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The wavelengths of given light waves in ...

The wavelengths of given light waves in air and in a medium are 6000 A and 4000 A, respectively. The angle of total internal reflection is .

A

`sin^(-1)(2/3)`

B

`sin^(-1)(3/4)`

C

`sin^(-1)(8/9)`

D

`sin^(-1)(1/2)`

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To solve the problem of finding the angle of total internal reflection given the wavelengths of light in air and in a medium, we can follow these steps: ### Step-by-Step Solution: 1. **Identify the Wavelengths:** - Wavelength in air (λ_air) = 6000 Å - Wavelength in medium (λ_medium) = 4000 Å 2. **Calculate the Refractive Index (n) of the Medium:** - The refractive index (n) is given by the formula: \[ n = \frac{\lambda_{\text{air}}}{\lambda_{\text{medium}}} \] - Substituting the values: \[ n = \frac{6000 \, \text{Å}}{4000 \, \text{Å}} = \frac{6000}{4000} = \frac{3}{2} \] 3. **Understanding Total Internal Reflection:** - Total internal reflection occurs when light travels from a denser medium (in this case, the medium with n = 3/2) to a rarer medium (air, where n = 1). - The critical angle (θ_c) is the angle of incidence at which the angle of refraction is 90 degrees. 4. **Apply Snell's Law:** - According to Snell's Law: \[ n_1 \sin(\theta_1) = n_2 \sin(\theta_2) \] - For total internal reflection: - \( n_1 = \frac{3}{2} \) (refractive index of the medium) - \( n_2 = 1 \) (refractive index of air) - \( \theta_2 = 90^\circ \) - Thus, we have: \[ \frac{3}{2} \sin(\theta_c) = 1 \cdot \sin(90^\circ) \] - Since \(\sin(90^\circ) = 1\), we can simplify this to: \[ \frac{3}{2} \sin(\theta_c) = 1 \] 5. **Solve for the Critical Angle (θ_c):** - Rearranging gives: \[ \sin(\theta_c) = \frac{2}{3} \] - Now, to find the critical angle: \[ \theta_c = \sin^{-1}\left(\frac{2}{3}\right) \] 6. **Conclusion:** - The angle of total internal reflection is: \[ \theta_c = \sin^{-1}\left(\frac{2}{3}\right) \]
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