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When a mica plate of thickness 0.1mm is ...

When a mica plate of thickness `0.1mm` is introduced in one of the interfering beams, the central fringe is displaced by a distance equal to 10 fringes. If the wavelength of the light is `6000 A^(0)`, the refractive index of the mica is

A

`1.06`

B

`1.6`

C

`2.4`

D

`1.2`

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To find the refractive index of the mica plate, we can follow these steps: ### Step 1: Understand the relationship between fringe shift and refractive index When a mica plate is introduced in one of the interfering beams, it causes a path length change that results in a fringe shift. The formula for the fringe shift (Δx) when a mica plate of thickness \( t \) and refractive index \( \mu \) is introduced is given by: \[ \Delta x = \frac{\beta}{\lambda} \cdot ( \mu - 1 ) \cdot t \] Where: - \( \Delta x \) = fringe shift (in terms of fringe width) - \( \beta \) = fringe width - \( \lambda \) = wavelength of light - \( t \) = thickness of the mica plate - \( \mu \) = refractive index of the mica ### Step 2: Relate fringe shift to the number of fringes It is given that the central fringe is displaced by a distance equal to 10 fringes. Therefore, we can express the fringe shift as: \[ \Delta x = 10 \cdot \beta \] ### Step 3: Substitute the expression for fringe shift into the formula Substituting \( \Delta x = 10 \cdot \beta \) into the original formula gives us: \[ 10 \cdot \beta = \frac{\beta}{\lambda} \cdot ( \mu - 1 ) \cdot t \] ### Step 4: Cancel out \( \beta \) Assuming \( \beta \neq 0 \), we can cancel \( \beta \) from both sides: \[ 10 = \frac{1}{\lambda} \cdot ( \mu - 1 ) \cdot t \] ### Step 5: Rearrange the equation to solve for \( \mu - 1 \) Rearranging the equation gives: \[ \mu - 1 = 10 \cdot \frac{\lambda}{t} \] ### Step 6: Substitute the known values Now, substitute the values for \( \lambda \) and \( t \): - \( \lambda = 6000 \, \text{Å} = 6000 \times 10^{-10} \, \text{m} \) - \( t = 0.1 \, \text{mm} = 0.1 \times 10^{-3} \, \text{m} = 10^{-4} \, \text{m} \) Substituting these values into the equation: \[ \mu - 1 = 10 \cdot \frac{6000 \times 10^{-10}}{0.1 \times 10^{-3}} \] ### Step 7: Calculate \( \mu - 1 \) Calculating the right side: \[ \mu - 1 = 10 \cdot \frac{6000 \times 10^{-10}}{10^{-4}} = 10 \cdot 6000 \times 10^{-6} = 60 \times 10^{-6} = 0.06 \] ### Step 8: Solve for \( \mu \) Now, adding 1 to both sides gives: \[ \mu = 1 + 0.06 = 1.06 \] ### Conclusion The refractive index of the mica is: \[ \mu = 1.06 \]
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AAKASH SERIES-WAVES OPTICS-EXERCISE -II (INTERFERENCE)
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  2. A screen is at a distance of 2m from narrow slits that are illuminated...

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  3. In Young's double slit experiment with a mono - chromatic light of wav...

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  4. In Young.s double slit interference experiment the wavelength of ligh...

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  5. The intensity of central fringe in the interference pattern produced b...

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  6. In the case of interference, the maximum and minimum intensities are i...

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  7. In a double slit experiment, the distance between two slits in 0.6 mm ...

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  8. In Young.s double slit experiment, blue-green light of wavelength 500n...

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  10. When a mica plate of thickness 0.1mm is introduced in one of the inter...

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  11. The maximum numbers of possible interference maxima for slit separatio...

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  14. In Young's double slit experiment, the 10^(th) maximum of wavelength ...

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  15. The path difference between two interfering waves at a point on the sc...

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  16. In Young.s double slit experiment with monochromatic source of light o...

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  17. A mixture of light, consisting of wavelength 590 nm and an unknown wav...

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  18. A monochromatice light beam of wavelength 5896 A^(0) is used in double...

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