Consider the matrix:
\[ A = \begin{bmatrix} 2 & 3 \\ 1 & 2 \end{bmatrix} \]
The eigenvalues of the matrix are 0.27 and ____ (rounded off to 2 decimal places).
The eigenvalues of a matrix \( A \) are found by solving the characteristic equation:
\[ \det(A - \lambda I) = 0 \]
Where \( \lambda \) is the eigenvalue and \( I \) is the identity matrix.
For the given matrix \( A \):
\[ A = \begin{bmatrix} 2 & 3 \\ 1 & 2 \end{bmatrix} \quad \Rightarrow \quad A - \lambda I = \begin{bmatrix} 2 - \lambda & 3 \\ 1 & 2 - \lambda \end{bmatrix} \]
Now, calculate the determinant:
\[ \det(A - \lambda I) = (2 - \lambda)(2 - \lambda) - 3 \cdot 1 \] \[ = (2 - \lambda)^2 - 3 \] \[ = 4 - 4\lambda + \lambda^2 - 3 = \lambda^2 - 4\lambda + 1 \]
Set the determinant equal to zero to find the eigenvalues:
\[ \lambda^2 - 4\lambda + 1 = 0 \]
Solve this using the quadratic formula:
\[ \lambda = \frac{4 \pm \sqrt{(-4)^2 - 4 \cdot 1 \cdot 1}}{2 \cdot 1} = \frac{4 \pm \sqrt{16 - 4}}{2} \] \[ \lambda = \frac{4 \pm \sqrt{12}}{2} = \frac{4 \pm 3.464}{2} \]
Thus, the two eigenvalues are:
\[ \lambda_1 = \frac{4 + 3.464}{2} = 3.73, \quad \lambda_2 = \frac{4 - 3.464}{2} = 0.27 \]
Therefore, the second eigenvalue is 3.73.
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).