
We use the Cayley-Hamilton theorem, which states that every square matrix satisfies its own characteristic equation.
The characteristic equation is given by $\det(A - \lambda I) = 0$. 
$(1-\lambda)(4-\lambda) - (2)(-1) = 0$
$4 - 5\lambda + \lambda^2 + 2 = 0$
$\lambda^2 - 5\lambda + 6 = 0$.
According to the Cayley-Hamilton theorem, the matrix A satisfies this equation:
$A^2 - 5A + 6I = 0$.
To find an expression for $A^{-1}$, we multiply the entire equation by $A^{-1}$ (assuming A is non-singular, which it is since $\det(A) = 4 - (-2) = 6 \neq 0$).
$A^{-1}(A^2 - 5A + 6I) = A^{-1}(0)$
$A^{-1}A^2 - 5A^{-1}A + 6A^{-1}I = 0$
$A - 5I + 6A^{-1} = 0$.
Now, solve for $A^{-1}$:
$6A^{-1} = 5I - A$
$A^{-1} = \frac{5}{6}I - \frac{1}{6}A$.
We are given that $A^{-1} = \alpha I + \beta A$. Comparing the two expressions, we get:
$\alpha = \frac{5}{6}$
$\beta = -\frac{1}{6}$
We need to calculate the value of $4(\alpha - \beta)$.
$4(\alpha - \beta) = 4\left(\frac{5}{6} - \left(-\frac{1}{6}\right)\right)$
$= 4\left(\frac{5}{6} + \frac{1}{6}\right) = 4\left(\frac{6}{6}\right) = 4(1) = 4$.
Let \[ R = \begin{pmatrix} x & 0 & 0 \\ 0 & y & 0 \\ 0 & 0 & z \end{pmatrix} \text{ be a non-zero } 3 \times 3 \text{ matrix, where} \]
\[ x = \sin \theta, \quad y = \sin \left( \theta + \frac{2\pi}{3} \right), \quad z = \sin \left( \theta + \frac{4\pi}{3} \right) \]
and \( \theta \neq 0, \frac{\pi}{2}, \pi, \frac{3\pi}{2}, 2\pi \). For a square matrix \( M \), let \( \text{trace}(M) \) denote the sum of all the diagonal entries of \( M \). Then, among the statements:
Which of the following is true?
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 : \(A_2 \rightleftharpoons 2A\)
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,