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Microscopy
Principles, working and application of Bright field
and Dark field microscope
Bright-field microscopy
 In Bright-field microscopy the Sample illumination is
transmitted (i.e., illuminated from below and observed from
above) white light and contrast in the sample is caused
by absorbance of some of the transmitted light in dense areas
of the sample.
 Bright-field microscopy typically has low contrast with most
biological samples as few absorb light to a great extent.
 Staining is often required to increase contrast, which prevents
use on live cells in many situations.
 Bright field illumination is useful for samples which have an
intrinsic colour, for example chloroplasts in plant cells.
 The light path consists of:
a transillumination light source,
commonly a halogen lamp in the
microscope stand;
a condenser lens which focuses light
from the light source onto the sample;
and
objective lens which collects light from
the sample and magnifies the image.
Oculars and/or a camera to view the
sample image
 Bright field microscopy may
use critical or Köhler illumination to
Dark Field Microscopy
 Dark field microscopy (dark ground microscopy) describes
microscopy methods, in both light and electron microscopy,
which exclude the unscattered beam from the image. As a
result, the field around the specimen (i.e., where there is no
specimen to scatter the beam) is generally dark.
 Light enters the microscope for illumination of
the sample.
 A specially sized disc, the patch stop (see
figure) blocks some light from the light source,
leaving an outer ring of illumination. A wide
phase annulus can also be reasonably
substituted at low magnification.
 The condenser lens focuses the light towards
the sample.
 The light enters the sample. Most is directly
transmitted, while some is scattered from the
sample.
 The scattered light enters the objective lens,
while the directly transmitted light simply
misses the lens and is not collected due to
a direct illumination block (see figure).
 Only the scattered light goes on to produce the
image, while the directly transmitted light is
omitted.
 Numerical Aperture
 Refractive Index
 Resolution
 Diffraction and interference effect
Phase contrast and Interference
Differential Interference Contrast
Microscope
Fluorescence Microscopy;
Immunofluorescence,
Confocal Microscopy,
Confocal Microscopy
 A confocal microscope creates sharp images of a
specimen that would otherwise appear blurred when
viewed with a conventional microscope.
 This is achieved by excluding most of the light from the
specimen that is not from the microscope’s focal plane.
 The image has less haze and better contrast than that
of a conventional microscope and represents a thin
cross-section of the specimen.
 Thus, apart from allowing better observation of fine
details it is possible to build three-dimensional (3D)
reconstructions of a volume of the specimen by
assembling a series of thin slices taken along the
vertical axis.
 Confocal microscopy was pioneered by Marvin Minsky in 1955
while he was a Junior Fellow at Harvard University.
 Minsky’s invention would perform a point-by-point image
construction by focusing a point of light sequentially across a
specimen and then collecting some of the returning rays.
 By illuminating a single point at a time Minsky avoided most of
the unwanted scattered light that obscures an image when the
entire specimen is illuminated at the same time.
 Additionally, the light returning from the specimen would pass
through a second pinhole aperture that would reject rays that
were not directly from the focal point.
 The remaining ‘‘desirable’’ light rays would then be collected by
a photomultiplier and the image gradually reconstructed using a
long-persistence screen.
 To build the image, Minsky scanned the specimen by moving the
stage rather than the light rays. This was to avoid the challenge
of trying to maintain sensitive alignment of moving optics.
 Using a 60 Hz solenoid to move the platform vertically and a
lower-frequency solenoid to move it horizontally, Minsky
managed to obtain a frame rate of approximately one image
every 10 sec.
MODERN CONFOCAL
MICROSCOPY
 Modern confocal microscopes have kept the key elements
of Minsky’s design: the pinhole apertures and point-by-
point illumination of the specimen.
 Advances in optics and electronics have been incorporated
into current designs and provide improvements in speed,
image quality, and storage of the generated images.
 The majority of confocal microscopes image either by
reflecting light off the specimen or by stimulating
fluorescence from dyes (fluorophores) applied to the
specimen.
 There are methods that involve transmission of light
through the specimen, but these are much less common
 If light is incident on a molecule, it may absorb the light
and then emit light of a different color, a process known as
fluorescence. At ordinary temperatures most molecules are
in their lowest energy state, the ground state.
 However, they may absorb a photon of light (for example,
blue light) that increases their energy causing an electron
to jump to a discrete singlet excited state.
 Typically, the molecule quickly (within 10-8 sec) dissipates
some of the absorbed energy through collisions with
surrounding molecules causing the electron to drop to a
lower energy level (the second black line).
 If the surrounding molecules are not able to accept the
larger energy difference needed to further lower the
molecule to its ground state, it may undergo spontaneous
emission, thereby losing the remaining energy, by emitting
light of a longer wavelength (for example, green light).
 Fluorescein is a common fluorophore that acts this way,
emitting green light when stimulated with blue excitation
light.
 The wavelengths of the excitation light and the color of the
emitted light are material dependent.
Specimen fixation, processing and staining in
Light Microscopy
ELECTRON MICROSCOPY
 Even the very best light microscopes have a resolution limit of
about 0.2 μm, which greatly compromises their usefulness for
detailed studies of many microorganisms.
 Viruses are too small to be seen with light microscopes.
Prokaryotes can be observed, but because they are usually
only 1 m to 2 m in diameter, just their general shape and
major morphological features are visible.
 The resolution of a light microscope increases with a
decrease in the wavelength of the light it uses for illumination.
 Electrons replace light as the illuminating beam. They can be
focused, much as light is in a light microscope, but their
wavelength is around 0.005 nm, approximately 100,000 times
shorter than that of visible light.
 Therefore, electron microscopes have a practical resolution
roughly 1,000 times better than the light microscope; with
many electron microscopes, points closer than 0.5 nm can be
distinguished, and the useful magnification is well over
100,000X
Transmission electron
microscope (TEM)
 A heated tungsten filament in the electron gun generates a
beam of electrons that is then focused on the specimen by
the condenser.
 Since electrons cannot pass through a glass lens, doughnut
shaped electromagnets called magnetic lenses are used to
focus the beam.
 The column containing the lenses and specimen must be
under high vacuum to obtain a clear image because electrons
are deflected by collisions with air molecules.
 The specimen scatters some electrons, but those that pass
through are used to form an enlarged image of the specimen
on a fluorescent screen.
 A denser region in the specimen scatters more electrons and
therefore appears darker in the image since fewer electrons
strike that area of the screen; these regions are said to be
“electron dense.” In contrast, electron-transparent regions are
brighter.
Which one is light
microscope?
 Bright field
 Dark field
 DIC
 Fluorescence
 Confocal
 EM
Sample Preparation for TEM
 Since electrons are deflected by air molecules and are
easily absorbed and scattered by solid matter, only
extremely thin slices (20 to 100 nm) of a microbial
specimen can be viewed in the average TEM. Such a
thin slice cannot be cut unless the specimen has
support of some kind; the necessary support is provided
by plastic.
 After fixation with chemicals like glutaraldehyde or
osmium tetroxide to stabilize cell structure, the
specimen is dehydrated with organic solvents (e.g.,
acetone or ethanol). Complete dehydration is essential
because most plastics used for embedding are not
water soluble.
 Next the specimen is soaked in unpolymerized, liquid
epoxy plastic until it is completely permeated, and then
the plastic is hardened to form a solid block.
 Thin sections are cut from this block with a glass or
diamond knife using a special instrument called an
ultramicrotome.
Staining
 The probability of electron scattering is determined by
the density (atomic number) of the specimen atoms.
 Biological molecules are composed primarily of atoms
with low atomic numbers (H, C, N, and O), and electron
scattering is fairly constant throughout the unstained
cell.
 Therefore specimens are prepared for observation by
soaking thin sections with solutions of heavy metal salts
like lead citrate and uranyl acetate.
 The lead and uranium ions bind to cell structures and
make them more electron opaque, thus increasing
contrast in the material.
 Heavy osmium atoms from the osmium tetroxide
fixative also “stain” cells and increase their contrast.
 The stained thin sections are then mounted on tiny
copper grids and viewed.
Shadowing
 Two other important techniques for preparing specimens are
negative staining and shadowing.
 In negative staining, the specimen is spread out in a thin film
with either phosphotungstic acid or uranyl acetate. Just as in
negative staining for light microscopy, heavy metals do not
penetrate the specimen but render the background dark,
whereas the specimen appears bright in photographs.
Negative staining is an excellent way to study the structure of
viruses, bacterial gas vacuoles, and other similar objects
(figure 2.17c).
 In shadowing, a specimen is coated with a thin film of
platinum or other heavy metal by evaporation at an angle of
about 45° from horizontal so that the metal strikes the
microorganism on only one side. In one commonly used
imaging method, the area coated with metal appears dark in
photographs, whereas the uncoated side and the shadow
region created by the object is light (figure 2.20). This
technique is particularly useful in studying virus
morphology, procaryotic flagella, and DNA.
Freeze-etching
 The TEM will also disclose the shape of organelles within
microorganisms if specimens are prepared by the freeze-
etching procedure.
 First, cells are rapidly frozen in liquid nitrogen and then
warmed to 100°C in a vacuum chamber. Next a knife that has
been precooled with liquid nitrogen (196°C) fractures the
frozen cells, which are very brittle and break along lines of
greatest weakness, usually down the middle of internal
membranes (figure 2.21).
 The specimen is left in the high vacuum for a minute or
more so that some of the ice can sublimate away and
uncover more structural detail. Finally, the exposed surfaces
are shadowed and coated with layers of platinum and carbon
to form a replica of the surface. After the specimen has been
removed chemically, this replica is studied in the TEM and
provides a detailed, three-dimensional view of intracellular
structure (figure 2.22).
 An advantage of freeze-etching is that it minimizes the
danger of artifacts because the cells are frozen quickly rather
than being subjected to chemical fixation, dehydration, and
plastic embedding.
The Scanning Electron
Microscope
 The scanning electron microscope (SEM) works in a
different manner. It produces an image from
electrons released from atoms on an object’s surface.
 Specimen preparation for SEM is relatively easy, and in
some cases air -dried material can be examined
directly.
 Most often, however, microorganisms must first be
fixed, dehydrated, and dried to preserve surface
structure and prevent collapse of the cells when are
exposed to the SEM’s high vacuum.
 Before viewing, dried samples are mounted and coated
with a thin layer of metal to prevent the buildup of an
electrical charge on the surface and to give a better
image.
 To create an image, the SEM scans a
narrow, tapered electron beam back and
forth over the specimen (figure 2.23).
 When the beam strikes a particular area,
surface atoms discharge a tiny shower of
electrons called secondary electrons, and
these are trapped by a special detector.
 Secondary electrons entering the detector
strike a scintillator causing it to emit light
flashes that a photomultiplier converts to
an electrical current and amplifies.
 The signal is sent to a cathode-ray tube
and produces an image like a television
picture, which can be viewed or
photographed.
 The number of secondary electrons
reaching the detector depends on the
nature of the specimen’s surface.
 When the electron beam strikes a raised
area, a large number of secondary
electrons enter the detector; in contrast,
fewer electrons escape a depression in the
surface and reach the detector.
 Thus raised areas appear lighter on the
screen and depressions are darker.
 A realistic three-dimensional image of the
microorganism’s surface results (figure
2.24). The actual in situ location of
microorganisms in ecological niches
such as the human skin and the lining of
the gut also can be examined.
Unit – 2 Microscopy
Unit – 2 Microscopy
Unit – 2 Microscopy

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Unit – 2 Microscopy

  • 1. Microscopy Principles, working and application of Bright field and Dark field microscope
  • 2. Bright-field microscopy  In Bright-field microscopy the Sample illumination is transmitted (i.e., illuminated from below and observed from above) white light and contrast in the sample is caused by absorbance of some of the transmitted light in dense areas of the sample.  Bright-field microscopy typically has low contrast with most biological samples as few absorb light to a great extent.  Staining is often required to increase contrast, which prevents use on live cells in many situations.  Bright field illumination is useful for samples which have an intrinsic colour, for example chloroplasts in plant cells.
  • 3.
  • 4.  The light path consists of: a transillumination light source, commonly a halogen lamp in the microscope stand; a condenser lens which focuses light from the light source onto the sample; and objective lens which collects light from the sample and magnifies the image. Oculars and/or a camera to view the sample image  Bright field microscopy may use critical or Köhler illumination to
  • 5. Dark Field Microscopy  Dark field microscopy (dark ground microscopy) describes microscopy methods, in both light and electron microscopy, which exclude the unscattered beam from the image. As a result, the field around the specimen (i.e., where there is no specimen to scatter the beam) is generally dark.
  • 6.
  • 7.  Light enters the microscope for illumination of the sample.  A specially sized disc, the patch stop (see figure) blocks some light from the light source, leaving an outer ring of illumination. A wide phase annulus can also be reasonably substituted at low magnification.  The condenser lens focuses the light towards the sample.  The light enters the sample. Most is directly transmitted, while some is scattered from the sample.  The scattered light enters the objective lens, while the directly transmitted light simply misses the lens and is not collected due to a direct illumination block (see figure).  Only the scattered light goes on to produce the image, while the directly transmitted light is omitted.
  • 8.
  • 9.  Numerical Aperture  Refractive Index  Resolution  Diffraction and interference effect
  • 10. Phase contrast and Interference Differential Interference Contrast Microscope
  • 12.
  • 13.
  • 14.
  • 15. Confocal Microscopy  A confocal microscope creates sharp images of a specimen that would otherwise appear blurred when viewed with a conventional microscope.  This is achieved by excluding most of the light from the specimen that is not from the microscope’s focal plane.  The image has less haze and better contrast than that of a conventional microscope and represents a thin cross-section of the specimen.  Thus, apart from allowing better observation of fine details it is possible to build three-dimensional (3D) reconstructions of a volume of the specimen by assembling a series of thin slices taken along the vertical axis.
  • 16.  Confocal microscopy was pioneered by Marvin Minsky in 1955 while he was a Junior Fellow at Harvard University.  Minsky’s invention would perform a point-by-point image construction by focusing a point of light sequentially across a specimen and then collecting some of the returning rays.  By illuminating a single point at a time Minsky avoided most of the unwanted scattered light that obscures an image when the entire specimen is illuminated at the same time.  Additionally, the light returning from the specimen would pass through a second pinhole aperture that would reject rays that were not directly from the focal point.  The remaining ‘‘desirable’’ light rays would then be collected by a photomultiplier and the image gradually reconstructed using a long-persistence screen.  To build the image, Minsky scanned the specimen by moving the stage rather than the light rays. This was to avoid the challenge of trying to maintain sensitive alignment of moving optics.  Using a 60 Hz solenoid to move the platform vertically and a lower-frequency solenoid to move it horizontally, Minsky managed to obtain a frame rate of approximately one image every 10 sec.
  • 17. MODERN CONFOCAL MICROSCOPY  Modern confocal microscopes have kept the key elements of Minsky’s design: the pinhole apertures and point-by- point illumination of the specimen.  Advances in optics and electronics have been incorporated into current designs and provide improvements in speed, image quality, and storage of the generated images.  The majority of confocal microscopes image either by reflecting light off the specimen or by stimulating fluorescence from dyes (fluorophores) applied to the specimen.  There are methods that involve transmission of light through the specimen, but these are much less common
  • 18.  If light is incident on a molecule, it may absorb the light and then emit light of a different color, a process known as fluorescence. At ordinary temperatures most molecules are in their lowest energy state, the ground state.  However, they may absorb a photon of light (for example, blue light) that increases their energy causing an electron to jump to a discrete singlet excited state.  Typically, the molecule quickly (within 10-8 sec) dissipates some of the absorbed energy through collisions with surrounding molecules causing the electron to drop to a lower energy level (the second black line).  If the surrounding molecules are not able to accept the larger energy difference needed to further lower the molecule to its ground state, it may undergo spontaneous emission, thereby losing the remaining energy, by emitting light of a longer wavelength (for example, green light).  Fluorescein is a common fluorophore that acts this way, emitting green light when stimulated with blue excitation light.  The wavelengths of the excitation light and the color of the emitted light are material dependent.
  • 19.
  • 20.
  • 21.
  • 22. Specimen fixation, processing and staining in Light Microscopy
  • 23. ELECTRON MICROSCOPY  Even the very best light microscopes have a resolution limit of about 0.2 μm, which greatly compromises their usefulness for detailed studies of many microorganisms.  Viruses are too small to be seen with light microscopes. Prokaryotes can be observed, but because they are usually only 1 m to 2 m in diameter, just their general shape and major morphological features are visible.  The resolution of a light microscope increases with a decrease in the wavelength of the light it uses for illumination.  Electrons replace light as the illuminating beam. They can be focused, much as light is in a light microscope, but their wavelength is around 0.005 nm, approximately 100,000 times shorter than that of visible light.  Therefore, electron microscopes have a practical resolution roughly 1,000 times better than the light microscope; with many electron microscopes, points closer than 0.5 nm can be distinguished, and the useful magnification is well over 100,000X
  • 24.
  • 25. Transmission electron microscope (TEM)  A heated tungsten filament in the electron gun generates a beam of electrons that is then focused on the specimen by the condenser.  Since electrons cannot pass through a glass lens, doughnut shaped electromagnets called magnetic lenses are used to focus the beam.  The column containing the lenses and specimen must be under high vacuum to obtain a clear image because electrons are deflected by collisions with air molecules.  The specimen scatters some electrons, but those that pass through are used to form an enlarged image of the specimen on a fluorescent screen.  A denser region in the specimen scatters more electrons and therefore appears darker in the image since fewer electrons strike that area of the screen; these regions are said to be “electron dense.” In contrast, electron-transparent regions are brighter.
  • 26. Which one is light microscope?  Bright field  Dark field  DIC  Fluorescence  Confocal  EM
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  • 29. Sample Preparation for TEM  Since electrons are deflected by air molecules and are easily absorbed and scattered by solid matter, only extremely thin slices (20 to 100 nm) of a microbial specimen can be viewed in the average TEM. Such a thin slice cannot be cut unless the specimen has support of some kind; the necessary support is provided by plastic.  After fixation with chemicals like glutaraldehyde or osmium tetroxide to stabilize cell structure, the specimen is dehydrated with organic solvents (e.g., acetone or ethanol). Complete dehydration is essential because most plastics used for embedding are not water soluble.  Next the specimen is soaked in unpolymerized, liquid epoxy plastic until it is completely permeated, and then the plastic is hardened to form a solid block.  Thin sections are cut from this block with a glass or diamond knife using a special instrument called an ultramicrotome.
  • 30. Staining  The probability of electron scattering is determined by the density (atomic number) of the specimen atoms.  Biological molecules are composed primarily of atoms with low atomic numbers (H, C, N, and O), and electron scattering is fairly constant throughout the unstained cell.  Therefore specimens are prepared for observation by soaking thin sections with solutions of heavy metal salts like lead citrate and uranyl acetate.  The lead and uranium ions bind to cell structures and make them more electron opaque, thus increasing contrast in the material.  Heavy osmium atoms from the osmium tetroxide fixative also “stain” cells and increase their contrast.  The stained thin sections are then mounted on tiny copper grids and viewed.
  • 31. Shadowing  Two other important techniques for preparing specimens are negative staining and shadowing.  In negative staining, the specimen is spread out in a thin film with either phosphotungstic acid or uranyl acetate. Just as in negative staining for light microscopy, heavy metals do not penetrate the specimen but render the background dark, whereas the specimen appears bright in photographs. Negative staining is an excellent way to study the structure of viruses, bacterial gas vacuoles, and other similar objects (figure 2.17c).  In shadowing, a specimen is coated with a thin film of platinum or other heavy metal by evaporation at an angle of about 45° from horizontal so that the metal strikes the microorganism on only one side. In one commonly used imaging method, the area coated with metal appears dark in photographs, whereas the uncoated side and the shadow region created by the object is light (figure 2.20). This technique is particularly useful in studying virus morphology, procaryotic flagella, and DNA.
  • 32. Freeze-etching  The TEM will also disclose the shape of organelles within microorganisms if specimens are prepared by the freeze- etching procedure.  First, cells are rapidly frozen in liquid nitrogen and then warmed to 100°C in a vacuum chamber. Next a knife that has been precooled with liquid nitrogen (196°C) fractures the frozen cells, which are very brittle and break along lines of greatest weakness, usually down the middle of internal membranes (figure 2.21).  The specimen is left in the high vacuum for a minute or more so that some of the ice can sublimate away and uncover more structural detail. Finally, the exposed surfaces are shadowed and coated with layers of platinum and carbon to form a replica of the surface. After the specimen has been removed chemically, this replica is studied in the TEM and provides a detailed, three-dimensional view of intracellular structure (figure 2.22).  An advantage of freeze-etching is that it minimizes the danger of artifacts because the cells are frozen quickly rather than being subjected to chemical fixation, dehydration, and plastic embedding.
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  • 37. The Scanning Electron Microscope  The scanning electron microscope (SEM) works in a different manner. It produces an image from electrons released from atoms on an object’s surface.  Specimen preparation for SEM is relatively easy, and in some cases air -dried material can be examined directly.  Most often, however, microorganisms must first be fixed, dehydrated, and dried to preserve surface structure and prevent collapse of the cells when are exposed to the SEM’s high vacuum.  Before viewing, dried samples are mounted and coated with a thin layer of metal to prevent the buildup of an electrical charge on the surface and to give a better image.
  • 38.  To create an image, the SEM scans a narrow, tapered electron beam back and forth over the specimen (figure 2.23).  When the beam strikes a particular area, surface atoms discharge a tiny shower of electrons called secondary electrons, and these are trapped by a special detector.  Secondary electrons entering the detector strike a scintillator causing it to emit light flashes that a photomultiplier converts to an electrical current and amplifies.  The signal is sent to a cathode-ray tube and produces an image like a television picture, which can be viewed or photographed.
  • 39.  The number of secondary electrons reaching the detector depends on the nature of the specimen’s surface.  When the electron beam strikes a raised area, a large number of secondary electrons enter the detector; in contrast, fewer electrons escape a depression in the surface and reach the detector.  Thus raised areas appear lighter on the screen and depressions are darker.  A realistic three-dimensional image of the microorganism’s surface results (figure 2.24). The actual in situ location of microorganisms in ecological niches such as the human skin and the lining of the gut also can be examined.