Common objects of the microscopeWood, J. G. (John George)
Science
Common objects of the microscope
Wood, J. G. (John George)
Microscopes; Microscopy
A remarkably pretty example of stomata and elongated cells is to be
obtained from the leaf of the common iris, and may be prepared for the
microscope by simply tearing off a strip of the epidermis from the
under side of the leaf, laying it on a slide, putting a little water on
it, and covering it with a piece of thin glass. (See Plate II. Fig. 2.)
There are a number of longitudinal bands running along the leaf where
these cells and stomata appear. The latter are not placed at regular
intervals, for it often happens that the whole field of the microscope
will be filled with cells without a single stoma, whilst elsewhere a
group of three or four may be seen clustered closely together.
Fig. 3 on the same Plate exhibits a specimen of the beautifully waved
cells, without mouths, which are found on the upper surface of the ivy
leaf. These are difficult to arrange from the fresh leaf, but are
easily shown by steeping the leaf in water for some time, and then
tearing away the cuticle. The same process may be adopted with many
leaves and cuticles, and in some cases the immersion must be continued
for many days, and the process of decomposition aided by a very little
nitric acid in the water, or by boiling.
On the same Plate are three examples of spiral and ringed vessels,
types of an endless variety of these beautiful and interesting
structures. Fig. 4 is a specimen of a spiral vessel taken from the
lily, and is a beautiful example of a double spire. The deposit which
forms this spiral is very strong, and it is to the vast number of
these vessels that the stalk owes its well-known elasticity. In many
cases the spiral vessels are sufficiently strong to be visible to the
naked eye, and to bear uncoiling. For example, if a leaf-stalk of
geranium be broken across, and the two fragments gently drawn asunder,
a great number of threads, drawn from the spiral vessels, will be seen
connecting the broken ends. In this case the delicate membranous walls
of the vessel are torn apart, and the stronger fibre which is coiled
spirally within it unrolls itself in proportion to the force employed.
In many cases these fibres are so strong that they will sustain the
weight of an inch or so of the stalk.
In Fig. 5 is seen a still more bold and complex form of this curious
structure; being a coil of five threads, laid closely against each
other, and forming, while remaining in their natural position, an
almost continuous tube. This specimen is taken from the root of the
water lily, and requires some little care to exhibit its structure
properly.
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