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2. LENS DISTORTION
There are a variety of ways by which the parameters of lens
distortion may be determined. These methods range from
laboratory calibrations using optical arrangements of collimators
or precise test ranges bristling with targets, to calibrations made.
“on—the—job” with the photography of control frames or “self—
calibration" techniques which utilise a multi-station approach
and a bundle adjustment to extract the details of the camera’s
lens characteristics.
In industrial applications where the situation usually demands
photography from a multi-station situation, the self—calibration
technique has proven to be most popular in the last decade.
The other technique worthy of further discussion is the
analytical plumb-line method which, unlike other methods,
only solves for the parameters of lens distortion and not for
principal distance nor offsets of the principal point from the
intersection of the fiducial axes.
2. Self-Calibration
The technique of self-calibration has been briefly described
above, but mention should be made of some of the features of
this technique. In the "purest" form of self-calibration one
would expect approximately four camera stations to be
convergently arranged around an object to which 50 to 500
targets may be affixed. Two or more photographs would be
taken from each station and it is desirable to roll the camera
through 90? between photographs in order to successfully
recover xy and yp. If convergent photography is not employed,
then the object must be non-planar.
Equations (1) and (2) are solved simultaneously to extract the
camera calibration data.
In reality, it may be necessary to alter the focus setting of the
camera between camera stations and this complication will lead
to the photogrammetrist nominating which parameters should be
constant (or block invariant) or variable from station to station
(block variant).
À most important feature of a self-calibrating bundle adjustment
is that the photogrammetrist need not know any values for
object-space control. In fact object space control is only
required for the actual object evaluation with the classical
minimum of two horizontal and three vertical control points
being known.
2.2 Analytical Plumb-Line
The analytical plumb-line method (Brown, 1971) was
developed as a rapid practical way to compute lens distortion
parameters at a range of focussed magnifications from 5X to
20X. The principle of this technique is the axiom that straight
lines in object space should project through a perfect lens as
straight lines onto the image plane. Any variations from
linearity is attributed to radial or decentering distortion.
Two photographs from one camera station are always taken:
one referred to as "horizontal" and the other as "vertical" since
the camera is rolled through 90? between shots.
The plumb-line technique is presently applied by many
researchers as their method for estimating the parameters of lens
distortion. It is a technique well suited to automation as line—
following is a relatively simple procedure. The Autoset
automatic monocomparator developed by Geodetic Services Inc
in Florida (e.g., Fraser, 1986) and the small format Adam
Technology MPS-2 analytical stereoplotter (Elfick, 1986) have
both been programmed to utilise this technique. Fryer and
Mason (1989) used the method for the close-range calibration
of a video camera with the data capture being via a frame—
grabber into a personal computer.
Typically, eight to ten plumb-lines are photographed and, say,
50 points on each line on each photograph are digitised.
Approximately 1000 points will then be provided as data
observations and only the five parameters of radial and
decentering distortion must be solved for in a least squares
solution, along with two parameters to define the spatial
location of each line.
The extrapolation of the plumb-line technique from a laboratory
situation at close-focus to the photography of man-made
straight objects such as long glass panels in multi-storey
buildings has been reported (Fryer, 1987). The further
extrapolation to the use of linear features such as railway-lines
for the calibration of aerial cameras has also been demonstrated
(Fryer and Goodwin, 1989). Also interesting to note is the
extension into aerial camera calibration of the close-range self—
calibration technique described in Section 2.1, where
convergent aerial photography has been used over a test range
was established on flat terrain (Merchant and Tudhope,
).
It is important to realise what the analytical plumb-line
technique does not provide: it does not provide a solution for
the principal distance c, nor the offsets of the principal point xp
and yp. The relevance of these parameters is discussed further
in the next Section when a comparison of the self-calibration
and plumb-line techniques is made.
Finally it should be remembered that the lines which are to be
photographed do not have to be “plumb” in any real sense of
that word. Straightness is the only criterion, the term “plumb-
lines” being derived from the earliest use of the technique when
wires with weights attached were used. The vertically of the
lines is not a feature of the mathematics involved.
2.3 Comparison of Lens Distortion Techniques
The importance of including an allowance for the parameters of
radial and decentering lens distortions has been demonstrated in
many studies including those conducted by Karara and Abdel-
Aziz (1974) and Murai et al., (1984). These studies showed the
effect of radial distortion to be almost an order of magnitude
larger than decentering distortion. In both these extensive
studies the rms values of the residual plate errors decreased by
up to a factor of seven when lens distortions were included.
Non-metric cameras were shown to be able to approach the
accuracy of metric cameras. The K term of radial distortion is
always the most significant, with K2 and K3 usually not
relevant for lenses in typical small format cameras.
A study by Fryer and Fraser (1986) compared the self—
calibration and plumb-line methods of lens calibration on some
small format cameras which were to be used both in and out of
water and in a watertight housing with a plane glass port. The
tests were interesting because of the large range of radial
distortion present in the situations examined. For example, a
50 mm Distagon f—4 lens fitted to a Rolleiflex SLX reseau
camera in an Aquamarin WKD-SLX/6006 submarine housing
produced radial distortions in air of 4273.2 um at r = 30 mm
and —1551.0 um under water. These extremely large ranges of
distortions were recovered by each of the two methods with an
average difference along the radial distortion profiles of 2 um
and a maximum difference of 4.5 um at r = 30 mm. Similar
close agreement occurred with the testing of a 35 mm Nikonos
V camera fitted with a Nikkor 28 mm f-3.5 lens.
The magnitude of the decentering distortion profile for the case
of the Rolleiflex camera in the underwater housing was the
largest experienced by this author in over ten years of
examining photogrammetric cameras. The value of 91 um at
r = 30 mm was undoubtedly a consequence of the 12 mm thick
plane glass port in the underwater housing not aligning
perpendicularly to the optical axis of the camera. The
discrepancy in this value of the decentering distortion profile
was only 2.1 um between methods, and since each technique
had a one-sigma error bound of slightly over 1 jum, the result
was most satisfying.