{\displaystyle z(r)} from the axis. r Lenses are made with at least one curved surface (convex or concave) and so lenses simply change the curvature of the waves that fall on them. converges the waves and negative if it decreases the curvature of the ways – i.e. r This means that the outer portions of the wave ‘catch up’ so increasing the curvature to form a converging beam. Solution: Given: The radius of curvature (R)= +4.00 m. Object distance(u) = -6.00 m. Image distance(v) = ? A surface with a small radius of curvature therefore has a large curvature. The distance from the vertex to the center of curvature is the radius of curvature of the surface. Radius of curvature (ROC) has specific meaning and sign convention in optical design. The radius of curvature of a convex mirror used for rearview on a car is 4.00 m. If the location of the bus is 6 meters from this mirror, find the position of the image formed. You can follow this change of curvature as the waves meet the lens and then pass through it, emerging at the other side. In the example below they are bent from a plane wave to form a converging wave in the lens. {\displaystyle r} S T U W X Z [ ] ^ ` a É Ê Ë ñ ò ú ø ú ø ø ø ø ø ø ø ø ø ø ø ø ú ø ú ø ø ø ø ø ö ø ø ú ø $a$ ò ó ü ı ı ø ı ø ı ø ı ø ı ı ı $a$ , 1�h°‚. The vertex of the lens surface is located on the local optical axis. K α This means that they have been given a curvature 1/f. {\displaystyle \alpha _{1}} A spherical lens or mirror surface has a center of curvature located either along or decentered from the system local optical axis. and For the general mathematical concept, see, https://en.wikipedia.org/w/index.php?title=Radius_of_curvature_(optics)&oldid=980175178, Creative Commons Attribution-ShareAlike License. r The shape of the incident waves have no effect on how much the lens changes their curvature and so we can say that a lens increases the curvature of waves that pass through it by a constant amount 1/f. The vertex of the lens surface is located on the local optical axis. describe the deviation of the surface from the axially symmetric quadric surface specified by The lens adds a constant curvature (1/f) to the wave and so the equation relating the object distance (u) image distance (v) and the focal length (f) is: using the above sign convention called the Cartesian sign convention This can be shown in the following diagram. (Remember that 1/f will be positive for a convex lens and negative for a concave lens) The example has been done with a plane wave but the same would occur with a spherical wave spreading outwards from a point object. Sign conventions 4 • Light travels from left to right • A radius of curvature is positive if the surface is convex towards the left • Longitudinal distances are positive if pointing to the right • Lateral distances are positive if pointing up • Ray angles are positive if the ray direction is obtained by rotating the . A spherical lens or mirror surface has a center of curvature located either along or decentered from the system local optical axis. ). °ÆA!°Š"°Š#� $� %° °Å°S�Ä As the wave hits the lens it is the centre of the wave that meets the glass first and so this part of the wave is slowed down first (light waves move slower in glass than they do in air). The coefficients The distance from the vertex to the center of curvature is the radius of curvature of the surface.[1][2]. R is the sag—the z-component of the displacement of the surface from the vertex, at distance Looking at the diagram you can see that waves with no curvature have been converged to a point a distance f (the focal length) from the lens. 0 For each R, the convention is such that we make R > 0 if the light hits the curved surface before the center of curvature, and R < 0 if the opposite is true. and Optical surfaces with non-spherical profiles, such as the surfaces of aspheric lenses, also have a radius of curvature. Waves and curved surfaces When light waves fall on a curved surface that surface changes the curvature of the wave. a convex lens This means that the outer portions move off more rapidly first and so the curvature of the wave is further increased so converging the light more strongly. These surfaces are typically designed such that their profile is described by the equation, where the optic axis is presumed to lie in the z direction, and is the radius of curvature and i D @ñÿ D N o r m a l $ CJ OJ QJ ^J _HaJ mH sH tH @ @ @ H e a d i n g 1 $@&. diverges the waves. Wavefronts Wavefronts spreading outwards from a point source are taken as having a negative curvature and so the distance from the lens to the object is negative Wavefronts that converge to an image are taken as having a positive curvature and so the distance from the lens to the image is positive. {\displaystyle R} ( {\displaystyle \alpha _{2}} z R diverges the waves. The sign convention for the optical radius of curvature is as follows: Thus when viewing a biconvex lens from the side, the left surface radius of curvature is positive, and the right radius of curvature is negative. a convex lens A surface that diverges a wavefront is taken as negative e.g. i α K is the conic constant, as measured at the vertex (where {\displaystyle K} This wave is further converged when it leaves the lens. α Sometimes this image is real (you can form it on a surface such as a piece of paper) and sometimes virtual (it cannot be formed on a surface) Curvature and the sign convention The radius of curvature (R) of a surface is taken as a positive number if it increases the curvature of the waves – i.e. This page was last edited on 25 September 2020, at 01:36. If For thin lenses we can use the lens maker's equation: 1 f = ( n − 1) ( 1 R 1 − 1 R 2) Where n is the index of refraction of the material, R 1 is the radius of curvature of the side the light hits first, and R 2 is the radius of curvature of the side the light hits last. a b ğ ñ H I Ì Í Î Ù p ú û w x z ¿ À í î ï ğ ñ ı ı ı ı ı ı ø ø ø ø ø ı ı ö ø ø ı ô ò ı ı ı ı ı ı ı ı ı $a$ ñ ú û ü F ” – ¤ Ê * , ’ ” ˜ š �   ¤ ¦ ¸ º ö ğ î ö ğ î î î î ì ì î ì ì ì ì ì î î î î î î î ç î $a$ „h]„h „øÿ„ &`#$ º Æ È ò ô $ & P R V X \ ^ b d h j n p t v z | � � ¦ ¨ ¼ ¾ ú ø ú ø ú ø ú ø ø ø ø ø ø ø ø ø ø ø ø ø ø ø ú ø ú ø ú ø $a$ ¦ ¨ ¼ ¾ Ú Ü ö ø S U W X Z [ ] ^ ` a É Ë ñ ó ü ı ı ı ı ı û û ÷ í ÷ ê ı ı ı ı CJ 5�OJ QJ \�^J 5�\� 5�CJ ¾ Ú Ü ö ø

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