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1 de 117
-DR. PARIKSHYA SHRESTHA
-P.G. 1ST YEAR
-DEPT OF ORAL PATHOLOGY AND MICROBIOLOGY
-RAJARAJESWARI DENTAL COLLEGE AND HOSPITAL
MICROSCOPE - I
CONTENTS
 INTRODUCTION
 HISTORY
 TYPES OF MICROSCOPE
 COMPONENTS OF MICROSCOPE
 LIGHT AND ITS PROPERTIES
 LENS
 COMPONENTS OF MICROSCOPE IN DETAIL
 MAGNIFICATION AND ILLUMINATION
 MICROMETRY
 CLEANING AND MAINTAINANCE OF MICROSCOPE
 DARK GROUND MICROSCOPY
 POLARIZING MICROSCOPY
 PHASE CONTRAST MICROSCOPY
 INTERFERENCE MICROSCOPY
 DIFFERENTIAL INTERFERENCE CONTRAST MICROSCOPY
 REFERENCE
Introduction
 The word microscope is derived from two Greek words ‘mikro’
meaning ‘small’ and ‘scopien’ meaning ‘to view’.
 Thus, it is an instrument which enables us to view small objects
by magnifying it and making it possible to be seen by the viewer.
 The science of investing small objects using such an instrument
is called Microscopy
History of microscope
1590 – Hans and Zachcharias Janssen of Holland claimed to
have invented microscope
1609 – Galileo Galileli developed a compound microscope with
convex, concave lens
1572-1633 – compound microscope with two convex lens, invented
in Rome by Carnelius Drebbel
1625 – Giovanni Faber coined the term microscope
History of microscope
1674 – Anton van Leeuwenhoek made and used a simple
microscope to view biological specimens.
Types of microscopes
Basically two types of microscope :
1. Simple Microscope : A simple microscope consists of a
single lens or a magnifying glass.
2. Compound microscope : A compound microscope consists
of two or more lenses.
Compound microscope can be further divided according to
different microscopic methods used .
Types of microscopes
Simple microscope Compound microscope
Microscopic Methods
A. Light Microscopy
1. Brightfield (light) microscopy
2. Darkfield microscopy
3. Phase-contrast microscopy
4. Interference microscopy
5. Differential interference contrast microscopy
6. Fluorescent microscopy
7. Polarizing microscope
B. Electron Microscopy
1. Transmission electron microscopy
2. Scanning electron microscopy
3. Scanning transmission electron microscopy
4. Atomic force microscopy
C. Scanning Probe Microscopes
Components of microscope
LIGHT
 Visible light is that portion of electromagnetic spectrum
that can be detected by human eyes, having wavelength
ranging from approx 400 nm to 800nm
 Light travels in straight lines. Light travels at different
speeds in air and in glass. Its path can be deflected or
reflected by means of mirrors or right angle prisms.
LIGHT
RETARDATION AND REFRACTION
 If light enters sheet of glass at right angle, light is retarded in
speed but direction is unchanged.
 If light enters the glass at any other angle, a deviation of direction
will occur in addition to retardation and this is called refraction.
LIGHT
 Light is slowed or retarded and “bent” or refracted
when it passes through air and enters a convex lens, gets
refracted when it leaves the convex lens and reenters air.
LIGHT
The curved lens will exhibit both retardation and refraction,
the extent of which is governed by :
a) Angle of incidence : angle at which light strikes the lens
b) Refractive index
c) Curvature of the lens
Angle of refraction : the angle to which the rays are deviated
within the glass or other transparent medium
LIGHT
 Refraction depends on the optical density of medium from
which lens is made, which is indicated by refractive index
(RI)
RI = velocity of light in air/velocity in subatance
 Refractive index is of great value in the computaion and
design of lenses, microscope slides and coverslip and
mounting media.
 RI of air = 1.00, water = 1.30, glass = 1.50
LIGHT
 Total internal reflection : light passing from glass into air
emerges parallel to the surface of lens if the angle of
incidence is increased. If the angle is too great, (critical
angle), the rays do not emerge but are totally internally
reflected.
LENS
 LENS
 Piece of glass or other transparent material, usually circular,
having the two surfaces ground and polished in a specific form
in order that rays of light passing through it shall either
converge or diverge.
 Two types of lens:
 Positive lens
 Negative lens
LENS
 Positive lens
 Thicker at centre
 Causes light rays to concentrate or converge to form a real
image
 Negative lens
 Thinner at centre
 Light passing will diverge or scatter and real image are
not seen
LENS
Focus
 When the lens concentrates the light rays to form a clear sharp
image of an object, the object is said to be in focus.
 The term ‘focus’ or ‘principal focus’ are used to indicate the
position in which a lens will form a sharp, clear picture of a
distant object.
 Conjugate foci : in addition to principal focus, a lens also has
conjugate foci; these are two points one on each side of the lens,
in one of which a clear image will be formed on a screen of an
object placed in the other.
LENS
 Image formation
LENS
Image formed
1. Real Image
 Formed by Objective lens of microscope
 Image is inverted, at greater magnification
 Can be seen on a screen
LENS
2. Virtual image
 Image formed within principal focus on same side of object
 Image appears the right way up and enlarged
 Cannot be focused on screen
 Formed by eyepiece of the microscope of real image
projected from the objective
Defects of Lens
1. Chromatic aberration
 Colours of white light, each refracted to different degree
 Shorter wavelength, greater degree of refraction
 White light entering a lens, on emerging forms a different
point of focus for each component colours, blue being
focused at a point nearer the lens than red
 Results in unsharp images with colored fringes
Defects of Lens
Correction : It is known as achromatism
 Done by using two component lens
 Positive lens is combined with a negative lens
 construction of compound lens of different glass element
a) Achromatic lens : will correct a thin positive lens for any two
colour
b) Apochromatic lens : fluorspar is incorporated, three colors can
be brought to the one focal point and the amount of chromatic
aberration visible in image is negligible.
Defects of Lens
2. Spherical aberration
 Due to entry of light rays into curved lens at its periphery
 Refracted more that at a centre and thus not brought to a
common focus
 Blurred image is formed
 Correction : same pattern used for chromatic aberration ie
using a powerful positive lens and partially neutralizing its
magnifying power with a negative lens made of glass having a
greater relative aberration
COMPONENTS OF MICROSCOPE
Eyepiece
 Function - to magnify the image formed by the objective
within the body tube, and present the eye with a virtual
image.
 Limits the field of view as seen by the eye
 Usually 5x, 7x, 10x, 20x, 40x type magnification are used.
 Can be used to correct the residual errors in objective lens.
 Undercorrected : blue ray refracted to greater degree than red;
blue fringe
 Overcorrected : orange fringe seen at edge of field diaphragm
Eyepiece
Types of eyepiece
1. Positive eyepiece : Ramsden eyepiece
2. Negative eyepiece : Huygenian eyepiece
Eyepiece
Positive eyepiece :
 With this, the focus is outside the
eyepiece lens system
 Field stop is outsidethe eyepiece,
from which the virtual image is
focused and magnified by entire
eyepiece.
 Ramsden eyepiece : lower lens has
its plane side towards object. These
are preferred for micrometer
eyepiece as they impart less
distortion to scales
Eyepiece
Negative eyepiece :
 With this, the focus is within the
eyepiece lens system
 Lower or field lens collects the image
that would have been formed by the
objective and cones it down to a
slightly smaller image at the level of
the field stop within eyepiece; upper
lens then produces an enlarged
virtual image that is seen by eye.
 Huygenian eyepiece : these are
undercorrected and are best suited
for use with achromatic objectives.
Eyepiece
 Other types :
 Compensating eyepiece
 Pointer eyepiece
 Micrometer eyepiece
 Double demonstration eyepiece
 High focal point eyepiece
Objective
 These are screwed into lower end of body tube by means of
standard thread, thus are interchangable.
 Designated by their focal length, dependent on tube length
 Consists of lenses and elements 5-15 in number, depending
on ratio, type and quality
Objective
 The main task of objective is to collect maximum light
possible from the object, unite it and form a high quality
magnified image some distance above.
 Every objective has a fixed working distance, focal length,
magnification and numerical aperture (NA) .
Objectives
Specifications mentioned on objective
Objective
 The working distance is the distance between an object in focus
and the front of the lens system of the objective.
 The focal length in the compound lens it is the distance between
an object in focus and a point approximately halfway between the
component lenses of the objective.
 Total Magnification is product of magnification values of
eyepiece and objective in a standard microscope.
Objective
Color Codes
 Microscope manufacturers label their objectives with color codes
to help in rapid identification of the objective.
Table : Color codes used for objectives
Magnification Color Code
4× Red
10× Yellow
40× Light Blue
100× White
Objective
Coverglass thickness
 is important if high-power 'dry’ objectives are being used, when
No. 1 coverglasses should be used, or an objective with a
correction collar may be employed which allows a range of
thickness or coverslip from 0.12 to 0.22 mm to be used (usually
0.17mm)
 oil-immersion objectives do not have coverglass restrictions since
they will have the same refractive index as the immersion oil.
Objective
Resolution
 The ability of the lens to distinguish fine structural details in a
specimen is known as the ‘resolving power’. It is the smallest
distance between two dots or lines that can be seen as separate
entities.
 It depends on the wavelength of light (λ) and the Numerical
Aperture of the lens.
 It is calculated as:
Resolution = 1.2 λ/2NA
Objective
Numerical Aperture
 This ability is of an object to resolve detail is expressed in terms
of numerical aperture(NA)
 Numerical aperture depends primarily on the extreme range of
the divergent rays that can be made to enter the lens (angular
aperture) and secondarily on the refractive index of the medium
between the object and the objective.
 The relation between numerical aperture, angular aperture and
refractive index is:
NA = n× Sin u
n=refractive index of medium between lens and object
sin u = the sine half the angle of aperture
Objective
Effect of high NA
 whilst a high numerical aperture increases the resolution
of an objective, it has the following disadvantages:
a) it reduces the depth of focus, i.e. the ability to focus on more
than one layer of an object at the same time, and
b) it reduces the flatness or the field, so that the edges are out of
focus.
Objective
Types of Objectives
 In most modern microscopes objectives are usually made up
more than one lens.
 This series of lenses is used to overcome certain limitations in
the lenses.
Types of Objective
 Achromatic: Corrected for two colors red and blue. It is the most
widely used for routine purposes.
 Fluorite: Corrected for yellow green color. Green light is
brought to a shorter focus and violet light to a longer focus.
 Apochromat: All colors are brought to same focus. It is fully
corrected for three colors. More highly corrected, often
incorporating fluorite glass. These lenses are used especially for
photomicrography and for screening cytological smears.
 Plan-achromat: Although histological sections are flat the
image produced by the microscope is not flat. It is saucer
shaped; it is not possible to focus the whole of the field sharply
at any one time. This aberration is corrected using flat-field
objective, also called as plan-achromat lenses.
Objective
Types of Objectives
Design and arrangement of lens in objective
Body tube
 Attached to limb, standard 160mm length
 Nosepiece/carrier for objectives fitted at lower end,
designated by number of objectives (2/3/4 based on
magnification needed.
 Three main forms : monocular, binocular and combined
photo-binocular
Body tube
Binocular
Microscope
Binocular tubes have provision made for
the adjustment of the interpupillary
distance, enabling each observer to adjust
for the individual facial proportion
Adjustments
a) Coarse adjustment knob
 enables the stage and substage to be moved rapidly up and
down
b) Fine adjustment knob
 enables the stage and substage to be moved slowly and
accurately
 Works by micrometer screws, levers and cams
Object Stage
A rigid platform above the condenser which supports the
glass slide is object stage.
Object Stage
 It has an aperture in the
center through which the light
can pass to illuminate the
specimen on the glass slide.
 The stage holds the slide
firmly and allows the slide
movements with a mechanical
vertical and horizontal
adjustment screws.
Object stage
 The mechanical stage is graduated with Vernier scales and the x
and y movements assist the operator to return to an exact
desired location in the specimen.
 Traveling range in most of the microscopes is 76 mm(X) 30 mm
(Y).
Illuminating apparatus
Substage :
 below the stage, attached to it and adjustable
 consists of:
1. Condenser
2. Iris-diaphragm
3. Filter carrier
4. Mirror
Condenser
 Light from the lamp is
directed into the sub stage
condenser either directly or
from a mirror or prism.
 The main purpose of the
condenser is to focus or
concentrate the available
light into the plane of the
object
Condensers
 Condensers should have the same numerical aperture as
objective.
 The ideal condenser should form a perfect image of the light
source.
 Three types of condensers are used :
 Abbe Condenser
 Aplanatic Condensers
 Achromatic Condensers
Iris diaphragm
 Also called aperture diaphragm
 Used to control the cone of light entering the condenser
 Intensity should always be reduced by using filters and not
by closing the diaphragm
 Adjustment of this iris diaphragm will alter the size and
volume of the cone of light focused on the object.
Iris diaphragm
 If the diaphragm is closed
too much, the image
becomes too contrasty and
refractile, whereas if the
diaphragm is left wide
open, the image will suffer
from glare due to
extraneous light
interference.
Iris diaphragm
 In both cases the resolution of the image is poor.
 The correct setting for the diaphragm is when the numerical
aperture of the condenser is matched to the numerical
aperture of the objective in use.
Filter carrier
 Usually a metal ring, pivoting on a screw to facilitate
the easy removal of filters
Mirror
 Plano concave mirror, fitted about 4 inch below stage
 Concave side have focus from object
 Plane mirror must always be used with condenser
 Built-in light source have mirrors fixed at the base.
MAGNIFICATION AND
ILLUMINATION
Magnification
 Magnification of lens will depend on its conjugate foci, i.e. the
distance from object to the lens and that from lens to image.
 Magnification is the product of the magnification of the
objectives and eyepieces and is dependent on following factors:
1. Focal length of objective
2. Distance between focal plane of objective and image it produces
3. Magnification of eyepiece
Magnification =Tube length × Eyepiece magnification
Focal length of the objective
Illumination
 Artificial illumination supplied by an electric filament lamp is
most commonly employed.
 Source of illumination should be:
1. Uniformly intense
2. Should completely flood the back lens of the condenser with
light when the lamp iris diaphragm is open
3. Make the object appear as though it were self-luminous
 In light microscope two different types of illuminations are used.
 • Critical illumination
 • Kohler illumination
Setting up microscope
Nelsonian method
 Light source should be
homogeneous and no lamp
condenser
 employed with bare light
source
 Light source should be
focused on the object plane
by racking the substage
condenser up or down
Setting up microscope
Kohler illumination
 Non homogeneous light
source
 Lamp condenser is essential
to project an image of lamp
filament onto the substage
iris diaphragm
 Lamp condensing lens
functions as light source
 Used with compound
microscope
Micrometry
 The standard unit of measurement in microscopy is a
micrometer(μm), which is 0.001mm
 To measure microscopic objects an eyepiece micrometer scale is
used in conjugation with stage micrometer.
A. Eyepiece micrometer
 Usually a disc on which arbitary scale is engraved
 Placed inside Huygenuan eyepiece, resting on the field stop.
 Gives sharp image of scale and have a greater eye clearance
B. Stage micrometer
 Consists of a 3 x 1 inch slide on which a millimeter scale is
engraved in 1/10 and 1/100 graduations
Cleaning and Maintainance
A. Daily cleaning routine
 Should be dusted daily and outer surface of lens of objective
polished with lens tissue or cotton wool
 Top lens of eyepiece polished to remove dust or fingerprints
and microscope set up for correct illumination. If dust still
present, eyepiece may need to be dismantled and both lenses
cleared.
 Substage condenser and mirror are cleaned in a similar
manner
 Removal of chemically active and sharp pieces of grits and
foreign material if present
Cleaning and Maintainance
B. Weekly cleaning routine
 Slides of adjustment, stage, substage wiped with cloth (in
xylene damp)
 Lens system checked
 Chip blower can be used for cleaning eyepiece and objective
Handling the Microscope
 Carry it with 2 hands-one on the arm and the other under the
base.
 Use lens paper (ONLY) to remove any oil from the 100X lens.
 Once oil has been added to the slide, do not move back to the
40X lens to focus: oil should never get on this lens. If this
happens, it will be very difficult to get all of the oil off.
 Turn the coarse adjustment knob so that the stage is far from the
lens.
 Place the microscope back into the correct spot in cabinet, with
the arm toward us, making sure that the 10X low power lens is
in place, pointing towards the stage-not the 100X oil immersion
lens. The lens could hit against the stage and get scratched.
DARK GROUND MICROSCOPY
Dark Field
 Fine structures can often not be seen in front of a bright
background as visibility is dependent on contrast between
object and the background.
Dark ground microscopy:
 the oblique light is thrown upon the object which does not
enter through the objective, they appear as self illuminous
objects on dark background.
 Only the reflected or scattered light forms the image of the
object.
Objectives and condensers:
 Objectives must have a lower
numerical aperture than the
condenser
 Low power- black
paper/glass inserted into filter
carrier.
 central rays are cut off and
peripheral rays from the
condenser passes through the
object but do not enter the
objective; the only light
entering the objective will be
that scattered by the object
Objectives and condensers:
 High power-special condenser
 Oil immersion must be used between the objective and object to
ensure maximum reflected light from the object enters the
objective
 Fixed-focus condenser: commonly used- thin glass slides and
coverslips( ideal no:1)
Setting up the microscope:
 Thin preparation- thin slide- coverslip
 Adjust light direct/through the condenser
 Place a drop of oil immersion on lower side of slide and also on top
lens of the condenser
 Move the rack up untill both surfaces meet without forming air
bubbles
 If correctly focused a small point of light will illuminate the object
on a dark background(low power)
 High power: place drop of oil on the coverslip and focused
Advantages and disadvantages
Advantages:
 Finer structures can be seen clearly hence can be best used
for spirochetes.
Disadvantages:
 Misleading impression of size
 When stained , difficult to see
 Need thinner sections without any refractory material like
oil, water droplets, air bubbles etc..
POLARIZING MICROSCOPY
POLARIZING MICROSCOPY
PRINCIPLE:
 Light rays when passed through a crystal are retarded in speed.
Being unevenly dense, the crystal will retard the rays to a different
degree hence the rays will be refracted or bent to differing degrees.
 This is known as DOUBLE REFRACTION OR BIREFRINGENCE
 The direction of vibration of the emergent rays will be at right
angles to each other.
Principle:
 A ray of light entering such a crystal will be converted
into two rays which will emerge at two different points.
 The emergent light rays will be polarized(one ray-on
single direction, second ray- single direction and right
angle to the first ray)
ISOTROPIC: substances through which light can pass in any
direction and at the same velocity , not able to produce polarized
light.
DICHROISM: A phenomenon given rise to by some substances and
crystals which can produce plane polarized light by differential
absorption.
PLEOCHORIC FILMS: Dichroic crystals are suspended in thin plastic
films and oriented in one direction .They can absorb all the colors
equally.
NICOL PRISM
 It is composed of a crystal made of Icelandic spar slit in half
and the halves cemented together with Canada balsam.
 Light rays having passed through it would emerge vibrating
in a single plane.
 The single direction in which the light is vibrating when it
emerges is known as the optical path of the prism.
POLAROID DISCS
 They are glass or celluloid covered discs with the ability to
polarize light
 Act as a single crystal of herpathite embedded in nitro cellulose
and mounted between plastic sheets which is not only
birefringent but has the ability to absorb the ordinary ray which
would be refracted out of a Nicol prism
 Only allows the extraordinary light to be transmitted.
MAIN COMPONENTS OF THE MICROSCOPE
The two polarizer's used are:
 POLARIZER
 ANALYSER
Polarization
Analyzer
Polarizer
POLARIZER
 Placed beneath the sub stage condenser
 Held in a rotatable graduated mount
 Can be removed from the light path when not required
ANALYSER
 Placed between the objective and eyepiece
 Is graduated-markings
 Enhances the image
POLARIZING MICROSCOPY
 In a polarizing microscope, a polarizing filter is placed
between light source and specimen.
 The second polarizer called analyzer is placed above
specimen between objective and eyepiece.
POLARIZING MICROSCOPY
 If the vibration directions
of the object correspond to
the vibration of the
polarizer when the
polarizer and analyzer are
at right angles there is
absence of light through
eyepiece.
Appearance of object depends on interference of the two
rays recombined in the analyzer which depends on phase of
difference between the two rays which in turn depends on the
difference in the two refractive indices of the crystal and on its
thickness
If the vibration direction do not correspond then the rays of
light transmitted by the object will be resolved in analyzer and
object appears bright on a dark background.
WORKING:
TYPES OF BIREFRINGENCE
 INTRINSIC OR CRYSTALLINE
 FORM
 STRAIN
 POSITIVE
 NEGATIVE
 QUARTZ AND COLLAGEN-POSITIVE BIREFRINGENCE
 POLAROID-
DISCS,CALCITE,URATES,CHROMOSOMES-NEGATIVE
BIREFRINGENCE
SIGN OF BIREFRINGENCE
 The ray passing through a medium of high RI is called slow and if
it passes through a medium of low RI it is called fast.
 If the slow ray is parallel to the length of the crystal, or fiber
birefringence is positive.
 If the slow ray is perpendicular to the long axis of the structure,
birefringence is negative.
 Determined by the use of a compensator either above the
specimen or below the polarizer at 45° to the direction of
polarized light.
 The compensator or specimen is rotated till the slow direction of
the compensator is parallel to the long axis of the crystal or fiber.
 The field is now red and if the crystal is blue the birefringence is
positive
 If the slow direction of compensator is parallel to the fast
direction of the crystal, it appears yellow and has negative
birefringence.
APPLICATIONS
It is used in the detection and observation of:
 Artifacts like formalin pigment
 Crystals of urate ,pyrophosphates etc
 Lipids, myelin etc
 Bone structure
 Proteins like collagen,amyloid,keratin
 Charcot-Leyden crystals, muscle striations etc.
PHASE CONTRAST MICROSCOPY
PHASE CONTRAST MICROSCOPY
 It is a technique which enables us to see very transparent
objects, which are almost invisible by ordinary transmitted light,
in clear detail and in good contrast to their surroundings, and to
see very small differences in thickness and density within the
objects.
 This is accomplished by converting these slight differences in
refractive index and thickness into changes of amplitude.
PRINCIPLE
 A ray of light is made of waves travelling together in a straight
line. When two such waves travel together,they are said to be in
phase. Such a ray will appear bright to the observer
 If one of the waves is held up or made to change the path, they
will no longer travel together and are said to interfere with each
other, differing in their intensity
 A special condenser and objective control the illumination in a
way that accentuates the differences in densities.
 It causes light to travel different routes through the various
parts of the cell
 The result is an image with differing degrees of darkness and
brightness collectively called contrast
Interference
CONSTRUCTIVE INTERFERENCE
 Light rays are in phase
 Amplitude or brightness is ‘doubled’ when recombined
DESTRUCTIVE INTERFERENCE
 Light rays are incoherent
 ½λ out of phase
 No light is seen
 Maximum interference
PARTS OF A PHASE CONTRAST
MICROSCOPE
ANNULUS:
 Made of opaque glass
 Has a hollow clear ring
 Can be centered by means of centering screws
PHAZE PLATE OR Z PLATE
 Clear glass disc with a circular trough etched in it to half the depth of disc
 The light passing through the trough has a phase difference of 1/4ƛ
compared to the rest of the plate
 Also contains a neutral density light absorbing material to reduce
brightness of direct rays.
PARTS OF A PHASE CONTRAST
MICROSCOPE
HIGH INTENSITY COMPOUND LAMP
 Usually used with a mercury green filter
AUXILLARY TELESCOPE
 Used in place of an eyepiece for examining the back focal
plane of the objective
Image formation in phase contrast microscope
WORKING OF THE MICROSCOPE
 Annulus is placed in the condenser and the phase plate is placed
in the objective
 It allows only a small ring of light to pass into the microscope
 The phase plate has a circle engraved on it which should match,
with the ring of light coming in from the annulus through the
condenser.
 Some rays of light will pass through unaltered while some
rays will be retarded or diffracted by approximately 1/4ƛ.
 On passing through a phase plate the diffracted ray is
retarded further by 1/4ƛ and will now interfere with the
direct light ray.
 The total retardation of diffracted rays is now 1/2ƛ and
interfere will produce image contrast thus revealing even
small details.
APPLICATIONS
 For examining unstained bacteria
 For examining wet preparations of specimens
 For examining faecal preparations for trophozoites or amoebae
 In searching for trypanosomes in blood and other body fluids
INTERFERENCE MICROSCOPY
 generates mutually interfering beams which produce the
contrast. It is this feature which enables very small phase
changes to be seen and measured.
 The two rays which eventually combine to produce image are
formed by a plate of birefringent material placed immediately
above the condenser.
 These two rays having passed through the object plane are
recombined by a similar plate of birefringent material below the
front lens of the objective.
 One ray passes through a point
in the object and the other
through an area adjacent to it.
 Each point in the final image is a
compound one made up of two
mutually interfering rays.
 A special Wollaston prism is
added to the condenser to split
the beam of light and also to
recombine the two dissimilar
beams.
APPLICATIONS
 To study individual parts of living cells with maximum
resolution of detail
 To estimate dry mass when it is applied as a highly accurate
optical balance
 To assess section thickness of specimen.
DIFFERENTIAL INTERFERENCE
CONTRAST MICROSCOPY
 Designed by Nomarski hence also called as Nomarskis
microscope.
 Relies on the interference of a pair of wave fronts to
generate contrast.
It comprises of:
-a polarizer
-a condenser with a modified Wollaston prism
-a beam splitting slide
This slide consists of a modified Wollaston prism oriented at
45° to anattached analyzer,mounted in an adjustable carriage
and accommodated in the analyzer slot between the
objective and the eyepiece.
Working of the microscope
 Polarized light passes through the prism below the
condenser
 The prism below the condenser acts as a compensator
 Every interference fringe of the upper prism is correlated
with an interference fringe of the same order but opposite
sign in this compensator
 The two rays pass in turn through the condenser the
object and the objective before passing through the
second prism and analyzer.
 The upper prism can be moved laterally enabling the rays
to be displaced laterally or sheared before being
recombined in the analyzer when they undergo
interference.
 This produces ‘interference contrast’ and together with
rotation of the polarizers enhances the three-dimensional
(3D) effect in the image.
ADVANTAGES
 Wide variety of interference colors can be used
 Improved image contrast
 No phase halo included
 Lateral shearing of rays is reduced so that excellent three
dimensional images can be produced.
USES
 As an infinitely variable phase contrast microscope,
individual parts of living cells can be studied.
 As a highly accurate optical balance, used for estimating dry
mass down to 1x10 gm
 Quantitative measurement of phase change or optical
path difference
 Studying live and unstained biological samples such as a
smear from a tissue culture or individual water borne celled
organism
References
 Textbook of oral pathology – Jaypee brothers, 1E; Anil Ghom,
Shubhangi Mhaske
 Histology A Text and Atlas - With Correlated Cell and Molecular
Biology, 7E (2015) ; Wojciech Pawlina
 Bancroft’s Theory and Practice of Histological Techniques ,7th edition
 CFA Culling’s Histological techniques
 Essentials of Microbiology; Surinder Kumar ,1st edition, 2016
 MICROSCOPE Basics and Beyond, Revised edition 2003, Mortimer
Abramowitz

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basics of microscope - part 1

  • 1. -DR. PARIKSHYA SHRESTHA -P.G. 1ST YEAR -DEPT OF ORAL PATHOLOGY AND MICROBIOLOGY -RAJARAJESWARI DENTAL COLLEGE AND HOSPITAL MICROSCOPE - I
  • 2. CONTENTS  INTRODUCTION  HISTORY  TYPES OF MICROSCOPE  COMPONENTS OF MICROSCOPE  LIGHT AND ITS PROPERTIES  LENS  COMPONENTS OF MICROSCOPE IN DETAIL  MAGNIFICATION AND ILLUMINATION  MICROMETRY  CLEANING AND MAINTAINANCE OF MICROSCOPE  DARK GROUND MICROSCOPY  POLARIZING MICROSCOPY  PHASE CONTRAST MICROSCOPY  INTERFERENCE MICROSCOPY  DIFFERENTIAL INTERFERENCE CONTRAST MICROSCOPY  REFERENCE
  • 3. Introduction  The word microscope is derived from two Greek words ‘mikro’ meaning ‘small’ and ‘scopien’ meaning ‘to view’.  Thus, it is an instrument which enables us to view small objects by magnifying it and making it possible to be seen by the viewer.  The science of investing small objects using such an instrument is called Microscopy
  • 4. History of microscope 1590 – Hans and Zachcharias Janssen of Holland claimed to have invented microscope 1609 – Galileo Galileli developed a compound microscope with convex, concave lens 1572-1633 – compound microscope with two convex lens, invented in Rome by Carnelius Drebbel 1625 – Giovanni Faber coined the term microscope
  • 5. History of microscope 1674 – Anton van Leeuwenhoek made and used a simple microscope to view biological specimens.
  • 6. Types of microscopes Basically two types of microscope : 1. Simple Microscope : A simple microscope consists of a single lens or a magnifying glass. 2. Compound microscope : A compound microscope consists of two or more lenses. Compound microscope can be further divided according to different microscopic methods used .
  • 7. Types of microscopes Simple microscope Compound microscope
  • 8. Microscopic Methods A. Light Microscopy 1. Brightfield (light) microscopy 2. Darkfield microscopy 3. Phase-contrast microscopy 4. Interference microscopy 5. Differential interference contrast microscopy 6. Fluorescent microscopy 7. Polarizing microscope B. Electron Microscopy 1. Transmission electron microscopy 2. Scanning electron microscopy 3. Scanning transmission electron microscopy 4. Atomic force microscopy C. Scanning Probe Microscopes
  • 10. LIGHT  Visible light is that portion of electromagnetic spectrum that can be detected by human eyes, having wavelength ranging from approx 400 nm to 800nm  Light travels in straight lines. Light travels at different speeds in air and in glass. Its path can be deflected or reflected by means of mirrors or right angle prisms.
  • 11. LIGHT RETARDATION AND REFRACTION  If light enters sheet of glass at right angle, light is retarded in speed but direction is unchanged.  If light enters the glass at any other angle, a deviation of direction will occur in addition to retardation and this is called refraction.
  • 12. LIGHT  Light is slowed or retarded and “bent” or refracted when it passes through air and enters a convex lens, gets refracted when it leaves the convex lens and reenters air.
  • 13. LIGHT The curved lens will exhibit both retardation and refraction, the extent of which is governed by : a) Angle of incidence : angle at which light strikes the lens b) Refractive index c) Curvature of the lens Angle of refraction : the angle to which the rays are deviated within the glass or other transparent medium
  • 14. LIGHT  Refraction depends on the optical density of medium from which lens is made, which is indicated by refractive index (RI) RI = velocity of light in air/velocity in subatance  Refractive index is of great value in the computaion and design of lenses, microscope slides and coverslip and mounting media.  RI of air = 1.00, water = 1.30, glass = 1.50
  • 15. LIGHT  Total internal reflection : light passing from glass into air emerges parallel to the surface of lens if the angle of incidence is increased. If the angle is too great, (critical angle), the rays do not emerge but are totally internally reflected.
  • 16. LENS  LENS  Piece of glass or other transparent material, usually circular, having the two surfaces ground and polished in a specific form in order that rays of light passing through it shall either converge or diverge.  Two types of lens:  Positive lens  Negative lens
  • 17. LENS  Positive lens  Thicker at centre  Causes light rays to concentrate or converge to form a real image  Negative lens  Thinner at centre  Light passing will diverge or scatter and real image are not seen
  • 18. LENS Focus  When the lens concentrates the light rays to form a clear sharp image of an object, the object is said to be in focus.  The term ‘focus’ or ‘principal focus’ are used to indicate the position in which a lens will form a sharp, clear picture of a distant object.  Conjugate foci : in addition to principal focus, a lens also has conjugate foci; these are two points one on each side of the lens, in one of which a clear image will be formed on a screen of an object placed in the other.
  • 20. LENS Image formed 1. Real Image  Formed by Objective lens of microscope  Image is inverted, at greater magnification  Can be seen on a screen
  • 21. LENS 2. Virtual image  Image formed within principal focus on same side of object  Image appears the right way up and enlarged  Cannot be focused on screen  Formed by eyepiece of the microscope of real image projected from the objective
  • 22.
  • 23. Defects of Lens 1. Chromatic aberration  Colours of white light, each refracted to different degree  Shorter wavelength, greater degree of refraction  White light entering a lens, on emerging forms a different point of focus for each component colours, blue being focused at a point nearer the lens than red  Results in unsharp images with colored fringes
  • 24. Defects of Lens Correction : It is known as achromatism  Done by using two component lens  Positive lens is combined with a negative lens  construction of compound lens of different glass element a) Achromatic lens : will correct a thin positive lens for any two colour b) Apochromatic lens : fluorspar is incorporated, three colors can be brought to the one focal point and the amount of chromatic aberration visible in image is negligible.
  • 25. Defects of Lens 2. Spherical aberration  Due to entry of light rays into curved lens at its periphery  Refracted more that at a centre and thus not brought to a common focus  Blurred image is formed  Correction : same pattern used for chromatic aberration ie using a powerful positive lens and partially neutralizing its magnifying power with a negative lens made of glass having a greater relative aberration
  • 27. Eyepiece  Function - to magnify the image formed by the objective within the body tube, and present the eye with a virtual image.  Limits the field of view as seen by the eye  Usually 5x, 7x, 10x, 20x, 40x type magnification are used.  Can be used to correct the residual errors in objective lens.  Undercorrected : blue ray refracted to greater degree than red; blue fringe  Overcorrected : orange fringe seen at edge of field diaphragm
  • 28. Eyepiece Types of eyepiece 1. Positive eyepiece : Ramsden eyepiece 2. Negative eyepiece : Huygenian eyepiece
  • 29. Eyepiece Positive eyepiece :  With this, the focus is outside the eyepiece lens system  Field stop is outsidethe eyepiece, from which the virtual image is focused and magnified by entire eyepiece.  Ramsden eyepiece : lower lens has its plane side towards object. These are preferred for micrometer eyepiece as they impart less distortion to scales
  • 30. Eyepiece Negative eyepiece :  With this, the focus is within the eyepiece lens system  Lower or field lens collects the image that would have been formed by the objective and cones it down to a slightly smaller image at the level of the field stop within eyepiece; upper lens then produces an enlarged virtual image that is seen by eye.  Huygenian eyepiece : these are undercorrected and are best suited for use with achromatic objectives.
  • 31. Eyepiece  Other types :  Compensating eyepiece  Pointer eyepiece  Micrometer eyepiece  Double demonstration eyepiece  High focal point eyepiece
  • 32. Objective  These are screwed into lower end of body tube by means of standard thread, thus are interchangable.  Designated by their focal length, dependent on tube length  Consists of lenses and elements 5-15 in number, depending on ratio, type and quality
  • 33. Objective  The main task of objective is to collect maximum light possible from the object, unite it and form a high quality magnified image some distance above.  Every objective has a fixed working distance, focal length, magnification and numerical aperture (NA) .
  • 35. Objective  The working distance is the distance between an object in focus and the front of the lens system of the objective.  The focal length in the compound lens it is the distance between an object in focus and a point approximately halfway between the component lenses of the objective.  Total Magnification is product of magnification values of eyepiece and objective in a standard microscope.
  • 36. Objective Color Codes  Microscope manufacturers label their objectives with color codes to help in rapid identification of the objective. Table : Color codes used for objectives Magnification Color Code 4× Red 10× Yellow 40× Light Blue 100× White
  • 37. Objective Coverglass thickness  is important if high-power 'dry’ objectives are being used, when No. 1 coverglasses should be used, or an objective with a correction collar may be employed which allows a range of thickness or coverslip from 0.12 to 0.22 mm to be used (usually 0.17mm)  oil-immersion objectives do not have coverglass restrictions since they will have the same refractive index as the immersion oil.
  • 38. Objective Resolution  The ability of the lens to distinguish fine structural details in a specimen is known as the ‘resolving power’. It is the smallest distance between two dots or lines that can be seen as separate entities.  It depends on the wavelength of light (λ) and the Numerical Aperture of the lens.  It is calculated as: Resolution = 1.2 λ/2NA
  • 39. Objective Numerical Aperture  This ability is of an object to resolve detail is expressed in terms of numerical aperture(NA)  Numerical aperture depends primarily on the extreme range of the divergent rays that can be made to enter the lens (angular aperture) and secondarily on the refractive index of the medium between the object and the objective.  The relation between numerical aperture, angular aperture and refractive index is: NA = n× Sin u n=refractive index of medium between lens and object sin u = the sine half the angle of aperture
  • 40. Objective Effect of high NA  whilst a high numerical aperture increases the resolution of an objective, it has the following disadvantages: a) it reduces the depth of focus, i.e. the ability to focus on more than one layer of an object at the same time, and b) it reduces the flatness or the field, so that the edges are out of focus.
  • 41. Objective Types of Objectives  In most modern microscopes objectives are usually made up more than one lens.  This series of lenses is used to overcome certain limitations in the lenses.
  • 42. Types of Objective  Achromatic: Corrected for two colors red and blue. It is the most widely used for routine purposes.  Fluorite: Corrected for yellow green color. Green light is brought to a shorter focus and violet light to a longer focus.  Apochromat: All colors are brought to same focus. It is fully corrected for three colors. More highly corrected, often incorporating fluorite glass. These lenses are used especially for photomicrography and for screening cytological smears.  Plan-achromat: Although histological sections are flat the image produced by the microscope is not flat. It is saucer shaped; it is not possible to focus the whole of the field sharply at any one time. This aberration is corrected using flat-field objective, also called as plan-achromat lenses.
  • 43. Objective Types of Objectives Design and arrangement of lens in objective
  • 44. Body tube  Attached to limb, standard 160mm length  Nosepiece/carrier for objectives fitted at lower end, designated by number of objectives (2/3/4 based on magnification needed.  Three main forms : monocular, binocular and combined photo-binocular
  • 45. Body tube Binocular Microscope Binocular tubes have provision made for the adjustment of the interpupillary distance, enabling each observer to adjust for the individual facial proportion
  • 46. Adjustments a) Coarse adjustment knob  enables the stage and substage to be moved rapidly up and down b) Fine adjustment knob  enables the stage and substage to be moved slowly and accurately  Works by micrometer screws, levers and cams
  • 47. Object Stage A rigid platform above the condenser which supports the glass slide is object stage.
  • 48. Object Stage  It has an aperture in the center through which the light can pass to illuminate the specimen on the glass slide.  The stage holds the slide firmly and allows the slide movements with a mechanical vertical and horizontal adjustment screws.
  • 49. Object stage  The mechanical stage is graduated with Vernier scales and the x and y movements assist the operator to return to an exact desired location in the specimen.  Traveling range in most of the microscopes is 76 mm(X) 30 mm (Y).
  • 50. Illuminating apparatus Substage :  below the stage, attached to it and adjustable  consists of: 1. Condenser 2. Iris-diaphragm 3. Filter carrier 4. Mirror
  • 51. Condenser  Light from the lamp is directed into the sub stage condenser either directly or from a mirror or prism.  The main purpose of the condenser is to focus or concentrate the available light into the plane of the object
  • 52. Condensers  Condensers should have the same numerical aperture as objective.  The ideal condenser should form a perfect image of the light source.  Three types of condensers are used :  Abbe Condenser  Aplanatic Condensers  Achromatic Condensers
  • 53. Iris diaphragm  Also called aperture diaphragm  Used to control the cone of light entering the condenser  Intensity should always be reduced by using filters and not by closing the diaphragm  Adjustment of this iris diaphragm will alter the size and volume of the cone of light focused on the object.
  • 54. Iris diaphragm  If the diaphragm is closed too much, the image becomes too contrasty and refractile, whereas if the diaphragm is left wide open, the image will suffer from glare due to extraneous light interference.
  • 55. Iris diaphragm  In both cases the resolution of the image is poor.  The correct setting for the diaphragm is when the numerical aperture of the condenser is matched to the numerical aperture of the objective in use.
  • 56. Filter carrier  Usually a metal ring, pivoting on a screw to facilitate the easy removal of filters
  • 57. Mirror  Plano concave mirror, fitted about 4 inch below stage  Concave side have focus from object  Plane mirror must always be used with condenser  Built-in light source have mirrors fixed at the base.
  • 59. Magnification  Magnification of lens will depend on its conjugate foci, i.e. the distance from object to the lens and that from lens to image.  Magnification is the product of the magnification of the objectives and eyepieces and is dependent on following factors: 1. Focal length of objective 2. Distance between focal plane of objective and image it produces 3. Magnification of eyepiece Magnification =Tube length × Eyepiece magnification Focal length of the objective
  • 60. Illumination  Artificial illumination supplied by an electric filament lamp is most commonly employed.  Source of illumination should be: 1. Uniformly intense 2. Should completely flood the back lens of the condenser with light when the lamp iris diaphragm is open 3. Make the object appear as though it were self-luminous  In light microscope two different types of illuminations are used.  • Critical illumination  • Kohler illumination
  • 61. Setting up microscope Nelsonian method  Light source should be homogeneous and no lamp condenser  employed with bare light source  Light source should be focused on the object plane by racking the substage condenser up or down
  • 62. Setting up microscope Kohler illumination  Non homogeneous light source  Lamp condenser is essential to project an image of lamp filament onto the substage iris diaphragm  Lamp condensing lens functions as light source  Used with compound microscope
  • 63. Micrometry  The standard unit of measurement in microscopy is a micrometer(μm), which is 0.001mm  To measure microscopic objects an eyepiece micrometer scale is used in conjugation with stage micrometer. A. Eyepiece micrometer  Usually a disc on which arbitary scale is engraved  Placed inside Huygenuan eyepiece, resting on the field stop.  Gives sharp image of scale and have a greater eye clearance B. Stage micrometer  Consists of a 3 x 1 inch slide on which a millimeter scale is engraved in 1/10 and 1/100 graduations
  • 64. Cleaning and Maintainance A. Daily cleaning routine  Should be dusted daily and outer surface of lens of objective polished with lens tissue or cotton wool  Top lens of eyepiece polished to remove dust or fingerprints and microscope set up for correct illumination. If dust still present, eyepiece may need to be dismantled and both lenses cleared.  Substage condenser and mirror are cleaned in a similar manner  Removal of chemically active and sharp pieces of grits and foreign material if present
  • 65. Cleaning and Maintainance B. Weekly cleaning routine  Slides of adjustment, stage, substage wiped with cloth (in xylene damp)  Lens system checked  Chip blower can be used for cleaning eyepiece and objective
  • 66. Handling the Microscope  Carry it with 2 hands-one on the arm and the other under the base.  Use lens paper (ONLY) to remove any oil from the 100X lens.  Once oil has been added to the slide, do not move back to the 40X lens to focus: oil should never get on this lens. If this happens, it will be very difficult to get all of the oil off.  Turn the coarse adjustment knob so that the stage is far from the lens.  Place the microscope back into the correct spot in cabinet, with the arm toward us, making sure that the 10X low power lens is in place, pointing towards the stage-not the 100X oil immersion lens. The lens could hit against the stage and get scratched.
  • 68. Dark Field  Fine structures can often not be seen in front of a bright background as visibility is dependent on contrast between object and the background.
  • 69. Dark ground microscopy:  the oblique light is thrown upon the object which does not enter through the objective, they appear as self illuminous objects on dark background.  Only the reflected or scattered light forms the image of the object.
  • 70. Objectives and condensers:  Objectives must have a lower numerical aperture than the condenser  Low power- black paper/glass inserted into filter carrier.  central rays are cut off and peripheral rays from the condenser passes through the object but do not enter the objective; the only light entering the objective will be that scattered by the object
  • 71. Objectives and condensers:  High power-special condenser  Oil immersion must be used between the objective and object to ensure maximum reflected light from the object enters the objective  Fixed-focus condenser: commonly used- thin glass slides and coverslips( ideal no:1)
  • 72. Setting up the microscope:  Thin preparation- thin slide- coverslip  Adjust light direct/through the condenser  Place a drop of oil immersion on lower side of slide and also on top lens of the condenser  Move the rack up untill both surfaces meet without forming air bubbles  If correctly focused a small point of light will illuminate the object on a dark background(low power)  High power: place drop of oil on the coverslip and focused
  • 73. Advantages and disadvantages Advantages:  Finer structures can be seen clearly hence can be best used for spirochetes. Disadvantages:  Misleading impression of size  When stained , difficult to see  Need thinner sections without any refractory material like oil, water droplets, air bubbles etc..
  • 75. POLARIZING MICROSCOPY PRINCIPLE:  Light rays when passed through a crystal are retarded in speed. Being unevenly dense, the crystal will retard the rays to a different degree hence the rays will be refracted or bent to differing degrees.  This is known as DOUBLE REFRACTION OR BIREFRINGENCE  The direction of vibration of the emergent rays will be at right angles to each other.
  • 76. Principle:  A ray of light entering such a crystal will be converted into two rays which will emerge at two different points.  The emergent light rays will be polarized(one ray-on single direction, second ray- single direction and right angle to the first ray)
  • 77. ISOTROPIC: substances through which light can pass in any direction and at the same velocity , not able to produce polarized light. DICHROISM: A phenomenon given rise to by some substances and crystals which can produce plane polarized light by differential absorption. PLEOCHORIC FILMS: Dichroic crystals are suspended in thin plastic films and oriented in one direction .They can absorb all the colors equally.
  • 78. NICOL PRISM  It is composed of a crystal made of Icelandic spar slit in half and the halves cemented together with Canada balsam.  Light rays having passed through it would emerge vibrating in a single plane.  The single direction in which the light is vibrating when it emerges is known as the optical path of the prism.
  • 79. POLAROID DISCS  They are glass or celluloid covered discs with the ability to polarize light  Act as a single crystal of herpathite embedded in nitro cellulose and mounted between plastic sheets which is not only birefringent but has the ability to absorb the ordinary ray which would be refracted out of a Nicol prism  Only allows the extraordinary light to be transmitted.
  • 80. MAIN COMPONENTS OF THE MICROSCOPE The two polarizer's used are:  POLARIZER  ANALYSER
  • 82. POLARIZER  Placed beneath the sub stage condenser  Held in a rotatable graduated mount  Can be removed from the light path when not required
  • 83. ANALYSER  Placed between the objective and eyepiece  Is graduated-markings  Enhances the image
  • 84. POLARIZING MICROSCOPY  In a polarizing microscope, a polarizing filter is placed between light source and specimen.  The second polarizer called analyzer is placed above specimen between objective and eyepiece.
  • 85. POLARIZING MICROSCOPY  If the vibration directions of the object correspond to the vibration of the polarizer when the polarizer and analyzer are at right angles there is absence of light through eyepiece.
  • 86. Appearance of object depends on interference of the two rays recombined in the analyzer which depends on phase of difference between the two rays which in turn depends on the difference in the two refractive indices of the crystal and on its thickness If the vibration direction do not correspond then the rays of light transmitted by the object will be resolved in analyzer and object appears bright on a dark background.
  • 88. TYPES OF BIREFRINGENCE  INTRINSIC OR CRYSTALLINE  FORM  STRAIN  POSITIVE  NEGATIVE  QUARTZ AND COLLAGEN-POSITIVE BIREFRINGENCE  POLAROID- DISCS,CALCITE,URATES,CHROMOSOMES-NEGATIVE BIREFRINGENCE
  • 89. SIGN OF BIREFRINGENCE  The ray passing through a medium of high RI is called slow and if it passes through a medium of low RI it is called fast.  If the slow ray is parallel to the length of the crystal, or fiber birefringence is positive.  If the slow ray is perpendicular to the long axis of the structure, birefringence is negative.  Determined by the use of a compensator either above the specimen or below the polarizer at 45° to the direction of polarized light.
  • 90.  The compensator or specimen is rotated till the slow direction of the compensator is parallel to the long axis of the crystal or fiber.  The field is now red and if the crystal is blue the birefringence is positive  If the slow direction of compensator is parallel to the fast direction of the crystal, it appears yellow and has negative birefringence.
  • 91. APPLICATIONS It is used in the detection and observation of:  Artifacts like formalin pigment  Crystals of urate ,pyrophosphates etc  Lipids, myelin etc  Bone structure  Proteins like collagen,amyloid,keratin  Charcot-Leyden crystals, muscle striations etc.
  • 93. PHASE CONTRAST MICROSCOPY  It is a technique which enables us to see very transparent objects, which are almost invisible by ordinary transmitted light, in clear detail and in good contrast to their surroundings, and to see very small differences in thickness and density within the objects.  This is accomplished by converting these slight differences in refractive index and thickness into changes of amplitude.
  • 94. PRINCIPLE  A ray of light is made of waves travelling together in a straight line. When two such waves travel together,they are said to be in phase. Such a ray will appear bright to the observer  If one of the waves is held up or made to change the path, they will no longer travel together and are said to interfere with each other, differing in their intensity
  • 95.  A special condenser and objective control the illumination in a way that accentuates the differences in densities.  It causes light to travel different routes through the various parts of the cell  The result is an image with differing degrees of darkness and brightness collectively called contrast
  • 96. Interference CONSTRUCTIVE INTERFERENCE  Light rays are in phase  Amplitude or brightness is ‘doubled’ when recombined DESTRUCTIVE INTERFERENCE  Light rays are incoherent  ½λ out of phase  No light is seen  Maximum interference
  • 97.
  • 98. PARTS OF A PHASE CONTRAST MICROSCOPE ANNULUS:  Made of opaque glass  Has a hollow clear ring  Can be centered by means of centering screws PHAZE PLATE OR Z PLATE  Clear glass disc with a circular trough etched in it to half the depth of disc  The light passing through the trough has a phase difference of 1/4ƛ compared to the rest of the plate  Also contains a neutral density light absorbing material to reduce brightness of direct rays.
  • 99. PARTS OF A PHASE CONTRAST MICROSCOPE HIGH INTENSITY COMPOUND LAMP  Usually used with a mercury green filter AUXILLARY TELESCOPE  Used in place of an eyepiece for examining the back focal plane of the objective
  • 100. Image formation in phase contrast microscope
  • 101. WORKING OF THE MICROSCOPE  Annulus is placed in the condenser and the phase plate is placed in the objective  It allows only a small ring of light to pass into the microscope  The phase plate has a circle engraved on it which should match, with the ring of light coming in from the annulus through the condenser.
  • 102.  Some rays of light will pass through unaltered while some rays will be retarded or diffracted by approximately 1/4ƛ.  On passing through a phase plate the diffracted ray is retarded further by 1/4ƛ and will now interfere with the direct light ray.  The total retardation of diffracted rays is now 1/2ƛ and interfere will produce image contrast thus revealing even small details.
  • 103. APPLICATIONS  For examining unstained bacteria  For examining wet preparations of specimens  For examining faecal preparations for trophozoites or amoebae  In searching for trypanosomes in blood and other body fluids
  • 104.
  • 105. INTERFERENCE MICROSCOPY  generates mutually interfering beams which produce the contrast. It is this feature which enables very small phase changes to be seen and measured.  The two rays which eventually combine to produce image are formed by a plate of birefringent material placed immediately above the condenser.  These two rays having passed through the object plane are recombined by a similar plate of birefringent material below the front lens of the objective.
  • 106.  One ray passes through a point in the object and the other through an area adjacent to it.  Each point in the final image is a compound one made up of two mutually interfering rays.  A special Wollaston prism is added to the condenser to split the beam of light and also to recombine the two dissimilar beams.
  • 107. APPLICATIONS  To study individual parts of living cells with maximum resolution of detail  To estimate dry mass when it is applied as a highly accurate optical balance  To assess section thickness of specimen.
  • 108. DIFFERENTIAL INTERFERENCE CONTRAST MICROSCOPY  Designed by Nomarski hence also called as Nomarskis microscope.  Relies on the interference of a pair of wave fronts to generate contrast.
  • 109. It comprises of: -a polarizer -a condenser with a modified Wollaston prism -a beam splitting slide This slide consists of a modified Wollaston prism oriented at 45° to anattached analyzer,mounted in an adjustable carriage and accommodated in the analyzer slot between the objective and the eyepiece.
  • 110. Working of the microscope  Polarized light passes through the prism below the condenser  The prism below the condenser acts as a compensator  Every interference fringe of the upper prism is correlated with an interference fringe of the same order but opposite sign in this compensator
  • 111.  The two rays pass in turn through the condenser the object and the objective before passing through the second prism and analyzer.  The upper prism can be moved laterally enabling the rays to be displaced laterally or sheared before being recombined in the analyzer when they undergo interference.  This produces ‘interference contrast’ and together with rotation of the polarizers enhances the three-dimensional (3D) effect in the image.
  • 112.
  • 113. ADVANTAGES  Wide variety of interference colors can be used  Improved image contrast  No phase halo included  Lateral shearing of rays is reduced so that excellent three dimensional images can be produced.
  • 114. USES  As an infinitely variable phase contrast microscope, individual parts of living cells can be studied.  As a highly accurate optical balance, used for estimating dry mass down to 1x10 gm  Quantitative measurement of phase change or optical path difference  Studying live and unstained biological samples such as a smear from a tissue culture or individual water borne celled organism
  • 115.
  • 116.
  • 117. References  Textbook of oral pathology – Jaypee brothers, 1E; Anil Ghom, Shubhangi Mhaske  Histology A Text and Atlas - With Correlated Cell and Molecular Biology, 7E (2015) ; Wojciech Pawlina  Bancroft’s Theory and Practice of Histological Techniques ,7th edition  CFA Culling’s Histological techniques  Essentials of Microbiology; Surinder Kumar ,1st edition, 2016  MICROSCOPE Basics and Beyond, Revised edition 2003, Mortimer Abramowitz

Notas do Editor

  1. The object AB to be magnified is placed just outside the principal focus of the objective so that its real image is formed on the other side of objective. The image formed is real, inverted and magnified. The image due to the objective acts as the object for the eye piece. The position of the eyepiece is so adjusted that the image lies within the focus of eyepiece Fe. Eyepiece acts as magnifying glass and to forms the final image is virtual, erect and magnified.
  2. Microscope manufacturers label their objectives with color codes to help in rapid identification of the magnification and any specialized immersion media requirements. This is very helpful when you have a nosepiece turret containing 5 or 6 objectives and you must quickly select a specific magnification. Some specialized objectives have an additional color code that indicates the type of immersion medium necessary to achieve the optimum numerical aperture.
  3. To check the setting for a particular specimen (where the coverslip thickness is unknown) first focus upon a high contrast area, then determine whether changing the collar setting increases or decreases the contrast.
  4. The main purpose of the condenser is to focus or concentrate the available light into the plane of the object i.e. the condenser collects the maximum possible light reflected by the mirror or the inbuilt light source and condenses or converges it to a very small area at the position of the specimen (Fig. 1.2).
  5. Rheinberg illumination, a form of optical staining, is a striking variation of low to medium power darkfield illumination using colored gelatin or glass filters to provide rich color to both the specimen and background.
  6. Rheinberg illumination, a form of optical staining, is a striking variation of low to medium power darkfield illumination using colored gelatin or glass filters to provide rich color to both the specimen and background.