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The Principles of Clinical Cytogenetics - Extra Materials - Springer

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84 Christopher McAleer<br />

measurements <strong>of</strong> their ability to gather highly diffracted light, thus a measure <strong>of</strong> a microscope’s<br />

resolving potential.<br />

How the condenser is used to illuminate the specimen will influence the number <strong>of</strong> light rays<br />

passing into an objective lens. A properly adjusted condenser will illuminate the small structures <strong>of</strong> a<br />

specimen from many different angles. This increases the likelihood <strong>of</strong> producing light rays with an<br />

angle <strong>of</strong> diffraction that will pass through the small opening <strong>of</strong> an objective and, thus, be present for<br />

viewing.<br />

Microscope condensers come in a variety <strong>of</strong> NAs, ranging from 1.4 to less than 1.0. Because the<br />

operating NA <strong>of</strong> an objective lens cannot be greater than that <strong>of</strong> the condenser, these components<br />

should have similar NA values.<br />

Condensers require correction for two basic groups <strong>of</strong> optical imperfections (aberrations) that are<br />

created as light passes through any lens. Monochromatic aberrations are those that can occur with<br />

any wavelength <strong>of</strong> light, whereas chromatic aberrations are problems unique to a specific range <strong>of</strong><br />

wavelengths. A microscope is equipped with one <strong>of</strong> three <strong>of</strong> condensers: abbe, aplanatic, or aplanatic/<br />

achromatic. <strong>The</strong>se differ in their ability to correct optical aberrations. Condensers are generally labeled<br />

with the type <strong>of</strong> optical correction they make and their NA.<br />

Abbe condensers are the most basic type <strong>of</strong> condenser and are not corrected for either type <strong>of</strong><br />

optical aberration. <strong>The</strong>y are not recommended for use in the cytogenetics laboratory.<br />

Aplanatic condensers are corrected solely for monochromatic aberrations and rely upon green<br />

light for the greatest degree <strong>of</strong> correction (2). <strong>The</strong> performance <strong>of</strong> aplanatic condensers is highest<br />

when a monochromatic green interference filter is used.<br />

Aplanatic/achromatic condensers are corrected for both types <strong>of</strong> optical aberration and do not<br />

require the use <strong>of</strong> green light for the correction (2).<br />

<strong>The</strong> aperture diaphragm <strong>of</strong> a condenser is adjusted to achieve a balance between the resolving<br />

power <strong>of</strong> the microscope and image contrast. When the aperture diaphragm is completely open, the<br />

small structures <strong>of</strong> a specimen are illuminated by light from the greatest number <strong>of</strong> angles and resolving<br />

capacity is at its highest. Unfortunately, the details <strong>of</strong> these structures are so well illuminated that<br />

they lose the “shadowing” or contrast variation that give such structures perspective.<br />

As the aperture diaphragm is closed, the structures <strong>of</strong> the specimen are illuminated from fewer<br />

angles, resulting in a loss <strong>of</strong> resolving power, but an improvement in the “shadowing” or contrast <strong>of</strong><br />

the image. Considering this, the aperture diaphragm should be set to produce a suitable balance<br />

between image contrast and resolution. Many microscope manufacturers recommend setting the condenser<br />

aperture between 66% and 75% open to achieve the best balance.<br />

Köhler Illumination<br />

Centering and focusing the condenser (Köhler illumination) are crucial for optimum image quality.<br />

<strong>The</strong> process begins by closing the field diaphragm so that light traveling through the condenser<br />

can be visually centered and focused. Once this is achieved, the field diaphragm is opened so that the<br />

light illuminates the specimen just beyond the field <strong>of</strong> view. Finally, the aperture diaphragm is adjusted<br />

to generate the desired image contrast.<br />

<strong>The</strong> Phase-Contrast Condenser<br />

Phase-contrast microscopes use a special condenser and objective lens to increase the contrast<br />

range <strong>of</strong> a specimen by darkening areas <strong>of</strong> greater density and lightening areas <strong>of</strong> lesser density.<br />

Phase contrast is <strong>of</strong>ten used for visualizing living or other unstained cells, but can be used successfully<br />

to increase the contrast range <strong>of</strong> G-banded specimens. A microscope equipped for phase contrast<br />

makes use <strong>of</strong> a special condenser and a phase objective lenses. Proper use <strong>of</strong> a phase-contrast<br />

microscope requires achievement <strong>of</strong> Köhler illumination, followed by an adjustment to align the<br />

phase components <strong>of</strong> the microscope. Of key importance is selection <strong>of</strong> a phase condenser setting<br />

that matches the “Ph” number <strong>of</strong> the phase objective.

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