Optics Flashcards
Energy of photon
E = hf
h -> planks constant
f -> frequency of light
law of reflection
angle of reflection equals angle of incidence
refraction angle and speed of light in medium
sinθ1/sinθ2 = v1/v2
index of refrction
n = speed of light in vacuum/speed of light in a medium
n = λ/λn
snell’s law of refraction
n1sinθ1 = n2sinθ2
critical angle of refraction
sinθc = n2/n1
at θc, beem is entirely reflected at material boundery
n1 is material from which light source originates
real image
light rays pass through and diverge from the image point
virtual image
light rays do not pass through image point, only appear to diverge from that point
magnification
M = image height/object height
mirror equation
1/p + 1/q = 2/R = 1/f
p -> object distance
q -> image distance
R -> radius of curvature
f -> focal point
focal point
f = R/2
positive object location for mirror (p)
positive when object is real
negative object location for mirror (p)
virtual image (behind mirror)
positive image location for mirror (q)
image is in front of mirror (real image)
negative image location for mirror (q)
image is behind mirror (virtual image)
positive image hight h’ for mirror
image is upright
negative image height h’ for mirror
image is inverted
positice focal length and radius of mirror
mirror is concave
negative flocal length and radius of mirror
mirror is convex
negative magnification of mirror
image is inverted
positive magnification of mirror
image is upright
object and image distance for refracting surface
n1/p + n2/q = (n2-n1)/R
positive object location for refracting surface (p)
object is in front of surface (real)
negative object location for refracting surface
object is in back of surface (virtual)
positive image location for refracting surface (q)
image is in back of surface (real)
negative image location for refracting surface
image is in front of surface (virtual)
positive R for refracting surface
center of curvature is in back of surface
negative R for refracting surface
center of curvature is in front of surface
lens makers’ equation
1/f = (n-1)(1/R1 - 1/R2)
thin lense equation
1/p + 1/q = 1/f
positive object location for thin lense (p)
object is in front of lense (real)
negative object location for thin lens
object is behind lens (virtual object)
positive image location for thin lens (q)
image is behind lens (real)
negative image location for thin lens (q)
image is in front of lens (virtual)
positive R1 and R2 for thin lens
center of curvature is behind lens
negative R1 and R2 for thin lens
center of curvature is in front of lens
positive focal length for thin lens
converging lens ()
negative focal length for thin lens
diverging lens )(
focal length of combination of thin lenses
1/f = 1/f1 + 1/f2
conditions for interference
sources must be coherent (in phase) and monochromatic (single wavelength)
conditions for constructive interference
δ = dsinθbright = mλ (m = 0, ±1, ±2, ±3…)
- δ -> path difference: diifference of distance light from slits travel*
- d-> distance between slits*
- θbright -> angle between bright bands*
conditions for destructive interference
dsinθdark = (m + 1/2)λ
m = (0,±1,±2,±3…)
position of bright interference bands using small angle approximation
ybright = λLm/d
position of dark interference bands using small angle approximation
ydark = (m+1/2)λL/d
intentsity for bands in double slit experiment
I = Imaxcos2(πdsinθ/λ)
intentsity for bands in double slit experiment using small angle approximation
I = Imaxcos2(πdy/λL)
constructive interference in thin films
2nt = (m + 1/2)λ
destrictive interference in thin films
2nt = mλ
destructive interference in single slit experiment
sinθdark = mλ/a
rayleigh’s condition
resolution occurs when the central maximum of one image falls on the first minimum of another images.
minimum angle for resolution of slit
θmin = λ/a
a -> width of slit
minimum angle for resolution in circular aperture
θmin = 1.22*λ/D
angle of maxima for difraction gratting
dsinθbright = mλ
Bragg’s law
describes difraction pattern from crystals
constructive interference:
2dsinθ = mλ
intensity of light through polarizer
I = Imaxcos2θ
Brewster’s law
defines polarizing angle of reflection
refracted beam is not polarized, reflected beam is
n = tanθp