Geometric optics
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Transcript of Geometric optics
Geometric Optics
Mirrors, lenses, light, and image formation
Geometric Optics
Understanding images and image formation, ray model of light, laws of reflection and refraction, and some simple geometry and trigonometry
REFLECTION AND REFRACTION AT A PLANE SURFACE
Reflection and refraction on plane mirrors
Key terms
• Anything from which light rays radiate–Object
• Anything from which light rays radiate that has no physical extent– Point object
• Real objects with length, width, and height– Extended objects
Key terms
Specular reflection
Reflection on a plane surface where reflected rays are in the same directions
Diffused reflection
Relfection on a rough surface
Key terms
Virtual image
Image formed if the outgoing rays
don’t actually pass through the
image point
Real image
Image formed if the outgoing rays actually pass through
the image point
Image formation by a Plane mirror
Image formation by a Plane mirror
Ray Diagrams
• a diagram that traces the path that light takes in order for a person to view a point on the image of an object
Line of Sight
Principle
• suggests that in order to view an image of an object in a mirror, a person must sight along a line at the image of the object.
Reflection at a Plane Surface
Image formation by a Plane mirror
V
θ
θ
θ θ
s s’M M’
Image formation by a Plane mirror
• M is the object and M’ is the virtual image
• Ray MV is incident normally to the plane mirror and it returns along its original path
• s= object distance• s’= image distance• s=-s’
Image formation by a Plane mirror
• Sign rulesFor the object distance:–When the object is on the same side of the
reflecting or the refracting surface as the incoming light, s is positive
For the image distance:–When the image is on the same side of the
reflecting or the refracting surface as the outgoing light, s’ is positive
Image of an extended object
V’
V
θθ
θ θ
s s’
y
M M’
Q Q’
θ
y’
Image of an extended object
• Lateral magnification–Ratio of image height to object
height–M=y’/y
• Image is erect• m for a plane mirror is always +1• Reversed means front-back
dimension is reversed
REFLECTION AT A SPHERICAL SURFACE
Reflection on Concave and Convex mirrors
Reflection at a Concave Mirror
P P’CV
Reflection at a Concave Mirror
• Radius of curvatureR• Center of curvature• The center of the sphere
of which the surface is a part
C
• Vertex• The point of the mirror
surfaceV
• Optic axisCV
IMAGE FORMATION ON SPHERICAL MIRRORS
Graphical Methods for Mirrors
Graphical Method
• Consists of finding the point of intersection of a few particular rays that diverge from a point of the object and are reflected by the mirror
• Neglecting aberrations, all rays from this object point that strike the mirror will intersect at the same point
Graphical Method
• For this construction, we always choose an object point that is not on the optic axis• Consists of four rays we can
usually easily draw, called the principal rays
Graphical MethodA ray parallel to the axis,
after reflection passes through F of a concave
mirror or appears to
come from the (virtual) F of a convex mirror
A ray through (or
proceeding toward) F is
reflected parallel to the
axis
A ray along the radius through or away from C intersects the
surface normally and is reflected back
along its original pathA ray to V is
reflected forming equal angles with
the optic axis
Object is at F
Object is between F and Vertex
Object is at C
Object is between C and F
Positions of objects for concave mirrors
Reflection at a Concave Mirror
If α dec, θi is nearly parallel
Rays nearly parallel or close to R Paraxial rays
Reflection at a Concave Mirror
If α inc, P’ is close to V Image is smeared out Spherical Aberration
Reflection at a Concave Mirror
FCV
s at infinity s’= R/2
Reflection at a Concave Mirror
• All reflected rays converge on the image point• Converging mirror• If R is infinite, the mirror
becomes plane
Reflection at a Concave MirrorThe incident parallel rays converge after reflecting from the
mirror
They converge at a F at a distance
R/2 from V
F is Focal point, where the rays are brought to focus
f is the focal length, distance from the vertex to the focal
point
f= R/2
Reflection at a Concave Mirror
FCV
s’ at infinity s= R/2
Reflection at a Concave Mirror
The object is at the focal
points=f=R/2
1/s +1/s’= 2/R 1/s’=0; s’ at infinity
1/s+ 1/s’= 1/fObject image relation, spherical mirror
Image of an Extended Object
m= y’/y Lateral magnification
m= y’/y= -s’/s
Lateral magnification for spherical mirrors
Example• A concave mirror forms an image, on a wall
3.00m from the mirror, of the filament of a headlight lamp 10.0cm in front of the mirror.
a. What is the radius of curvature and focal length of the mirror?
b. What is the height of the image if the height of the object is 5.00mm?
c. R=19.4cm; f= 9.7cm; m= -30.0; y’= 150mm
Example
• An object, 1cm high, is 20cm from the vertex of a concave mirror whose radius of curvature is 50cm. Compute the position and size of the image. Is it real or virtual? Upright or inverted?• s’=-100cm; y’=5cm, m is pos., erect,
virtual
Reflection at a Convex Mirror
F C
s or s’ at infinitys’ or s= R/2
Image formation on spherical mirrors
• Sign rulesFor the object distance:–When the object is on the same side
of the reflecting or the refracting surface as the incoming light, s is positive; otherwise, it is negative
Image formation on spherical mirrors
• Sign rulesFor the image distance:–When the image is on the same side
of the reflecting or the refracting surface as the outgoing light, s’ is positive; otherwise, it is negative
Image formation on spherical mirrors
• Sign rules:For the radius of curvature of a
spherical surface:–When the center of curvature C is
on the same side as the outgoing light, the radius of curvature is positive, otherwise negative
Reflection at a Convex Mirror
• The convex side of the spherical mirror faces the incident light
• C is at the opposite side of the outgoing rays, so R is neg.
• All reflected rays diverge from the same point
• Diverging mirror
Reflection at a Convex MirrorIncoming rays are
parallel to the optic axis and are not
reflected through F
Incoming rays diverge, as though they had come from point F behind the mirror
F is a virtual focal point
s is positive, s’ is negative
Example • Santa checks himself for soot, using his
reflection in a shiny silvered Christmas tree ornament 0.750m away. The diameter of the ornament is 7.20cm. Standard reference work state that he is a “right jolly old elf,” so we estimate his height to be 1.6m. Where and how tall is the image of Santa formed by the ornament? Is it erect or inverted?
• s’= -1.76cm; m= 2.34x10-2 ; y’= 3.8cm
REFRACTION AT A SPHERICAL SURFACE
Refraction at spherical interface
Refraction at a Spherical Surface
VC
Refraction at a Spherical Surface
na/s + nb/s’= (nb-na)/R
Object-image relation, spherical refracting surface
m=y’/y= -(nas’/nbs)
Lateral magnification, spherical refracting
surface
na/s + nb/s’=0At a plane refracting
surface
Example
A cylindrical glass rod in air has an index of refraction 1.52. and one end is ground to a hemispherical surface with radius R=2.00cm. a.) find the image distance of a small object on the axis of the rod, 8cm to the left of the vertex. b.) find the lateral magnification.
n=1.00
s’= 11.3cm
m= -0.929
ExampleA ray of light in air makes an angle of incidence of 45° at the surface of a sheet of ice. The ray is refracted within the ice at an angle of 30°A. What is the critical angle for the ice?B. A speck of dirt is embedded 3/4in below the surface of the ice. What is it’s apparent depth when viewed at normal incidence?
A. θcrit= 45°B. s’= -0.53in or 0.53in below
GRAPHICAL METHOD FOR LENSES
Biconcave and biconvex thin lenses
Lenses
LensesBiconvex lens; converging
Biconcave lens; diverging
LensesOnly F is
needed for the ray
diagram
Chief ray through the
center is undeviatedRay parallel is
refracted in such a way that it goes through
F on transmission
through the lensFocal ray is parallel to the axis of
transmission
For concave lens, the rays
appear to have passed through F on the object’s side of the lens
Lenses
An object is placed 30cm from a biconcave lens with a focal length of 10cm. Determine the image characteristics graphically.
ANALYTICAL METHOD FOR THIN LENSES
Lens maker's equation
Equations for thin lenses
1/s + 1/s’= 1/f Object-image relation, thin lenses
m=y’/y= -s’/sLateral
magnification, thin lenses
1/f=(n-1) [(1/R1)- (1/R2)]Lensmaker’s equation
Example• A biconvex lens is made of glass with n
= 1.65 and has radii of curvature R=R1=R2= 42 cm. Determine its focal length.
• f=32cm• A biconcave lens is made of glass with
n = 1.65 and has radii of curvature R=R1=R2= 42 cm. What is its focal length?
• f=-32cm
Example
An object is placed 30cm from a biconcave lens with a focal length of 10cm. Determine the image characteristics analytically.
s’=-7.5cmm=0.25
Virtual, upright, half the size of the object