Documents / Report

The Roswell Report: Fact vs. Fiction in the New Mexico Desert

USAF / The Black Vault · 1995 · 882 pages · text by OCR

The Roswell Report: Fact versus Fiction in the New Mexico Desert was published by Headquarters United States Air Force in 1995. The Black Vault distributes this copy. It reproduces the report by Col. Richard L. Weaver and the synopsis by 1st Lt. James McAndrew, both written after a General Accounting Office inquiry requested by Representative Steven Schiff. The Air Force search found no evidence of an extraterrestrial craft or crew. It concluded that the Roswell debris most likely came from NYU Flight No. 4, a Project MOGUL balloon train.

  • p. 9 …Appendices to the McAndrew Synopsis are identified by gray tabs which appear at the top right…
  • p. 25 …The rubber was smoky gray in color and scattered over an area about 200 yards in…
  • p. 35 …a thick, foil like metallic gray substance; a brittle, brownish-black plasticlike material, like Bakelite; and…
  • p. 40 …the ruptured and shredded neoprene would "almost look like dark gray or black flakes or ashes…
  • p. 173 …Some of the material would almost look like dark gray or black flakes or ashes after…
  • p. 187 …He talks about the smoky gray rubber... Q: Which these samples here, as you say, if…
  • p. 206 …There's a gray area here. I was certainly aware that what we were doing in…
  • p. 308 …The rubber was smoky gray in color and scattered over an area about 200 yards in…
The force due to friction or drag $ F_{D}=C_{D}\frac{r}{2} A D z $ (This assumes that there is no vertical motion of the air in which the balloon system is floating. We shall later consider the case where an atmospheric force is causing vertical motion of the air.) Where:

P = mass density of the air surrounding the balloon system

A = projected area of the balloon on a plane perpendicular to the relative velocity

Dz = vertical velocity of the balloon system (Velocity in the direction of greater altitude is considered positive.)

$ C_{D}= $ a coefficient of drag, dependent on Reynolds number $ N_{R}=\frac{D_{Z}d\rho}{\mu} $ where: $ d $ = diameter of sphere (ft. )

$ \rho $ = mass density of surrounding fluid $ (\frac{1 b.\ sec.^{2}}{f t.^{4}}) $

$ \mu = $ viscosity of surrounding fluid $ (\frac{\mathrm{lb.\ sec.}}{\mathrm{ft.2}}) $

A plot of drag coefficient against Reynolds number for a sphere is shown in Figure 27.

Figure 27. Drag coefficient vs. Reynolds Number, for sphere.

Cited by

Cases discussed

About this file

Report, cited by the archive. The PDF is mirrored here; the original link is under it. The text was read from the page images by an OCR model; expect the odd misread word. 882 pages are in the text index: search them above, or from the library's search.