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Oblique parallel rays and focal plane

We have seen that rays parallel to the optical axis are directed to the focal point of a converging lens. In the case of a diverging lens, they come out in a direction such that they appear to be coming from the focal point on the opposite side of the lens (i.e., the side from which parallel rays enter the lens). What happens to parallel rays that are not parallel to the optical axis ( [link] )? In the case of a converging lens, these rays do not converge at the focal point. Instead, they come together on another point in the plane called the focal plane    . The focal plane contains the focal point and is perpendicular to the optical axis. As shown in the figure, parallel rays focus where the ray through the center of the lens crosses the focal plane.

Figure shows rays that are parallel to each other but not to the optical axis, entering a bi-convex lens and converging on the other side at a point on the focal plane. The cross section of the focal plane is shown as a line that is perpendicular to the optical axis and intersects it at the focal point.
Parallel oblique rays focus on a point in a focal plane.

Thin-lens equation

Ray tracing allows us to get a qualitative picture of image formation. To obtain numeric information, we derive a pair of equations from a geometric analysis of ray tracing for thin lenses. These equations, called the thin-lens equation and the lens maker’s equation, allow us to quantitatively analyze thin lenses.

Consider the thick bi-convex lens shown in [link] . The index of refraction of the surrounding medium is n 1 (if the lens is in air, then n 1 = 1.00 ) and that of the lens is n 2 . The radii of curvatures of the two sides are R 1 and R 2 . We wish to find a relation between the object distance d o , the image distance d i , and the parameters of the lens.

Figure shows a bi-convex lens with thickness t and radii of curvature of front and back surfaces R1 and R2 respectively. The refractive index of air and lens are n1 and n2 respectively. Rays from an object at point P on the optical axis in front of the lens strike the first surface and are refracted within the lens. The back extensions of the refracted rays converge at point Q prime to form intermediate image. Q prime is in front of the lens, further away from it than P. The rays within the lens refract further as they emerge from the second surface. They converge at point Q behind the lens to form final image. The distances from the lens to the object, intermediate image and final image are d0, d0 prime and di respectively. d0 prime is also the same as di prime.
Figure for deriving the lens maker’s equation. Here, t is the thickness of lens, n 1 is the index of refraction of the exterior medium, and n 2 is the index of refraction of the lens. We take the limit of t 0 to obtain the formula for a thin lens.

To derive the thin-lens equation , we consider the image formed by the first refracting surface (i.e., left surface) and then use this image as the object for the second refracting surface. In the figure, the image from the first refracting surface is Q , which is formed by extending backwards the rays from inside the lens (these rays result from refraction at the first surface). This is shown by the dashed lines in the figure. Notice that this image is virtual because no rays actually pass through the point Q . To find the image distance d i corresponding to the image Q , we use [link] . In this case, the object distance is d o , the image distance is d i , and the radius of curvature is R 1 . Inserting these into [link] gives

n 1 d o + n 2 d i = n 2 n 1 R 1 .

The image is virtual and on the same side as the object, so d i < 0 and d o > 0 . The first surface is convex toward the object, so R 1 > 0 .

To find the object distance for the object Q formed by refraction from the second interface, note that the role of the indices of refraction n 1 and n 2 are interchanged in [link] . In [link] , the rays originate in the medium with index n 2 , whereas in [link] , the rays originate in the medium with index n 1 . Thus, we must interchange n 1 and n 2 in [link] . In addition, by consulting again [link] , we see that the object distance is d o and the image distance is d i . The radius of curvature is R 2 Inserting these quantities into [link] gives

Questions & Answers

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Swagatika Reply
hi
Tr
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Youte
Hi
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hi
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1.79×10_¹⁹ km per hour
Swagatika
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কাজের একক কী
Jasim
কাজের একক কী
Jasim
friction ka direction Kaise pata karte hai
Rahul Reply
friction is always in the opposite of the direction of moving object
Punia
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Varia Reply
b) symmetric of time only
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Alvin
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mallam Reply
according to de Broglie any matter particles by attaining the higher velocity as compared to light'ill show the wave nature and equation of wave will applicable on it but in practical life people see it is impossible however it is practicaly true and possible while looking at the earth matter at far
Manikant
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he related wave to matter
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Practice Key Terms 5

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Source:  OpenStax, University physics volume 3. OpenStax CNX. Nov 04, 2016 Download for free at http://cnx.org/content/col12067/1.4
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