Physical Principles of Electron Microscopy: An Introduction to TEM ...
Physical Principles of Electron Microscopy: An Introduction to TEM ...
Physical Principles of Electron Microscopy: An Introduction to TEM ...
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120 Chapter 4<br />
At this stage it is convenient <strong>to</strong> cut a 3-mm-diameter disk out <strong>of</strong> the slice.<br />
For reasonably s<strong>of</strong>t metals (e.g., aluminum, copper), a mechanical punch<br />
may be used. For harder materials, an ultrasonic drill is necessary; it<br />
consists <strong>of</strong> a thin-walled tube (internal diameter = 3 mm) attached <strong>to</strong> a<br />
piezoelectric crystal that changes slightly in length when a voltage is applied<br />
between electrodes on its surfaces; see Fig. 4-20a. The tube is lowered on<strong>to</strong><br />
the slice, which has been bonded <strong>to</strong> a solid support using by heat-setting wax<br />
and its <strong>to</strong>p surface pre-coated with a silicon-carbide slurry (SiC powder<br />
mixed with water). Upon applying a high-frequency ac voltage, the tube<br />
oscillates vertically thousands <strong>of</strong> times per second, driving SiC particles<br />
against the sample and cutting an annular groove in the slice. When the slice<br />
has been cut through completely, the wax is melted and the 3-mm disk is<br />
retrieved with tweezers.<br />
The disk is then thinned further by polishing with abrasive paper (coated<br />
with diamond or silicon carbide particles) or by using a dimple grinder. In<br />
the latter case (Fig. 4-20b), a metal wheel rotates rapidly against the surface<br />
(covered with a SiC slurry or diamond paste) while the specimen disk is<br />
rotated slowly about a vertical axis. The result is a dimpled specimen whose<br />
thickness is 10 � 50 �m at the center but greater (100 � 400 �m) at the<br />
outside, which provides the mechanical strength needed for easy handling.<br />
In the case <strong>of</strong> biological tissue, a common procedure is <strong>to</strong> use an<br />
ultramicro<strong>to</strong>me <strong>to</strong> directly cut slices � 100 nm or more in thickness. The<br />
tissue block is lowered on<strong>to</strong> a glass or diamond knife that cleaves the<br />
material apart (Fig. 4-20c). The ultramicro<strong>to</strong>me can also be used <strong>to</strong> cut thin<br />
slices <strong>of</strong> the s<strong>of</strong>ter metals, such as aluminum.<br />
Some inorganic materials (e.g., graphite, mica) have a layered structure,<br />
with weak forces between sheets <strong>of</strong> a<strong>to</strong>ms, and are readily cleaved apart by<br />
inserting the tip <strong>of</strong> a knife blade. Repeated cleavage, achieved by attaching<br />
adhesive tape <strong>to</strong> each surface and pulling apart, can reduce the thickness <strong>to</strong><br />
below 1 �m. After dissolving the adhesive, thin flakes are mounted on 3-mm<br />
<strong>TEM</strong> grids. Other materials, such as silicon, can sometimes be persuaded <strong>to</strong><br />
cleave along a plane cut at a small angle relative <strong>to</strong> a natural<br />
(crystallographic) cleavage plane. If so, a second cleavage along a<br />
crystallographic plane results in a wedge <strong>of</strong> material whose thin end is<br />
transparent <strong>to</strong> electrons. Mechanical cleavage is also involved when a<br />
material is ground in<strong>to</strong> a fine powder, using a pestle and mortar, for example<br />
(Fig. 4-20d). The result is a fine powder, whose particles or flakes may be<br />
thin enough for electron transmission. They are dispersed on<strong>to</strong> a 3-mm <strong>TEM</strong><br />
grid covered with a thin carbon film (sometimes containing small holes so<br />
that some particles are supported only at their edges).