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Photographic
Case 46
University
of Colorado
Final Report
of the Scientific Study of U.F.O.s
( under U.S.A.F.contract
# F44620-67-C-0035) 1968
McMinnville,
Oregon
11
May 1950
Investigator:
Hartmann
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 2 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 (I ) 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.
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 2 ran to the car, thinking it was there but Witness I remembered it was in the house and brought it (1,6). Witness 2 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 2 explained that he took the first picture, rewound 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 2] 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 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 11 (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 2 had no way of knowing its size (2), although one of the references quotes Witness 2 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 2 remarked both at the time and in 1967
that he thought it was a secret U.S. craft (I)."..... you hear so much
about those things . . . I didn't believe all that talk about flying saucers
before, but now I have an idea the Army knows what they are"' (3).
Witness
2 recalls finishing his roll of film on Mother's Day (4) and had it developed
locally (1). Witness 2 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 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. 9 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 Trents' 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 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 2 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: I ) 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 overall 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. 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 possible
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.
sin
i = b/a (2)
Measures on several copies of photo I (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 ph oto. 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 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 11'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 map of the locale (based on ref. 7) is shown
in Fig. I 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.
Possibility
of fabrication
The
above tests all appear to be consistent the 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
the 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 ap cars 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 reoriented 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 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.
Table
I
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, X Overly sophisticated
recopying
Physical
fabrications
"Frisbee"-type
model X No rotation
in
flight
Model
suspended from Under same part of wire in
wire
each photo
Extraordinary
Photometry suggests large distance
Flying
Object
The
luminance, or apparent surface brightness at distance r of an object of
intrinsic luminance
B.
(r = 0) is
B
= B sky ( 1 - e (-Pr) ) + B. e (-Pr), (4)
where
P 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 P 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 (-Pr) ( B. - 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, B, and the observed brightness
B., one may solve for the distance r. The first necessary step is to determine
the scattering coefficient P
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 background foliage gives B. = .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 B. = .495, so that r = 0.073 km.
Table
2
Values
of B for Objects Photographed*
Based
on densitometry of original negatives,. aperture 75,u x 75,u
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
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 B. = .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 B. @ 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.
B. 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 (B. = .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: B. = 0). An estimated value is B. = .43.
This gives a distance or r = 0.32 km, only 14% less than the measured distance
of 0.37 km. Naive use of B,, = 0.41, known to be too low. would have given
r =.O.4 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. 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
Fig. 2
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 B. = .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. B. >/= 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 consistent 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 an uncertainty introduced by the difficulty of measuring the true shadow intensity on the tank. The distance is given as a function of the assumed increase in brig htness over the value for the illuminated or shaded side of the aluminum-painted tank, respectively.
Fig.3
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. wit the same albedo, the photometry indicates that the UFO distant, at roughly r = 1.3 =/- 0.4 km (est. P. E.). The witnesses referred to a slightly different hue of the bottom 4 of the UFO: they said it was more bronze than the silver 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 been ruled out. Suppose the object is a small model with a pale gray 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 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.
Sources:
Early sources in approx. chronological order)
1.
The Telephone Register, McMinnville,Ore., June 8. 1950.
2.
The Portland Oregonian, Portland, Ore., June 10, 1950.
3.
The Los Angeles Examiner, Los Angeles, Calif., June 11. 1950
4.
Life, June, 1950
5.
Scheiman, G.E., Project Bluebook Photo Analysis Report 66-22, June 9,1966.
6.
Hartman, W.K., interview with Mr. and Mrs. Trent, June 6, 1967.
7.
U.S. Geo Survey map, Ballston, Oregon 15' quad.
8.
Correspondence between Colorado Committee and United Press International.
9.
Middleton, W.K., Vision through the Atmosphere (Toronto: Univ.Toronto Press)