CHAPTER XXVI

MAP MAKING

=Technique of Negative Making.=—Stated in its simplest terms, the whole

problem of making a photographic map from the air consists in taking a

large number of slightly overlapping negatives, all from the same

altitude, with the plane flying uniformly level. When trimmed and

mounted in juxtaposition, or pasted together so as to overlap in their

common portions, the prints from these negatives constitute a complete

pictorial map. There is thus furnished by a few hours' labor topographic

information which would be the work of months to obtain by other means.

The making of map photographs involves all the special technique of

spotting, with much in addition. The pilot's task is not merely to go

over one object; he must navigate a narrow path, at a constant altitude,

on an even keel. If he is to make not merely a ribbon, but a map of

considerable width, he must take successive trips parallel to the first,

each displaced just far enough from the previous course to insure that

no portion is missed—a difficult task indeed.

It is the observer's duty to so time the intervals between exposures

that they overlap enough, but not so much as to be wasteful of plates or

film. He must also change magazines or films so quickly as to miss no

territory, or if some be missed, his is the task of directing the pilot

back to the point of the last exposure, where they begin a new series.

Level flying is entirely a pilot's problem. Its importance will be

realized when we consider the accompanying diagrams (Figs. 134 and 135),

where the effect on the resultant picture is shown of climbing, gliding,

or banking to either side. Prints from negatives distorted in this way

neither will be true representations of the territory photographed, nor

will they match when juxtaposed. In fact, they can be utilized only if

special rectifying apparatus is available for printing. Flying at a

constant altitude is similarly necessary if the prints are to be

utilized without enlargement or reduction in order to make them fit.

[Illustration:

FIG. 134.—Diagram showing effect of banking on aerial photograph.]

[Illustration:

FIG. 135.—Diagram showing effect of climbing and diving on aerial

photograph.]

Assuming a skilled pilot who will do his part, the next step is to

calculate the exposure intervals in order to insure an adequate overlap.

If a negative lens is installed which has been marked with a rectangle

the size of the camera field, the simplest method is to estimate the

proper instant for exposure by watching the progress of objects across

the lens face. This of course requires constant attention, and it is

easier to do this only occasionally, in order to determine the ground

speed in terms of camera fields traversed per minute. Thereafter

exposures are to be made by time, as determined by a watch or clock. Any

desired degree of overlap can be chosen, and either estimated, or more

or less accurately fixed by lines marked on the negative lens at a

shorter distance apart than the edges of the field. The most usual

overlap is 20 per cent., except for stereos, which call for 50 to 75 per

cent.

In the absence of a negative lens or some other sight to show the whole

camera field, it is necessary to resort to calculation from the speed

and altitude of the plane, the focus of the lens and the dimensions of

the plate. If _A_ is the altitude, _a_ the focal length of the lens, _d_

the diameter of the plate in the direction of travel (usually the short

length is chosen for economy of flights to cover a given width), _f_ the

fractional part by which one negative is desired to overlap the next,

and _V_ the ground speed of the plane, then we have, by simple

proportion, that the interval between exposures, _t_, must be—

_Ad_(1 - _f_)

_t_ = —————————————

_aV_

If _A_ = 2000 meters, _d_ = 18 centimeters, _f_ = ⅕, _a_ = 50

centimeters, and _V_ = 200 kilometers per hour, this relation gives—

2000 × .18 × .8 × 3600

_t_ = —————————————————————— = 10.3 seconds

.5 × 200,000

The principle of overlapping map exposures is shown in the accompanying

diagram (Fig. 129), together with data calculated as above for a 4 × 5

inch plate.

It is particularly to be noted that it is the _ground speed_ of the

plane that is used. This may be calculated by knowing the air speed and

the wind velocity and direction. Fig. 136 shows the method of doing this

graphically. First an arrow is drawn representing the direction it is

desired to fly. Next a second arrow is drawn of length to represent the

wind velocity. This must be inclined toward the first arrow in the

direction of the wind, and its head is to touch the head of the first

arrow. Then with the farther end of this second arrow as a center,

describe a circle of such a length as to represent the air speed of the

plane, in the same units as the wind velocity. Connect the point where

this circle cuts the arrow of flight direction to the center of the

circle by a straight line. This line constitutes the air speed arrow,

giving the direction it is necessary to fly, at the given air speed, to

make the course desired. The length of the flight direction arrow

between its head and its point of intersection with the air speed arrow

gives the ground speed.

[Illustration:

FIG. 136.—Diagram showing method of calculating ground speed from air

speed and wind velocity.]

When the wind is ahead or astern this calculation reduces to the simple

subtraction or addition of the wind velocity to the air speed of the

plane. Whenever possible, mapping should be done up and down the wind

(Fig. 137). If the plane is “crabbing,” the above calculations for

overlap are only valid if the camera can be turned normal to the

direction of travel over the ground. If the camera cannot be so turned

the corners of the successive pictures overlap instead of their sides,

with quite unsatisfactory results (Fig. 138).

Calculation of the distance apart of the parallel flights necessary to

make a map of any width is done by the use of a formula similar to the

longitudinal overlap formula above, distance figuring instead of time.

Using the same symbols, and denoting the distance by _D_, we have—

_Ad_(1 - _f_)

_D_ = —————————————

_a_

With the same figures as before, but substituting 24 centimeters for the

plate dimension, this relation gives—

2000 × .24 × .8

_D_ = ——————————————— = 768 meters

.5

[Illustration:

FIG. 137.—Overlaps made when flying with or against the wind.]

[Illustration:

FIG. 138.—Unsatisfactory overlaps made when plane is “crabbing.”]

It is of course largely a pilot's problem to steer the plane over

parallel courses at a given distance apart, although the observer,

noting conspicuous objects through a properly marked negative lens, may

direct the pilot by any of the means of communication already mentioned.

An alternative method of securing parallel strips, which is to be highly

recommended where enough photographically equipped airplanes are

available, is for several planes to fly side by side, maintaining their

proper separation (Fig. 139).

=Cameras and Auxiliaries for Map Making.=—Mapping can be done quite

satisfactorily by hand operated or semi-automatic cameras, provided the

observer has not too many other duties. On the other hand, the operation

of exposing at more or less definite intervals of time, irrespective of

the object immediately presented to the camera, is a largely mechanical

one. It naturally suggests the employment of an automatic mechanism,

whose speed of operation only is it necessary to watch.

If a non-automatic camera is used the timing of exposures may be done by

watching a negative lens, as described above, or by reference to a

clock, assuming that the ground speed is known through calculation. A

very practical advance over the ordinary use of a clock is to attach a

stop-watch to the shutter release, so that it is turned back to zero and

re-started at each exposure (Fig. 70). In passing, it may be noted that

if the stop-watch hand makes an electric contact which throws the

shutter release, then the device constitutes an attachment for turning

any semi-automatic camera into an automatic. The most suitable cameras

for mapping are unquestionably those of the entirely automatic type. The

use of such cameras always demands a knowledge of the ground speed. This

demand has led to many suggestions for _ground speed indicators_. The

common idea of these is to provide a moving part on the plane—either a

disc of large diameter, or a chain, or a revolving screw—whose speed may

be varied until any point upon it appears to keep in coincidence with a

point on the moving landscape below. The ground speed is then to be read

off a properly calibrated dial. Or, as a further step, the frequency of

the exposures may be directly controlled by the ground speed indicator

mechanism. The entire control of the camera would then consist merely in

occasional adjustment of the ground speed indicator.

[Illustration:

FIG. 139.—Planes starting out to make a map by flying in parallel.]

While entirely possible in theory, these devices are not easy to work

with in practice, because the plane is always subject to some pitching

and rolling, which make it difficult to hold any object constantly on

the moving point. This is especially true at high altitudes, where the

apparent motion of the earth is quite slow compared to the swervings of

the plane. This objection is in part removed if the ground speed

indicator is carried by a gyro stabilizer.

Ordinary mapping does not demand such exquisite rendering of detail as

does trench mapping. Nor is it necessary to fly in peace-time at such

high altitudes as in war. In consequence, mapping cameras are preferably

of the short focus, wide angle type, say, 25 centimeter focus for an 18

× 24 centimeter plate. Film is to be preferred over plates because of

the greater number of exposures it is possible to make on a flight. The

shutter of the mapping camera must be extremely uniform in its rate of

travel so that the elements of the map may match in tone (Fig. 140). A

mount which permits the camera to be turned normal to the direction of

flight, such as the British turret mount (Fig. 87), is particularly

desirable if flying across the wind is necessary, as will often be the

case in mapping strips between towns or between flying fields. Devices

to indicate compass direction and altitude are called for in new and

poorly mapped territory, and may be expected to receive intensive study

in the future. The question of their utility is, however, bound up with

the whole question of the sphere of aerial photographic mapping. Up to

the present this has been almost entirely a matter of filling in details

on maps obtained by the regular surveying methods, or of making

pictorial maps for aviators. To what extent primary mapping can be done

by the airplane is yet to be determined.

[Illustration:

FIG. 140.—A strip map, showing effect of uneven focal plane shutter

action.]

At this point mention must be made of special cameras for securing

extremely wide angle views, thereby minimizing the number of flights.

The _Bagley camera_, devised by Major Bagley of the U. S. Engineers, is

an example. It has three lenses, a middle one pointing directly

downward, and one to either side at an angle of 35 degrees. The pictures

obtained with the side cameras are of course greatly distorted, and must

be rectified in a special rectifying camera. The resultant definition is

not good, but as the maps are made on a much smaller scale than the

original pictures, this is not a serious objection. It is a matter for

the future to decide whether the additional labor on the ground

necessary for the rectifying process is to be more expensive than the

extra flights which must be made with the ordinary types of cameras

covering a smaller angle.

=Printing and Mounting Mosaics.=—With an ordinary set of overlapping

negatives the first step toward producing a map is to _scale_ the

negatives. For this purpose one should be selected which by comparison

with a map shows no distortion, and which is on the desired scale, or is

known to have been made at the average altitude of flight. A sketch map

of the territory should then be drawn, on this scale, based on available

maps. This sketch is preferably made on a large ground glass illuminated

from behind (Fig. 141). On this all the negatives should be laid, and

their proper relative positions sought. When this is done it is evident

at once whether all the territory has been covered, and whether there

are any superfluous negatives. Each negative should then be examined as

to its scale and distortion. If it can be made to fit the scale by

simple enlargement or reduction, a line can be drawn on one edge of a

length indicating its scale. This line will later be used as a guide in

the enlarging camera. If the picture is badly distorted it must either

be replaced by another negative, or if rectifying apparatus is

available, it must be set aside for the making of a rectified print.

[Illustration:

FIG. 141.—Scaling negatives for mosaic map-making.]

The next step is to make prints from the negatives, which may be done

either by contact, or, necessarily if differences of scale must be

compensated, in the enlarging camera. If prints to an exact scale are

required the shrinkage of the paper must be determined and allowed for.

The prints must all show the same tone, and must be uniform from edge to

edge. If the focal-plane shutter is not uniform in its travel, as is

frequently the case, this means that the print must be “dodged,” or

exposed more at one edge than the other, by locally shielding the plate

and paper during exposure. A case of the step-like effect caused by

uneven shutter action is shown in Fig. 140. The effect due to uneven

shutter action is of course absent with a between-the-lens shutter,

which constitutes a strong argument in favor of that type for use in

mapping cameras.

[Illustration:

FIG. 142.—Arranging prints for a mosaic map.]

When the prints are made they must be mounted together on a large card

or cloth background. For a very small mosaic they may be juxtaposed by

simple examination, matching corresponding details in successive prints.

For a mosaic of any size an accurate outline map must be drawn on the

surface to which the prints are to be attached. The prints are then laid

out on this outline, moved to their correct positions, and held down by

pins (Fig. 142). When they are all arranged the final mounting may be

begun. The excess paper, beyond what is necessary for safe overlaps, may

be trimmed off, exercising judgment as to which print of each adjacent

pair is of the better quality, and utilizing it for the top one at the

overlapping junction. If one print shows serious distortion it may be

placed under its fellows on all four edges, thus minimizing its weight.

The edges are best made irregular by _tearing_. Straight edges are apt

to force themselves on one's attention in the final mosaic and give an

erroneous impression of the existence of straight roads or other

features. Both forms of edging are shown in Figs. 124 and 143.

An alternative method of securing the final print mosaic, where film

negatives are used, is to trim successive film negatives so that the

trimmed sections will exactly juxtapose, instead of overlap. The

sections are then mounted, by stickers at their edges, on a large sheet

of glass, and printed together. Captured German prints show that this

was the method commonly used with the German film camera (Fig. 62).

It will be noted that the procedure which has been described and

illustrated by Figs. 142 and 143 assumes the previous existence of a map

accurately placing at least the chief features of the country covered.

This draws attention at once to the limitations and true sphere of

aerial photographic mapping at the present time. With the cameras thus

far it is not possible, nor is it attempted, to do primary mapping of

unknown regions. Distortions due to lens, shutter, film warping and

paper shrinkage considerably exceed the figures permitted in precision

mapping. From the standpoint of geodetic accuracy the cumulative errors

of deviations in direction, altitude and level, peculiar to flying,

would soon become prohibitive.

[Illustration:

FIG. 143.—A partly completed map. Prints mounted over an outline

sketch map to proper scale.]

The great field for aerial photographic mapping in the near future lies

in filling in detail on maps heretofore completed as to general

outlines, or, as in the war, on maps far out of date. The war-time

procedure in country largely unknown, such as Mesopotamia, was probably

closely that which will be necessary in peace. Conspicuous points in the

landscape were first triangulated from friendly territory, and from

these the outline map was drawn, whose details were to be supplied by

aerial photographs. Much of the “mapping” of cross country aerial routes

so far done is frankly of a pictorial nature, showing conspicuous

landmarks and good landing fields—extremely valuable and useful, but not

to be confused with precision mapping. In assembling mosaics of this

kind the elaborate procedure described above is not followed. The

process is the simple one of juxtaposing adjacent prints as accurately

as possible by visual examination. Errors are of course cumulative, but

as long as exact distances are not in question this is no matter.

Airplane Photography · 第 26 / 33 章