For an incoherent wave:
The intensity \( I_1 \) is the sum of the individual intensities \( I_A \) and \( I_B \):
\[ I_1 = I_A + I_B \quad \Rightarrow \quad I_1 = I_0 + 9I_0 = 10I_0 \]
For a coherent wave:
The intensity \( I_2 \) is given by the formula:
\[ I_2 = I_A + I_B + 2 \sqrt{I_A I_B} \cos(60^\circ) \]
Substituting the values and simplifying:
\[ I_2 = I_0 + 9I_0 + 2 \sqrt{I_0 I_0} \cdot \cos(60^\circ) = 13I_0 \]
Finally, the ratio of the intensities \( I_1 \) and \( I_2 \) is:
\[ \frac{I_1}{I_2} = \frac{10I_0}{13I_0} = \frac{10}{13} \]
For incoherent waves:
\[ I_1 = I_A + I_B = I_0 + 9I_0 = 10I_0 \]For coherent waves:
\[ I_2 = I_A + I_B + 2\sqrt{I_A I_B} \cos 60^\circ \] \[ I_2 = I_0 + 9I_0 + 2\sqrt{I_0 \times 9I_0} \cdot \frac{1}{2} = 13I_0 \]Given:
\[ \frac{I_1}{I_2} = \frac{10}{13} \]Thus:
\[ x = 13 \]
An infinitely long straight wire carrying current $I$ is bent in a planar shape as shown in the diagram. The radius of the circular part is $r$. The magnetic field at the centre $O$ of the circular loop is :



Two loudspeakers (\(L_1\) and \(L_2\)) are placed with a separation of \(10 \, \text{m}\), as shown in the figure. Both speakers are fed with an audio input signal of the same frequency with constant volume. A voice recorder, initially at point \(A\), at equidistance to both loudspeakers, is moved by \(25 \, \text{m}\) along the line \(AB\) while monitoring the audio signal. The measured signal was found to undergo \(10\) cycles of minima and maxima during the movement. The frequency of the input signal is _____________ Hz.
(Speed of sound in air is \(324 \, \text{m/s}\) and \( \sqrt{5} = 2.23 \)) 
Consider the following reaction sequence.

Foot of perpendicular from origin on a line passing through $(1, 1, 1)$ having direction ratios $\langle 2, 3, 4 \rangle$, is: