Let the refractive index of a denser medium with respect to a rarer medium be `n_(12)` and its critical angle be `theta_(c)`. At an angle of incidence A when light is travelling from denser medium to rarer medium, a part of the light is reflected and the rest is refracted and the angle between reflected and refracted rays is `90^(@)`, Angle A given by -
Let the refractive index of a denser medium with respect to a rarer medium be `n_(12)` and its critical angle be `theta_(c)`. At an angle of incidence A when light is travelling from denser medium to rarer medium, a part of the light is reflected and the rest is refracted and the angle between reflected and refracted rays is `90^(@)`, Angle A given by -
A
`"tan"^(-1)("sin" theta_(c))`
B
`(1)/("tan"^(-1) ("sin"theta_(c)))`
C
`"cos"^(-1) ("sin"theta_(c))`
D
`(1)/("cos"^(-1)("sin"theta_(c)))`
Text Solution
AI Generated Solution
The correct Answer is:
To solve the problem, we need to find the angle of incidence \( A \) in terms of the critical angle \( \theta_c \) when light travels from a denser medium to a rarer medium, and the angle between the reflected and refracted rays is \( 90^\circ \).
### Step-by-Step Solution:
1. **Understanding the Critical Angle**:
The critical angle \( \theta_c \) is defined as the angle of incidence in the denser medium at which the angle of refraction in the rarer medium is \( 90^\circ \). According to Snell's law:
\[
n_{12} \sin(\theta_c) = n_{21} \sin(90^\circ)
\]
Since \( \sin(90^\circ) = 1 \), we can simplify this to:
\[
n_{12} \sin(\theta_c) = n_{21}
\]
2. **Using Snell's Law**:
When light is incident at an angle \( A \) from the denser medium to the rarer medium, we can apply Snell's law:
\[
n_{12} \sin(A) = n_{21} \sin(R)
\]
where \( R \) is the angle of refraction.
3. **Relationship Between Reflected and Refracted Rays**:
Given that the angle between the reflected ray and the refracted ray is \( 90^\circ \), we have:
\[
R + R' = 90^\circ
\]
where \( R' \) is the angle of reflection. Since the angle of reflection is equal to the angle of incidence, we have:
\[
R' = A \quad \text{and thus} \quad R + A = 90^\circ \quad \Rightarrow \quad R = 90^\circ - A
\]
4. **Substituting for R in Snell's Law**:
Substitute \( R \) into Snell's law:
\[
n_{12} \sin(A) = n_{21} \sin(90^\circ - A)
\]
Using the identity \( \sin(90^\circ - A) = \cos(A) \), we can rewrite it as:
\[
n_{12} \sin(A) = n_{21} \cos(A)
\]
5. **Rearranging the Equation**:
Rearranging gives:
\[
\frac{\sin(A)}{\cos(A)} = \frac{n_{21}}{n_{12}} \quad \Rightarrow \quad \tan(A) = \frac{n_{21}}{n_{12}}
\]
6. **Expressing in Terms of the Critical Angle**:
From the critical angle relationship, we know:
\[
\frac{n_{21}}{n_{12}} = \sin(\theta_c)
\]
Thus, we can substitute this into our equation:
\[
\tan(A) = \sin(\theta_c)
\]
7. **Finding A**:
Finally, we take the inverse tangent to find \( A \):
\[
A = \tan^{-1}(\sin(\theta_c))
\]
### Final Answer:
\[
A = \tan^{-1}(\sin(\theta_c))
\]
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