PHOTOGRAMMETRIC ENGINEERING
nized as the expected standard of terrain
model flatness when the vertical measure-
ments in a stereoscopic model are made with
a first-order stereoplotting instrument.
The pattern of residual errors was observed
on numerous strips which had been adjusted
by the general equation that has been pre-
viously described, namely, Equation (2).
Specifically, thirty-five stereophotogrammet-
ric extensions ranging in length from 7 to 59
stereoscopic models were examined. The total
amount of control utilized in each extension
varied from 10 to 39 control points; control
was randomly distributed in 15 of the strips
and in three to ten bands on the remaining
20 strips. Flying heights ranged from 10,000
to 30,000 feet; the mean height of all flights
tested was approximately 18,500 feet. It
should be noted that the general equation
corrected for a parabolic pattern of error,
propagated in the longitudinal direction,
and permitted one reversal in the direc-
tion of lateral tilt accumulation. Any de-
viation from this pattern of error propaga-
tion would be reflected in the residual error
pattern after adjustment. It was hoped, by
the utilization of this technique, that a con-
sistent error pattern would be revealed and,
as a result, an algebraic equation of the re-
quired degree could be written which would
satisfy all extensions. After examination of
these patterns, it concluded that the
equation would have to be tailored, as to de-
gree and terms, according to the distribution
of the control. Obviously, the residual errors
from “curve fitting" were random: the next
consideration was to make certain that the
accuracy of the adjusted pass points improved
with the
was
to the control on
which the solution was based.
“goodness of fit"
Two specific extensions, containing a super-
abundance of control, were adjusted several
times. The solutions were based respectively
on 20 and 21 control points distributed in six
bands on each strip. Furthermore, these strips
contained approximately the same number of
withheld control which occurred on alternate
bands and were used subsequently to check
the accuracy of the resulting solutions. The
mean square errors both for the control used
in the least squares solutions, and also on the
withheld control are shown numerically and
graphically in Figure 1.
From the above referenced graph, it can
be seen that although the mean square error
on the withheld control was always larger
than the standard error on the control used
in the respective solution, the accuracy of the
adjusted points will generally improve di-
4
rectly with the ‘‘goodness of fit" to the con-
trol on which the solution is based. The lack
of significant improvement between the
fifth & sixth degree equations has not been
satisfactorily explained; although it possibly
results from the limitation of computing
precision (this condition is currently being
checked). Tests with other strips have shown
that there is present a “maximum’ degree
equation depending upon the amount and
distribution of the control. Thus, if excessive
flexibility is permitted in fitting to the con.
trol, this same flexibility resulting from total
compensation for the random error will have
an adverse effect in ''
pass points.
In practice, the ‘rule of thumb” has been
to include one (A;x?) term for each band of
vertical control or isolated control point and
one (B;x'y)term for each band of control
starting with 7=0. The general algebraic
equation is merely an extension of the poly-
nomial in equation (2): that is,
Ao = Boy + A IX + Bixy + A»x? + B» vy
+... + Agx$ + Bexty + H, = H.
over correcting" the
(3)
where all symbols are the same as defined for
equation (2).
This vertical adjustment (equation 3) has
been programmed for the UNIVAC. The
program has the following features:
l. The terms of the general equation are
selected by indicating the highest 4 ;x‘ and
independently Bx'y
(4 «6).
2. With the average scale for the extension
terms to be deleted
or a changing scale coefficient predetermined,
all stereo-photogrammetric elevations (Z
coordinates) are converted to feet or meters.
3. Earth curvature correction is optional.
When it is significant, as from high altitude
photography, the correction is applied as a
function of the lateral or y distance (y;— 5);
that is,
(vi — $)*S
=
7 (304.8)(5280) (8000)
where
Ze=the correction for earth curvature
(mm)
vi= photogrammetric coordinate of point
(2)
Vy=mean photogrammetric coordinate of
all the control points on the extension
$ — denominator of the scale ratio for the
average scale of the extension.
The error accumulation due to earth curva-
ature along the line of flight (x-direction) is,
35
30
25
20 |
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solutioi
meters
control
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