A straightforward approach is to evaluate each term numerically (for example, via a calculator or a short computational script) and sum them. Recall that \(\sin^2 \theta = \dfrac{1 - \cos(2\theta)}{2}\). One way to see if the sum simplifies nicely is to convert each term using this identity; however, direct numerical evaluation is simple and sufficient for this finite sum: \[ \sin^2 \theta = \bigl(\sin \theta \bigr)^2. \] Using a calculator or short program: \[ \sin^2(18^\circ) + \sin^2(24^\circ) + \sin^2(36^\circ) + \sin^2(42^\circ) \]\[ + \sin^2(78^\circ) + \sin^2(90^\circ) + \sin^2(96^\circ) + \sin^2(102^\circ) + \sin^2(138^\circ) + \sin^2(162^\circ) \approx 5.5. \] Since \(5.5 = \frac{11}{2}\), the exact value of the sum is \[ \boxed{\frac{11}{2}}. \]
Let $E_1$ and $E_2$ be two independent events of a random experiment such that
$P(E_1) = \frac{1}{2}, \quad P(E_1 \cup E_2) = \frac{2}{3}$.
Then match the items of List-I with the items of List-II:
The correct match is:
In the given circuit, the potential difference across the 5 \(\mu\)F capacitor is