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Question: For incident ray parallel to principle axis of one convex lens emerges parallel rays from other conv...

For incident ray parallel to principle axis of one convex lens emerges parallel rays from other convex lens, if focal length of each lens is of magnitude is ff and separation between convex lenses is D and between left convex and concave is x.

A

For distance between concave and convex x=f2x = \frac{f}{2}, then D=52fD = \frac{5}{2}f

B

For x=f2x = \frac{f}{2}; virtual image is being formed by concave lens.

C

For x=fx = f the deviation caused by concave lens is zero.

Answer

A, C

Explanation

Solution

The problem describes an optical system consisting of three lenses: a convex lens (Lens 1), a concave lens, and another convex lens (Lens 2). We are given information about the incident and emergent rays, and the focal lengths of the lenses. We need to evaluate the given statements.

Given:

  • Focal length of each convex lens: f1=+ff_1 = +f, f2=+ff_2 = +f.
  • Magnitude of focal length of concave lens: ff. So, fc=ff_c = -f.
  • Incident rays on Lens 1 are parallel to the principal axis.
  • Emergent rays from Lens 2 are parallel to the principal axis.
  • Separation between Lens 1 and concave lens is xx.
  • Separation between Lens 1 and Lens 2 is DD.

Step-by-step Ray Tracing and Calculations:

  1. Rays through Lens 1 (Convex):

    • Since incident rays are parallel to the principal axis, they converge at the focal point of Lens 1.
    • Image I1I_1 is formed at v1=+fv_1 = +f (to the right of Lens 1).
  2. Rays through Concave Lens:

    • The image I1I_1 acts as the object for the concave lens.
    • The concave lens is at a distance xx from Lens 1.
    • The position of I1I_1 relative to the concave lens is uc=(fx)u_c = (f - x).
    • We assume f>xf > x, meaning I1I_1 is to the right of the concave lens. This makes I1I_1 a virtual object for the concave lens, so uc=+(fx)u_c = +(f-x).
    • Using the lens formula for the concave lens: 1vc1uc=1fc\frac{1}{v_c} - \frac{1}{u_c} = \frac{1}{f_c} 1vc1+(fx)=1f\frac{1}{v_c} - \frac{1}{+(f-x)} = \frac{1}{-f} 1vc=1fx1f=f(fx)f(fx)=xf(fx)\frac{1}{v_c} = \frac{1}{f-x} - \frac{1}{f} = \frac{f - (f-x)}{f(f-x)} = \frac{x}{f(f-x)} So, vc=f(fx)xv_c = \frac{f(f-x)}{x}.
    • Since f>xf>x and f,xf,x are positive, vcv_c will be positive. A positive image distance (vc>0v_c > 0) indicates a real image formed to the right of the concave lens.
  3. Rays through Lens 2 (Convex):

    • The emergent rays from Lens 2 are parallel to the principal axis. This implies that the object for Lens 2 must be at its principal focus.
    • So, the image IcI_c (formed by the concave lens) must be located at u2=f2=fu_2 = -f_2 = -f (i.e., at a distance ff to the left of Lens 2).
    • The distance between the concave lens and Lens 2 is (Dx)(D-x).
    • Therefore, the position of IcI_c from the concave lens (vcv_c) must be (Dx)f(D-x) - f. This implies IcI_c is formed to the right of the concave lens and to the left of Lens 2.
    • Equating the two expressions for vcv_c: f(fx)x=(Dx)f\frac{f(f-x)}{x} = (D-x) - f f2fxx=Dxf\frac{f^2 - fx}{x} = D-x-f D=f2fxx+x+fD = \frac{f^2 - fx}{x} + x + f D=f2fx+x2+fxxD = \frac{f^2 - fx + x^2 + fx}{x} D=f2+x2xD = \frac{f^2 + x^2}{x}

Evaluating the Options:

  • A. For distance between concave and convex x=f2x = \frac{f}{2}, then D=52fD = \frac{5}{2}f Substitute x=f2x = \frac{f}{2} into the derived formula for DD: D=f2+(f2)2f2=f2+f24f2=5f24f2=5f24×2f=5f2D = \frac{f^2 + (\frac{f}{2})^2}{\frac{f}{2}} = \frac{f^2 + \frac{f^2}{4}}{\frac{f}{2}} = \frac{\frac{5f^2}{4}}{\frac{f}{2}} = \frac{5f^2}{4} \times \frac{2}{f} = \frac{5f}{2}. This statement is correct.

  • B. For x=f2x = \frac{f}{2}; virtual image is being formed by concave lens. For x=f2x = \frac{f}{2}, we calculated vc=f(ff2)f2=f(f2)f2=fv_c = \frac{f(f-\frac{f}{2})}{\frac{f}{2}} = \frac{f(\frac{f}{2})}{\frac{f}{2}} = f. Since vc=+fv_c = +f (positive), the image formed by the concave lens is a real image (formed to the right of the concave lens by actual intersection of rays). This statement is incorrect.

  • C. For x=fx = f the deviation caused by concave lens is zero. If x=fx = f, the image I1I_1 formed by Lens 1 is at a distance ff from Lens 1. Since the concave lens is also at a distance x=fx=f from Lens 1, the image I1I_1 is formed exactly at the position of the concave lens. This means the rays from Lens 1 are converging towards the optical center of the concave lens. When rays pass through the optical center of any lens, they go undeviated. Therefore, the deviation caused by the concave lens is zero. This statement is correct. (Also, substituting x=fx=f into the formula for DD: D=f2+f2f=2f2f=2fD = \frac{f^2+f^2}{f} = \frac{2f^2}{f} = 2f. This means the system acts like an afocal system, which is consistent with the rays passing undeviated through the middle lens.)

Since both A and C are correct, and the question asks for the correct option(s), we list both.