[meteorite-list] Cali chondrite fell extremely cold!

Alexander Seidel gsac at gmx.net
Sat Jul 28 23:27:04 EDT 2007


Thanks a bunch, Sterling, hi "Mexico Doug", where art thou????
So it is no surprise an OC can be pretty cold at the touch upon
arrival on earth, as was experienced in Cali/Colombia - qed...

Best from early morning Berlin,
Alex



-------- Original-Nachricht --------
Datum: Sat, 28 Jul 2007 22:06:16 -0500
Von: "Sterling K. Webb" <sterling_k_webb at sbcglobal.net>
An: "Alexander Seidel" <gsac at gmx.net>, "Michael Farmer" <meteoriteguy at yahoo.com>, meteorite-list at meteoritecentral.com
Betreff: Re: [meteorite-list] Cali chondrite fell extremely cold!

> Dear Alex, Mike, List,
> 
>     Alex said:
> > several posts about this on the list in the past...
> 
>     Mexico Doug has done more work on this than anyone
> else I can think of. Go to the website http://www.diogenite.com/
> and click on the item "Meteoroid" in the left-hand menu.
> There is Doug's graph of the space equilibrium temperatures
> for irons, ordinary condrites, and carbonaceous chondrites
> for any distance from the sun.
> 
>     From the graph, we can see that an OC orbiting at about
> the same distance from the Sun as the Earth would have a
> "natural" temperature of about -10 degrees C. The heating
> of ablation is too brief to penetrate far into the stone, and
> the cooling of dark fall is likely to completely nullify exterior
> heating (as Marcin said).
> 
>     Above the graph, Doug provides a link to his post to The
> List where he detailed the assumptions the graph is based on,
> but the List archives no longer go back that far. Mine do,
> however, so here's Doug's full explanation:
> 
> 
> Part I
> 
> There is no minimum size  to absorb energy from the Sun, even a molecule
> can
> do it - heat of everything is  actually principally caused by molecular
> vibrational motion in the Infrared  range under normal circumstances - 
> molecular
> vibrations.  So that answers  the easy question.
> 
> On the temperature of a meteoroid traveling in space,  that is a
> complicated
> question because the question is really millions of  questions in one
> depending on what temperature you mean - and where you measure  it.
> 
> But I think I can give a shot at a satisfying at everything you  wanted to
> know on the first question and weren't afraid to ask, with the  following
> calculations you kept me awake doing.  You can make a lot of  interesting
> observations here.  I'd add a Eucrite and an Enstatite  Achondrite, which
> I 
> expect the
> former would not be closer to OC, and the later  more on the way to the 
> irons.
> I guess:)
> 
> Distance Energy flux  <-------T (degrees C)-------->     T(Planet av.
> Surf.)
> AU  W/m2            CC   OC  Fe-Ni   "ideal" note
> 0.31 14,214           216   195   378       227 Mercury (p) 167
> 0.47   6,184           124   107   255       133 Mercury (ap) 167
> 0.72   2,635             48    34    154        55 Venus  464
> 1.00   1,366              -1   -12     89          6 Earth  15
> 1.52   591               -52   -62     21       -47 Mars  -63
> 2.80   174             -110 -117    -57      -107
> 3.00   152             -116 -123    -64      -112
> 4.00    85              -137 -143    -92      -134
> 5.00    55              -151 -156   -111     -148
> 5.2      51              -154 -159   -114     -151 Jupiter  -144
> 9.5      15              -185 -188   -155     -183 Saturn  -176
> 19.2      3.7           -211  -214  -190     -209  Uranus  -215
> 29.7      1.5           -223  -225   -207    -222 Pluto  (p) -223
> 30.1      1.5           -223  -226   -207    -222 Neptune   -215
> 49.3      0.6           -234  -236   -221    -233 Pluto (ap)  -223 
> Kuiper, 
> Comets (ap)
> 50K      0.000001  -272  -272   -271    -272   Oort Cloud
> 
> (Table may not display well in text, but if  you copy it into excel and
> use
> text-to-columns it should look  great.)
> 
> 
> Part II
> 
> Assumptions & Discussion:
> T =  [(absorptivity/emissivity)*(Energy  flux/sigma)*(a/A)]^(1/4)
> where:
> Emissivity = energy ratio emitted at a  temperature = compositional 
> property.
> Absorptivity = energy fraction absorbed  at a temperature = compositional
> property.
> 
> Temperature is proportional to  absorptivity but proportional to the
> inverse
> of emissivity, i.e.  T^(4)=k*(absorptivity/emissivity).
> 
> The useful form of this law is called  the Stephan-Boltzmann Law:  Energy
> =
> sigma*T^4 (S-B law constant, sigma =  5.67*10^-8*Wm^-2*K^-4)
> That the integrated energy radiated from a black booty  is proportional to
> the fourth power of the temperature.  This "law" is  useful to convert the
> energy hitting an object into the temperature and is  really the
> scientific 
> key to
> address your question  approximately.
> 
> Kirchoff's (other) Law:
> For a body in radiative  equilibrium energy absorption = energy emission.
> So we consider the very  plausible scenario that the meteoroid's position
> in
> orbit doesn't alter  radically (it doesn't travel near light speed!)
> Solar energy is mainly  provided for absorption in the UV-Visible range.
> Energy is emitted in the IR  range (vibrational energy, the meteoroid 
> doesn't
> emit much light  energy:-).
> Meteoroide is spherical in shape (OK not generality, so could vary  maybe 
> 50%
> either way for example when a planar shaped meteoroid had verrry low
> rotational energy w/r to the Sun)
> 
> ABSORPTIVITY = CC = 0.8, OC = 0.65,  Fe-Ni = 0.80, "ideal" = 1
> EMISSIVITY = CC = 0.88, OC = 0.85, weathered Fe-Ni  = 0.28, "ideal" = 1
> 
> Assumed constant emissivities, but actually they  vary, for example,
> decreasing somewhat (and then only by a square root) as the  AU's increase
> for Iron,
> and a lot for Nickel, though I expect the "weathered"  surface might 
> somewhat
> mitigate this.
> 
> The temperature of a meteoroid in  space will of course depend on the
> latitude, depth, it's cross sectional  exposure vs. overall mass 
> distribution and
> distance to the Sun, just like any  other non-radioactive cooled body 
> whether in
> orbit or passing through.
> 
> 
> Part III
> 
> So the directional answer is best gotten to by a  bunch of assumptions and
> simplifications, including that the thing is rotating  on a nice skewer
> and
> isn't too big so that depth becomes an issue, which adds  some calculus
> for 
> all
> those onion rinds.  So sticking to something say a  couple of meters in
> diameter... Otherwise we deal with things like what is the  temperature of
> Mercury
> (Solar side, mass, backside, transition zone, latitude,  rotation, 
> greenhouse
> effect if any, and composition which will affect what  radiation can be 
> absorbed
> and converted into heat.  A simple way to think  about the latter is 
> thinking
> about a microwave oven.  If the object to be  heated is made with lots of
> water, it has a strong absorbance in that range, but  the glass door
> doesn't 
> (even
> on the inside).  So a Tektite sent in orbit  very well could have a lower
> temperature than a cometary water containing  carbonaceous type body which
> in
> turn creates nice effects in part due to these  warmings in the estelas. 
> An
> example like Mercury, of one not rotating with  respect to the Sun causes 
> other
> complications.  So best to think of an ant  in a spacesuit when asking
> your
> question.  The center of the meteoroid will  be cooler at its equilibrium
> temperature so wherever the ant walks or burrows  will depend on the 
> temperature.
> Average temperature is a much easier  proposition, but knowing that
> wouldn't 
> help
> the ant's survival chances at all if  he ends up in the Ant:-)arctic vs.
> Sahara of the meteoroid.
> 
> If one  assumes that a meteoroid has no greenhouse effect and is made of
> stone or  iron-nickel, and absorbs typically a full spectrum in the range
> of 
> what
> the sun  mainly radiates for heating i.e. UV-Visible light, lots of
> simplifying  assumptions can be made.  You can look at Venus and see what
> a
> Greenhouse  effect does, or even Jupiter, which I suspect is somehat
> warmer
> still than the  NASA page reference I used, because it actually puts out 
> more
> energy than it  received that little stunted star...or figure out at what 
> distance
> comets get  tails (snowball's sublimation temperature).  You get the
> idea:)
> 
> The  basics would include the following, I would think, calling the 
> meteoroid
> shape a  sphere for simplification, which of course is not true but good
> enough, also  that the Sun is like a Black Body at 5800 degrees K from
> Wein's  Law.
> 
> Taken together with the idea that radiation from any source drops  off as 
> the
> square of the distance from the source. (Which is understandable by 
> knowing
> that the surface area of a sphere, ie, non-directional emmiting source,
> 4*Pi*r^2 increases by the square of the radius.), you can get a handle on
> temperature caused by the Sun on objects floating in the Solar System. 
> And 
> in the
> case of the meteroid, we only get a quarter of the total area exposed to 
> the
> Sun in the simplified case of a spherical meteoroid (area sphere =
> 4*pi*r^2 
> vs.
> great circle exposed = pi*r^2, a factor of 1/4).
> 
> Using the two laws  in a numer of ways, but sparing the the tedious math, 
> the
> Sun's photosphere  ("surface") clocks at near 5800 degrees K being
> basically
> a heat source  (150,000,000 km from earth minus Sun's radius, aww lets
> just
> say the center of  the Sun since we can then measure in AU and are not 
> dealing
> generally with the  inner Solar System to make a huge difference with the 
> Sun's
> 700,000 km or so  radius.  Using the inverse square law then you get the
> energies in my table  I gave you.
> 
> Then, I derived the temperature in the above table (all in an  excel
> spreadsheet) using the Stephan-Boltzmann Law, for you with this exact 
> formula:
> T = [R/sigma*(a/e)*(areacrosssec/areatot)*(1/R^2)]^(1/4)
> and  substituded the differewnt absorptivities and emissivities...presto,
> a
> solar  meteorite thermometer.  You can graph them too and it is easy to
> look
> at,  but I couldn't figure out how to graph in plain text for the list:)
> 
> [End of Doug's explanation]
> 
> 
> Sterling K. Webb
> -------------------------------------------------------------------
> ----- Original Message ----- 
> From: "Alexander Seidel" <gsac at gmx.net>
> To: "Michael Farmer" <meteoriteguy at yahoo.com>; 
> <meteorite-list at meteoritecentral.com>
> Sent: Saturday, July 28, 2007 9:18 PM
> Subject: Re: [meteorite-list] Cali chondrite fell extremely cold!
> 
> 
> Mike, your comment was obviously triggered by my earlier post to the list 
> this day. I always thought stones of a meteorite fall would be rather
> "cold" 
> after touchdown. Then again one has to look at typical equilibrium temps
> for 
> a tumbling stone meteoroid at a typical Earth orbit cruising distance
> before 
> encounter with the Earth atmosphere. There were several posts about this
> on 
> the list in the past, may be someone can retrieve them from the archives. 
> The hot phase of atmospheric entry, before reaching the retardation point,
> will most likely only affect the very outer zones of a meteoroid large 
> enough to not disintegrate, while the inner parts will remain effectively
> at 
> the former equilibriums temps due to a rather low heat transfer process
> for 
> typical stony meteorites in the few seconds or minutes of atmospheric 
> transit. And the final dark flight will cool down the former temporary
> high 
> temps on the outsides of the stone pretty soon.
> 
> If I ever had the chance to pick up a freshly fallen stone immediately
> after 
> the event, I would expect it to be rather "cold" to the touch.... :)
> 
> Alex
> Berlin/Germany
> 
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