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Astronaut Scientific Debriefings, 1962-1963

National Aeronautics and Space Administration · 1962 · 216 pages · text from the file's own layer

This NASA file of astronaut scientific debriefing papers from 1962 collects internal Office of Space Sciences material on the science observations made on early Mercury flights. A February 1962 memo from Maurice Dubin asks for more detail on John Glenn's report of luminous particles and the atmospheric horizon layer. A draft memo concludes that the particles were tied to the spacecraft and were not extraterrestrial. The file also holds a Los Alamos letter that attributes the high haze layer to nitrogen peroxide, and notes on Carpenter's airglow observations.

From the source:Release of 2026-06-12 This file contains memoranda, correspondence, reports, and other materials relating to contemporary scientific interest in investigating the nature of luminous phenomena reported by astronauts John Glenn and Walter Schirra during spaceflight. This collection includes transcripts from NASA interviews and debriefings with both astronauts regarding those observations. It also contains details relating to scientific observations of atmospheric phenomena, including brief descriptions of luminous particles, experiences while aboard spacecraft, and circa 1955 theoretical analysis of meteoric particles entering the atmosphere. Pages 34-35, 55-56, 57-63, 64-113, and 122-127 feature content relevant to the PURSUE initiative.

  • p. 64 …J Cooper: No. If I had no prev;ous experience on the light·, I don Vt…
  • p. 65 …because you ha~ e , as background'l Cooper: I think possibly so~ Of course it's…
  • p. 66 …F,.. ~ ...,, ., , - • I • l •, • 'I- - • •~ -, • ' , was? ,. • -,-~ ;' _·•: ... .,~ '-.. .. - Cooper:. I Just don't have any idea. I kept doubting…
  • p. 67 …ghtning par'tfcularly in that area. .: • '.o:. Cooper: · Well, · this is .,one possibility· that there was…
  • p. 68 Scientific Debriefing -5- Cooper: The moon was probably 14-al. It was down to about a…
  • p. 69 I' .' Scientific Debriefing -6- Cooper: Well, not realq. As I went into both night sides I…
  • p. 70 Scientific Debriefing -1- Cooper: .Almost. Almost as it began to get dark. Of course it gets…
  • p. 72 …Probably about 30 degrees G Cooper: I had a ~-:few comments that I made · on the…
  • p. 73 Scientific Debriefing Cooper: Just once. Bill Armstrong: Did you do it twice or Just once? ·'.1…
  • p. 74 ,. • I Scientific Debriefing • -ll- Cooper: I think so. I think with that brightness~ if you know…
  • p. 75 …I • l • .' • . ~ l • • . •. • - ' ' Cooper: Yeso Bill: That 1s one of t he main things we wanted…
  • p. 76 . Scientific Debriefing -13- Cooper: Those deploy marks worked real well. They were excellent for getting in…
  • p. 77 …Did you make attempts to see it· on the day side'l Cooper: I sure did…
  • p. 78 …Did .you see the ·stars during this• ~'l , I Cooper: Not this particular ··orbit. No I…
  • p. 79 …the · center of' the window? Cooper: Noo More slight¥ to the le:f't of' the…
  • p. 80 ',' I Scientific Debriefing -17- I Cooper: Maybe as long as a minute. I doubt if it…
  • p. 81 ,. 1' ' Scientific Debriefing -J.8- Cooper: Yes, it got dimmer. Mercer: Cou1d you see _lights of…
  • p. 82 Scientific Debriefing -19- Cooper: ~finite~: The ideal would be a series of lights. A better combination…
  • p. 83 I i ' I Scientific Debriefing -20- Cooper: You 're going to have to be right on…
  • p. 85 …Is this maneuver an expensive and troublesome· thing to do'l Cooper: It takes control power…
  • p. 86 …worked •very well. ' • And the lens opening of 5.6? 'Cooper: ·It was exactly-on ·what…
  • p. 87 …aey more information? There was none in the tra.ns9ript. ~ Cooper: What base was this oni…
  • p. 88 Scientific Debri efing -25- ( Cooper continued) ·a brown look, Everything predominantly had a. bluish cast . .All…
  • p. 89 Scientific Debriefing Cooper: I could not see distinct lightning patterns. It ju,st all lit ~• . I…
  • p. 90 Scientific Debriefing -27- Cooper: No. I noticed several large cyclonics. I did not notice any very…
  • p. 91 …Was the horizon always ·a sharp line? Cooper: Yes, day and 'night the hqrizon was sharp…
  • p. 92 …Which is darker, the earth or the 11ttl.e band of sky? Cooper: When there was…
  • p. 93 …Does the earth appear as blue to your eye , , as it does in the photos? Cooper…
  • p. 94 …You could see the griton\ the window? • Cooper : You could see the light actually impinging on…
  • p. 95 …More like a patch? Cooper: Smoother. It was a good sized area. • Roach: You didn't…
  • p. 96 …We are interested in horizon effect after sunset • . \' (Cooper draws some more pict~es.) Cooper: You…
  • p. 97 …Did you 'notice this was cone shaped? Cooper: A little bit cone shaped. J Roach : Did…
  • p. 98 …I Cooper : Sunset is more of a golden orange. Dr. Voas : Did you notice any of…
  • p. 99 …Then, is there some structure above the blue layer? Cooper: I never could see pattern structure…
  • p. 100 …What are your attitude tolerances •in ASCS? Cooper: I would say within about 5 l/2…
  • p. 101 …was the camera easy to use'l Cooper: Yes, after I once got it out of…
  • p. 102 …Di"d you place it vertically? Where did you place it? Cooper: I placed it vertically…
  • p. 103 …That is all I had. ' Cooper : Did you get anything at all? Warren : Particul.a.rly…
  • p. 104 …Were you listening for it at the time'l Cooper: Yes, except I had my visor…
  • p. 105 …Over the Himalayas, shot number 12, was the green true? Cooper: Yes, fairly true. Shepard : I…
  • p. 106 …Did you see any distinct shadows from the terrai!n? Mountains? l t .Cooper: •Yes. You…
  • p. 107 …O'Keefe: .Did you see anything that looked like a crater? ! I Cooper: No. I sure…
  • p. 108 …Did they actually seem to curve in? Cooper: If I would be sitting facing this way…
  • p. 109 …the smoke? Cooper : was bl~ Hanel: Hanel: in polar Cooper: an airplane. ·clouds Hanel: pictures? Cooper…
  • p. 110 …Question: · Did you see any dust storms? Cooper: At no time· did I note a dust…
  • p. 111 …I Cooper: No. I think this was purely a feeling of the straps. You're floating…
  • p. 112 …Did you see ,Calcutta? I Cooper: No. Fisher : Did you see any airports? Cooper : Ye~, I…
  • p. 113 …Could you hear better? Cooper : No. \ Dr. voas: Did you at any time hear an unusual…
  • p. 183 …it should have been (capped) ooo Gordon Cooper knows this and will have a cap on…
  • p. 184 …Schirra - Cooper will have this very same type of li ght meter. Nordberg - You know why…
  • p. 196 …Schirra = I feel at this point, for example, in Cooper 0 s flight , what we are…
"Meteors" (A Symposium on Meteor Physics): Special Supplement (Vol. 2) toJ. Atmosph. T err. Phys. (1955)
Meteor Ionization in the E-region
MAURICE D UBIN
Air Force Cambridge Research Center, U.S.A.
ABSTRACT
The theories of meteoric interaction with the atmosphere h ave been reviewed to determine the total
contribution by m eteors to t he ionization content of the E-region. From Herlofson's t heoretical
treatment of this interaction, and Watson's distribution of t he size and numbers of meteoric particles
entering the atmosphere per day, t h e number of electrons produced at various altitudes in the E-region
was computed. These computations indicated that most of the ionization at higher altitudes resulted
from meteors oflarge visual magnitude. Since, as Whipple has shown, the ablation process would probably
not occur in the case of micrometeorites because of heat loss by radiation, the collision processes for
ionization were r eviewed; it seems that the ion ization process is mainly a function of the relative energy
of the co11·'ion, and therefore ablation prior to ionization would not be required for small particles.
Using the Jue (of GREENHOW and H AWKINS, 1952) for t he efficiency of t he ionization process and the
recently re ised value for the amount of meteoric material entering the atmospher e per day, the rate of
production f electrons was found to be 20 electrons/cc sec. From this value and the r ecombination
coefficients ·n the E-region, t he equilibrium electron den sity in t he E-region was found to b e between
2 x 104 and 7 x 104 electrons/cc. It is therefore proposed that the night-time value for the electron
density in the E -region results from meteoric bombardment, and that sporadic Eis caused by the same
process on the assumption t hat the distribution of meteoric particles in space is non-isotropic and
contains centres of high density. P erhaps, also, the interaction of charged micrometeorites with the
earth's magnetic field, may be considered as a mechanism for t he production of magnetic storms.
1. INTRODUCTION
METEORS, as commonly known, are extra-terrestrial part icles of only a few milli
grams, which enter the earth's atmosphere at relatively high velocities. In their
interaction with the air, they are vaporized by the heat generated and ~re respon
sible for the emission of light and. production of ions along the meteor trail. The
major portion of the kinetic energy of the meteoric particles is absorbed in the
altitude region between 80 and 120 km. It is attempted below to consider whether
the integrated effects of this meteoric interaction might contribute to the structure
of the E-region.
2. THEORY
HERLOFSON (1948) has constructed a model for the interaction of meteoric particles
with the atmosphere. It is assumed that in the region of meteoric flash , the mean
free path of the molecule is much greater than the radius of the meteor. Under
such conditions, the front surface of the meteor is bombarded by single air mole
cules and the major portion of them is trapped in the metal surface. The kinetic
energy relative to the meteor which is given up to the meteor suffices to bring the
temperature to that of ev:aporation. The meteor atoms evaporate off the meteor
(ablation) with velocities appropriate to the temperature and the relative velocity
of the meteor with respect to the air.
From consideration of the physical interaction.of the meteor with the air mass,
using the differential form of the conservation of energy and momentum, HERLOFSON
determined the equation for the rate of evaporation at any point along th!;) trail.
r
n = ¾nmax(P/Pmax ) [l - ¼(P/Pmax)]2 (1)
wher.e nmax = 7 X 1023 r 00
3 = the maximum rate of evaporation.
p = the pressure at any point along the trail.
Pmax = 4 X 10- 2 r 00 = pressure along the trail where nmax occurs.
00 = the initial radius of the meteoric particle.
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Official release, from the pursue collection. The PDF is mirrored here; the original link is above. 216 pages are in the text index: search them above, or from the library's search.