Title: mirrors and lenses
1mirrors and lenses
- PHY232
- Remco Zegers
- zegers_at_nscl.msu.edu
- Room W109 cyclotron building
- http//www.nscl.msu.edu/zegers/phy232.html
2quiz (extra credit)
- a ray of light moves from air to a material with
ngt1, at an initial angle of 300 with the normal.
After reaching the material, the ray bends and
has an outgoing angle of 200 with the normal. Now
consider the reverse case a ray of light travels
from the same material with ngt1 to air. The
incident angle is 200. After reaching air, the
angle with the normal will be - a) 200
- b) between 200 and 300
- c) 300
- d) greater than 300
?0
300
200
200
3an important point
- objects do not emit rays of light that get seen
by your eye. Light (from a bulb or the sun) gets
reflected off the object towards your eye.
4we saw
- that light can be reflected or refracted at
boundaries between material with a different
index of refraction. - by shaping the surfaces of the boundaries we can
make devices that can focus or otherwise alter an
image. - Here we focus on mirrors and lenses for which the
properties can be described well by a few
equations.
5the flat mirror
- in the previous chapter we already saw flat
mirrors. - The distance from the object to the mirror the
object distance p - The distance from the image to the mirror is the
image distance q - in case of a flat mirror, an observer sees a
virtual image, meaning that the rays do not
actually come from it. - the image size (h ) is the same as the object
size (h), meaning that the magnification h/h1 - the image is not inverted
p
q
NOTE a virtual image cannot be projected on a
screen but is visible by the eye or another
optical instrument.
6question
- You are standing in front (say 1 m) of a mirror
that is less high than your height. Is there a
chance that you can still see your complete
image? - a) yes b) no
7ray diagrams
- to understand the properties of optical elements
we use ray diagrams, in which we draw the most
important elements and parameters to understand
the elements
h
h
p
q
8concave mirrors
F
M
C
C center of mirror curvature
F focal point
9concave mirrors an object outside F
O
F
step 3 note that a ray from the bottom of the
object just reflects back.
10concave mirrors an object outside F
O
F
I
- The image is
- inverted (upside down)
- real (light rays pass through it)
- smaller than the object
11concave mirrors an object outside F
O
F
I
distance object-mirror p distance image-mirror
q distance focal point-mirror f
- mirror equation 1/p 1/q 1/f
- given p,f this equation can be used to calculate
q - magnification M-q/p
- can be used to calculate magnification.
- if negative the image is inverted
- if smaller than 1, object is demagnified
12example
- An object is placed 12 cm in front of a a concave
mirror with focal length 5 cm. What are - a) the location of the image
- b) the magnification
- 1/p1/q1/f so 1/121/q1/5
- 1/q1/5-1/12 so q8.57 cm
- b) M-q/p-8.57/12-0.71
- this means that size of the image is only 71
of the - the size of the object and that it is
inverted.
13concave mirrors an object inside F
O
F
I
- the image is
- not inverted
- virtual
- magnified
step 3 note that a ray from the bottom of the
object just reflects back.
14concave mirrors an object inside F
O
F
I
- the image is
- not inverted
- virtual
- magnified
The lens equation and equation for magnification
are still valid. However, since the image is now
on the other side of the mirror, its sign should
be negative
15example
- an object is placed 2 cm in front of a lens with
a focal length of 5 cm. What are the a) image
distance and b) the magnification?
- 1/p1/q1/f so 1/21/q1/5
- 1/q1/5-1/2 so q-3.3 cm (note the -
sign!) - b) M-q/p-(-3.3)/21.65
- this means that size of the image is 65
larger than - the size of the object and that it is not
inverted ().
16demo the virtual pig
17convex mirrors an object outside F (pgtf)
O
F
F is now located on the other side of the mirror
step 3 note that a ray from the bottom of the
object just reflects back.
18convex mirrors an object outside F (pgtf)
O
F
I
F is now located on the other side of the mirror
- the image is
- not inverted
- virtual
- demagnified
The lens/mirror equation and equation for
magnification are still valid. However, since
the image and focal point are now on the other
side of the mirror, their signs should be negative
19example
- an object with a height of 3 cm is placed 6 cm in
front of a convex mirror, with f-3 cm. What are
a) the image distance and b) the magnification?
answer a) 1/p1/q1/f with p6 cm f-3 cm 1/6
1/q -1/3 so q-2 cm b) M-q/p-(-2)/61/3 th
e image is only 33 of the height of the object.
20convex mirrors with p lt f
- the situation is exactly the same as for the
situation with p gt f. The demagnification
will be different though
O
I
F
F
21Mirrors an overview
type p? image image direction M q f
concave pgtf real inverted Mgt0 M -
concave pltf virtual not inverted Mgt1 M -
convex pgtf virtual not inverted Mlt1 M - -
convex pltf virtual not inverted Mlt1 M - -
- mirror equation 1/p 1/q 1/f
- fR/2 where R is the radius of the mirror
- magnification M-q/p
22lon-capa
- now do problems 7,8,11 of lon-capa 8
23question (extra credit)
- a object is placed in front of a concave mirror,
exactly at the location of the focal point (pf).
What is the image distance q? - a) qp
- b) qf
- c) q0
- d) q infinity
24Lenses
- Lenses function by refracting light at their
surfaces - Their action depends on
- radii of the curvatures of both surfaces
- the refractive index of the lens
- converging (positive lenses) have positive focal
length and are always thickest in the center - diverging (negative lenses) have negative focal
length and are thickest at the edges
used in drawings
-
25lensmakers equation
object
1
2
R2
f focal length of lens n refractive index of
lens R1 radius of front surface R2 radius of back
surface
R1
R2 is negative if the center of the circle is on
the left of curvature 2 of the lens R1 is
positive if the center of the circle is on the
right of curvature 1 of the lens
if the lens is not in air then (nlens-nmedium)
26example
- Given R110 cm and R25 cm, what is the focal
length? The lens is made of glass (n1.5)
object
1
2
R2
R1
R1 is on the right of the curvature, so positive
10 cm R2 is on the left of the curvature, so
negative 5 cm n1.5 1/f0.5(0.1-(-0.2))0.15
f6.67 cm
27example 2
- Given R15 cm and R210 cm, what is the focal
length? The lens is made of glass (n1.5)
object
1
2
R1
R2
R1 is on the left of curvature 1 so R1-5 cm R2
is on the right of curvature 2 so R210
cm n1.5 1/f0.5(-0.2-0.1)-0.15 f-6.67 cm
28example 3
- Given R15 cm and R2?, what is the focal length?
The lens is made of glass (n1.5)
object
1
2
R1
R2
R1 is on the left of curvature 1, so R1-5 cm R2
is infinity (either positive or
negative) n1.5 1/f0.5(-0.2 0.)-0.1 f-10
cm
29question
- A person is trying to make a lens but decides to
make both surfaces flat, resulting in essentially
a flat piece of glass on both sides. What is the
focal length of this lens? - a) infinity
- b) 0
- c) cannot say, depends on the index of refraction
n
30converging lens pgtf
O
F
F
A real inverted image is created. The
magnification depends on p M can be lt1, 1 or gt1
31lens equation
I
O
F
F
The equation that connects object distance p,
image distance q and focal length f is (just like
for mirrors) 1/p 1/q 1/f Similarly for the
magnification M-q/p
q is positive if the image is on the opposite
side of the lens as the object NOTE THAT THIS IS
DIFFERENT THAN THE CASE FOR MIRRORS
32example
- an object is put 20 cm in front of a positive
lens, with focal length of 12 cm. a) What is the
image distance q? b) What is the magnification?
a) p20 cm, f12 cm use 1/p 1/q 1/f 1/20
1/q 1/12 solve for q gives q30 cm b)
M-q/p-30/20-1.5 The image is inverted (M
negative). The image is magnified (Mgt1)
33converging lens pltf
O
F
F
A virtual non-inverted image is created.
Magnification gt1
34example
- an object is put 2 cm in front of a positive
lens, with focal length of 3 cm. a) What is the
image distance q? b) What is the magnification?
a) p2 cm, f3 cm use 1/p 1/q 1/f 1/2 1/q
1/3 solve for q gives q-6 cm NOTE q is
negative which means it is on the same side of
the lens as the object b) M-q/p-(-6)/23 The
image is not inverted (M positive). The image is
magnified (Mgt1) The image is virtual
35question
- An object is placed in front of a converging
(positive) lens with the object distance larger
than the focal distance. An image is created on a
screen on the other side of the lens. Then, the
lower half of the lens is covered with a piece of
wood. Which of the following is true - a) the image on the screen will become less
bright only - b) half of the image on the screen will disappear
only - c) half of the image will disappear and the
remainder of the image will become less bright.
I
O
F
F
screen
36NOT CORRECT
37diverging lens pgtf
O
F
F
-
A virtual non-inverted image is created. The
magnification Mlt1
38example
- an object is put 5 cm in front of a negative
lens, with focal length of -3 cm. a) What is the
image distance q? b) What is the magnification?
a) p5 cm, f-3 cm use 1/p 1/q 1/f 1/5 1/q
-1/3 solve for q gives q-1.88 cm b)
M-q/p-(-1.88)/50.375 The image is
non-inverted (M positive). The image is
demagnified (Mlt1)
39diverging lens pltf
F
F
O
-
A virtual non-inverted image is created. The
magnification Mlt1 similar to case with pgtf
40example
- an object is put 2 cm in front of a negative
lens, with focal length of -3 cm. a) What is the
image distance q? b) What is the magnification?
a) p2 cm, f-3 cm use 1/p 1/q 1/f 1/2 1/q
-1/3 solve for q gives q-1.2 cm b)
M-q/p-(-1.2)/20.6 The image is non-inverted
(M positive). The image is demagnified (Mlt1)
41lenses, an overview
type p? image image direction M q f
converging pgtf real inverted Mgt0 M -
converging pltf virtual not inverted Mgt1 M -
diverging pgtf virtual not inverted Mlt1 M - -
diverging pltf virtual not inverted Mlt1 M - -
- mirror equation 1/p 1/q 1/f
- magnification M-q/p
- lens makers equation 1/f(n-1)(1/R1-1/R2)
42spherical aberrations Hubble space telescope
spherical aberrations are due to the rays hitting
the lens at different locations have a different
focal point
perfect
distorted
example Hubble
before after correction
43chromatic aberrations
Chromatic aberrations are due to light of
different wavelengths having a different index
of refraction Can be corrected by combining
lenses/mirrors
If n varies with wavelength, the focal length
f changes with wavelength
44two lenses
- an object, 1 cm high, is placed 5 cm in front of
a converging mirror with a focal length of 3 cm.
This setup is placed in front of a diverging
mirror with a focal length of 5 cm. The distance
between the two lenses is 10 cm. Where is the
image located, and what are its properties?
-
3cm
5cm
5 cm
15 cm
45answer
-
O
5cm
3cm
15 cm
5 cm
46lon-capa
- now do problems 9,10,12 of lon-capa 8