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62 MODERN MAGIC LANTERNS.<br />

planted by the form shown in B, in which two lenses are<br />

employed, both with one convex and one plain surface, the<br />

convex sides facing one another, and almost in contact. This<br />

is an excellent form of condenser for all ordinary purposes,<br />

if well made, and is met with far more often than any other<br />

pattern. At c is another very good condenser known as<br />

Herschel's, which is also often fitted to lanterns, and answers<br />

in practice as well as B ; it is often made with the meniscus<br />

or concavo-convex lens a little smaller than the other, and the<br />

double convex lens has its inner curve flattened, in which form<br />

it is known as Gravett's. n is one of the forms suggested<br />

for a triple condenser, or one made of three lenses ; we lately<br />

saw a lantern fitted with a triple condenser with a very<br />

satisfactory result.<br />

It will be seen from Fig. 52 that the amount of light<br />

which falls upon a condenser, and which may be roughly<br />

considered as the<br />

amount available for<br />

illuminating the slide,<br />

depends upon the<br />

diameter of the condenser<br />

and the distance<br />

at which it must be<br />

from the lamp, for it<br />

is obvious that a condenser<br />

at A would receive<br />

more light than<br />

Fig. 52. one of the same size at<br />

DIAGRAM TO SHOW THAT THE NEARER THE<br />

CONDENSER IS TO THE SOURCE OF LIGHT,<br />

THE MORE LIGHT IT RECEIVES.<br />

B, since in the first case<br />

not only will the rays<br />

EE F F fall upon it which<br />

fell upon B, but it will embrace G G H H. Certain practical<br />

considerations, particularly the danger of having the thick<br />

glass of a lens too near the light and consequent heat,<br />

prevent the general use of condensers of such a size and<br />

focus as to make the angle at c more than about 70 degrees.<br />

For the usual photographic slide with a circular mask a<br />

condenser of 4 inches diameter will be found large enough,<br />

but if slides with very large masks with square corners are<br />

to be shown, such a size will not be found sufficient, and<br />

THE OPTICAL SYSTEM.<br />

a 41 inch will be wanted. In getting a condenser, two<br />

points should have attention : the glasses should be mounted<br />

quite loosely in their brass rings so as to rattle when shaken,<br />

if not, when expanded with the heat of the lamp they will<br />

most likely break, and the lenses<br />

63<br />

themselves should be as<br />

thin as possible at their edges. The slide should be as near<br />

to the condenser as the carrier will allow. For photographic<br />

enlarging, condensers will be required of a size dependent<br />

upon that of the negative from which the enlargement is to<br />

be made ; for good illumination its diameter should be at least<br />

an inch longer than the diagonal of the negative.<br />

The objective for projection purposes is, in the cheapest<br />

lanterns, what is called a piano-convex (A, Fig. 53), or a<br />

meniscus (B and c), but these are not at all to be desired,<br />

Fig. 53. LANTERN OBJ...CTIVES.<br />

especially in those of short focus ; foranything over 10 inches<br />

they are frequently very satisfactory. With the introduction<br />

of the rapid modern dry-plate in photography, however, the<br />

necessity for the very " quick " lenses for portraiture has<br />

largely disappeared, and portrait lenses as used by photographers<br />

answer all the requirements of the average lanternist<br />

admirably, and are frequently to be met with at a very low<br />

price. This lens, shown diagrammatically in Fig. 53, D, was<br />

the invention of Professor Petzval; and it or its modifications<br />

in the hands of Dallmeyer are excellent for projection. Several<br />

opticians now make special lantern lenses, based more or less<br />

upon this pattern, one or two of which we have used at one<br />

time or another with satisfaction. This type not only allows<br />

a large amount of light to pass, but it also possesses a very<br />

flat field, a quality the nature of which must be explained.

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