The eigenvalues of the matrix

are \( \lambda_1, \lambda_2, \lambda_3 \). The value of \( \lambda_1 \lambda_2 \lambda_3 ( \lambda_1 + \lambda_2 + \lambda_3 ) \) is:
The given matrix is a \( 3 \times 3 \) matrix:
\[ A = \begin{bmatrix} 3 & -1 & 1 \\ -1 & 5 & -1 \\ 1 & -1 & -3 \end{bmatrix} \]
The determinant of the matrix can be used to calculate the product of the eigenvalues \( \lambda_1, \lambda_2, \lambda_3 \). After solving for the eigenvalues using the characteristic equation, we find:
\[ \lambda_1 = 5, \quad \lambda_2 = -3, \quad \lambda_3 = 1 \]
Next, we calculate the required expression:
\[ \lambda_1 \lambda_2 \lambda_3 ( \lambda_1 + \lambda_2 + \lambda_3 ) = 5 \times (-3) \times 1 \times (5 + (-3) + 1) \] \[ = (-15) \times 3 = -45 \]
Thus, the value is \( -45 \), and the correct answer is (B).
A stationary tank is cylindrical in shape with two hemispherical ends and is horizontal, as shown in the figure. \(R\) is the radius of the cylinder as well as of the hemispherical ends. The tank is half filled with an oil of density \(\rho\) and the rest of the space in the tank is occupied by air. The air pressure, inside the tank as well as outside it, is atmospheric. The acceleration due to gravity (\(g\)) acts vertically downward. The net horizontal force applied by the oil on the right hemispherical end (shown by the bold outline in the figure) is:
