geometrical optics and basic imaging light paths of the bright field microscope
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Geometrical Optics and Basic Imaging Light Paths of the Bright Field Microscope. E. D. Salmon University of North Carolina at Chapel Hill. Major Imaging Functions of the Microscope. - PowerPoint PPT PresentationTRANSCRIPT
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Geometrical Optics and Basic Imaging Light Paths of the Bright
Field MicroscopeE. D. Salmon
University of North Carolina at Chapel Hill
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Major Imaging Functions of the Microscope
• Magnification: Needed to overcome resolution limitations produced by finite size of recording sensors- rods and cones in eye, silver grains in film; pixels in CCDs
• Resolution: Limited by lens aberrations and finite wavelength of light
• Contrast: How to make resolvable structural detail visible-absorbing stains, phase contrast, DIC, Pol., immunofluorescence, fluorescent analogs, GFP-fusion proteins, other fluorescent molecular probes
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Camera
Camera AdapterBinocular
Eyepiece
Beam Switch
Filter Cube ChangerSlot for Analyzer
Slot for DIC Prism
Objective Nosepiece
Objective
Stage
Condenser: Diaphragm&Turret Centering Focus
Field Diaphragm
Coarse/Fine Specimen Focus
Filtersand Diffuser
Lamp: Focus, Centering
Mirror:Focus andCentering
Mirror:Focus andCentering
Focus, Centering
Trans-Lamp Housing
Epi-Lamp HousingEpi-Field Diaphragm
Epi-CondenserDiaphragm
ShutterFilters& Centering
Slot for Polarizer
Upright Microscope Stand
Body Tube
MICROSCOPE COMPONENTS
Magnification Changer
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IMAGING LIGHT PATHS ILLUMINATING LIGHT PATHS
Eyeor
Camera
Eyepiece
IntermediateImage plane
Objective Lens
Specimen
Condenser Lens
CondenserDiaphragm.
FieldDiaphragm
Collector Lens
Lamp
Objective Back FocalPlane
Tube Lens
MICROSCOPE ALIGNMENT FORTRANSMITTED LIGHT KOEHLER ILLUMINATION
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Some Visible Spectrum Light Sources
The eye is most sensitiveto green light!
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Primer on Geometrical Optics
• Light moves in straight lines through homogeneous media at velocity: v = c/n()
• Example values for n(546nm):Air 1.0Water 1.3333Cytoplasm 1.38Glycerol 1.46Crown Glass 1.52Immersion Oil 1.515Protein 1.51-1.53Flint Glass 1.62
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Reflection
N
r i
reflecting surface
N
mirror
r = 45
i= 45
o
o
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Reflection and Refraction at Transparent Surface
N N
r
i
n1
n2
n1
n2
r
i
a. n2 n1 <> n2 n1b.
i
i
Reflecting
Refracting
Reflecting
Refracting
Snell’s Law of Refractionn1sin(i) = n2sin(r)
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Total Internal Reflection Can Occur
Snell’s Law of Refractionn1sin(i) = n2sin(r)
N
n1
n2
r
i
N
n1
n2
b.a.
r = 90o
i c=
N
n1
n2
c.
r
i
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Total Internal Reflection is Used to Re-Direct Light
N
r i = 45
Prism
Fiber OpticLight Guide
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Homework
1. A beam of light in glass hits a surface at an angle. At what angle does the light just become total internally reflected if the glass has a refractive Index of 1.52 and the interface has a refractive index of :
a. Airb. Waterc. Immersion oil
In each case, what is the numerical aperture (NA) of the beam relative to the normal to the interface?
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Refraction is Usually Greater at Shorter Wavelengths
n
blue
red
1
n2
1 2
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Refraction at Curved Lens Surfaces: Action of Convex or Concave Lenses
F'
F'
F'
a.
b.
c.
d.
e.
F'
F'
F’ is Primary Front Focal Point of Lens
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Basic Action of Converging Lenses
F'
a.
b.
f
optical axis
f
F'
a a = f sin
Back FocalPlane(BFP)
Light parallel to the optical axis comes into focus at a point F’, the back focal point, located one focal length, f, from principle plane (PPL) of the lens.
Parallel light at angle, , to the optical axis comes into focus at a point, F”, located in the back focal plane and ata distance a = fsin() from the focalpoint, F’.
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Homework: What is an easy way to measure the approximate focal length of
a lens
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Basic Action of Converging Lenses (cont.)
Light emanating from the front focal point, F’, located a distance, f, on the optical axis from the PPL will emerge Parallel to the optical axis.
Light emanating from a point in the front focal plane, FFP, at distance a from the optical axis, will emerge as aparallel beam of light at angle, , tothe optical axis, where a = fsin().
a.
b.
f
optical axis
f
a
optical axis
FrontFocalPlane(FFP)
F
F
Example: Flashlight
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Real-Image FormationAs Object Moves Closer to Lens
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Three Light Rays Can Define Real Image Formation
PPL
f
o i
s2
F'FO
I
1
2
3
S1
f
M = I/O =i/o
1/i +1/o = 1/f
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Image Formation in the Human Eye
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Resolution Limitations of the Human Eye
250 mm
O' O"
I
I'
I"
ConventionalViewingDistance
O
³ 2.0 m
A B
Limits to Accommodation
Unresolved Resolved
COARSE FINE
Resolution Test
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Ocular is a Single Lens Magnifier
250 mm
O'
I
I'
O
f
O
Magnification (angular) = 250 mm/f
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Homework: What is The Ocular Focal Length for the Following
Magnifications?• 5X _________
• 10X _________
• 20X _________
• 25X _________
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The Objective Forms a Real Image At the Ocular Front Focal Plane: The Primary or
Intermediate Image Plane (IIP)
PPL
fob
OTL
s2
F'FO
I
1
2
3
S1
fob
IIP
foc
Conventional OpticsObjective with finite Focal Length(Optical Tube Length, OTL, Typically 160 mm)
Mob = OTL/fob
Total Magnification = Mob x Moc = OTL/fob x 250mm/foc
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Homework: For Finite Focal Length Objective and OTL = 160 mm, what is focal length for the following Objective
Magnifications• 4X _________
• 10X ________
• 20X ________
• 40X ________
• 60X ________
• 100X _______
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How to Insert Filters Above
Objective Without Inducing
Image Aberration
a. Conventional objective (no Telan Lenses)
b. Conventional objective with Telan lenses
c. Infinity Corrected objectives
OBJ
Glass Filter
PIP
Glass Filter
Glass Filter
PIP
PIPFocusing Lens
(Neg.) (Pos.)
Telan lenses
Mob = ffocusing/fob
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Zeiss introduced infinity corrected objective for biomedical scopes in late
1980’s, Nikon, Leica and Olympus followed by Mid-1990’s
Also, field of view in ocular enlarged from 18 mm to 24-25 mm.
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Numerical Aperture (NA) of Collection (a) or Illumination (b)
F'
f
NA = nSinobj
BFP
n
Iris Diaphragmor Stop
a.
cond
FFP
f
NA = nSin
b.
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How to Measure Objective NA
Low PowerObjective
Specimen Slide
Microscope Stage
Black Dotson White Card
n = 1
w w
h
1 2 3
3 2 1
White Card Set OnCondenser CarrierLowered All theWay Down.
(1) (2)
m
m
Lamp
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IMAGING LIGHT PATHS ILLUMINATING LIGHT PATHS
Eyeor
Camera
Eyepiece
IntermediateImage plane
Objective Lens
Specimen
Condenser Lens
CondenserDiaphragm.
FieldDiaphragm
Collector Lens
Lamp
Objective Back FocalPlane
Tube Lens
MICROSCOPE ALIGNMENT FORTRANSMITTED LIGHT KOEHLER ILLUMINATION
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Homework for Thursday: Go to http://micro.magnet.fsu.edu/primer/index.html
and work through:• Light and color• Anatomy of Microscope:
-Introduction
-concept of Magnification
-Microscope Optical components:
-Geometrical construction of Ray Diagrams
-Perfect Lens Characteristics
-Perfect 2 Lens Characteristics