Related Formula
μ = ( δ + A2) ((A)/(2))$$\mu = \frac{\sin\left(\frac{\delta_{\min} + A}{2}\right)}{\sin\left(\frac{A}{2}\right)}$$
δ = 2i - A$$\delta_{\min} = 2i - A$$
Core Logic
Given δ = A$\delta_{\min} = A$.
μ = n = ( ((A + A)/(2)))/( ((A)/(2))) = ( A)/( (A/2))$$\mu = n = \frac{\sin\left(\frac{A + A}{2}\right)}{\sin\left(\frac{A}{2}\right)} = \frac{\sin A}{\sin(A/2)}$$
n = (2 (A/2) (A/2))/( (A/2)) = 2 (A/2)$$n = \frac{2 \sin(A/2) \cos(A/2)}{\sin(A/2)} = 2 \cos(A/2)$$
Since A > 0$A > 0$, (A/2) < 1$\cos(A/2) < 1$. Thus, n < 2$n < 2$.
Step 1: Applying Physical Bounds
At minimum deviation, i = δ + A2$i = \frac{\delta_{\min} + A}{2}$.
Since δ = A$\delta_{\min} = A$, we have i = (2A)/(2) = A$i = \frac{2A}{2} = A$.
For light to enter the prism, the angle of incidence must be less than 90^°$90^\circ$ (grazing incidence is the limit).
Thus, i < 90^° ⇒ A < 90^°$i < 90^\circ \Rightarrow A < 90^\circ$.
Step 2: Calculate Limits for n
Since A < 90^°$A < 90^\circ$, we have A/2 < 45^°$A/2 < 45^\circ$.
The cosine function is strictly decreasing in the first quadrant, so:
If A/2 < 45^°$A/2 < 45^\circ$, then (A/2) > (45^°) = 1√(2)$\cos(A/2) > \cos(45^\circ) = \frac{1}{\sqrt{2}}$.
Therefore:
n = 2 (A/2) > 2 × 1√(2) = √(2)$$n = 2 \cos(A/2) > 2 \times \frac{1}{\sqrt{2}} = \sqrt{2}$$
Combining the limits:
√(2) < n < 2$$\sqrt{2} < n < 2$$
Pattern Recognition
When δmin = A$\delta_{min} = A$, μ = 2 (A/2)$\mu = 2\cos(A/2)$. The extreme bounding conditions arise from A > 0$A > 0$ and i < 90^°$i < 90^\circ$. This guarantees the theoretical range √(2) < μ < 2$\sqrt{2} < \mu < 2$.
Chapter Mix
Class 12 Physics: Ray Optics and Optical Instruments