A ray of light passes through an equilateral glass prism in such a manner that the angle of incidence is equal to the angle of emergence, and each of these angles is equal to (3/4)th of the angle of the prism. The angle of deviation is:
30°
Understanding how light behaves when it passes through a prism is a fundamental concept in optics. This problem involves calculating the angle of deviation for a ray of light passing through an equilateral glass prism under specific conditions.
Let's break down the given information:
First, let's calculate the value of the angle of incidence ($i$) and the angle of emergence ($e$).
Given $A = 60^\circ$, we have:
$$i = e = \frac{3}{4} \times 60^\circ$$
$$i = e = 3 \times \frac{60^\circ}{4}$$
$$i = e = 3 \times 15^\circ$$
$$i = e = 45^\circ$$
So, the angle of incidence and the angle of emergence are both 45°.
Now, we need to find the angle of deviation ($\delta$). The general formula relating the angle of deviation, angle of incidence, angle of emergence, and angle of the prism is:
$$\delta = i + e - A$$
Substitute the calculated values of $i$, $e$, and $A$ into this formula:
$$\delta = 45^\circ + 45^\circ - 60^\circ$$
$$\delta = 90^\circ - 60^\circ$$
$$\delta = 30^\circ$$
Thus, the angle of deviation is 30°.
Let's recap the key terms used in this problem:
There is also a relationship between the angles inside the prism and the angle of the prism:
$$A = r_1 + r_2$$
And as used above, the angle of deviation is given by:
$$\delta = i + e - A$$
The condition where the angle of incidence is equal to the angle of emergence ($i=e$) corresponds to the condition of minimum deviation ($\delta_{min}$). When a prism is at minimum deviation, the ray inside the prism is parallel to the base of the prism, and the angles of refraction are also equal ($r_1 = r_2$).
In our problem, $i=e$, which suggests this is a minimum deviation case. Let's check if $r_1=r_2$. At minimum deviation, $r_1 = r_2 = A/2$. For $A=60^\circ$, $r_1 = r_2 = 60^\circ/2 = 30^\circ$.
We can also use Snell's Law at the first surface: $n_1 \sin(i) = n_2 \sin(r_1)$, where $n_1$ is the refractive index of the medium outside (usually air, $n_1 \approx 1$) and $n_2$ is the refractive index of the prism glass ($n_2$).
Using our calculated values: $i=45^\circ$ and $r_1=30^\circ$ (assuming minimum deviation):
$$1 \times \sin(45^\circ) = n_2 \times \sin(30^\circ)$$
$$\frac{\sqrt{2}}{2} = n_2 \times \frac{1}{2}$$
$$n_2 = \sqrt{2} \approx 1.414$$
This refractive index is reasonable for glass. This confirms that the given conditions ($i=e = \frac{3}{4}A$) indeed correspond to the case of minimum deviation for a glass prism with refractive index $\sqrt{2}$. However, calculating the refractive index was not required to find the angle of deviation, as the formula $\delta = i + e - A$ directly uses the given information.
| Parameter | Symbol | Value (Given/Calculated) |
|---|---|---|
| Angle of Prism | $A$ | $60^\circ$ (Equilateral) |
| Relation $i, e$ to $A$ | $i=e$ | $i = e = \frac{3}{4}A$ |
| Angle of Incidence | $i$ | $45^\circ$ |
| Angle of Emergence | $e$ | $45^\circ$ |
| Angle of Deviation | $\delta$ | $30^\circ$ |
| Concept | Formula |
|---|---|
| Angle of Deviation | $\delta = i + e - A$ |
| Relationship of internal angles to Prism Angle | $A = r_1 + r_2$ |
| Snell's Law at first surface | $n_1 \sin i = n_2 \sin r_1$ |
| Snell's Law at second surface | $n_2 \sin r_2 = n_1 \sin e$ |
| Minimum Deviation Condition | $i = e$ and $r_1 = r_2 = A/2$ |
| Angle of Minimum Deviation ($\delta_{min}$) | $\delta_{min} = 2i_{min} - A$ (where $i_{min}$ is angle of incidence at min deviation) |
| Refractive Index ($n_2$) at Minimum Deviation | $n_2 = \frac{\sin((A + \delta_{min})/2)}{\sin(A/2)}$ |
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