Enlargements (part 1 of 2)
From: THE BARNET BOOK OF PHOTOGRAPHY
How to make Enlargements (part 1 of 2)
By John A. Hodges, 1898
Enlargements may be made by daylight, or by artificial light, and there are two methods of producing them, namely, by enlarging direct from the negative on to a sheet of bromide paper; or by first making a small transparency, and from that producing an enlarged negative upon a slow dry plate. The first is the method usually adopted by amateurs, probably because the necessary operations are fewer, and perhaps more simple. The second plan, however, possesses the advantage that the prints may be made by any process, be it carbon, platinum, or silver, and thus a great variety of effect obtained.
The first point however that the reader must decide is whether he will work by artificial light or by daylight. Each may be said to possess certain advantages, and with many the question resolves itself into one of personal convenience. Artificial light is, or should be, fairly constant in intensity, and if adopted there will probably be less waste of material through miscalculation of exposure. But if the source of light employed be other than a mixed jet, or the arc-light, if in fact it be of low intensity, negatives of a somewhat delicate type will be required in order to produce enlargements of the highest excellence. If the negatives are dense and strong, illuminants of low intensity, like oil or gas, do not possess sufficient penetration to duly register the denser portions of the negative, and the enlargements so made are apt to be deficient in half-tone, and hard.
With well-graded negatives of suitable quality, however, most excellent enlargements may be produced by artificial light. When artificial light is used work may be carried on at any time of day or night, in winter or summer. Those who adopt the daylight plan will, of course, be subjected to greater restrictions, at any rate, during the winter months, but amateurs who take a real interest in the work will do well to adopt the writer’s plan, and provide themselves with apparatus for each method of working.
ENLARGING BY DAYLIGHT.
There are two ways of enlarging by daylight. The first involves the exclusion of all actinic light from a room except that which passes through the negative. The alternative method of working is to employ an ordinary enlarging camera, such as are made by Middlemiss, or Lancaster. It is desirable, but not necessary, if the first plan be adopted, to secure the exclusive use of a room. One with a northerly aspect should be chosen, for if sunlight falls upon the window shadows will at some period of the day fall upon the negative, and produce unevenly lighted enlargements.
An upper room will be most suitable, and, if the light be a northern one, and there are no trees, or buildings to obstruct the view, a reflector may be dispensed with. If external objects intervene, however, one must be employed. It should be fixed outside the window-sill, at an angle of 45 degrees, and should be capable of adjustment. Let it be the full width of the, window and securely fixed for obvious reasons. A plate-glass mirror is effective, but expensive. A large drawing board painted dead white also answers well, but should not be left outside exposed to the weather.


In setting up an enlarging apparatus, whether it be for day or artificial light, it is absolutely essential to preserve the parallelism of its various parts, otherwise it will be impossible to produce sharp or evenly defined enlargements, and for this reason I have described somewhat fully the construction of a suitable easel. I may add that it will serve equally well for either daylight or artificial illumination, and I strongly advise the reader to construct, or have constructed, an easel on the lines I have laid down. With it either direct enlargements on paper can be produced, or plates may be used and enlarged negatives made. The easiest way of holding the paper during exposure is to procure two sheets of clear glass, patent plate is most suitable, sandwich the bromide paper between them, and secure with two strong bands of elastic. The complete apparatus in position for working is shown at Figure 3.


Before describing the actual process of making an enlargement it will be well to deal with the alternative method of working, namely, by artificial light, as the manipulations of the sensitive material used are the same in either case. Practically the most satisfactory way of working by the latter method is to use an enlarging lantern properly fitted with a condenser. The general principles of such an apparatus are identical with those which obtain in an ordinary optical lantern. Methods which dispense with the use of a condenser are more or less unsatisfactory, and should be avoided. In the space at the disposal of the writer it is not possible to give directions for the construction of an enlarging lantern, but those who may desire to make their own, will find full instructions and working drawings in “Practical Enlarging.”

The smaller and more intense the light, the nearer we approach to the ideal projection illuminant, and the better will be the definition of our enlargements. The arc-light most nearly fulfills the desired conditions, and if it be available it should certainly be employed. Next in point of utility comes the lime-light, preferably in the form of the mixed jet, and those who understand its manipulation are recommended to adopt it, but the majority of amateurs will probably find it more convenient to use either incandescent gaslight or an oil-lamp. Parallel wick-lamps should be avoided on account of the unequal illumination they produce, and if oil must be used a good circular wick burner will be found more suitable. Where house gas is available the incandescent gaslight is however much to be preferred. The light is perhaps not so powerful as that given by a really good parallel wick-lamp, but it is far more actinic and penetrating. The writer has used this light with great satisfaction, and therefore has no hesitation in recommending it. Some workers have been troubled by the appearance of an image of the mantle on the screen, but this can usually be got rid of by a suitable adjustment of the lenses and the light, and in any case by the interposition of a piece of ground glass between condenser and negative.