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88 MODERN MAGIC LANTERNS.<br />

appertaining to a lantern by some long Greek name, are often<br />

called Aphengescopes. It is a useful device occasionally for<br />

demonstration purposes, but owing to the very great loss<br />

of light, can only be employed with limelight or with the<br />

electric arc, and then is never very satisfactory. In Fig. 65<br />

the source of light is shown at B, and the condensers at<br />

c c, the object, which is placed at n, having its imago<br />

focussed upon the screen by means of the objective, E.<br />

There is no need to get a special lantern for the purpose,<br />

as a box is easily arranged to carry the objective at one end<br />

and to receive the nozzle of the lantern in the direction<br />

shown. Such a box should have its interior lined with black<br />

paper, or better, with black velvet. The back can be arranged<br />

to carry the objects it is desired to exhibit, access<br />

being obtained by the side A, which is closed with a curtain.<br />

When the Aphengescope is being used, and, indeed, in a<br />

large number of other cases, it will be found that, unless<br />

steps are taken to prevent it, harm will very frequently occur<br />

from delicate instruments or inflammable substances being<br />

exposed to the intense heat concentrated upon them by the<br />

condenser. To obviate this, what is known as an alum cell<br />

is employed. This is an arrangement similar to that shown<br />

in Fig. 61; in fact, the same cell can be employed for<br />

either purpose, as required. It is filled with a cold saturated<br />

solution of alum, which must have been carefully filtered so<br />

as to be quite free from dust or other floating particles. The<br />

solution will in course of time get fairly hot, but while allowing<br />

nearly all the light to pass, it will absorb the heat, which<br />

would otherwise be doing harm. In the absence of the alum<br />

solution, plain water can be employed. It is not quite so<br />

efficient, but is satisfactory enough for most purposes.<br />

Another arrangement of the lantern for demonstration<br />

purposes is that shown in Fig. 66, which shows the method<br />

of making vertical projections, as they are called. The<br />

beam of light from A, as it leaves the condenser, B, falls<br />

upon a mirror, F F, placed at an angle of 45 degrees<br />

with the horizontal, from which it is reflected vertically<br />

upwards. The table, n D, upon which the object to be<br />

projected is placed, is immediately over the mirror, while<br />

above it is placed the objective, E, bearing above it again a<br />

LANTERN EXPERIMENTS.<br />

reflector, G, which once more directs the beam in a horizontal<br />

direction to the screen. For most purposes such<br />

an arrangement can be fixed up at very little expense to<br />

answer all requirements except where great brilliancy and<br />

crispness of definition is desired. The bottom mirror can be<br />

a piece of the usual silvered plate glass, the top one is best<br />

of the thinnest silvered glass procurable, as if not, the<br />

Fig. 66.<br />

ARRANGEMENT OF LANTERN FOR VERTICAL PROTECTIONS.<br />

secondary reflection, that from the surface of the glass itself,<br />

may become troublesome. It will be seen that the two<br />

component lenses of the condenser have to be separated, one<br />

remaining in the usual position in front of the illuminant,<br />

and the other immediately beneath the table carrying the object<br />

to be projected. With this arrangement of the apparatus<br />

many experiments, such as those showing crystallisation,<br />

etc., can be performed. For this purpose a glass dish with<br />

an even flat bottom is required. This is placed upon the<br />

89

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