The intensity in an interference pattern is given by: \[ I = I_0 \left( 1 + \cos \delta \right) \] where \( \delta \) is the phase difference given by: \[ \delta = \frac{2\pi}{\lambda} \cdot \text{path difference} \] Substitute the given path difference \( \frac{\lambda}{8} \): \[ \delta = \frac{2\pi}{\lambda} \cdot \frac{\lambda}{8} = \frac{\pi}{4} \] Thus, the intensity is: \[ I = I_0 \left( 1 + \cos \frac{\pi}{4} \right) = I_0 \left( 1 + \frac{\sqrt{2}}{2} \right) \] \[ I = I_0 \left( 1 + 0.707 \right) = 1.707 I_0 \] Thus, the intensity at the point is \( 1.707 I_0 \).
In a Young's double-slit experiment, two light waves with intensity \( I_0 \) interfere at a point on the screen, and the path difference between them is \( \frac{\lambda}{8} \). We are tasked with finding the intensity at this point.
- Interference of Light: In an interference experiment, such as Young's double-slit, light waves from two slits interfere with each other. The resulting intensity depends on the phase difference between the waves at the point where they meet.
- Path Difference and Phase Difference: The phase difference (\( \Delta \phi \)) between the two waves is related to the path difference (\( \Delta x \)) by the equation:
\[ \Delta \phi = \frac{2 \pi \Delta x}{\lambda} \]
- Here, the path difference is \( \Delta x = \frac{\lambda}{8} \), so the phase difference is:
\[ \Delta \phi = \frac{2 \pi \times \frac{\lambda}{8}}{\lambda} = \frac{\pi}{4} \]
The total intensity \( I \) at the point where two waves interfere is given by the formula:
\[ I = I_1 + I_2 + 2 \sqrt{I_1 I_2} \cos(\Delta \phi) \]
- Since both waves have the same intensity \( I_0 \), the formula becomes:
\[ I = I_0 + I_0 + 2 \sqrt{I_0 I_0} \cos(\Delta \phi) \]
\[ I = 2I_0 + 2I_0 \cos(\frac{\pi}{4}) \]
We know that \( \cos\left(\frac{\pi}{4}\right) = \frac{1}{\sqrt{2}} \), so the intensity is:
\[ I = 2I_0 + 2I_0 \times \frac{1}{\sqrt{2}} \]
\[ I = 2I_0 \left( 1 + \frac{1}{\sqrt{2}} \right) \]
Now, simplifying this expression:
\[ I = 2I_0 \left( \frac{\sqrt{2} + 1}{\sqrt{2}} \right) \]
The intensity at the point on the screen where the path difference is \( \frac{\lambda}{8} \) is:
\[ I = 2I_0 \left( \frac{\sqrt{2} + 1}{\sqrt{2}} \right) \]
Alexia Limited invited applications for issuing 1,00,000 equity shares of ₹ 10 each at premium of ₹ 10 per share.
The amount was payable as follows:
Applications were received for 1,50,000 equity shares and allotment was made to the applicants as follows:
Category A: Applicants for 90,000 shares were allotted 70,000 shares.
Category B: Applicants for 60,000 shares were allotted 30,000 shares.
Excess money received on application was adjusted towards allotment and first and final call.
Shekhar, who had applied for 1200 shares failed to pay the first and final call. Shekhar belonged to category B.
Pass necessary journal entries for the above transactions in the books of Alexia Limited. Open calls in arrears and calls in advance account, wherever necessary.
