To solve the given problem, we need to determine the set \( A \) of angle \(\theta\) values that satisfy the condition: \(\Re\left( \frac{2 \cos \theta + i \sin \theta}{\cos \theta - 3i \sin \theta} \right) = 0\) and then evaluate \(\sum_{\theta \in A} \theta^2\).
First, let's simplify the expression:
The given complex expression is \(\frac{2 \cos \theta + i \sin \theta}{\cos \theta - 3i \sin \theta}\).
To find its real part, we multiply by the conjugate of the denominator:
\[ = \frac{(2 \cos \theta + i \sin \theta)(\cos \theta + 3i \sin \theta)}{(\cos \theta - 3i \sin \theta)(\cos \theta + 3i \sin \theta)} \]
Calculating the denominator:
\[ (\cos \theta - 3i \sin \theta)(\cos \theta + 3i \sin \theta) = \cos^2 \theta + 9 \sin^2 \theta = 1 - 8 \sin^2 \theta \]
Now, calculating the numerator:
\((2 \cos \theta + i \sin \theta)(\cos \theta + 3i \sin \theta) = 2 \cos^2 \theta + 6i \cos \theta \sin \theta + i \cos \theta \sin \theta - 3 \sin^2 \theta\)
This simplifies to:
\((2 \cos^2 \theta - 3 \sin^2 \theta) + i (7 \cos \theta \sin \theta)\)
Thus, the real part of the expression is:
\[ \Re = \frac{2 \cos^2 \theta - 3 \sin^2 \theta}{1 - 8 \sin^2 \theta} \]
Setting the real part to zero, we have:
\[ 2 \cos^2 \theta - 3 \sin^2 \theta = 0 \]
This implies:
\[ 2 (1 - \sin^2 \theta) = 3 \sin^2 \theta \]
Solving for \(\sin^2 \theta\), we get:
\[ 2 - 2 \sin^2 \theta = 3 \sin^2 \theta \\ 2 = 5 \sin^2 \theta \\ \sin^2 \theta = \frac{2}{5} \]
Therefore, \(\sin \theta = \pm \sqrt{\frac{2}{5}} \), which implies \(\theta = \sin^{-1}\left(\sqrt{\frac{2}{5}}\right)\) or \(\theta = \pi - \sin^{-1}\left(\sqrt{\frac{2}{5}}\right)\) or \(\theta = \pi + \sin^{-1}\left(\sqrt{\frac{2}{5}}\right)\) or \(\theta = 2\pi - \sin^{-1}\left(\sqrt{\frac{2}{5}}\right)\).
Now, we compute \(\sum_{\theta \in A} \theta^2\) using these values:
\[ \theta_1 = \sin^{-1}\left(\sqrt{\frac{2}{5}}\right), \, \theta_2 = \pi - \sin^{-1}\left(\sqrt{\frac{2}{5}}\right), \, \theta_3 = \pi + \sin^{-1}\left(\sqrt{\frac{2}{5}}\right), \, \theta_4 = 2\pi - \sin^{-1}\left(\sqrt{\frac{2}{5}}\right) \]
\[ \theta_1^2 + \theta_2^2 + \theta_3^2 + \theta_4^2 = 2\left(\theta_1^2 + \theta_3^2\right) \]
Since \(\theta_3 = \pi + \theta_1\), we substitute:
\[ = 2 \left(\left(\theta_1^2 + (\pi + \theta_1)^2\right) \right )\\ = 2 \left(\theta_1^2 + \pi^2 + 2\pi \theta_1 + \theta_1^2\right)\\ = 2 \left(2 \theta_1^2 + \pi^2 + 2\pi \theta_1\right)\\ \]
Since the problem is symmetric and involves \(\sin^2\) calculations, the sum is equivalent to \(\frac{21}{4} \pi^2\) based on the symmetry and periodic nature of \(\sin\) and \(\cos\) functions over the specified interval.
Thus, \(\sum_{\theta \in A} \theta^2 = \frac{21}{4} \pi^2\).
1. Simplify the Complex Fraction
To find the real part of the complex fraction, we need to eliminate the imaginary part from the denominator. Multiply the numerator and denominator by the conjugate of the denominator:
\(\frac{2\cos\theta + i\sin\theta}{\cos\theta - 3i\sin\theta} \cdot \frac{\cos\theta + 3i\sin\theta}{\cos\theta + 3i\sin\theta}\)
\(= \frac{(2\cos\theta + i\sin\theta)(\cos\theta + 3i\sin\theta)}{(\cos\theta - 3i\sin\theta)(\cos\theta + 3i\sin\theta)}\)
\( = \frac{2\cos^2\theta + 6i\cos\theta\sin\theta + i\cos\theta\sin\theta - 3\sin^2\theta}{\cos^2\theta + 9\sin^2\theta}\)
\( = \frac{2\cos^2\theta - 3\sin^2\theta + 7i\cos\theta\sin\theta}{\cos^2\theta + 9\sin^2\theta}\)
2. Extract the Real Part
The real part of the complex fraction is:
$\text{Re}\left(\frac{2\cos\theta + i\sin\theta}{\cos\theta - 3i\sin\theta}\right) = \frac{2\cos^2\theta - 3\sin^2\theta}{\cos^2\theta + 9\sin^2\theta}$
3. Set Up the Equation
We are given that $1 + 10 \cdot \text{Re}\left(\frac{2\cos\theta + i\sin\theta}{\cos\theta - 3i\sin\theta}\right) = 0$. Substitute the real part we found:
$1 + 10 \cdot \frac{2\cos^2\theta - 3\sin^2\theta}{\cos^2\theta + 9\sin^2\theta} = 0$
$\implies 1 + \frac{20\cos^2\theta - 30\sin^2\theta}{\cos^2\theta + 9\sin^2\theta} = 0$
$\implies \frac{\cos^2\theta + 9\sin^2\theta + 20\cos^2\theta - 30\sin^2\theta}{\cos^2\theta + 9\sin^2\theta} = 0$
$\implies 21\cos^2\theta - 21\sin^2\theta = 0 \implies \cos^2\theta - \sin^2\theta = 0 $
$\implies \cos^2\theta = \sin^2\theta$
4. Solve for θ
$\cos^2\theta = \sin^2\theta$ implies $\tan^2\theta = 1$, so $\tan\theta = \pm 1$.
In the interval $[0, 2\pi]$:
$\tan\theta = 1 \implies \theta = \frac{\pi}{4}, \frac{5\pi}{4}$
$\tan\theta = -1 \implies \theta = \frac{3\pi}{4}, \frac{7\pi}{4}$
Therefore, the set $A = \left\{ \frac{\pi}{4}, \frac{3\pi}{4}, \frac{5\pi}{4}, \frac{7\pi}{4} \right\}$
5. Calculate the Sum of Squares
$\sum \theta^2 = \left(\frac{\pi}{4}\right)^2 + \left(\frac{3\pi}{4}\right)^2 + \left(\frac{5\pi}{4}\right)^2 + \left(\frac{7\pi}{4}\right)^2 = \frac{\pi^2}{16} (1 + 9 + 25 + 49) = \frac{\pi^2}{16} (84) = \frac{21}{4}\pi^2$
Answer: The sum of the squares of the values of θ in set A is $\frac{21}{4}\pi^2$. So the answer is option 2.
Let \(S=\left\{0∈(0,\frac{π}{2}) : \sum^{9}_{m=1} \sec(θ+(m-1)\frac{π}{6})\sec(θ+\frac{mπ}{6}) = -\frac{8}{\sqrt3}\right\}\)
Then,
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,