To determine the angle of minimum deviation (\( \delta_m \)) for a prism when the refractive index (\( n \)) is given as \( \cot\left(\frac{A}{2}\right) \), we proceed as follows:
First, let's understand the relation between the refractive index, the angle of the prism (\( A \)), and the angle of minimum deviation (\( \delta_m \)). The formula for the refractive index \( n \) in terms of the angle of deviation is:
\(n = \frac{\sin\left(\frac{A + \delta_m}{2}\right)}{\sin\left(\frac{A}{2}\right)}\)
Given that the refractive index \( n \) is \( \cot\left(\frac{A}{2}\right) \), we can set up the equation:
\(\cot\left(\frac{A}{2}\right) = \frac{\sin\left(\frac{A + \delta_m}{2}\right)}{\sin\left(\frac{A}{2}\right)}\)
We know that \(\cot\left(\frac{A}{2}\right) = \frac{\cos\left(\frac{A}{2}\right)}{\sin\left(\frac{A}{2}\right)}\). Therefore, the equation becomes:
\(\frac{\cos\left(\frac{A}{2}\right)}{\sin\left(\frac{A}{2}\right)} = \frac{\sin\left(\frac{A + \delta_m}{2}\right)}{\sin\left(\frac{A}{2}\right)}\)
Canceling \(\sin\left(\frac{A}{2}\right)\) from both sides, we get:
\(\cos\left(\frac{A}{2}\right) = \sin\left(\frac{A + \delta_m}{2}\right)\)
Using the identity \(\sin(\theta) = \cos\left(\frac{\pi}{2} - \theta\right)\), we have:
\(\sin\left(\frac{A + \delta_m}{2}\right) = \sin\left(\frac{\pi}{2} - \frac{A}{2}\right)\)
Equating angles since both are sine functions:
\(\frac{A + \delta_m}{2} = \frac{\pi}{2} - \frac{A}{2}\)
Solving for \( \delta_m \):
Thus, the angle of minimum deviation (\( \delta_m \)) is \( \pi - 2A \), confirming that the correct answer is \(\pi - 2A\).
To find the angle of minimum deviation \( \delta_{\text{min}} \):
Step 1. Given Relation:
\( \cot \frac{A}{2} = \frac{\sin \frac{A + \delta_{\text{min}}}{2}}{\sin \frac{A}{2}} \)
Step 2. Rearrange and Simplify: Take the cosine of both sides:
\( \cos \frac{A}{2} = \sin \frac{A + \delta_{\text{min}}}{2} \)
Step 3. Solve for \( \delta_{\text{min}} \): Equate the arguments, giving:
\( \frac{A + \delta_{\text{min}}}{2} = \frac{\pi}{2} - \frac{A}{2} \)
- Solving, we get:
\( \delta_{\text{min}} = \pi - 2A \)
Thus, the angle of minimum deviation is \( \pi - 2A \).
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,

Given below are two statements: One is labelled as Assertion $A$ and the other is labelled as Reason $R$
Assertion (A) : The beam of electrons show wave nature and exhibit interference and diffraction
Reason (R) : Davisson Germer Experimentally verified the wave nature of electrons
In the light of the above statements, choose the most appropriate answer from the options given below :
A small object at rest, absorbs a light pulse of power $20 \,mW$ and duration $300\, ns$. Assuming speed of light as $3 \times 10^8 \,m / s$, the momentum of the object becomes equal to :
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 : \(A_2 \rightleftharpoons 2A\)
When a light ray falls on any object, it is bounced back from the object. This process is known as the Reflection of light. The light reflected from the object falls into our eyes, making the object visible to us. All the things we see around us are because of reflection.
The reflection of light depends on the type of object. A polished or smooth surface reflects most of the light falling on it, while a rough surface absorbs some amount of light and reflects back the rest of the light. The direction of reflected rays depends upon the surface of the object.