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A glass sphere of refractive index 1.5 f...

A glass sphere of refractive index `1.5` forms the real image of object `O` at point `I` as shown in the figure when kept in air of refractive index `1`. If the value of `x` is `kR`. Find `k`

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To solve the problem, we need to analyze the behavior of light as it passes through the glass sphere and forms images at specific points. Here’s a step-by-step breakdown of the solution: ### Step 1: Understand the Setup We have a glass sphere with a refractive index of \( n_2 = 1.5 \) in air with a refractive index of \( n_1 = 1 \). The object \( O \) forms a real image \( I \) at a distance \( x \) from the center of the sphere. ### Step 2: First Refraction When light travels from the object \( O \) to the first surface of the sphere, we can denote the radius of the sphere as \( R \). The object distance \( u \) for the first refraction (from the image point \( I \)) is taken as \( u = -R \) (the negative sign indicates that the object is on the same side as the incoming light). Using the lens maker's formula for refraction at a spherical surface: \[ \frac{n_2}{v} - \frac{n_1}{u} = \frac{n_2 - n_1}{R} \] Substituting the values: \[ \frac{1.5}{v} - \frac{1}{-R} = \frac{1.5 - 1}{R} \] This simplifies to: \[ \frac{1.5}{v} + \frac{1}{R} = \frac{0.5}{R} \] Rearranging gives: \[ \frac{1.5}{v} = \frac{0.5}{R} - \frac{1}{R} = -\frac{0.5}{R} \] Thus, \[ v = -3R \] ### Step 3: Second Refraction Now, the image \( I_1 \) acts as the object for the second refraction at the second surface of the sphere. The distance from the center of the sphere to the image \( I_1 \) is \( 3R \), but we need to consider the total distance from the second surface, which is \( 5R \) (since it is \( 3R + 2R \)). Now, we have: \[ u = -5R \] Using the lens maker's formula again for the second refraction: \[ \frac{n_3}{x} - \frac{n_2}{u} = \frac{n_3 - n_2}{R} \] Substituting the values: \[ \frac{1}{x} - \frac{1.5}{-5R} = \frac{1 - 1.5}{R} \] This simplifies to: \[ \frac{1}{x} + \frac{1.5}{5R} = -\frac{0.5}{R} \] Rearranging gives: \[ \frac{1}{x} = -\frac{0.5}{R} - \frac{1.5}{5R} \] Finding a common denominator: \[ \frac{1}{x} = -\frac{2.5}{5R} - \frac{1.5}{5R} = -\frac{4}{5R} \] Thus, \[ x = -\frac{5R}{4} \] ### Step 4: Finding \( k \) Given that \( x = kR \), we can equate: \[ kR = -\frac{5R}{4} \] Thus, \[ k = -\frac{5}{4} \] ### Final Answer The value of \( k \) is \( -\frac{5}{4} \). ---

To solve the problem, we need to analyze the behavior of light as it passes through the glass sphere and forms images at specific points. Here’s a step-by-step breakdown of the solution: ### Step 1: Understand the Setup We have a glass sphere with a refractive index of \( n_2 = 1.5 \) in air with a refractive index of \( n_1 = 1 \). The object \( O \) forms a real image \( I \) at a distance \( x \) from the center of the sphere. ### Step 2: First Refraction When light travels from the object \( O \) to the first surface of the sphere, we can denote the radius of the sphere as \( R \). The object distance \( u \) for the first refraction (from the image point \( I \)) is taken as \( u = -R \) (the negative sign indicates that the object is on the same side as the incoming light). ...
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