1. Rationalize the denominator:
To determine when the expression is purely real, we need to eliminate the imaginary part from the denominator. We do this by multiplying both the numerator and the denominator by the complex conjugate of the denominator:
$\frac{1 - i \sin \alpha}{1 + 2i \sin \alpha} \cdot \frac{1 - 2i \sin \alpha}{1 - 2i \sin \alpha}$
2. Expand and Simplify:
Expanding the numerator and the denominator:
Numerator: $(1 - i \sin \alpha)(1 - 2i \sin \alpha) = 1 - 2i \sin \alpha - i \sin \alpha + 2i^2 \sin^2 \alpha = 1 - 3i \sin \alpha - 2 \sin^2 \alpha$
Denominator: $(1 + 2i \sin \alpha)(1 - 2i \sin \alpha) = 1 - (2i \sin \alpha)^2 = 1 + 4 \sin^2 \alpha$
3. Combine and Separate Real and Imaginary Parts:
Therefore, the expression becomes:
$\frac{1 - 2 \sin^2 \alpha - 3i \sin \alpha}{1 + 4 \sin^2 \alpha} = \frac{1 - 2 \sin^2 \alpha}{1 + 4 \sin^2 \alpha} - i \frac{3 \sin \alpha}{1 + 4 \sin^2 \alpha}$
4. Condition for Purely Real:
For the expression to be purely real, the imaginary part must be zero. This means:
$\frac{3 \sin \alpha}{1 + 4 \sin^2 \alpha} = 0$
5. Solve for α:
This implies that $\sin \alpha = 0$. The solutions to this equation are:
$\alpha = n\pi$, where n is an integer.
6. Consider the domain (n ∈ N):
Since n ∈ N (natural numbers), the solution remains $\alpha = n\pi$.
Conclusion: The real value of 'α' for which the given expression is purely real is $\alpha = n\pi$, where n is a natural number.
Correct Answer: (C) $n\pi$, n ∈ N
Let the given expression be denoted by \( z \):
\[ z = \frac{1 - i \sin \alpha}{1 + 2i \sin \alpha} \]For \( z \) to be purely real, its imaginary part must be zero. We can find the real and imaginary parts by multiplying the numerator and denominator by the conjugate of the denominator:
\[ z = \frac{(1 - i \sin \alpha)(1 - 2i \sin \alpha)}{(1 + 2i \sin \alpha)(1 - 2i \sin \alpha)} = \frac{1 - 2i \sin \alpha - i \sin \alpha + 2i^2 \sin^2 \alpha}{1 + 4 \sin^2 \alpha} = \frac{1 - 3i \sin \alpha - 2 \sin^2 \alpha}{1 + 4 \sin^2 \alpha} \]Separating the real and imaginary parts:
For \( z \) to be purely real, the imaginary part must be zero:
\[ \frac{-3 \sin \alpha}{1 + 4 \sin^2 \alpha} = 0 \]This implies that the numerator must be zero:
\[ -3 \sin \alpha = 0 \] \[ \sin \alpha = 0 \]The general solution for \( \sin \alpha = 0 \) is given by:
\[ \alpha = n\pi \]where \( n \) is an integer (\( n \in \mathbb{Z} \)).
Therefore, the real values of \( \alpha \) for which the given expression is purely real are \( \alpha = n\pi \), where \( n \) is an integer.
Final Answer: The final answer is \( {n\pi} \).
In an experiment to determine the figure of merit of a galvanometer by half deflection method, a student constructed the following circuit. He applied a resistance of \( 520 \, \Omega \) in \( R \). When \( K_1 \) is closed and \( K_2 \) is open, the deflection observed in the galvanometer is 20 div. When \( K_1 \) is also closed and a resistance of \( 90 \, \Omega \) is removed in \( S \), the deflection becomes 13 div. The resistance of galvanometer is nearly:
A wooden block of mass M lies on a rough floor. Another wooden block of the same mass is hanging from the point O through strings as shown in the figure. To achieve equilibrium, the coefficient of static friction between the block on the floor and the floor itself is