physics for scientists and engineers ii, summer semester 2009 1 lecture 26: july 29 th 2009 physics...
Post on 22-Dec-2015
212 views
TRANSCRIPT
Physics for Scientists and Engineers II , Summer Semester 2009
1
Lecture 26: July 29th 2009
Physics for Scientists and Engineers II
Physics for Scientists and Engineers II , Summer Semester 2009
2
Ray Diagrams for Thin Lenses
1F 2F
Incoming Ray Outgoing Ray
Parallel to principal axis As if coming from focal point in front of the lens (F1)
Towards focal point behind the lens (F2)
Parallel to principal axis
Through center of lens Goes straight through
O I
Physics for Scientists and Engineers II , Summer Semester 2009
3
Combination of Thin Lenses
Similar to the procedure we used when calculating the effect of two refracting surfaces:
Step 1: Ignore lens 2 and calculate the image position due to lens 1.
Step 2: Determine whether image position from Step 1 is in front or behind lens 2. In front of lens 2: Object position for lens 2 positive (real object) Behind lens 2: Object position for lens 2 is negative (virtual object)
….and determine the distance to lens 2, of course.
Step 3: Determine the image position (of the object determined in step 2) due to lens 2.
21MMM Overall magnification:
Physics for Scientists and Engineers II , Summer Semester 2009
4
Example of Combination of Thin Lenses
O
cmf 201
cmf 252
cmd 15cmp 351
Physics for Scientists and Engineers II , Summer Semester 2009
5
Example – Step 1 (ignore lens 2)
1O
cmp 351
F
F1I
cmcmcm
cmcm
fp
fpq 47
2035
2035
11
111
34.135
47
1
11
cm
cm
p
qM
Physics for Scientists and Engineers II , Summer Semester 2009
6
Example – Step 2 (ignore lens 2)
1O
cmp 351
21 OI
cmq 471
cmcmcmp 3215472 cmd 15
Physics for Scientists and Engineers II , Summer Semester 2009
7
Example – Step 3 (ignore lens 1)
object) virtual(a 2O
cmp 322
cm
cmcm
cmcm
fp
fpq
1142532
253222
222
image) virtual(a 2I
57.332
114
2
22
cm
cm
p
qM
Physics for Scientists and Engineers II , Summer Semester 2009
8
Example of Combination of Thin Lenses
O
cmd 15cm35
I
cm114
cm99
Physics for Scientists and Engineers II , Summer Semester 2009
9
The Simple Magnifier – Angle Subtended
OEye
Objects appear larger if the angle subtended at the eye is larger.
Get closer to the object and becomes larger object appears larger.
Eye
cm
hθθ
25tan 00
Problem: At some point the human eye can no longer focus on the object. Typically, the closest distance is 25cm, the “near point of the eye” (varies individually, especially with age).
0θh
cm25
Physics for Scientists and Engineers II , Summer Semester 2009
10
The Simple Magnifier
OEye
Adding a lens and putting eye close to the lens such that the image appears at 25cm(able to focus on the image).
FI
cm25
p
h
cm
hθθ
25
'tan'h
p
fcm
fcmp
fcmp
25
25
1
25
11
Physics for Scientists and Engineers II , Summer Semester 2009
11
The Simple Magnifier
f
cm
f
fcm
fcmfcm
cm
p
cm
cmh
ph
Definition
251
25
2525
2525
25
m
)(m
max
0
Angular Magnification:
f
cm
f
cm 25m
251m :Glass Magnifying Simple minmax
f
cm
cmh
fh
cmh
ph
mf
h
p
h
fpfp
25
2525
point) focalat (Object 111
:at is image theif relaxedmost is eye The :However
min
Physics for Scientists and Engineers II , Summer Semester 2009
12
The Compound Microscope – Two converging lenses
Oof
Objective EyepieceefLfL ;0
cm) few (aef
L
cmfo 1
efo
o
f
fp
distance
small1
ofLforLq 1
oo f
L
p
qM
1
1:Objective Magnif.e
e f
cmm
25
:eyepiece Magnif.
1I
2I
Physics for Scientists and Engineers II , Summer Semester 2009
13
The Compound Microscope – Magnification
oo f
L
p
qM
1
1
:magnif.) (lateral Objective Magnif.
ee f
cmm
25
:magnific.)(angular eyepiece Magnif.
eoeo f
cm
f
LmMM
25
Magnification Using Compound Microscope:
Physics for Scientists and Engineers II , Summer Semester 2009
14
The Refracting Telescope
of
Objective Eyepiece
efef
1p ofq 1
ooo f
h'tan
e
o
o
e
o f
f
fh
fh
m
'
'
: Magnif.
oo
ef
h'tan
1I
2I
Physics for Scientists and Engineers II , Summer Semester 2009
15
Chapter 37: Condition for Interference of Light Waves
Interference = Superposition (adding) of waves
S1
S2
S1 S2
Example of Constructive Interference
Physics for Scientists and Engineers II , Summer Semester 2009
16
Condition for Interference of Light Waves
S1
S2
S1 S2
Example of Destructive Interference
Conditions for Interference: 1) Light from two sources must be “coherent”. That means, the relative phase
between S1 and S2 must remain constant.2) The light should be monochromatic (single wavelength).
Physics for Scientists and Engineers II , Summer Semester 2009
17
Young’s Double-Slit Experiment
Barrier with two small openings.Monochromaticlight.
Diffraction of light occurs.
Physics for Scientists and Engineers II , Summer Semester 2009
18
Young’s Double-Slit Experiment
Screen
Maximum
Maximum
Maximum
Minimum
Minimum
Constructive and destructive interference depending on direction.
Physics for Scientists and Engineers II , Summer Semester 2009
19
Center: Bright Spot
Constructive interference(bright fringe on screen)
Screen
Physics for Scientists and Engineers II , Summer Semester 2009
20
First Minimum (Destructive Interference)
Destructive interference(Dark fringe on screen)
Screen
Physics for Scientists and Engineers II , Summer Semester 2009
21
The next Maximum
Constructive interference(Bright fringe on screen)
Screen
Physics for Scientists and Engineers II , Summer Semester 2009
22
Light Waves in Interference
Od
S2
S1
y
P
Q
2r
1r
sin12 drr