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© 2010 Pearson Education, Inc. PowerPoint ® Lectures for College Physics: A Strategic Approach, Second Edition Wave Optics
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J.M. Gabrielse Wave Optics
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J.M. Gabrielse Optics K.G. Suastika
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J.M. Gabrielse Diskripsi Kuliah Optics Basic Reflection Diffuse reflection Refraction Index of refraction Speed of light Snell’s law Geometry problems Critical angle Total internal reflection Brewster angle Fiber optics Mirages Dispersion Prisms Rainbows Plane mirrors Spherical aberration Concave and convex mirrors Focal length & radius of curvature Mirror / lens equation Convex and concave lenses Human eye Chromatic aberration Telescopes Huygens’ principle Diffraction K.G. Suastika
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J.M. Gabrielse What do you know? About optics?
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J.M. Gabrielse Instrumen & Fenomena Optik Basics K.G. Suastika
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J.M. Gabrielse Optika: Cabang fisika yang mempelajari perilaku cahaya dan gelombang elektromagnetik K.G. Suastika
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J.M. Gabrielse A ray of light is an extremely narrow beam of light. K.G. Suastika
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J.M. Gabrielse All visible objects emit or reflect light rays in all directions. K.G. Suastika
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J.M. Gabrielse Our eyes detect light rays. K.G. Suastika
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J.M. Gabrielse We think we see objects. We really see images. K.G. Suastika
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J.M. Gabrielse converge: come together Images are formed when light rays converge. K.G. Suastika
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J.M. Gabrielse When light rays go straight into our eyes, we see an image in the same spot as the object. object & image K.G. Suastika
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J.M. Gabrielse Vocabulary Terms angle of refraction chromatic aberration converging lens critical angle diffuse reflection dispersion diverging lens eyepiece fiber optics focal length focal plane focal point Focus the center point of the sphere geometric optics image image relay incident ray index of refraction law of reflection optical axis magnification magnifying glass mirror normal line object objective optical axis radius of curvature optics prism ray diagram real image reflected ray refracting telescope Snell’s law specular reflection spherical aberration telescope thin lens formula internal reflection Virtual the focal distance K.G. Suastika
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J.M. Gabrielse Mirrors object image It is possible to see images when converging light rays reflect off of mirrors. K.G. Suastika
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J.M. Gabrielse Reflection Reflection is when light changes direction by bouncing off a surface. When light is reflected off a mirror, it hits the mirror at the same angle (θ i, the incidence angle) as it reflects off the mirror (θ r, the reflection angle). The normal is an imaginary line which lies at right angles to the mirror where the ray hits it. θrθr θiθi Mirror normal incident ray reflected ray K.G. Suastika
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J.M. Gabrielse Senin, 14 September 201517 Hukum refleksi dan refraksi 1.Sinar yang masuk/datang, sinar yang direfleksikan, dan sinar yang direfraksikan dan normal terhadap permukaan semuanya terletak pada bidang yang sama. 2.Sudut refleksi θ r sama dengan sudut masuk θ i untuk semua panjang gelombang dan untuk setiap pasangan material adalah θ i = θ r (1-2) (hukum refleksi) K.G. Suastika
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J.M. Gabrielse Problem
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J.M. Gabrielse Spherical Mirrors (concave & convex) K.G. Suastika
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J.M. Gabrielse Concave & Convex (just a part of a sphere) r C K.G. Suastika r
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J.M. Gabrielse Mirrors reflect light rays. K.G. Suastika
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J.M. Gabrielse How do we see images in mirrors? K.G. Suastika
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J.M. Gabrielse objectimage Light from the object reflects off the mirror and converges to form an image. How do we see images in mirrors? K.G. Suastika
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J.M. Gabrielse Sight Lines objectimage We perceive all light rays as if they come straight from an object. The imaginary light rays that we think we see are called sight lines. K.G. Suastika
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J.M. Gabrielse Sight Lines objectimage We perceive all light rays as if they come straight from an object. The imaginary light rays that we think we see are called sight lines. K.G. Suastika
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J.M. Gabrielse Image Types objectimage Real images are formed by light rays. Virtual images are formed by sight lines. mirror object & image window K.G. Suastika
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J.M. Gabrielse Plane (flat) Mirrors objectimage Images are virtual (formed by sight lines) and upright Objects are not magnified: object height (h o ) equals image height (h i ). Object distance (d o ) equals image distance (d i ). dodo didi hihi hoho K.G. Suastika
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J.M. Gabrielse Concave & Convex (just a part of a sphere) C: the center point of the sphere r: radius of curvature (just the radius of the sphere) F: the focal point of the mirror or lens (halfway between C and the sphere) f: the focal distance, f = r/2 r f C F K.G. Suastika
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J.M. Gabrielse optical axis Concave Mirrors (caved in) F Light rays that come in parallel to the optical axis reflect through the focal point. K.G. Suastika
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J.M. Gabrielse optical axis Concave Mirror (example) F K.G. Suastika
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J.M. Gabrielse optical axis Concave Mirror (example) F The first ray comes in parallel to the optical axis and reflects through the focal point. K.G. Suastika
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J.M. Gabrielse optical axis Concave Mirror (example) F The first ray comes in parallel to the optical axis and reflects through the focal point. The second ray comes through the focal point and reflects parallel to the optical axis. K.G. Suastika
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J.M. Gabrielse optical axis Concave Mirror (example) F The first ray comes in parallel to the optical axis and reflects through the focal point. The second ray comes through the focal point and reflects parallel to the optical axis. A real image forms where the light rays converge. K.G. Suastika
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J.M. Gabrielse optical axis Concave Mirror (example 2) F K.G. Suastika
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J.M. Gabrielse optical axis Concave Mirror (example 2) F The first ray comes in parallel to the optical axis and reflects through the focal point. K.G. Suastika
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J.M. Gabrielse optical axis Concave Mirror (example 2) F The first ray comes in parallel to the optical axis and reflects through the focal point. The second ray comes through the focal point and reflects parallel to the optical axis. K.G. Suastika
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J.M. Gabrielse optical axis Concave Mirror (example 2) F The first ray comes in parallel to the optical axis and reflects through the focal point. The second ray comes through the focal point and reflects parallel to the optical axis. The image forms where the rays converge. But they don’t seem to converge. K.G. Suastika
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J.M. Gabrielse optical axis Concave Mirror (example 2) F The first ray comes in parallel to the optical axis and reflects through the focal point. The second ray comes through the focal point and reflects parallel to the optical axis. A virtual image forms where the sight rays converge. K.G. Suastika
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J.M. Gabrielse optical axis Your Turn (Concave Mirror) F object concave mirror Note: mirrors are thin enough that you just draw a line to represent the mirror Locate the image of the arrow K.G. Suastika
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J.M. Gabrielse optical axis Your Turn (Concave Mirror) F object concave mirror Note: the mirrors and lenses we use are thin enough that you can just draw a line to represent the mirror or lens Locate the image of the arrow K.G. Suastika
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J.M. Gabrielse Convex Mirrors (curved out) Light rays that come in parallel to the optical axis reflect from the focal point. optical axis F The focal point is considered virtual since sight lines, not light rays, go through it. K.G. Suastika
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J.M. Gabrielse Convex Mirror (example) optical axis F K.G. Suastika
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J.M. Gabrielse Convex Mirror (example) optical axis F The first ray comes in parallel to the optical axis and reflects through the focal point. K.G. Suastika
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J.M. Gabrielse Convex Mirror (example) optical axis F The first ray comes in parallel to the optical axis and reflects through the focal point. The second ray comes through the focal point and reflects parallel to the optical axis. K.G. Suastika
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J.M. Gabrielse Convex Mirror (example) optical axis F The first ray comes in parallel to the optical axis and reflects through the focal point. The second ray comes through the focal point and reflects parallel to the optical axis. The light rays don’t converge, but the sight lines do. K.G. Suastika
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J.M. Gabrielse Convex Mirror (example) optical axis F The first ray comes in parallel to the optical axis and reflects through the focal point. The second ray comes through the focal point and reflects parallel to the optical axis. The light rays don’t converge, but the sight lines do. A virtual image forms where the sight lines converge. K.G. Suastika
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J.M. Gabrielse optical axis Your Turn (Convex Mirror) F Note: you just draw a line to represent thin mirrors Locate the image of the arrow object convex mirror K.G. Suastika
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J.M. Gabrielse optical axis Your Turn (Convex Mirror) F Note: you just draw a line to represent thin mirrors Locate the image of the arrow object convex mirror image K.G. Suastika
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J.M. Gabrielse Lens & Mirror Equation ƒ = focal length d o = object distance d i = image distance f is negative for diverging mirrors and lenses d i is negative when the image is behind the lens or mirror K.G. Suastika
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J.M. Gabrielse Magnification Equation m = magnification h i = image height h o = object height If height is negative the image is upside down if the magnification is negative the image is inverted (upside down) K.G. Suastika
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J.M. Gabrielse Refraction (bending light) Refraction is when light bends as it passes from one medium into another. When light traveling through air passes into the glass block it is refracted towards the normal. When light passes back out of the glass into the air, it is refracted away from the normal. Since light refracts when it changes mediums it can be aimed. Lenses are shaped so light is aimed at a focal point. normal air θrθr θiθi θrθr θiθi glass block K.G. Suastika
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J.M. Gabrielse Lenses The first telescope, designed and built by Galileo, used lenses to focus light from faraway objects, into Galileo’s eye. His telescope consisted of a concave lens and a convex lens. Light rays are always refracted (bent) towards the thickest part of the lens. convex lens concave lens light from far away object K.G. Suastika
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J.M. Gabrielse Concave Lenses Concave lenses are thin in the middle and make light rays diverge (spread out). If the rays of light are traced back (dotted sight lines), they all intersect at the focal point (F) behind the lens. optical axis F K.G. Suastika
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J.M. Gabrielse F optical axis Light rays that come in parallel to the optical axis diverge from the focal point. Concave Lenses The light rays behave the same way if we ignore the thickness of the lens. K.G. Suastika
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J.M. Gabrielse Concave Lenses optical axis F Light rays that come in parallel to the optical axis still diverge from the focal point. K.G. Suastika
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J.M. Gabrielse Concave Lens (example) The first ray comes in parallel to the optical axis and refracts from the focal point. optical axis F K.G. Suastika
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J.M. Gabrielse Concave Lens (example) optical axis F The first ray comes in parallel to the optical axis and refracts from the focal point. The second ray goes straight through the center of the lens. K.G. Suastika
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J.M. Gabrielse Concave Lens (example) optical axis F The first ray comes in parallel to the optical axis and refracts from the focal point. The second ray goes straight through the center of the lens. The light rays don’t converge, but the sight lines do. K.G. Suastika
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J.M. Gabrielse Concave Lens (example) optical axis F The first ray comes in parallel to the optical axis and refracts from the focal point. The second ray goes straight through the center of the lens. The light rays don’t converge, but the sight lines do. A virtual image forms where the sight lines converge. K.G. Suastika
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J.M. Gabrielse optical axis Your Turn (Concave Lens) F Note: lenses are thin enough that you just draw a line to represent the lens. Locate the image of the arrow. object concave lens K.G. Suastika
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J.M. Gabrielse optical axis Your Turn (Concave Lens) F Note: lenses are thin enough that you just draw a line to represent the lens. Locate the image of the arrow. object concave lens image K.G. Suastika
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J.M. Gabrielse Convex Lenses Convex lenses are thicker in the middle and focus light rays to a focal point in front of the lens. The focal length of the lens is the distance between the center of the lens and the point where the light rays are focused. K.G. Suastika
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J.M. Gabrielse Convex Lenses optical axis F K.G. Suastika
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J.M. Gabrielse Convex Lenses optical axis Light rays that come in parallel to the optical axis converge at the focal point. F K.G. Suastika
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J.M. Gabrielse Convex Lens (example) F The first ray comes in parallel to the optical axis and refracts through the focal point. optical axis K.G. Suastika
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J.M. Gabrielse Convex Lens (example) F The first ray comes in parallel to the optical axis and refracts through the focal point. The second ray goes straight through the center of the lens. optical axis K.G. Suastika
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J.M. Gabrielse Convex Lens (example) optical axis F The first ray comes in parallel to the optical axis and refracts through the focal point. The second ray goes straight through the center of the lens. The light rays don’t converge, but the sight lines do. K.G. Suastika
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J.M. Gabrielse Convex Lens (example) optical axis F The first ray comes in parallel to the optical axis and refracts through the focal point. The second ray goes straight through the center of the lens. The light rays don’t converge, but the sight lines do. A virtual image forms where the sight lines converge. K.G. Suastika
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J.M. Gabrielse optical axis Your Turn (Convex Lens) F Note: lenses are thin enough that you just draw a line to represent the lens. Locate the image of the arrow. object convex lens K.G. Suastika
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J.M. Gabrielse optical axis Your Turn (Convex Lens) F Note: lenses are thin enough that you just draw a line to represent the lens. Locate the image of the arrow. object convex lens image K.G. Suastika
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J.M. Gabrielse Thanks Faulkes Telescope Project: Light & Optics by Sarah RobertsFaulkes Telescope Project: Light & Optics Fundamentals of Optics: An Introduction for Beginners by Jenny ReinhardFundamentals of Optics: An Introduction for Beginners PHET Geometric Optics (Flash Simulator) Thin Lens & Mirror (Java Simulator) by Fu-Kwun HwangThin Lens & Mirror (Java Simulator) K.G. Suastika
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