Optics, Waves, Lasers 1 Flashcards
real image
converge at P’
virtual image
diverge at P’
image either
erect or inverted
if lateral magnification positive
erect
if lateral magnification negative
inverted
lateral magnification=
hi/ho
focal point
point where parallel rays converge after reflection from concave or diverge after reflection from convex
focal length
focal point to vertex
object/image distances - plane mirror
1/s+1/s’=0
object/image distances - spherical mirror
1/s+1/s’=2/R=1/f
object/image distances - plane refracting surface
na/s+nb/s’=0
object/image distances - spherical refracting surface
na/s+nb/s’=nb-na/R
lateral magnification - plane mirror
m=-s’/s=1
lateral magnification - spherical mirror
m=-s’/s
lateral magnification - plane refracting surface
m=-nas’/nbs=1
lateral magnification - spherical refracting surface
m=-nas’/nbs
non paraxial rays
do not converge precisely - spherical abberation
thin lenses - 1/s+1/s’=
1/f
thin lenses 1/f=
(n-1)(1/R1-1/R2)
s>0 when
object on incoming side (real object)
s’>0 when
image is on outgoing side (real image)
R>0 when
centre of curvature is on outgoing side
m>0 when
image is erect
what do cameras form?
real, inverted image
camera - what controls the amount of light
shutter speed an aperture
camera - intensity is inversely proportional to
square of f-number
f number
f/D
refraction at surface of cornea forms
real image on retina
what adjusts for object distances
squeezing lens
nearsighted eye
too long for its lens
farsighted eye
too short for its lens
power of corrective lens
reciprocal of focal length
in diopters
simple magnifyer
creates virtual image theta’>theta at a distance of 25cm
25cm
normal closest distance for comfortable viewing
compound microscope
objective lens forms a first image in barrel of instrument and eyepiece forms a final virtual image of the first image
telescope
same idea as microscope but object far away
reflecting telescope
objective lens replaced by concave mirror
(this eliminates chromatic abberations)