18 ANALYTICAL AERIAL TRIANGULATION, SCHUT
triangulation with respect to an arbitrary coordinate system. In this case the six orien-
tation elements of the first photograph will be chosen arbitrarily. The first model will
then be obtained in both procedures by establishing the relative orientation of the second
photograph from the condition that corresponding rays must intersect. An arbitrary
scale will be assumed by assigning an arbitrary value to the base or to one of the base
components of the first model.
A transformation of the strip coordinates to the ground control system is then nec-
essary. Leaving out of consideration a transformation which includes deformation of the
strip by adjustment to redundant ground eontrol or with other extraneous data, the
transformation consists of rotation, sealing and translation of the strip.
This transformation is possible if three ground control points of which all three
coordinates are known occur in the first photograph. This makes absolute orientation of
this photograph possible and thus rotation and shift of the strip. For scaling at least one
such point must occur in the second photograph. It is evident that in this case it is pos-
sible to triangulate the strip directly in the ground control system. This is actually the
practice in contemporary applications of the Herget Method. If more than one ground
control point occurs in the second photograph it is possible to employ two or more of these
points in the orientation of that photograph. However, in the second triangulation pro-
cedure this is extremely undesirable. Identification errors will then affect the relative
orientation of the photograph and, consequently, those of all following photographs.
The transformation is possible also if the ground control occurs in different models.
Very often not enough control will occur in any one photograph or model to enable this
to be oriented separately. In this case, which may be expected to occur most often in
practice, triangulation of the strip with respect to an arbitrary coordinate system is the
only possibility.
14. The coordinate system in which the ground control points are given will be an
orthogonal three-dimensional system. Possible choices are:
1. a geocentric system,
2. a local system with its origin in or near the arca of the strip, with one of its axes
approximately vertical and with a known relation to a geocentric system, and
3. a map coordinate system consisting of plane map coordinates and terrain heights.
Since map coordinates of the measured points are required ultimately, the choice of
a map coordinate system is the most natural one. Local coordinates must be transformed
to geocentric coordinates and geocentric coordinates must be converted to latitude, longi-
tude and height above a reference surface. Latitude and longitude must in turn be con-
verted to map coordinates.
For long strips a local or geocentric system is often advocated. These systems have
the advantage that neither earth curvature nor the use of different map projections for
different parts of the strip causes complications. However, besides requiring the labo-
rious conversion via latitude and longitude they have a second disadvantage. Very often
either the plane position or the height of a control point is not known. Use of such points
in a geocentric or local system causes complications. As yet therefore applications of the
Herget Method have been confined to the case where all three coordinates of all control
points are known.
Because of these disadvantages of geocentric and local systems the author at the
National Research Council of Canada has chosen the map coordinate system as the sys-
tem in which to give the coordinates of the ground control points.
The use of this system brings with it its own complications. In the first place the
strip will follow the curvature of the earth while the map is a plane representation.
Therefore the strip must be corrected for earth curvature either before transformation
to the map coordinate system or during a direct computation in this system.
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