We start with the given expression: \[ \alpha = \tan^2 x + \cot^2 x \] This can be transformed using the identity \( \tan x \cdot \cot x = 1 \) to relate \( \tan x \) and \( \cot x \).
Recognizing that \( \tan^2 x \) and \( \cot^2 x \) are reciprocal squares, we can apply the identity: \[ \tan^2 x + \cot^2 x = \sec^2 x + \csc^2 x - 2 \] Using the pythagorean identities \( \sec^2 x = 1 + \tan^2 x \) and \( \csc^2 x = 1 + \cot^2 x \), we realize: \[ \sec^2 x + \csc^2 x = (1 + \tan^2 x) + (1 + \cot^2 x) = 2 + (\tan^2 x + \cot^2 x) = 2 + \alpha \] Thus, we see: \[ \alpha = \sec^2 x + \csc^2 x - 2 \] The values \( \sec^2 x \) and \( \csc^2 x \) are always greater than or equal to 1 in the interval \( (0, \frac{\pi}{2}) \), so \( \alpha = \sec^2 x + \csc^2 x - 2 \) must be greater than or equal to 2: \[ \alpha \geq 2 \] Given that \( \alpha \) can grow infinitely as \( x \) approaches 0 or \( \frac{\pi}{2} \) (where \( \tan x \) or \( \cot x \) blow up), \( \alpha \) indeed lies in the interval \( [2, \infty) \).
The area bounded by the parabola \(y = x^2 + 2\) and the lines \(y = x\), \(x = 1\) and \(x = 2\) (in square units) is:
For the reaction:
\[ 2A + B \rightarrow 2C + D \]
The following kinetic data were obtained for three different experiments performed at the same temperature:
\[ \begin{array}{|c|c|c|c|} \hline \text{Experiment} & [A]_0 \, (\text{M}) & [B]_0 \, (\text{M}) & \text{Initial rate} \, (\text{M/s}) \\ \hline I & 0.10 & 0.10 & 0.10 \\ II & 0.20 & 0.10 & 0.40 \\ III & 0.20 & 0.20 & 0.40 \\ \hline \end{array} \]
The total order and order in [B] for the reaction are respectively: