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Reflection and refraction of light Mirrors and lenses Ch 22: Reflection and refraction Reflection –part of the light encountering the second medium bounces off that medium Refraction- the light is passing into the second medium bends through an angle with respect to the normal to the boundary Reflection of light: -specular reflection -diffuse reflection Normal- a line perpendicular to the surface v Refraction sinθf/sinθi=v2/v1=ct The path of a light ray through a refracting surface is reversible The Law of Refraction The index of refraction is a ration n=c/v n= speed of light in vacuum/ speed of light in a medium As light travels from one medium to another, its frequency doesn’t change. v= f λ λ1/λ2=v1/v2=(c/n1)/(c/n2)=n2/n1 λ1n1=λ2n2 Snell’s law of refraction: n1sinθ1=n2sinθ2 Dispersion and Prisms Dispersion – the dependence of the index of refraction on a wavelength Snell: the angle of refraction made when light enters a material depends on the wavelength of the light Total internal reflection Total internal reflection occur when light encounters the boundary between a medium with a higher index of refraction and one with a lower index of refraction Critical angle: θ2=90o n1>n2: sinθc=n2/n1 Ch 23: Mirrors and Lenses Consider a point source of light (object), after reflection, the rays diverge , but they appear to the viewer to come from a point behind a mirror (image) Images are formed at the point where rays of light actually intersect or where they appear to originate p- object distance; q-image distance; -Real image- light asses through the image point -Virtual image- light doesn’t pass through the image point but appears to come (diverge) from there The image formed by an object placed in front of a flat mirror is as far behind the mirror as the object is in the front of the mirror the object height h = the image height h’ The lateral magnification (def): M=h’/h =the image height/ the object height Mirror properties: The image is as far behind the mirror as the object is in the front The image is unmagnified, virtual and upright Spherical mirrors: Concave mirrors M=h’/h =-q/p Mirror equation: 1/p + 1/q =2/ R f=R/2 → 1/p +1/q =1/f (q- image distance; p- object distance, R-radius of curvarture) Convex mirrors (divergin mirrors) Ray diagrams for mirrors: 1. Rays 1 is parallel to the principal axis and is reflected back through the focal point 2. Ray 2 is drawn through the focal point and is reflected parallel to the principal axis 3. Ray 3 is drawn through the center of curvature, C, and is reflected back on itself Flat Refracting surfaces: n1/p=-n2/q q=- (n2/n1)p The image formed by a flat refracting surface is on the same side of the surface as the object Thin lenses: converging lenses and diverging lenses M=hi/ho=-q/p tanθ=AC/f → tan θ=-hi/q-f ho/f =-hi/q-f → q/p =q-f/f → 1/p +1/q =1/f –thin lenses equation 1/f=(n-1)(1/R1 – 1/R2) –lens maker’s equation Combination of thin lenses: