring as shown in the figure. The piston is frictionless and massless. The spring constant is 10 kN/m. At the initial equilibrium state (shown in the figure), the spring is unstretched. The gas is expanded reversibly by adding 362.5 J of heat. At the final equilibrium state, the piston presses against the stoppers. Neglecting the heat loss to the surroundings, the final equilibrium temperature of the gas is __________ K (rounded off to the nearest integer).
The residence-time distribution (RTD) function of a reactor (in min$^{-1}$) is 
The mean residence time of the reactor is __________ min (rounded off to 2 decimal places).}
Ideal nonreacting gases A and B are contained inside a perfectly insulated chamber, separated by a thin partition, as shown in the figure. The partition is removed, and the two gases mix till final equilibrium is reached. The change in total entropy for the process is _________J/K (rounded off to 1 decimal place).
Given: Universal gas constant \( R = 8.314 \) J/(mol K), \( T_A = T_B = 273 \) K, \( P_A = P_B = 1 \) atm, \( V_B = 22.4 \) L, \( V_A = 3V_B \).
The following data is given for a ternary \(ABC\) gas mixture at 12 MPa and 308 K:
\(y_i\): mole fraction of component \(i\) in the gas mixture
\(\hat{\phi}_i\): fugacity coefficient of component \(i\) in the gas mixture at 12 MPa and 308 K
The fugacity of the gas mixture is __________ MPa (rounded off to 3 decimal places).