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Microscopy
Dr. Heena Dave; Ph.D.
M.Sc. Course, Semester I
Nirma Institute of Sciences
Email: daveheena@gmail.com
“Microscope is an instrument for viewing
objects that are too small to be seen easily
by the naked eye”
Microscopy : Principle
Basic Principles: What do
Microscopes do?
Microscopes are an important
tool of biologists,
and are used to study cells,
tissues, and
microorganisms
Timeline
▪ Circa 1000AD – The first vision aid was invented called a reading stone ; made up of glass
sphere that magnified when laid on top of reading materials (inventor unknown)
▪ 1021 – Ibn al-Haytham (Alhazen) (965 -c.1039): describes the properties of magnifying glass in
his Book of Optics.
▪ Circa 1284 - Italian, Salvino D'Armate : credited with inventing the first wearable eye glasses.
▪ 1590 – Dutch lens grinders Hans and Zacharias Janssen make the first microscope by placing
two lenses in a tube. Janssens observed that viewed objects in front of the tube appeared
greatly enlarged, creating both the forerunner of the compound microscope and the telescope.
▪ 1619 – Cornelius Drebbel (1572-1633): presents a compound microscope made of two convex
lenses.
▪ 1625 – Giovanni Faber (1574-1629): coins the word microscope.
▪ 1665 – English physicist, Robert Hooke looked at a sliver of cork through a microscope lens and
noticed some "pores" or "cells" in it.
Timeline
▪ 1674 – Anton van Leeuwenhoek built a simple microscope with only one lens to examine blood,
yeast, insects and many other tiny objects. Leeuwenhoek was the first person to describe
bacteria, and he invented new methods for grinding and polishing microscope lenses that allowed
for curvatures providing magnifications of up to 270 diameters, the best available lenses at that
time.
▪1678 – Cherubin d’Orleans: develops a binocular microscope out of two monocular
systems.
▪1690 – Christiaan Huygens (1629-1695): formulates the wave theory of light and
constructs oculars made of two lenses and a diaphragm.
▪1700 – John Marshall (1633-1725): Develops a microscope base with an
illumination system.
▪1712 – Christian Gottlieb Hertel: uses mirrors for illumination and constructs a
micrometer eyepiece using horse hair for a grid
▪1744 – John Cuff (1708-1772): used a condenser lens to increase light intensity
• 1755 – Georg Adams (1704-1773): constructed microscopes with a revolving nose piece to
change objectives.
• 18th century – Several technical innovations make microscopes better & easier to handle,
which leads to microscopy becoming more and more popular among scientists. An important
discovery is that lenses combining two types of glass could reduce the chromatic effect,
with its disturbing halos resulting from differences in refraction of light.
• 1830 – Joseph Jackson Lister reduces the problem with spherical aberration by showing that
several weak lenses used together at certain distances gave good magnification without
blurring the image
• 1834 – William Henry Fox Talbot (1800-1877): develops polarization microscopy and makes
photomicrographs
• 1847 – Giovanni Battsta Amici (1786-1873): first person to use immersion objectives.
• 1863 – Henry Clifton Sorby: development of a metallurgical microscope to observe
meteorites
Timeline
Timeline
• 1872 – Ernst Abbe, then research director of the Zeiss Optical Works, wrote a mathematical
formula called the "Abbe Sine Condition". His formula provided calculations that allowed
for the maximum resolution in microscopes possible.
• 1878 – Ernst Abbe formulates a mathematical theory correlating resolution to the
wavelength of light. Abbes formula makes calculations of maximum resolution in
microscopes possible.
• Abbe’s Law
“minimum resolving distance (d) is related to the wavelength of light (lambda) divided by the
Numeric Aperture, which is proportional to the angle of the light cone (theta) formed by a
point on the object, to the objective”.
• 1903 – Richard Zsigmondy develops the ultra-microscope and is able to study objects below
the wavelength of light.
• 1931 – Ernst Ruska co-invented the electron microscope; won the Nobel Prize in Physics
in 1986. An electron microscope depends on electrons rather than light to view an object,
electrons are speeded up in a vacuum until their wavelength is extremely short, only one
hundred-thousandth that of white light. Electron microscopes make it possible to view
objects as small as the diameter of an atom.
Timeline
• 1932 – Frits Zernike invents the phase-contrast microscope that allows the study of colorless
and transparent biological materials.
• 1938 – Ernst Ruska develops the electron microscope. The ability to use electrons in
microscopy greatly improves the resolution and greatly expands the borders of exploration.
• 1955 – George Nomarski (1919-1997): develops differential interference contrast microscopy.
• 1981 – Gerd Binnig and Heinrich Rohrer invent the scanning tunnelling microscope that
gives three-dimensional images of objects down to the atomic level.
• In the 20th new developments and improvements have rendered the 19th century useless.
– The new microscopes are not only able to use light as a way of reflecting the image of the sample, but
they are more versatile and capable of using electrons of high resolution power to examine a sample
and reproduce its image.
– The versatility of the microscopes allows one to observe a sample in a 3-dimensional fashion
rather than on a flat pain like the conventional microscopes.
– Also, the magnification power of these new microscopes is incredible; it can easily reach the 200,000x,
or 10,000 times more than the earliest microscopes.
http://www.youtube.com/watch?v=zD2u74VOK3A
Principles of Microscopy
r =  /2NA
As the wave length () r Resolution
As the NA r Resolution
Magnification : Objects are made to appear larger than they are;
Magnification that does not reveal further detail
Resolution: The ability to see close together objects as distinct;
The ability to distinguish two close points as separate entities.
The minimum resolvable distance(r) is determined by the Numerical aperture (NA) and
the wavelength of the light ().
Microscope Resolution
• ability of a lens to separate or distinguish small objects that are close
together
• wavelength of light used is major factor in resolution
shorter wavelength  greater resolution
NUMERICAL APERTURE (NA)
What does NA mean?
Lens opening
OR
The value of the fraction of the light
wave front admitted by lens.
NA= n x sin 
n = the refractive index of the medium
between the object and the lens.
2  = the angle of cone of the light admitted
by the lens
NUMERICAL APERTURE (NA)
•NA= n x sin 
(sin  can not exceed 1)
NAmax = n, Refractive index of the immersion medium
NA of dry objective </= 1 (RI of air)
NA of oil lens </= 1.52 (RI of oil)
Thus the resolving power of the microscope depends on the NA and
quality of the objective and the refractive index of the mounting
medium.
Numerical Aperture is a mathematical calculation of the light-
gathering capabilities of a lens
Parts/Components of Microscope:
1. Eyepiece (ocular lens)
2. Body
3. Nose piece : Objective turret, revolver, or revolving nose piece (to
hold multiple objective lenses)
4. Objective lenses
5. Focus knobs (to move the stage)
1. Coarse adjustment
2. Fine adjustment
6. Mechnical Stage (to hold the specimen)
7. Light source (a light or a mirror)
8. Diaphragm
9. Substage condenser
10. Light intensity control
Parts/Components of Microscope
14
Light path of Microscope
Illumination systems
There are different condensers for each type of illumination:
1. Bright field 2. Dark field 3. Phase contrast
An essential factor in producing a good image with the light microscope is
obtaining adequate levels of light in the specimen, or object plane.
It is not only necessary to obtain bright light around the object, but for optimal
imaging, the light should be uniform across the field of view.
The best way to illuminate the specimen involves the use of yet another lens
system, known as a condenser.
CONDENSERS
Condenser top lens
• Numerical Aperture of the Condenser:
NA of condenser >/= NA of the objective
If NAcon< NAobj Resolution
• Iris diaphragm: Adjusts working aperture of the condenser
• The lens of a condenser is often marked with NA value.
LENSES: Characteristic
Curvature of field: For photomicroscopy camera demands
entirely focused field of view
– must use a plano lens, preferably a planapo.
Depth of field: The range of distances on which an objective can
focus reasonably well without any adjustment is called the depth
of field of that lens.
NA depth of field
Working distance: The distance between the lowest point of the
objective and the object in focus.
Magnification power Working distance
If the thickness of coverglass exceeds working distance, it is impossible to focus on the object.
LENSES: Characteristic
Lens magnification: Tube length/ Focal length
❑ Tube length = The distance from the rear focal plane of the objective to the
position of the primary image.
❑ Focal length = The distance from the surface of the lens to the point of
convergence of the rays.
Most modern microscopes: Tube length 160mm
Focal length of 10X: 16mm
Focal length of 40X: 4mm
Most achromatic oil immersion lenses’ focal length:1.8 to2mm
Do not interchange objectives between microscopes unless their tube length match
LENSES: Characteristic
Oil immersion lenses: NA= n sin 
NAmax = n
RI of air = 1
RI of crown glass = 1.51-1.56
RI of the immersion oil = 1.515-1.520 at 230 C
Objective Lenses
I. Achromatic
II. Apochromatic
III. Semiapochromatic/ fluorite
IV. Quartz lenses for ultraviolet microscopy
OBJECTIVE LENSES
1. Least expensive
2. Corrected for two colours:
Blue & Green
3. Green Filters: Helps filter out
violet light not corrected by
achromats
I. Achromatic
OBJECTIVE LENSES
1. Much more expensive
2. Greatly superior to achromats
3. Correct three or four
wavelengths
4. Usually have higher NA
II. Apochromatic
OBJECTIVE LENSES
Meniscus lens
1. Have optical corrections intermediate between
achromats and apochromates.
2. Quite good for fluorescence microscopy
III. Semiapochromatic/ fluorite
IV. Quartz lenses for ultraviolet microscopy
LENS MARKINGS
• Ph followed by a number: used for phase contrast and the phase annulus
number on the condenser that matches the phase ring in the lens.
Or 60:1
In millimeters
OR“0” OR “-”
Correction for color and
flatness
EYEPIECES (OCCULARS)
Components of
Eyepiece
Eye lens
Field stop
Field lens
Plano convex lens
Field diaphragm
Plano convex lens
Simplest Eyepiece
(Huygen lens)
Markings:
Magnifications: 8X, 10X, 12.5X
Avoid Empty magnification
C, K, or com: Compensative eyepieces
for flat field objectives.
Symbol of eye glasses:Designed for
glass wearers but any one can use.
Pl (Flat field), Field of view, infinity corrected
•working distance
— distance between the front surface of lens and surface of cover
glass or specimen
The properties of Microscope Objectives
Scanning Low Power High Power Oil
immersion
Magnification 4x 10x 40-45x 90-100x
Numerical Aperture 0.10 0.25 0.55-0.65 1.25-1.4
Approx Focal Length (f) 40mm 16mm 4mm 1.8-2.0mm
Working distance 17-20 mm 4-8 mm 0.5-0.7 mm 0.1 mm
Approx. resolving
power with light of
450nm (blue light)
2.3 m 0.9 m 0.35 m 0.18 m
Microscopic Techniques
Optical Microscopy (Light Microscopy)
Electron Microscopy
Transmission Electron Microscopy
Scanning Electron Microscopy
Scanning Probe Microscopy
The Optical / Light Microscope
• An optical instrument containing one or more lenses that produce an enlarged image
of an object placed in the focal plane of the lens
• With optical microscopy, the light microscope is used to study the microstructure;
optical and illumination systems are its basic elements.
Resolution limit: submicron particles approaches the wavelength of visible
light (400 to 700nm)
1. Transmission: beam of light passes through the sample; e.g. Polarizing or petrographic
microscope; Samples are usually fine powder or thin slices (transparent)
2. Reflection: beam of light reflected off the sample surface; e.g. Metallurgical or reflected
light microscope; Surface of materials, especially opaque ones
• For materials that are opaque to visible light (all metals and many ceramics and polymers),
only the surface is subject to observation, and the light microscope must be used in a reflecting
mode.
• Contrasts in the image produced result from differences in reflectivity of the various regions of the
microstructure.
• Investigations of this type are often termed metallographic, since metals were first examined
using this technique.
The Optical / Light Microscope
▪ Simple Microscopes : There are two basic configurations of the
conventional optical microscope: the simple (single lens); microscopes
consisted of a small, single converging lens mounted on a brass plate,
with a screw mechanism to hold the sample or specimen to be
examined.
▪ Compound microscopes (many lenses) : image formed by action of
2 lenses; multiple lenses to collect light from the sample and then a
separate set of lenses to focus the light into the eye or camera
▪ bright-field microscope
▪ dark-field microscope
▪ phase-contrast microscope
▪ fluorescence microscopes
SIMPLE & COMPOUND MICROSCOPES
Compond Microscope
LensI
LensII
Simple/Dissecting Microscope
Lens
The Bright-Field Microscope
produces a dark image against a brighter background; The name "brightfield" is
derived from the fact that the specimen is dark and contrasted by the surrounding
bright viewing field
• has several objective lenses
– parfocal microscopes remain in focus when objectives are changed
• total magnification
– product of the magnifications of the ocular lens and the objective lens
Algae under the microscope with
visible cells using bright field
illumination.
Different stains and staining techniques are used
depending upon the type of specimen and cell
structure being examined.
For example :
• Fuchsin is used to stain smooth muscle cells
• Methylene blue is used to stain cell nuclei
• Gram stain is used on bacteria and gives rise to the
name gram-negative or gram-positive bacteria
based on the reaction of the bacteria to the stain.
Limitations of bright-field microscopy
• Unstained objects such as cells present a unique
problem for the light microscopist because their
images generate very little contrast and are
essentially invisible in ordinary bright-field microscopy
The Dark-Field Microscope
• produces a bright image of the object against a dark
background
• used to observe living, unstained preparations
• very sensitive because images based on small amounts of
diffracted light from minute phase objects are seen clearly
against a black or very dark background.
• commonly used for minute light-diffracting specimens
such as diatoms, bacteria and bacterial flagella, isolated
organelles and polymers such as cilia, flagella, microtubules,
and actin filaments, & silver grains and gold particles in
histochemically labelled cells and tissues.
.
where image formation is based solely on diffracted wave components
OR
in which the nondiffracted rays are removed altogether so that the image is composed
solely of diffracted wave components
The Phase-Contrast Microscope
• enhances the contrast between
intracellular structures having slight
differences in refractive index
• produces high-contrast images of
transparent specimens such as
cells and micro-organisms, tissue
slices, lithographic patterns, and
particles such as organelles.
• Living cells in tissue culture can
also be examined directly, without
fixation and staining
This microscopy which transforms differences in the relative phase of object
waves to amplitude differences in the image
The Fluorescence Microscope
• exposes specimen to ultraviolet,
violet, or blue light
• fluorescence microscopy allows
visualization of specific
molecules that fluoresce in the
presence of excitatory light.
• shows a bright image of the
object resulting from the
fluorescent light emitted by the
specimen
The Fluorescence Microscope
• specimens usually stained with fluorochromes
– Examples of these are DAPI and the Hoechst dyes used to directly label nuclear
DNA or rhodamine-labeled phalloidin used to indirectly label cytoplasmic actin
filaments.
– The amount, intracellular location, and movement of macromolecules, small
metabolites, and ions can be studied using this technique
• Alternatively, fluorochrome-labeled antibodies can be used to label fixed,
permeabilized cells in a method known as immunoflorescence microscopy
– These techniques are commonly used to visualize the distribution of certain proteins
in a cell or to make visible specific organelles, filaments, and biochemically distinct
membrane regions.
• A variety of new tagging methods is also employed, including inserting short DNA
sequences of known epitopes into the coding sequences of proteins (epitope tagging),
constructing protein chimeras with green or red fluorescent proteins (GFP, RFP),
20X 20X 20X
20X 20X 20X
40X 40X 40X
Normal Mammary G;and - 3Mo Sac
Negative
Nuclear
Cytoplasmic Background/
Nonspecific
Negative
Nuclear
Cytoplasmic Nuclear
20X 20X
20X 20X 20X
Negative
Colocalization
CK14+CK18
Both
CK14/CK18
Normal Mammary Gland - 3Mo Sac CK 18 CK 14
Classification of Cytokeratins
20X
Electron microscopy
• The upper limit to the magnification possible with an optical microscope
is approximately 2000 times.
• Consequently, some structural elements are too fine or small to permit
observation using optical microscopy. Under such circumstances the
electron microscope, which is capable of much higher magnifications,
may be employed
– Scanning electron microscopy (SEM),
– Transmission electron microscopy, (TEM),
– Scanning transmission electron microscopy (STEM),
– Focus ion beam microscopy (FIB)
Electron Microscopy
• beams of electrons are
used to produce images
• wavelength of electron beam
is much shorter than light,
resulting in much higher
resolution
Electron Microscopy
An image of the structure under investigation is formed using beams of
electrons instead of light radiation.
According to quantum mechanics, a high-velocity electron will become wave-
like, having a wavelength that is inversely proportional to its velocity. When
accelerated across large voltages, electrons can be made to have
wavelengths on the order of 0.003 nm (3 pm).
High magnifications and resolving powers of these microscopes are
consequences of the short wavelengths of electron beams. The electron
beam is focused and the image formed with magnetic lenses; otherwise the
geometry of the microscope components is essentially the same as with
optical systems.
Both transmission and reflection beam modes of operation are possible
for electron microscopes.
Transmission Electron Microscopy
The image seen with a transmission electron microscope (TEM) is formed by
an electron beam that passes through the specimen.
Details of internal microstructural features are accessible to observation;
contrasts in the image are produced by differences in beam scattering or
diffraction produced between various elements of the microstructure or defect.
Since solid materials are highly absorptive to electron beams, a specimen to
be examined must be prepared in the form of a very thin foil; this ensures
transmission through the specimen of an appreciable fraction of the incident
beam.
The transmitted beam is projected onto a fluorescent screen or a photographic film
so that the image may be viewed. Magnifications approaching 1,000,000× are
possible with transmission electron microscopy, which is frequently utilized in the
study of dislocations.
44
• electrons scatter when they
pass through thin sections
of a specimen
• transmitted electrons (those
that do not scatter) are used
to produce image
• denser regions in specimen,
scatter more electrons and
appear darker
Scanning Electron Microscopy
A more recent and extremely useful investigative tool is the scanning
electron microscope (SEM).
The surface of a specimen to be examined is scanned with an electron beam,
and the reflected (or back-scattered) beam of electrons is collected, then
displayed at the same scanning rate on a cathode ray tube (similar to a CRT
television screen).
The image on the screen, which may be photographed, represents the
surface features of the specimen. The surface may or may not be polished
and etched, but it must be electrically conductive; a very thin metallic surface
coating must be applied to nonconductive materials.
Magnifications ranging from 10 to in excess of 50,000 times are possible, as
are also very great depths of field.
Accessory equipment permits qualitative and semiquantitative analysis of the
elemental composition of very localized surface areas.
Scanning Electron Microscope
• uses electrons reflected
from the surface of a
specimen to create image
• produces a 3-dimensional
image of specimen’s
surface features
47
Newer Techniques in Microscopy
• confocal microscopy and
scanning probe microscopy
• have extremely high
resolution
• can be used to observe
individual atoms
Confocal Microscopy
• confocal scanning laser microscope
• laser beam used to illuminate spots on specimen
• computer compiles images created from each point to generate a 3-
dimensional image
Scanning Probe Microscopy
• scanning tunneling microscope
– steady current (tunneling current) maintained between microscope probe and
specimen
– up and down movement of probe as it maintains current is detected and used to
create image of surface of specimen
• atomic force microscope
– sharp probe moves over surface of specimen at constant distance
– up and down movement of probe as it maintains constant distance is detected and
used to create image
• Examination on the nanometer scale is possible inasmuch as magnifications as high as
109× are possible; much better resolutions are attainable than with other microscopic
techniques.
Size ranges for several structural features
found in materials
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01-CellBio-Microscopy-HVD.pdf

  • 1. Microscopy Dr. Heena Dave; Ph.D. M.Sc. Course, Semester I Nirma Institute of Sciences Email: daveheena@gmail.com “Microscope is an instrument for viewing objects that are too small to be seen easily by the naked eye”
  • 2. Microscopy : Principle Basic Principles: What do Microscopes do? Microscopes are an important tool of biologists, and are used to study cells, tissues, and microorganisms
  • 3. Timeline ▪ Circa 1000AD – The first vision aid was invented called a reading stone ; made up of glass sphere that magnified when laid on top of reading materials (inventor unknown) ▪ 1021 – Ibn al-Haytham (Alhazen) (965 -c.1039): describes the properties of magnifying glass in his Book of Optics. ▪ Circa 1284 - Italian, Salvino D'Armate : credited with inventing the first wearable eye glasses. ▪ 1590 – Dutch lens grinders Hans and Zacharias Janssen make the first microscope by placing two lenses in a tube. Janssens observed that viewed objects in front of the tube appeared greatly enlarged, creating both the forerunner of the compound microscope and the telescope. ▪ 1619 – Cornelius Drebbel (1572-1633): presents a compound microscope made of two convex lenses. ▪ 1625 – Giovanni Faber (1574-1629): coins the word microscope. ▪ 1665 – English physicist, Robert Hooke looked at a sliver of cork through a microscope lens and noticed some "pores" or "cells" in it.
  • 4. Timeline ▪ 1674 – Anton van Leeuwenhoek built a simple microscope with only one lens to examine blood, yeast, insects and many other tiny objects. Leeuwenhoek was the first person to describe bacteria, and he invented new methods for grinding and polishing microscope lenses that allowed for curvatures providing magnifications of up to 270 diameters, the best available lenses at that time. ▪1678 – Cherubin d’Orleans: develops a binocular microscope out of two monocular systems. ▪1690 – Christiaan Huygens (1629-1695): formulates the wave theory of light and constructs oculars made of two lenses and a diaphragm. ▪1700 – John Marshall (1633-1725): Develops a microscope base with an illumination system. ▪1712 – Christian Gottlieb Hertel: uses mirrors for illumination and constructs a micrometer eyepiece using horse hair for a grid ▪1744 – John Cuff (1708-1772): used a condenser lens to increase light intensity
  • 5. • 1755 – Georg Adams (1704-1773): constructed microscopes with a revolving nose piece to change objectives. • 18th century – Several technical innovations make microscopes better & easier to handle, which leads to microscopy becoming more and more popular among scientists. An important discovery is that lenses combining two types of glass could reduce the chromatic effect, with its disturbing halos resulting from differences in refraction of light. • 1830 – Joseph Jackson Lister reduces the problem with spherical aberration by showing that several weak lenses used together at certain distances gave good magnification without blurring the image • 1834 – William Henry Fox Talbot (1800-1877): develops polarization microscopy and makes photomicrographs • 1847 – Giovanni Battsta Amici (1786-1873): first person to use immersion objectives. • 1863 – Henry Clifton Sorby: development of a metallurgical microscope to observe meteorites Timeline
  • 6. Timeline • 1872 – Ernst Abbe, then research director of the Zeiss Optical Works, wrote a mathematical formula called the "Abbe Sine Condition". His formula provided calculations that allowed for the maximum resolution in microscopes possible. • 1878 – Ernst Abbe formulates a mathematical theory correlating resolution to the wavelength of light. Abbes formula makes calculations of maximum resolution in microscopes possible. • Abbe’s Law “minimum resolving distance (d) is related to the wavelength of light (lambda) divided by the Numeric Aperture, which is proportional to the angle of the light cone (theta) formed by a point on the object, to the objective”. • 1903 – Richard Zsigmondy develops the ultra-microscope and is able to study objects below the wavelength of light. • 1931 – Ernst Ruska co-invented the electron microscope; won the Nobel Prize in Physics in 1986. An electron microscope depends on electrons rather than light to view an object, electrons are speeded up in a vacuum until their wavelength is extremely short, only one hundred-thousandth that of white light. Electron microscopes make it possible to view objects as small as the diameter of an atom.
  • 7. Timeline • 1932 – Frits Zernike invents the phase-contrast microscope that allows the study of colorless and transparent biological materials. • 1938 – Ernst Ruska develops the electron microscope. The ability to use electrons in microscopy greatly improves the resolution and greatly expands the borders of exploration. • 1955 – George Nomarski (1919-1997): develops differential interference contrast microscopy. • 1981 – Gerd Binnig and Heinrich Rohrer invent the scanning tunnelling microscope that gives three-dimensional images of objects down to the atomic level. • In the 20th new developments and improvements have rendered the 19th century useless. – The new microscopes are not only able to use light as a way of reflecting the image of the sample, but they are more versatile and capable of using electrons of high resolution power to examine a sample and reproduce its image. – The versatility of the microscopes allows one to observe a sample in a 3-dimensional fashion rather than on a flat pain like the conventional microscopes. – Also, the magnification power of these new microscopes is incredible; it can easily reach the 200,000x, or 10,000 times more than the earliest microscopes. http://www.youtube.com/watch?v=zD2u74VOK3A
  • 8. Principles of Microscopy r =  /2NA As the wave length () r Resolution As the NA r Resolution Magnification : Objects are made to appear larger than they are; Magnification that does not reveal further detail Resolution: The ability to see close together objects as distinct; The ability to distinguish two close points as separate entities. The minimum resolvable distance(r) is determined by the Numerical aperture (NA) and the wavelength of the light ().
  • 9. Microscope Resolution • ability of a lens to separate or distinguish small objects that are close together • wavelength of light used is major factor in resolution shorter wavelength  greater resolution
  • 10. NUMERICAL APERTURE (NA) What does NA mean? Lens opening OR The value of the fraction of the light wave front admitted by lens. NA= n x sin  n = the refractive index of the medium between the object and the lens. 2  = the angle of cone of the light admitted by the lens
  • 11. NUMERICAL APERTURE (NA) •NA= n x sin  (sin  can not exceed 1) NAmax = n, Refractive index of the immersion medium NA of dry objective </= 1 (RI of air) NA of oil lens </= 1.52 (RI of oil) Thus the resolving power of the microscope depends on the NA and quality of the objective and the refractive index of the mounting medium. Numerical Aperture is a mathematical calculation of the light- gathering capabilities of a lens
  • 13. 1. Eyepiece (ocular lens) 2. Body 3. Nose piece : Objective turret, revolver, or revolving nose piece (to hold multiple objective lenses) 4. Objective lenses 5. Focus knobs (to move the stage) 1. Coarse adjustment 2. Fine adjustment 6. Mechnical Stage (to hold the specimen) 7. Light source (a light or a mirror) 8. Diaphragm 9. Substage condenser 10. Light intensity control Parts/Components of Microscope
  • 14. 14 Light path of Microscope
  • 15. Illumination systems There are different condensers for each type of illumination: 1. Bright field 2. Dark field 3. Phase contrast An essential factor in producing a good image with the light microscope is obtaining adequate levels of light in the specimen, or object plane. It is not only necessary to obtain bright light around the object, but for optimal imaging, the light should be uniform across the field of view. The best way to illuminate the specimen involves the use of yet another lens system, known as a condenser.
  • 16. CONDENSERS Condenser top lens • Numerical Aperture of the Condenser: NA of condenser >/= NA of the objective If NAcon< NAobj Resolution • Iris diaphragm: Adjusts working aperture of the condenser • The lens of a condenser is often marked with NA value.
  • 17. LENSES: Characteristic Curvature of field: For photomicroscopy camera demands entirely focused field of view – must use a plano lens, preferably a planapo. Depth of field: The range of distances on which an objective can focus reasonably well without any adjustment is called the depth of field of that lens. NA depth of field Working distance: The distance between the lowest point of the objective and the object in focus. Magnification power Working distance If the thickness of coverglass exceeds working distance, it is impossible to focus on the object.
  • 18. LENSES: Characteristic Lens magnification: Tube length/ Focal length ❑ Tube length = The distance from the rear focal plane of the objective to the position of the primary image. ❑ Focal length = The distance from the surface of the lens to the point of convergence of the rays. Most modern microscopes: Tube length 160mm Focal length of 10X: 16mm Focal length of 40X: 4mm Most achromatic oil immersion lenses’ focal length:1.8 to2mm Do not interchange objectives between microscopes unless their tube length match
  • 19. LENSES: Characteristic Oil immersion lenses: NA= n sin  NAmax = n RI of air = 1 RI of crown glass = 1.51-1.56 RI of the immersion oil = 1.515-1.520 at 230 C
  • 20. Objective Lenses I. Achromatic II. Apochromatic III. Semiapochromatic/ fluorite IV. Quartz lenses for ultraviolet microscopy
  • 21. OBJECTIVE LENSES 1. Least expensive 2. Corrected for two colours: Blue & Green 3. Green Filters: Helps filter out violet light not corrected by achromats I. Achromatic
  • 22. OBJECTIVE LENSES 1. Much more expensive 2. Greatly superior to achromats 3. Correct three or four wavelengths 4. Usually have higher NA II. Apochromatic
  • 23. OBJECTIVE LENSES Meniscus lens 1. Have optical corrections intermediate between achromats and apochromates. 2. Quite good for fluorescence microscopy III. Semiapochromatic/ fluorite IV. Quartz lenses for ultraviolet microscopy
  • 24. LENS MARKINGS • Ph followed by a number: used for phase contrast and the phase annulus number on the condenser that matches the phase ring in the lens. Or 60:1 In millimeters OR“0” OR “-” Correction for color and flatness
  • 25. EYEPIECES (OCCULARS) Components of Eyepiece Eye lens Field stop Field lens Plano convex lens Field diaphragm Plano convex lens Simplest Eyepiece (Huygen lens) Markings: Magnifications: 8X, 10X, 12.5X Avoid Empty magnification C, K, or com: Compensative eyepieces for flat field objectives. Symbol of eye glasses:Designed for glass wearers but any one can use. Pl (Flat field), Field of view, infinity corrected
  • 26. •working distance — distance between the front surface of lens and surface of cover glass or specimen The properties of Microscope Objectives Scanning Low Power High Power Oil immersion Magnification 4x 10x 40-45x 90-100x Numerical Aperture 0.10 0.25 0.55-0.65 1.25-1.4 Approx Focal Length (f) 40mm 16mm 4mm 1.8-2.0mm Working distance 17-20 mm 4-8 mm 0.5-0.7 mm 0.1 mm Approx. resolving power with light of 450nm (blue light) 2.3 m 0.9 m 0.35 m 0.18 m
  • 27. Microscopic Techniques Optical Microscopy (Light Microscopy) Electron Microscopy Transmission Electron Microscopy Scanning Electron Microscopy Scanning Probe Microscopy
  • 28. The Optical / Light Microscope • An optical instrument containing one or more lenses that produce an enlarged image of an object placed in the focal plane of the lens • With optical microscopy, the light microscope is used to study the microstructure; optical and illumination systems are its basic elements. Resolution limit: submicron particles approaches the wavelength of visible light (400 to 700nm) 1. Transmission: beam of light passes through the sample; e.g. Polarizing or petrographic microscope; Samples are usually fine powder or thin slices (transparent) 2. Reflection: beam of light reflected off the sample surface; e.g. Metallurgical or reflected light microscope; Surface of materials, especially opaque ones • For materials that are opaque to visible light (all metals and many ceramics and polymers), only the surface is subject to observation, and the light microscope must be used in a reflecting mode. • Contrasts in the image produced result from differences in reflectivity of the various regions of the microstructure. • Investigations of this type are often termed metallographic, since metals were first examined using this technique.
  • 29. The Optical / Light Microscope ▪ Simple Microscopes : There are two basic configurations of the conventional optical microscope: the simple (single lens); microscopes consisted of a small, single converging lens mounted on a brass plate, with a screw mechanism to hold the sample or specimen to be examined. ▪ Compound microscopes (many lenses) : image formed by action of 2 lenses; multiple lenses to collect light from the sample and then a separate set of lenses to focus the light into the eye or camera ▪ bright-field microscope ▪ dark-field microscope ▪ phase-contrast microscope ▪ fluorescence microscopes
  • 30. SIMPLE & COMPOUND MICROSCOPES Compond Microscope LensI LensII Simple/Dissecting Microscope Lens
  • 31. The Bright-Field Microscope produces a dark image against a brighter background; The name "brightfield" is derived from the fact that the specimen is dark and contrasted by the surrounding bright viewing field • has several objective lenses – parfocal microscopes remain in focus when objectives are changed • total magnification – product of the magnifications of the ocular lens and the objective lens Algae under the microscope with visible cells using bright field illumination. Different stains and staining techniques are used depending upon the type of specimen and cell structure being examined. For example : • Fuchsin is used to stain smooth muscle cells • Methylene blue is used to stain cell nuclei • Gram stain is used on bacteria and gives rise to the name gram-negative or gram-positive bacteria based on the reaction of the bacteria to the stain.
  • 32. Limitations of bright-field microscopy • Unstained objects such as cells present a unique problem for the light microscopist because their images generate very little contrast and are essentially invisible in ordinary bright-field microscopy
  • 33. The Dark-Field Microscope • produces a bright image of the object against a dark background • used to observe living, unstained preparations • very sensitive because images based on small amounts of diffracted light from minute phase objects are seen clearly against a black or very dark background. • commonly used for minute light-diffracting specimens such as diatoms, bacteria and bacterial flagella, isolated organelles and polymers such as cilia, flagella, microtubules, and actin filaments, & silver grains and gold particles in histochemically labelled cells and tissues. . where image formation is based solely on diffracted wave components OR in which the nondiffracted rays are removed altogether so that the image is composed solely of diffracted wave components
  • 34. The Phase-Contrast Microscope • enhances the contrast between intracellular structures having slight differences in refractive index • produces high-contrast images of transparent specimens such as cells and micro-organisms, tissue slices, lithographic patterns, and particles such as organelles. • Living cells in tissue culture can also be examined directly, without fixation and staining This microscopy which transforms differences in the relative phase of object waves to amplitude differences in the image
  • 35.
  • 36. The Fluorescence Microscope • exposes specimen to ultraviolet, violet, or blue light • fluorescence microscopy allows visualization of specific molecules that fluoresce in the presence of excitatory light. • shows a bright image of the object resulting from the fluorescent light emitted by the specimen
  • 37. The Fluorescence Microscope • specimens usually stained with fluorochromes – Examples of these are DAPI and the Hoechst dyes used to directly label nuclear DNA or rhodamine-labeled phalloidin used to indirectly label cytoplasmic actin filaments. – The amount, intracellular location, and movement of macromolecules, small metabolites, and ions can be studied using this technique • Alternatively, fluorochrome-labeled antibodies can be used to label fixed, permeabilized cells in a method known as immunoflorescence microscopy – These techniques are commonly used to visualize the distribution of certain proteins in a cell or to make visible specific organelles, filaments, and biochemically distinct membrane regions. • A variety of new tagging methods is also employed, including inserting short DNA sequences of known epitopes into the coding sequences of proteins (epitope tagging), constructing protein chimeras with green or red fluorescent proteins (GFP, RFP),
  • 38. 20X 20X 20X 20X 20X 20X 40X 40X 40X Normal Mammary G;and - 3Mo Sac Negative Nuclear Cytoplasmic Background/ Nonspecific Negative Nuclear Cytoplasmic Nuclear
  • 39. 20X 20X 20X 20X 20X Negative Colocalization CK14+CK18 Both CK14/CK18 Normal Mammary Gland - 3Mo Sac CK 18 CK 14 Classification of Cytokeratins 20X
  • 40. Electron microscopy • The upper limit to the magnification possible with an optical microscope is approximately 2000 times. • Consequently, some structural elements are too fine or small to permit observation using optical microscopy. Under such circumstances the electron microscope, which is capable of much higher magnifications, may be employed – Scanning electron microscopy (SEM), – Transmission electron microscopy, (TEM), – Scanning transmission electron microscopy (STEM), – Focus ion beam microscopy (FIB)
  • 41. Electron Microscopy • beams of electrons are used to produce images • wavelength of electron beam is much shorter than light, resulting in much higher resolution
  • 42. Electron Microscopy An image of the structure under investigation is formed using beams of electrons instead of light radiation. According to quantum mechanics, a high-velocity electron will become wave- like, having a wavelength that is inversely proportional to its velocity. When accelerated across large voltages, electrons can be made to have wavelengths on the order of 0.003 nm (3 pm). High magnifications and resolving powers of these microscopes are consequences of the short wavelengths of electron beams. The electron beam is focused and the image formed with magnetic lenses; otherwise the geometry of the microscope components is essentially the same as with optical systems. Both transmission and reflection beam modes of operation are possible for electron microscopes.
  • 43. Transmission Electron Microscopy The image seen with a transmission electron microscope (TEM) is formed by an electron beam that passes through the specimen. Details of internal microstructural features are accessible to observation; contrasts in the image are produced by differences in beam scattering or diffraction produced between various elements of the microstructure or defect. Since solid materials are highly absorptive to electron beams, a specimen to be examined must be prepared in the form of a very thin foil; this ensures transmission through the specimen of an appreciable fraction of the incident beam. The transmitted beam is projected onto a fluorescent screen or a photographic film so that the image may be viewed. Magnifications approaching 1,000,000× are possible with transmission electron microscopy, which is frequently utilized in the study of dislocations.
  • 44. 44 • electrons scatter when they pass through thin sections of a specimen • transmitted electrons (those that do not scatter) are used to produce image • denser regions in specimen, scatter more electrons and appear darker
  • 45. Scanning Electron Microscopy A more recent and extremely useful investigative tool is the scanning electron microscope (SEM). The surface of a specimen to be examined is scanned with an electron beam, and the reflected (or back-scattered) beam of electrons is collected, then displayed at the same scanning rate on a cathode ray tube (similar to a CRT television screen). The image on the screen, which may be photographed, represents the surface features of the specimen. The surface may or may not be polished and etched, but it must be electrically conductive; a very thin metallic surface coating must be applied to nonconductive materials. Magnifications ranging from 10 to in excess of 50,000 times are possible, as are also very great depths of field. Accessory equipment permits qualitative and semiquantitative analysis of the elemental composition of very localized surface areas.
  • 46. Scanning Electron Microscope • uses electrons reflected from the surface of a specimen to create image • produces a 3-dimensional image of specimen’s surface features
  • 47. 47 Newer Techniques in Microscopy • confocal microscopy and scanning probe microscopy • have extremely high resolution • can be used to observe individual atoms
  • 48. Confocal Microscopy • confocal scanning laser microscope • laser beam used to illuminate spots on specimen • computer compiles images created from each point to generate a 3- dimensional image
  • 49.
  • 50. Scanning Probe Microscopy • scanning tunneling microscope – steady current (tunneling current) maintained between microscope probe and specimen – up and down movement of probe as it maintains current is detected and used to create image of surface of specimen • atomic force microscope – sharp probe moves over surface of specimen at constant distance – up and down movement of probe as it maintains constant distance is detected and used to create image • Examination on the nanometer scale is possible inasmuch as magnifications as high as 109× are possible; much better resolutions are attainable than with other microscopic techniques.
  • 51. Size ranges for several structural features found in materials