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roswell

Office of the Secretary of Defense · 993 pages · text from the file's own layer

The Roswell Report: Fact versus Fiction in the New Mexico Desert was published in 1995 by Headquarters United States Air Force. It was written in response to Representative Steven H. Schiff's request and a General Accounting Office audit, and it contains Col. Richard L. Weaver's report and 1st Lt. James McAndrew's synopsis, along with attachments, appendices and photographs. The report says researchers found no evidence of an extraterrestrial craft or crew. It concludes that the 1947 debris came from a Project MOGUL balloon train.

  • p. 31 …Evidence in Search of Proof" (1985) by Moore; The UFO Crash at Roswell (1991) by Kevin…
  • p. 36 …There were no ancillary records in Air Force files to indicate the potential existence of such…
  • p. 76 …All of this organization's UFO study files were transferred to the National Archives and made…
  • p. 78 …These primary documents should have been part of this organization's UFO study files and currently…
  • p. 98 …On 2 March 1994, Inquiries Branch staff developed a list of possible file locations which might…
  • p. 100 …ROSWELL UFO UFOS UNIDENTIFIED FLYING OBJECT UNIDENTIFIED FLYING OBJECTS WEATHER BALLOON WEATHER BALLOONS The IRIS search…
  • p. 114 …These files ~on tain policy guidance and AFOSI District reports of investigation concerning UFOs (filed primarily…
  • p. 273 …He appeared to want to substantiate the existence of the UFO incident as a UFO. I…
The actual atmospheric distribution. however. does not indicate an
adiabatic lapse rate for air but rather a lapse rate which varies
with altitude. For. the troposphere the lapse rate of the atmosphere
averages -1.980C/1000 .ft. It may be shcrrm then that in the tropo-
sphere a rising balloon will get warm with respect to the air
(neglecting ventilation and radiation effects} at a rate of
1.98 - .57 : 1.4lOC/lOOO ft. In the tropopause the lapse rate of
the atmosphere is zero. Thus the lifting gas (if helium} will
oool relative to the air at a rate of .570C/1000 ft.
Similarly, in the stratosphere, the lifting gas will cool relative
to the air at a rate of 2.24 ~ .57 : 2.81°0/1000 ft. This effect
is plotted as Figure 22.
...0
:;)
TEMP. OF LIFTING
GAS DUE TO
AD.IABATIC EXPAN-
SION WITH AL'riTUDE
STRATOSPHERE
~ TROPOSPHERE
~~----------------\---~--~~~~~~~
c
TEMPERATURE
Figure 22. Lapse rate of air and helium.
Here. below point A, the lifting gas will be warmer than the air.
Above point A, the lifting gas will be cooler than 'the e.ir. The
effect of this temperature difference on the lift (as shovom in the
previous section} is approximately lll = L ..ai I
T (I- 8)
Thus. as a balloon system passes through point A. it will have less
lift then at release. This effect has been observed on several
flights. where a balloon system slowed down during ascent through
a ~mperature inversion.
Since the effect of the sun in heating the lifting gas decreases
the effect of different lapse rates, the effect is not as noticeable
during the day as at night. At night the balloon system may pass
through an inversion, lose its lift, and remain at an altitude much
below its estimated floating altitude until warmed by the sun's rays
at sunrise.
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FOIA release, from the osd collection. The PDF is mirrored here; the original link is under it. 993 pages are in the text index: search them above, or from the library's search.