If \( 0 \leq \alpha \leq \frac{\pi}{2} \) and \(\sin \left(\alpha - \frac{\pi}{12}\right) = \frac{1}{2}\), then \(\alpha\) is equal to:
The equation \(\sin \left(\alpha - \frac{\pi}{12}\right) = \frac{1}{2}\) suggests that \(\alpha - \frac{\pi}{12}\) must equal angles where the sine is \(\frac{1}{2}\).
These angles are typically \(\frac{\pi}{6}\) and \(\frac{5\pi}{6}\), but since \(\alpha\) is between \(0\) and \(\frac{\pi}{2}\), the angle \(\frac{5\pi}{6}\) can be disregarded.
Thus, set the equation to: \[ \alpha - \frac{\pi}{12} = \frac{\pi}{6} \] Solve for \(\alpha\): \[ \alpha = \frac{\pi}{6} + \frac{\pi}{12} = \frac{2\pi}{12} + \frac{\pi}{12} = \frac{3\pi}{12} = \frac{\pi}{4} \]
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: