| Abstract:
Witness I reportedly saw a metallic-looking, disk-shaped UFO. She called
her husband, they located their camera, and he took photographs of the
object before it disappeared in the distance.
Background:
Time: 7:45 p.m. PST (1,2); 7:30 p.m. (3).
Position: Approx. 10 mi. SW of McMinnville, Ore. on the farm of the witnesses:
123 19' 50" W, 45 06' 15" N (7).
Terrain: Rolling farm country, elv. 210 ft.; houses several hundred meters
apart (7).
Weather Conditions: Dull with an overcast at about 5,000 ft. (2, confirmed
by the photos).
Sighting, General Information:
The sighting occurred in the back yard of a farm about 0.2 mi. S of the
"Salmon River Highway" (U.S. 99W (7). Witness was feeding rabbits in the
back yard, S of the house and E of the garage when the object was first
sighted (1,2,3,6), apparently toward the NE (6). Witness II was apparently
in the house at this moment, as three of the accounts (2,3,6) refer to
Witness I calling to him and running into the house to fetch him from
the kitchen, although one account (1) states that they had "been out in
the back yard," and "both... saw it at the same time."
As far as Witness I could remember 17 yr. later (6), the rabbits gave
no indication of disturbance.
[[607]]
Immediately after they both saw the object, apparently as it was still
in a NE direction, moving slowly toward the W (6), they thought of their
camera (1,2,3,6). Witness II ran to the car, thinking it was there, but
Witness I remembered it was in the house and brought it (1,6). Witness
II took the camera, which was already loaded. The roll of film had been
purchased during the winter and already had two or three shots on it (4).
At this time "the object was coming in toward us and seemed to be tipped
up a little bit. It was very bright -- almost silvery -- and there was
no noise or smoke" (1).
Witness II explained that he took the first picture, re-wound his film
as fast as possible and then as the object gathered speed and turned toward
the northwest, he had to move rapidly to his right to get the second picture.
Both were snapped within thirty seconds, he estimated (1). According to
another early reference: "[Witness II] elaborated, 'There wasn't any flame
and it was moving fairly slow. Then I snapped the first picture. It moved
a little to the left and I moved to the right to take another picture.'"
(3). Plates 23 and 24 show the two photographs in the sequence taken.
During this interval the object was moving quite slowly, apparently almost
hovering, and it apparently shifted both its position and orientation
in a complex way, changing direction and tipping just before it moved
away, as indicated in Plate 25 (2,6). However, Witness I described it
as "not undulating or rotating, just 'sort of gliding'" (2). The UFO accelerated
slowly during or just after the second photograph and moved away rapidly
toward the west (2) . Witness I ran into the house to call her mother-in-law,
got no answer, and returned outside just in time to see the UFO 'dimly
vanishing toward the west' (2).
Investigation:
The witnesses described the object as "very bright - almost silvery"
(1); "brightly metallic, silver or aluminum colored, with a touch of bronze...appeared
to have a sort of superstructure... 'like
[[608]]
a good-sized parachute canopy without the strings, only silvery- bright
mixed with bronze'" (2); silvery on top but with more bronze on the bottom,
the bottom being different (but, this being seventeen years later, Witness
I was unsure whether it was darker)...shiny but not as bright as a hub
cap...resembling a dull, aluminum-painted tank (which Witness I pointed
out to the writer in our interview)... "awful pretty" (6). The rather
bright, aluminum-like, but not specular, reflecting surface appears, to
be confirmed by analysis of the photos (see below). There was no noise,
visible exhaust, flames, or smoke (1,3,6).
When the object tipped up, exposing its under side to the witnesses,
they felt a gust of wind which they thought may have come from the UFO.
"'...there was a breeze as it went overhead... which died down later'"
(2). In the interview with the writer, Witness I stressed this, remarking
the wind was "about to knock you over," though Witness II (interviewed
separately) remarked that it made only a "very little" breeze as it was
getting ready to fly off (6).
As to size, speed, and distance, the witnesses were reluctant to hazard
a guess (1,2), as Witness II had no way of knowing its size (2), although
one of the references quotes Witness II as estimating a diameter of "20
or 30 ft." (3), and Witness I compared its appearance (though not explicitly
its size) to a parachute canopy (2,6).
As to the origin of the UFO, Witness II remarked both at the time and
in 1967 that he thought it was a secret U.S. craft (1). "'...you hear
so much about those things...1 didn't believe all that talk about flying
saucers before, but now I have an idea the Army knows what they are'"
(3).
Witness II recalls finishing his roll of film on Mother's Day (4) and
had it developed locally (1). Witness II mentioned his observation and
showed the pictures to a few friends. He did not seek publicity about
the pictures, admitting that he was "'kind of
[[609]]
scared of it'" (2,3), and "afraid they would get in trouble with the
'government' and be bothered by the publicity" (2). However, McMinnville
Telephone Register reporter Bill Powell learned of the sighting
from two McMinnville bankers, Ralph and Frank Wortman, and followed up
the story (1,2). He found the negatives "on the floor under a davenport
where the Witnesses' children had been playing with them" (2). The Telephone
Register broke the story Thursday, 8 June 1950 with a front page article
containing the two pictures and Editor's Note:
"...in view of the variety of opinion and reports attendant
to the saucers over the past two years, every effort has been made to
check Trent's photos for authenticity. Expert photographers declared there
has been no tampering with the negatives. [The] original photos were developed
by a local firm. After careful consideration, there appears to be no possibility
of hoax or hallucination connected with the pictures. Therefore the Telephone
Register believes them authentic..." (1).
Various McMinnville residents, including the bankers Wortman, offered to
sign affidavits vouching unreservedly for the reputation and veracity of
the witnesses (1,2,4).
On Friday and Saturday, 9 and 10 June, the Portland, Ore., and Los Angeles
newspapers carried the story (2,3). Life magazine carried the pictures
the following week (4). The witnesses accepted an invitation to appear
on a television program "We the People," in New York (6). Witness I remarked
that they were encouraged by the people responsible for this show to make
statements they (the Witnesses) regarded as inaccurate. The witnesses,
however, did not make such statements, but told only what they saw (6).
While in New York, the witnesses were to receive their negatives from
Life magazine, but were informed that the negatives were temporarily
misplaced (6). Life promised to return them by mail to
[[610]]
Oregon, but apparently never recovered them (6). With the cooperation
of Life the Colorado project discovered that in 1950 the negatives
had been in the possession of International News Photo Service later merged
with United Press International. The Project located the original negatives
and was permitted to examine them.
As mentioned above, various reputable individuals volunteered to attest
to the witnesses' veracity. They appear to be sincere, though not highly
educated or experienced observers. During the writer's interview with
them, they were friendly and quite unconcerned about the sighting. Witness
II was at work plowing his field and did not even get off his tractor.
From interviews throughout this district one gained the impression that
these were very industrious farm people, not given to unusual pranks.
Two inferences appear to be justified: 1) It is difficult to see any
prior motivation for a fabrication of such a story, although after the
fact, the witnesses did profit to the extent of a trip to New York; 2)
it is unexpected that in this distinctly rural atmosphere, in 1950, one
would encounter a fabrication involving sophisticated trick photography
(e.g. a carefully retouched print). The witnesses also appear unaffected
now by the incident, receiving only occasional inquiries (6).
The over-all appearance of the photographs, in particular the slightly
underexposed land foreground and properly exposed sky, is consistent with
the reported time 7:30 PST (sunset being roughly a few minutes after 7:15,
and twilight lasting until after 8:45). There could be a possible discrepancy
in view of the fact that the UFO, the telephone pole, possibly the garage
at the left, and especially the distant house gables (left of the distant
barn) are illuminated from the right, or east. The house, in particular,
appears to have a shadow under its roof that would suggest a daylit photo,
and combined with the eastward incidence, one could argue that the photos
were taken on a dull, sunlit day at, say, 10 a.m.
[[611]]
But accepting the UFO makes scarcely less sense than arguing that the
witnesses staged a hoax at 10 a.m. and then claimed the photographs were
taken at 7:30. Densitometry of the original negatives shows that the sky
itself is brighter toward the west, as expected. It seems posslble that,
half an hour after sunset, the cloud distribution could result in a dull
illumination preferentially from the NE (certainly there will be skylight
from above).
Reality of physical object. As stated previously, it is unlikely
that a sophisticated "optical fabrication" was performed. The negatives
had not been tampered with.
Further, a geometric test was performed to determine whether the object
shown in Plate 24 in approximate cross section was the same object photographed
in Plate 23 at a different angle. The apparent inclination, i, can be
determined from the ratio of the axes of the apparent ellipse in Plate
23.
i = b/a (2)
Measures on several copies of photo 1 (the UPI print, an enlargement
thereof, and two magazine reproductions) gave sin i = 0.368, and
i = 21°.6 ± 0°.1 (est. P.E.).
(3)
Plate 26 shows enlargements from UPI print with lines of sight superimposed
on the Plate 24 "cross section" at 21°.6. The way in which these lines
cut the image is in perfect agreement with the appearance of the object
in Plate 23. Judging from the apparent position of the pole it is likely
that the object has simply tipped, without rotation, between the two photos.
The lighting is also consistent with that in the rest of the photo. Both
photographs, therefore, show real objects and that the object in Plate
23 is a view of the same object in Plate 24, seen in different perspective.
Asymmetry of UFO. It will be noted in Plate 26 that the UFO is
distinctly asymmetric. The "pole" is off center and inclined, and there
appears to be a difference in the profiles of the right and left sides
(Plate 24), the left having a more pronounced notch defining the flange.
The shading of the object also indicates a
[[612]]
more distinct flange on the left in Plate 24. The asymmetries are judged
physical, not optical effects.
Absence of rotation. The top of the "pole," barely visible in
photo 1, is off center to the left by the same amount as in photo 2. This
would be rather improbable if the object were rotating, and supports Witness
II's statement that it was not rotating. This is a rather strong argument
against a fabrication using a necessarily (for stability) spinning model
similar to a "frisbee," especially in view of the fact that only 2 exposures
were made in the middle of an intact roll of film.
Angular size of object. From measurements of recent photos (6)
the photos were scaled and the UFO diameters estimated to be:
| Plate 23: |
1°.4 |
| Plate 24: |
1°.3. |
The P.E. is probably about 0°.1, but the object subtends a smaller
angle in photo 2, consistent with the allegation that photo 2 was made
as the UFO was beginning to depart.
It follows immediately that the distance-diameter relation is determined,
and a man of the locale (based on ref. 7) is shown in Fig. 1 with the
azimuths, angular sizes, and example, that the object was less than a
meter in diameter and over the driveway.
Psychological reaction. I judge it reasonable that as the object
allegedly drifted to the left, in danger of being lost to sight behind
the garage, that the observer should step unconsciously to his right,
as the photos show he did, although one might expect the observer even
more reasonably to step forward, to get in front of the garage. The reason
for the first response may have been that the second would put the observer
close to the house, where the object might be lost to sight if it moved
back to the east, while by moving away from the garage, one moves toward
the open Yard SE of the house. In summary, the movement of the observer
is consistent with the alleged observation.
[[613]]
Possibility of fabrication. The above tests all appear to be consistent
with the witnesses' testimony. The possibility of optical fabrication
seems remote. A model thrown into the air by hand appears an unlikely
possibility because of the evidence for absence of rotation.
Another possibility can be considered, however. The object appears beneath
a pair of wires, as is seen in Plates 23 and 24. We may question, therefore,
whether it could have been a model suspended from one of the wires. This
possibility is strengthened by the observation that the object appears
beneath roughly the same point in the two photos, in spite of their having
been taken from two positions. This can be determined from irregularities,
or "kinks," in the wires. The wires pass between the camera positions
and the garage (left). We know from the change in orientation of the object
that it moved, or was re-oriented by hand, between exposures. The possibility
that it is a model hanging beneath a point on the wire suggests a further
test: Is the change in distance of the object in Plates 23 and 24 equal
to the change in distance from the wires? Measures of the disk indicate
that it is about 8% further away in Plate 24. Measures of the irregularities
in the wires indicate that they are further away from the camera in Plate
24. The amount of the latter increase from the wires (measured by the
separation of rather ill-defined "kinks") is less certain than the distance
increase from the disk, but it is measured to be about 10%. These tests
do not rule out the possibility that the object was a small model suspended
from the nearby wire by an unresolved thread.
Given the foregoing analysis, one must choose between an asymmetric model
suspended from the overhead wire, and an extraordinary flying object (See
Table 1).
Photometric analysis. Although it is often stated that a single
photograph of an object contains no information on the distance, this
is not strictly true. Atmospheric extinction and
[[614]]
scattering, combined, serve to reduce contrast as distance increases,
an effect perhaps best appreciated by artists. The shadowed bottom of
the UFO in Plate 23 has a particularly pale look, suggestive of scattering
between observer and object, and if such scattering is detectable, it
may be possible to make some estimate of the distance involved.
[[615]]
Table 1
Summary of Possible Interpretations
| Interpretations |
Rejected |
Comments |
| Optical fabrications |
|
|
| Double exposure |
X |
UFO darker than sky background |
| Retouch; drawn image |
X |
Negatives unretouched |
| Multiple copies, recopying |
(X) |
Overly sophisticated |
| Physical fabrications |
|
|
| "Frisbee"-type model in flight |
X |
No rotation |
| Model suspended from wire |
|
Under same part of wire in each photo |
| Extraordinary Flying Object |
|
Photometry suggests large distance |
[[616]]
The luminance, or apparent surface brightness at distance r of an object
of intrinsic luminance Bo (r = 0) is
B = Bsky (1 - e-Beta · r) + Bo
e-Beta · r
(4)
where Beta is the scattering coefficient. The first term represents scattered
light; the second, extinction. Since all measures must be based on the
witnesses' two photographs, we will determine Beta for the given day from
the photographs themselves. Normalizing all brightnesses (measured from
the film and assuming that the images measured fall on the linear portion
of the gamma curve) to that of the sky near the horizon, i.e. on a line
within a few thousand feet of the ground, where the UFO is constrained
to be by the reported cloud height and probably nearness to the camera,
we have
B = 1 + e-Beta · r (Bo - 1)
(5)
Notice that if an object is sufficiently far away, its brightness equals
the sky brightness (in physical terms, the optical depth T >> 1).
Given the brightness of an object at zero distance, Bo, and
the observed brightness B, one may solve for the distance r. The first
necessary step is to determine the scattering coefficient Beta. The original
negatives were subjected to densitometric analysis, and Table 2 lists
observed values of B. "Hill 2" lies at a distance of about 2.2 km (7).
The photometry indicates that B = .685 for the distant hill, but the foreground
foliage gives Bo = .403. This gives
= 0.289 km-1,
or optical depth T = 1 at r
= 3.5 km, (6)
which appears consistent with the appearance of the photos.
At this point the theory was checked against objects of known distance.
For example, the roof of the distant barn ("B" in Fig. 1 ) has B = .506.
If one assumes that its intrinsic brightness equals that of the foreground
garage, then Bo = .495, so that r = 0.073 km.
[[617]]
Table 2
Values of B for Objects Photographed*
Based on densitometry of original negatives; aperture 75µ
x 75µ
| Object |
Plate 23 |
Plate 24 |
| UFO "Pole" |
1.07 |
|
| |
Illuminated right side |
1.29 |
1.23 |
| |
Illuminated left side |
(1.35) |
1.05 |
| |
Shaded bottom |
.675 |
|
| Garage roof |
.489 |
.501 |
| |
Shadows under eaves |
.396 |
.426 |
| Metallic tank: |
|
|
| |
Illuminated |
.86 |
.91 |
| |
Shaded bottom |
(.48) |
(.40) |
| Foreground underbrush |
.417 |
.389 |
| Barn (roof) |
.511 |
.501 |
| Hill |
|
|
| |
1 |
.63 |
.59 |
| |
2 |
.71 |
.66 |
| House |
|
|
| |
Illuminated wall |
(.77) |
(.77) |
| |
Shadow |
(.44) |
(.52) |
| Sky |
|
|
| |
Upper right |
1.29 |
1.26 |
| |
Upper left |
1.51 |
1.62 |
| |
Horizon |
1.00 |
1.00 |
| Unexposed edge of film |
.32 |
.34 |
Measures in parentheses have lower weight
* B values are normalized to horizon sky brightness
[[618]]
The true r is about 0.32 km, and our error is a factor 4. One can resolve
the discrepancy by assuming the barn roof was slightly (7%) darker than
the garage roof.
Again, one can check the theory on the distant "Hill 1." B = .610 and
Bo = .403 as measured in the foreground foliage.
This gives r = 1.5 km. The true r is in the range 1.3 to
1.9 km, depending on the part of the hill observed, and the error is negligible.
A third check, more comparable to the UFO problem, is the distant house
("H" in Fig. 1 ). Unfortunately the densitometer did not clearly resolve
the illuminated white facade from the intervening branches; however, supplementary
measures with enlargements indicate that the facade brightness should
be only slightly more than 1.00, e.g. B = 1.02, and Bo
= 1.04, which means that the apparent brightness nearly equals
sky brightness and hence is very insensitive to distance and gives no
good solution. There are shadows visible on the house on the white surface
under the eaves. Measures indicate B = .48. Bo
for the shadows on this white surface, illuminated by the ambient illumination,
should be intrinsically measurably brighter than the shadows under the
dark wooden garage eaves and under the tank beside the garage (Bo
= .41), but not as much brighter as the white illuminated surface
is brighter than the darker wood. (If there were no ambient illumination,
all shadows would be intrinsically black; Bo = 0).
An estimated value is Bo = .43. This gives a distance
of r = 0.32 km, only 14% less than the measured distance of 0.37 km. Naive
use of Bo = 0.41, known to he too low, would have
given r = 0.44 km, 19% too great.
It is concluded that by careful consideration of the parameters involved
in the case of recognizable objects in the photographs, distances can
be measured within a factor-four error. This justifies the assumption
that we are on the linear part of the gamma curve.
[[619]]
Figure 1: Sighting Locale
[[620]]
If such a good measure could be made for the UFO, we could distinguish
between a distant extraordinary object and a hypothetical small, close
model.
At this point we must be explicit about the geometry of the situation.
We represent the environment as in Fig. 2 . We assume that the UFO is
within a homogeneous scattering layer with T = 1 at 3.5 km. If the UFO
were far away and at an altitude greater than the characteristic dimension
of the layer (C in Fig. 2), it would be large and extraordinary in any
case. If it is relatively close, r = 1 km, the assumptions are justified.
Our objective is to distinguish between cases A and B in Fig. 2 . The
sky brightness, to which all the brightness values are normalized, must
be the sky brightness at the horizon, since this is the value characteristic
of long path length through the scattering layer.
For the solution of the UFO distance, we have two independent solutions
from two independent observations: the illuminated and shadowed surfaces
of the UFO. As was remarked above, it is the shadowed surface in particular
that looks pale and hence suggests large distance.
Immediately from Table 2 we see that B = 1.21 describes the part of the
UFO, while the illuminated part of the nearby dull aluminum-painted tank
Bo = .885. Since, as the UFO recedes, B must approach 1.00.
We thus know that 1.21 is the minimum intrinsic brightness of the UFO
surface, i.e. Bo>1.21. Thus the UFO in any interpretation
is known to have a brighter surface than the foreground tank. Thus, the
photometry at once confirms the witnesses' report that the UFO was shiny,
like a fresh, aluminum-painted surface, but not a specular surface.
The question is, how bright is the surface intrinsically, and what surface
properties would be consistant with both the observed illuminated and
shadowed side? Fig. 3 shows two families of solutions, one for the illuminated
top surface and one for the shaded bottom side. Solutions for the latter
have
[[621]]
Figure 2: Sighting Geometry
[[622]]
Figure 3: Brightness/Diameter/Distance Plot
Click on thumbnail to see full-size image.
[[623]]
an uncertainty introduced by the difficulty of measuring the true shadow
intensity or the tank. The distance is given as a function of the assumed
increase in brightness over the value for the illuminated or shaded side
of the aluminum-painted tank, respectively.
Fig. 3 graphically illustrates the problem. For example, if the object
is a model suspended from the wire only a few meters away, its surface
is some 37% brighter than that of the tank, and the shaded side is probably
more than 40% brighter than the shadow on the tank. But this is nearly
impossible to maintain in the face of the photometry. Although the distant
house's surface is roughly twice as bright as the tank's surface, its
shadows can be only a few percent brighter, intrinsically, than those
on the tank. This is basically the problem that was suggested by initial
inspection of the photos: the shadowed side of the UFO appears to be so
bright that it suggests significant scattering between it and the observer.
The upshot is that if the top and bottom surfaces of the UFO are made
out of essentially the same material, i.e. with the same albedo, the photometry
indicates that the UFO is distant, at roughly r = 1.3 ± 0.4 km
(est. P. E.). The witnesses referred to a slightly different hue of the
bottom side of the UFO: they said it was more bronze than the silvery
top side. We have assumed this change in tint had negligible effect on
the photometry, although the implication is that the bottom has slightly
lower albedo. If so the UFO would be still more distant.
There is one last possibility for fabrication which has not been ruled
out. Suppose the object is a small model with a pale grey top and a bright
white bottom (e.g. an aluminum pie pan sealed on the bottom with white
paper). Could this account for the apparent lightness of the bottom, shaded
side of the UFO?
It is difficult to defend this idea in the face of the photometry. Our
analysis of the house indicated that its shaded white surface had an intrinsic
brightness of 0.43, which is very
[[624]]
close to the value measured for the shaded part of the aluminum-painted
tank. Yet hypothetical fabrication requires a surface on the shaded bottom
of the model that is of intrinsic shaded brightness 0.68, considerably
brighter than the shaded part of the white house. In other words, the
photometry appears to indicate that a very white surface on the
bottom of a small model would be required to match the appearance of the
photographs.
To the extent that the photometric analysis is reliable, (and the measurements
appear to be consistent), the photographs indicate an object with a bright
shiny surface at considerable distance and on the order of tens of meters
in diameter. While it would be exaggerating to say that we have positively
ruled out a fabrication, it appears significant that the simplest, most
direct interpretation of the photographs confirms precisely what the witnesses
said they saw. Yet, the fact that the object appears beneath the same
part of the overhead wire in both photos can be used as an argument favoring
a suspended model.
Conclusion:
This is one of the few UFO reports in which all factors investigated,
geometric, psychological, and physical appear to be consistent with the
assertion that an extraordinary flying object, silvery, metallic, disk-shaped,
tens of meters in diameter, and evidently artificial, flew within sight
of two witnesses. It cannot be said that the evidence positively rules
out a fabrication, although there are some physical factors such as the
accuracy of certain photometric measures of the original negatives which
argue against a fabrication.
[[625]]
|