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of random noise. This fact--leaving aside economical con-
siderations--may prove to constitute a major challenge to
the design and manufacture of completely automatized measur
ing equipment.
The 930 single camera reductions--ranging from about bo
to 100 plates per lens cone—demonstrate, with the quanti
tative terms of their specific scale, radial and decentering
distortion parameters, that the photogrammetric bundle can be
simulated reliably by a specific mathematical model over a
temperature range from +20°C to -36°C. The similarity of
these parameters, when normalized for temperature influences,
gives evidence that the series of 1? Wild BC-b Cosmotar cones
were manufactured to extremely close tolerances, resembling each
other closely and performing close to theoretical expectations.
The application of the analytical reduction method to the
calibration of wide-angle precision cameras has so far pro
duced residual errors compatible with the results obtained
during the data reduction of the satellite triangulation pro
cedure. This fact suggests that the theoretical potential
of aerial triangulation can be realized, provided proper
precautions are taken to control or monitor the environ
mental conditions of the aerial camera during flight.
The contribution of random errors of the 103E emulsion
on glass plates was statistically isolated and determined
to be +1.0 micron, a result which agrees exactly with the
result of independent laboratory tests made by Eastman-Kodak.
Atmospheric scintillation, with an average of ±2.1 micron
(±1"0) for star and ±2.7 microns (±1"2) for satellite images,
constitutes one of the major error sources in photogrammetric
satellite triangulation. The performance of a comparator
with respect to its random behavior therefore need not be
better than ±1.0 micron for the type of application under
consideration.
Following re-evaluation of all presently available and
future raw data with a new generation of existing computer
programs, more statistical analysis, involving correlation
techniques, will be applied, designed to investigate the
components of the photogrammetric procedure in finer detail.
As a by-product of the program information will become available
in areas outside of photogrammetry. Examples are: the quan
titative determination of electromagnetic propagation delays
by comparing received time signals with the station clocks
whose performances are monitored by frequent comparisons,