Page 62 - Fundamentals of Light Microscopy and Electronic Imaging
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IMAGE FORMATION BY A SIMPLE LENS        45


                        Note: Real and Virtual Images

                        Images can be defined as regions where rays, or the extensions of rays, become con-
                        vergent as the result of refraction by a lens or reflection by a mirror. If the rays inter-
                        sect and physically reunite, the image is said to be real. A real image can be seen on
                        a viewing screen or recorded on a piece of film when a screen or film is placed in the
                        image plane. If rays diverge, but the imaginary backward extensions of the rays
                        become convergent and intersect, the image is said to be virtual. The plane occupied
                        by a virtual image cannot be observed on a viewing screen or recorded on film. To
                        be perceived, a real image must be formed on the retina of the eye. In the case of
                        viewing an image in a microscope, a real image is formed on the retina but is per-
                        ceived as a virtual image located some 25 cm in front of the eye. Lens configurations
                        giving real and virtual images are described in this chapter.




                          The geometric parameters of a simple thin lens are described in Figure 4-3, where
                       the vertical line represents the combined principal planes of a thin biconvex lens of focal
                       length f. The object, an arrow on the left-hand side of the figure, is examined by the lens
                       and imaged as a magnified real image (magnified inverted arrow) in the image plane on
                       the right. The focal length is shown as the distance f from the principal plane of the lens
                       to its focal point F, the front and rear focal lengths having the same value. The optic axis
                       is shown by a horizontal line passing through the center of the lens and perpendicular to
                       its principal plane. The object distance a (distance from the object to the principal plane
                       of the lens) and image distance b (distance from the image to the principal plane of the
                       lens) are also indicated.
                          The focal length of any simple lens can be determined by aiming the lens at a bright
                       “infinitely distant” light source (  30 times the focal length) such as a lamp across the
                       room or a scene outdoors; by focusing the image on a sheet of paper held behind the
                       lens, the focal length is readily determined (Fig. 4-4). We will now examine the basic
                       rules that determine the action of a simple convex lens.





                                             a                    b
                                                          f
                                Object
                                           F                   F
                                                f
                                                                                Image



                                                   Lens
                       Figure 4-3
                       Geometrical optics of a simple lens. The focal length f, focal point F, object-lens distance a,
                       and lens-image distance b are indicated.
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