The elastic potential energy stored in a stretched wire is given by: \[ U = \frac{1}{2} \times \frac{F \Delta L}{A Y}, \] where:
Rearranging the formula for \( A \): \[ A = \frac{F \Delta L}{2 U Y}. \] The force \( F \) is given by: \[ F = Y \times \frac{\Delta L}{L}. \] Substitute \( F \) back into the equation for \( A \): \[ A = \frac{Y \times \frac{\Delta L}{L} \times \Delta L}{2 U Y} = \frac{\Delta L^2}{2 U \times L}. \] Substitute the given values: \[ A = \frac{(0.02)^2}{2 \times 80 \times 20} = \frac{0.0004}{3200}. \] Simplify: \[ A = 1.25 \times 10^{-7} \, \text{m}^2. \] Convert \( \text{m}^2 \) to \( \text{mm}^2 \): \[ A = 1.25 \times 10^{-7} \times 10^{6} = 0.125 \, \text{mm}^2. \]
Let \( a \in \mathbb{R} \) and \( A \) be a matrix of order \( 3 \times 3 \) such that \( \det(A) = -4 \) and \[ A + I = \begin{bmatrix} 1 & a & 1 \\ 2 & 1 & 0 \\ a & 1 & 2 \end{bmatrix} \] where \( I \) is the identity matrix of order \( 3 \times 3 \).
If \( \det\left( (a + 1) \cdot \text{adj}\left( (a - 1) A \right) \right) \) is \( 2^m 3^n \), \( m, n \in \{ 0, 1, 2, \dots, 20 \} \), then \( m + n \) is equal to:
Rate law for a reaction between $A$ and $B$ is given by $\mathrm{R}=\mathrm{k}[\mathrm{A}]^{\mathrm{n}}[\mathrm{B}]^{\mathrm{m}}$. If concentration of A is doubled and concentration of B is halved from their initial value, the ratio of new rate of reaction to the initial rate of reaction $\left(\frac{\mathrm{r}_{2}}{\mathrm{r}_{1}}\right)$ is