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Today’s agenda: Death Rays. You must know when to run from Death Rays.

Today’s agenda covers the crucial topics of dealing with death rays, calculating properties of images formed by refraction at spherical surfaces, understanding thin lenses, drawing ray diagrams, and solving lens equations. Learn about lens combinations, optical instruments, and the complexities of refraction at spherical surfaces. Explore the geometry of convex and concave lenses and understand the formation of real and virtual images. Dive into the sign conventions and approximations used in optics to effectively navigate through these concepts.

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Today’s agenda: Death Rays. You must know when to run from Death Rays.

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  1. Today’s agenda: Death Rays. You must know when to run from Death Rays. Refraction at Spherical Surfaces. You must be able to calculate properties of images formed by refraction at spherical surfaces. Thin Lenses: Concave and Convex Lenses, Ray Diagrams, Solving the Lens Equation. You must understand the differences between these two kinds of lenses, be able to draw ray diagrams for both kinds of lenses, and be able to solve the lens equation for both kinds of lenses. Lens Combinations, Optical Instruments. You should be aware of this useful information, which will not be presented in lecture.

  2. Refraction at Spherical Surfaces Convex surface: 1 2 axis C F R f na nb>na Geometry: a light ray parallel to the axis passes through F.

  3. An extended object will form an image inside the nb medium. 1 Ray 1: parallel to the axis, through F. Ray 3: through C. 2 axis R C F s f s’ na nb>na This image is real and inverted.

  4. Concave surface: R F C axis f na nb>na Geometry: a light ray parallel to the axis seems to have come from F.

  5. An extended object will form an image inside the na medium. Ray 1: parallel to the axis, through F. Ray 3: through C. R F C axis f na nb>na The image is virtual and upright. There are three different places to put the object. The different images formed are always virtual and upright.

  6. We can use geometry to derive an equation relating the image and source positions, and an equation for the magnification. axis C F R s f s’ na nb

  7. The same equations work for concave surfaces. R F C s axis s’ f na nb

  8. Approximations Were Used! The equations in this section are excellent approximations if both the angles of incidence and refraction are small.

  9. Sign Conventions  R is positive when it is in the medium into which the light propagates. R is negative when it is in the medium from which the light radiates. • The image distance is positive when the image is in the medium into which the light propagates, and negative if it is in the medium from which the light radiates (virtual image).  The object distance is positive when the object is in the medium from which the light radiates (the usual case—a real object), and negative if on the side opposite to the light source (a virtual object). These are really “the same” as for mirrors.

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