1.33
1.6
1.25
1.45
1.4
\[ \frac{1}{f} = (n_{\text{lens}} - n_{\text{medium}}) \left( \frac{1}{R_1} - \frac{1}{R_2} \right) \]
where:
- \( f \) is the focal length of the lens,
- \( n_{\text{lens}} \) is the refractive index of the lens material,
- \( n_{\text{medium}} \) is the refractive index of the surrounding medium,
- \( R_1 \) and \( R_2 \) are the radii of curvature of the lens surfaces.
Given:
- \( n_{\text{lens}} = 1.5 \),
- \( f_{\text{air}} = 10 \text{ cm} \),
- \( f_{\text{fluid}} = 70 \text{ cm} \).
First, we find the curvature term using the focal length in air (\( n_{\text{medium}} = 1 \)):
\[ \frac{1}{10} = (1.5 - 1) \left( \frac{1}{R_1} - \frac{1}{R_2} \right) \]
\[ \frac{1}{10} = 0.5 \left( \frac{1}{R_1} - \frac{1}{R_2} \right) \]
\[ \frac{1}{R_1} - \frac{1}{R_2} = \frac{1}{10 \times 0.5} = \frac{1}{5} \]
Next, we use the same curvature term with the focal length in the fluid to find the refractive index of the fluid \( n_{\text{fluid}} \):
\[ \frac{1}{70} = (1.5 - n_{\text{fluid}}) \left( \frac{1}{R_1} - \frac{1}{R_2} \right) \]
Substitute \( \frac{1}{R_1} - \frac{1}{R_2} = \frac{1}{5} \):
\[ \frac{1}{70} = (1.5 - n_{\text{fluid}}) \times \frac{1}{5} \]
\[ \frac{1}{70} = \frac{1.5 - n_{\text{fluid}}}{5} \]
\[ 5 \times \frac{1}{70} = 1.5 - n_{\text{fluid}} \]
\[ \frac{1}{14} = 1.5 - n_{\text{fluid}} \]
\[ n_{\text{fluid}} = 1.5 - \frac{1}{14} \]
\[ n_{\text{fluid}} = 1.5 - 0.0714 \]
\[ n_{\text{fluid}} = 1.4286 \]
Thus, the refractive index of the fluid is approximately \( 1.42 \).
So The correct answer is Option(E):1.4 nearest matching answer
Step 1: Recall the lens maker's formula.
The focal length of a thin convex lens is given by the lens maker's formula:
\[ \frac{1}{f} = (n - 1) \left( \frac{1}{R_1} - \frac{1}{R_2} \right), \]
where:
In air, the refractive index of the lens relative to air is \( n_{\text{air}} = \frac{n_{\text{lens}}}{n_{\text{air}}} = 1.5 \), where \( n_{\text{lens}} = 1.5 \) and \( n_{\text{air}} = 1 \).
In the fluid, the refractive index of the lens relative to the fluid is \( n_{\text{fluid}} = \frac{n_{\text{lens}}}{n_{\text{fluid}}} \), where \( n_{\text{fluid}} \) is the refractive index of the fluid.
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Step 2: Write the lens maker's formula for both cases.
(i) In air:
\[ \frac{1}{f_{\text{air}}} = (n_{\text{air}} - 1) \left( \frac{1}{R_1} - \frac{1}{R_2} \right). \]
Substitute \( f_{\text{air}} = 10 \, \text{cm} \) and \( n_{\text{air}} = 1.5 \):
\[ \frac{1}{10} = (1.5 - 1) \left( \frac{1}{R_1} - \frac{1}{R_2} \right). \]
Simplify:
\[ \frac{1}{10} = 0.5 \left( \frac{1}{R_1} - \frac{1}{R_2} \right). \]
\[ \frac{1}{R_1} - \frac{1}{R_2} = \frac{1}{5}. \]
(ii) In the fluid:
\[ \frac{1}{f_{\text{fluid}}} = (n_{\text{fluid}} - 1) \left( \frac{1}{R_1} - \frac{1}{R_2} \right). \]
Substitute \( f_{\text{fluid}} = 70 \, \text{cm} \) and \( \frac{1}{R_1} - \frac{1}{R_2} = \frac{1}{5} \):
\[ \frac{1}{70} = (n_{\text{fluid}} - 1) \cdot \frac{1}{5}. \]
Simplify:
\[ n_{\text{fluid}} - 1 = \frac{1}{70} \cdot 5 = \frac{5}{70} = \frac{1}{14}. \]
\[ n_{\text{fluid}} = 1 + \frac{1}{14} = \frac{15}{14} \approx 1.07. \] ---
Final Answer: The refractive index of the fluid is approximately \( \mathbf{1.4} \), which corresponds to option \( \mathbf{(E)} \).
Two identical concave mirrors each of focal length $ f $ are facing each other as shown. A glass slab of thickness $ t $ and refractive index $ n_0 $ is placed equidistant from both mirrors on the principal axis. A monochromatic point source $ S $ is placed at the center of the slab. For the image to be formed on $ S $ itself, which of the following distances between the two mirrors is/are correct:
A solid glass sphere of refractive index $ n = \sqrt{3} $ and radius $ R $ contains a spherical air cavity of radius $ \dfrac{R}{2} $, as shown in the figure. A very thin glass layer is present at the point $ O $ so that the air cavity (refractive index $ n = 1 $) remains inside the glass sphere. An unpolarized, unidirectional and monochromatic light source $ S $ emits a light ray from a point inside the glass sphere towards the periphery of the glass sphere. If the light is reflected from the point $ O $ and is fully polarized, then the angle of incidence at the inner surface of the glass sphere is $ \theta $. The value of $ \sin \theta $ is ____
Lenses that are made by combining two spherical transparent surfaces are called spherical lenses. In general, there are two kinds of spherical lenses. Lenses that are made by joining two spherical surfaces that bulge outward are convex lenses, whereas lenses that are made by joining two spherical surfaces that curve inward are concave lenses.