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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

what is cathodic protection
Ebe Reply
its just a technique used for the protection of a metal from corrosion by making it cathode of an electrochemical cell.
what is interferometer
Sonu Reply
Show that n1Sino1=n2Sino2
javan Reply
what's propagation
Vikas Reply
is it in context of waves?
It is the manner of motion of the energy whether mechanical(requiring elastic medium)or electromagnetic(non interference with medium)
determine displacement cat any time t for a body of mass 2kg under a time varrying force ft=bt³+csinkt
Felix Reply
A round diaphragm S with diameter of d = 0.05 is used as light source in Michelson interferometer shown on the picture. The diaphragm is illuminated by parallel beam of monochromatic light with wavelength of λ = 0.6 μm. The distances are A B = 30, A C = 10 . The interference picture is in the form of concentric circles and is observed on the screen placed in the focal plane of the lens. Estimate the number of interference rings m observed near the main diffractive maximum.
Jyoti Reply
A Pb wire wound in a tight solenoid of diameter of 4.0 mm is cooled to a temperature of 5.0 K. The wire is connected in series with a 50-Ωresistor and a variable source of emf. As the emf is increased, what value does it have when the superconductivity of the wire is destroyed?
Rupal Reply
how does colour appear in thin films
Nwjwr Reply
yaaa ☺
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Kimani Reply
derivation of lateral shieft
James Reply
total binding energy of ionic crystal at equilibrium is
All Reply
How does, ray of light coming form focus, behaves in concave mirror after refraction?
Bishesh Reply
Refraction does not occur in concave mirror. If refraction occurs then I don't know about this.
What is motion
Izevbogie Reply
Anything which changes itself with respect to time or surrounding
and what's time? is time everywhere same
how can u say that
do u know about black hole
Not so more
Radioactive substance
These substance create harmful radiation like alpha particle radiation, beta particle radiation, gamma particle radiation
But ask anything changes itself with respect to time or surrounding A Not any harmful radiation
explain cavendish experiment to determine the value of gravitational concept.
Celine Reply
 Cavendish Experiment to Measure Gravitational Constant. ... This experiment used a torsion balance device to attract lead balls together, measuring the torque on a wire and equating it to the gravitational force between the balls. Then by a complex derivation, the value of G was determined.
For the question about the scuba instructor's head above the pool, how did you arrive at this answer? What is the process?
Evan Reply
Practice Key Terms 5

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