Puzzling Attributes of
                           Small Asteroids
                             Clark R. Chapman
                           Southwest Research Institute
                             Boulder, Colorado, USA
Pat Rawlings, SAIC
Pat Rawlings, SAIC


                       Session: “Planetary Science: Small Bodies,
                                “Planetary
                              Collisions, and Satellites I”
                                                         I”
                     International Workshop on Paolo Farinella
                       (1953-2000): The Scientist and the Man
                       (1953-2000):
                                 11:50, 15 June 2010
                                University of Pisa, Italy
Paolo Attacked Puzzles…

  I’ll Discuss a Few More:
 Double asteroids don’t
  match double craters
 Space weathering is very
  fast, yet very slow
 2008 TC3 was a 3 meter
  jumble of meteorite types
 NEAs in microgravity
Doublet Craters: History of Topic
   “Martian doublet craters,” V.R. Oberbeck & M. Aoyagi, J. Geophys.
    Res., 77, 2419 - 2432 (1972).
   1978: Woronow inconclusively debated Oberbeck about whether
    spatial randomness was correctly modeled. Conclusion back then:
    Mars may or may not have an over-abundance of paired craters.
   Topic resurrected in 1991 by Melosh & Stansberry who argued that 3
    doublets on Earth must have been formed by impact of binary
    asteroids (this was before any asteroid satellites had been discovered).
   Farinella & Chauvineau (1993): slow synchronized spinning binaries
    would be at correct separation for doublet craters; binaries might later
    separate or, more likely, coalesce into contact-binary configuration
    (common in radar delay-Doppler images of NEAs).
   In 1990s, Melosh, Bottke, Cook, et al. re-examined Martian doublets and
    extended the analysis of doublets to Venus.
   Dactyl was discovered and the tidally disrupted SL-9 comet impacted
    Jupiter, so doublet/multiple craters were analyzed in that context.
Methods of Forming Doublets
          Random impacts (unavoidable)
          Very oblique impacts, ricochet
          (Messier, Messier A)
          Endogenic crater formation
          (volcanoes, collapse pits, etc.)
          Atmospheric break-up, explosion
          (Henbury)
          Tidal break-up (Shoemaker-Levy 9)
          Spatially clustered secondaries
         Impact of binary asteroid or comet
How to Recognize Doublets
     The certain way
       Adjacent craters with same
        measured ages (Earth only)
       Overlapping craters with
        shared walls (septum)
     The very likely way
       Adjacent craters with similar
        relative ages
       Other unusual similarities
        indicating, e.g., same oblique
        impact angle
     The statistical approach
         Find a greater abundance of
          doublets than predicted by
          chance (doesn’t say which
          ones are the true doublets,
          unless the characteristics are
          very unusual)
Observed Frequencies of
   Doublets on Several Planets
 Earth
      3 pairs among 28 craters > 20 km diameter;
       statistically significant because of very sparse
       crater densities on Earth and same ages
 Mars
      Melosh et al. (1996) studied 133 craters on
       northern plains, 5-100 km diam., and found 3
       likely pairs with separations exceeding random
       expectations  2.3% doublets, less than on
       Earth and Venus
 Venus
      Cook, Melosh & Bottke (2003) found 2.2% of 10
       to 150 km diameter craters were doublets, but
       that “splotches” (due to smaller impactors
       unable to penetrate the Venus atmosphere)
       imply ~14% doublets on Venus
 Moon, Mercury, planetary satellites
      I’ve found no definitive studies
      But doublets exist (Moon; Mercury )
NEA Binaries are too Close to
                               Make Doublets
                           Main Issue:
                           Impacting NEAs form craters 10 – 20
                           times their own diameter. Most NEA
                           pairs are so close that, even with
                           favorable geometry, they form a
                           single crater. How can there be so
                           many doublet craters?
Walsh
                           Plot shows that typical           Separation can be larger
(2009)                     separation of satellites and        for oblique impacts
                           binaries is about 4 times the
                                                             Separation of craters can
                           radius of the primary.
                                                              be zero if pair are un-
                           Only 1 out of the sample of 35     favorably aligned, even if
                           is separated widely enough         widely separated
                           (~15 times primary radius) to     Tidal forces can affect
                           produce a double crater.           separation
                           ~15% of NEAs have satellites
                           or are binaries so <0.5% of
                           craters made by NEAs should
         Perihelion (AU)   be visibly double.
Space Weathering is Fast…
                                   Or is it? (It is a Puzzle!)
    Binzel et al. (2010)    “Space weathering” is the process that
                             transforms the spectral reflectance (colors and
                             albedo) of the surface of an airless body by
                             reddening and/or darkening it (mainly by solar
                             wind; also micrometeorite impacts).
                            Vernazza et al. (2009) study dynamically very
Walsh et al. (2008)
Walsh et al. (2008)          young family asteroids and find that most space
                             weathering color changes occur in ~1 million yrs.
                            Following a suggestion of Nesvorny et al. (2005),
                             Binzel et al. (2010) find that frequent, distant tidal
                             encounters with Earth by NEAs produce color
                             changes (tidal rejuvenation of surfaces?). Few
                             NEAs (or MBAs) are Q’s. [Can YORP spin-up help?]
                            Yet bright crater rays persist for 100s of m.y.
                                  Rays from Tycho crater on the Moon (~100 m.y.
                                   old) dominate the full Moon
                                  Copernicus rays are still prominent after 800 m.y.
                            Mercury is periodically bombarded by solar wind,
                              yet rays from large, infrequent craters are vivid.
Catalina Sky Survey
                                    2008 TC3: Linking an Asteroid to
                                    a Bolide to a Meteorite!
                                                                                       TC3 Reflectance Spectrum: Wm. Herschel
                                                                                       Telescope (Fitzsimmons, Hsieh, Duddy & Ramsay)
                                            TC3 Lightcurve (Clay Center Observatory)



           TC3 asteroid moving
           (W. Boschin, TNG)




TC3 atmospheric train (M. Mahir)    2008 TC3 was the 1st NEA ever discovered (Catalina
                                      Sky Survey, 7 Oct. 2008) that was then predicted, for
                                      sure, to impact Earth. Telescopic observations were
                                      made before impact: lightcurve, reflectance spectrum.
                                    19 h after discovery, impact occurred and was
                                      recorded over Sudan; ~700 paired meteorites (named
                                      Almahata Sitta) have been collected so far.
Almahata Sitta fragment on the
ground in Sudan (P. Jenniskens)     This first-ever event was not a fluke: we must expect
                                     future (maybe annual) predictions of meteorite strikes,
                                     from existing and proposed modest telescopes,
                                     without waiting for “next generation” surveys.
                                    But this meteorite is S T R A N G E !
TC3 = Almahata Sitta = a Jumble!
 Paolo and others have shown how small asteroids and meteorites are
    produced by collisional disruption of their “parent bodies,” drift into
    resonances by Yarkovsky, pumped-up e’s then deliver them to Earth.
   Almahata Sitta was first thought to be an unusual ureilite.
   But the 3-meter wide F-type asteroid is only 2/3rd ureilite; 1/3rd consists
    of 5 different E chondrite lithologies, 2 H chondrites, and anomalous
    achondrites (e.g. Bischoff, Horstmann, et al. “LPSC 41” & “Meteoroids 2010” ).
   How did this conglomerate breccia come together in the asteroid belt?
    What would the spectrum of its parent asteroid look like? What held it
    together (spinning once every 97 sec!) on its way to Earth?
   Other processes, not yet understood, must be at work!
Non-Intuitive Processes on Small
Asteroids that May Yield Meteorites
 Classical/cartoon model: chips from
  solid rocky asteroids.
 1990s model: meteoroids dislodged by
  cratering events and catastrophic
  disruptions on “rubble pile” asteroids,
  drift by Yarkovsky Effect into orbital
  resonances, and are thereby converted
  into Earth-crossing orbits.
 Very recent alternative (or additional)
  modes: landslides and equatorial
  escape after spin-up of “rubble pile”
  near-Earth asteroids by YORP… or
  distortion/disruption by planetary tides
 Scheeres et al. (2010) propose that
  NEAs behave in microgravity with the
  non-intuitive physics that governs
  microscopic dust aggregates
Once Upon a Time: Collisions Ruled…
                          Now it’s mainly Sunlight and Tides

  Tidal Mass-           Interasteroidal collisions (both catastrophic
   Shedding              disruptions and frequent, small cratering events) were
                         invoked to explain everything that happened to
Following a sug-sug-     asteroids after early accretion and thermal
gestion by Nes-
              Nes-       processing: size distribution, spin rates and axis tilts,
vorny et al., Bin-
           al., Bin-
zel et al. (2010)
       al.               liberation and delivery of smaller asteroids and
show that tidal          meteorite fragments into resonances, asteroid
encounters with          satellite formation, regolith properties, etc.
Earth (perhaps
even very distant       Yarkovsky Effect (reintroduced for 3rd time in the 20th
ones) “freshen”          century by D. Rubincam in 1980s) shown by Farinella,
the colors of the        Vokrouhlicky, Bottke and others to cause meteoroids
space-weathered
space-                   from anywhere in inner half of main asteroid belt to
surfaces of NEAs.
               NEAs.     drift into resonances, which deliver them to Earth.
                        YORP Effect (resurrected from mid-20th century by D.
                         Rubincam in 1998) shown to be the major process
                         shaping the axial tilts and spin rates of smaller
                         asteroids. [Radzievskii 1954: “A mechanism for the disintegration of
                           asteroids and meteorites.”]
                        These two Yarkovsky Effects may dominate the
                           physical and dynamical behavior of smaller asteroids.
YORP Spin-Up, Binary Formation,
                                  and Mass Shedding…and Tides…
                                        Ostro et al. (2006)
                                        Ostro et al. (2006)
    Gravitational
    slope on KW4-α




   Arecibo radar data on NEA 66391 (1999 KW4; Ostro et al.), and                   How do Small
    analyses/modeling by Scheeres, Fahnestock, Walsh, Michel, Richardson, et      Asteroids Behave
    al. open a new paradigm for the evolution of small rubble piles:               in Microgravity?
   Asymmetric solar radiation spins some of them up, so mass moves to
    zero-G equatorial ridge, shedding mass, forming satellite/s, escape or
                                                                                  What happened
    reimpact of satellites, and escape of meteoroids into interplanetary space.   to Itokawa’s
                                                                                  dust? What are
   ~1/3 of NEAs are binaries, or have satellites or contact-binary shapes,       porosities of
    implying a common evolutionary track. An NEA may undergo generations          NEA’s? Are we
                                                                                  NEA’s?
    of satellite formation during its dynamical life in the inner solar system.   entering a
   No modeling has yet been done on meteoroid production rates, but this         microscopic
    could be a major source of meteorites. CRE ages may reflect such surficial    world writ large?
    landslide processes rather than impact-churned regolith processes.            Expect surprise!
K. Walsh, P. Michel & D. Richardson (2008)
K. Walsh, P. Michel & D. Richardson (2008)
Conclusions…

 Intuition from our one-Earth-
  gravity environment fails us
  for small solar system bodies
 They evolve in their physical
  traits very quickly…faster than
  we can understand
 We’ve known that we have
  asteroid pieces (the meteorites)
  for more than 2 centuries, yet we
  still don’t understand asteroidal
  parent bodies
 These are the kinds of puzzles
  Paolo would still be researching,
  were he still with us.
Example: Rosetta and (21) Lutetia
Lutetia/meteorite spectral comparisons
Lutetia/meteorite                                  Rosetta flies by 100 km Lutetia in July
                                                   Arguments abound about meteorite
                         Barucci et al. (2005)
                                                     analog/s for this M(W)-type asteroid
                                                         “M” is mnemonic for “metal” but
                                                          Rivkin (2000) showed that a subset of
                                                          M’s have a 3µm hydration band (‘Wet’)
                                                         Also, I suggested (1970s) that M-like
                                                          spectra might be enstatite chondrites
                                                   But Lutetia was selected as flyby
                                                    target because of arguments that it
                                                    may be a carbonaceous chondrite
                         Vernazza et al. (2009)    Relevant data include polarization,
                                                    visible and radar albedos, thermal IR
                                                    emission spectra, UV/visible/near-IR
                                                    reflectance spectra, mass+shape →
                                                    bulk density
                                                   Truth table → “wet” enstatite chondrite
                                                   Rosetta may yield ambiguous results:
                                                     We need a TC3-like-event for an M(W)!
Short-Term Warnings: Spaceguard Survey
                   does Better than We Thought!
 Was it a miracle that telescopes saw what was plausibly the largest NEA to
  impact Earth in 2008? No! Capability to see “final plungers” was overlooked.
 Analyses in the 1990s of the “Spaceguard Survey” only considered
  cataloging of near-Earth asteroids (NEAs); short-term warning was evaluated
  only for rare comets.
 Thus it was thought that there was only a tiny chance that a dangerous
  inbound 30-m NEA would be seen, let alone a 3-m “TC3”.
 Short-term hazard warning was evaluated (NASA SDT 2003) for the “next
  generation” surveys, but not for small NEAs and meteorite recovery.


                        “Consider a 30–40-m office-building-sized object striking
                        at 100 times the speed of a jetliner…. Even with the
                        proposed augmented Spaceguard Survey, it is unlikely
                        that such a small object would be discovered in advance;
                        impact would occur without warning.” – C. Chapman,
                        EPSL (2004).

                        “a short lead time for an NEO is extremely unlikely –
                        we can expect either decades of warning or none at
                        all” – Morrison, Harris, Sommer, Chapman & Carusi
                        (“Asteroids III” 2002)

N.18 chapman puzzling-attributes-of-small-asteroids

  • 1.
    Puzzling Attributes of Small Asteroids Clark R. Chapman Southwest Research Institute Boulder, Colorado, USA Pat Rawlings, SAIC Pat Rawlings, SAIC Session: “Planetary Science: Small Bodies, “Planetary Collisions, and Satellites I” I” International Workshop on Paolo Farinella (1953-2000): The Scientist and the Man (1953-2000): 11:50, 15 June 2010 University of Pisa, Italy
  • 2.
    Paolo Attacked Puzzles… I’ll Discuss a Few More:  Double asteroids don’t match double craters  Space weathering is very fast, yet very slow  2008 TC3 was a 3 meter jumble of meteorite types  NEAs in microgravity
  • 3.
    Doublet Craters: Historyof Topic  “Martian doublet craters,” V.R. Oberbeck & M. Aoyagi, J. Geophys. Res., 77, 2419 - 2432 (1972).  1978: Woronow inconclusively debated Oberbeck about whether spatial randomness was correctly modeled. Conclusion back then: Mars may or may not have an over-abundance of paired craters.  Topic resurrected in 1991 by Melosh & Stansberry who argued that 3 doublets on Earth must have been formed by impact of binary asteroids (this was before any asteroid satellites had been discovered).  Farinella & Chauvineau (1993): slow synchronized spinning binaries would be at correct separation for doublet craters; binaries might later separate or, more likely, coalesce into contact-binary configuration (common in radar delay-Doppler images of NEAs).  In 1990s, Melosh, Bottke, Cook, et al. re-examined Martian doublets and extended the analysis of doublets to Venus.  Dactyl was discovered and the tidally disrupted SL-9 comet impacted Jupiter, so doublet/multiple craters were analyzed in that context.
  • 4.
    Methods of FormingDoublets  Random impacts (unavoidable)  Very oblique impacts, ricochet (Messier, Messier A)  Endogenic crater formation (volcanoes, collapse pits, etc.)  Atmospheric break-up, explosion (Henbury)  Tidal break-up (Shoemaker-Levy 9)  Spatially clustered secondaries  Impact of binary asteroid or comet
  • 5.
    How to RecognizeDoublets  The certain way  Adjacent craters with same measured ages (Earth only)  Overlapping craters with shared walls (septum)  The very likely way  Adjacent craters with similar relative ages  Other unusual similarities indicating, e.g., same oblique impact angle  The statistical approach  Find a greater abundance of doublets than predicted by chance (doesn’t say which ones are the true doublets, unless the characteristics are very unusual)
  • 6.
    Observed Frequencies of Doublets on Several Planets  Earth  3 pairs among 28 craters > 20 km diameter; statistically significant because of very sparse crater densities on Earth and same ages  Mars  Melosh et al. (1996) studied 133 craters on northern plains, 5-100 km diam., and found 3 likely pairs with separations exceeding random expectations  2.3% doublets, less than on Earth and Venus  Venus  Cook, Melosh & Bottke (2003) found 2.2% of 10 to 150 km diameter craters were doublets, but that “splotches” (due to smaller impactors unable to penetrate the Venus atmosphere) imply ~14% doublets on Venus  Moon, Mercury, planetary satellites  I’ve found no definitive studies  But doublets exist (Moon; Mercury )
  • 7.
    NEA Binaries aretoo Close to Make Doublets Main Issue: Impacting NEAs form craters 10 – 20 times their own diameter. Most NEA pairs are so close that, even with favorable geometry, they form a single crater. How can there be so many doublet craters? Walsh Plot shows that typical  Separation can be larger (2009) separation of satellites and for oblique impacts binaries is about 4 times the  Separation of craters can radius of the primary. be zero if pair are un- Only 1 out of the sample of 35 favorably aligned, even if is separated widely enough widely separated (~15 times primary radius) to  Tidal forces can affect produce a double crater. separation ~15% of NEAs have satellites or are binaries so <0.5% of craters made by NEAs should Perihelion (AU) be visibly double.
  • 8.
    Space Weathering isFast… Or is it? (It is a Puzzle!) Binzel et al. (2010)  “Space weathering” is the process that transforms the spectral reflectance (colors and albedo) of the surface of an airless body by reddening and/or darkening it (mainly by solar wind; also micrometeorite impacts).  Vernazza et al. (2009) study dynamically very Walsh et al. (2008) Walsh et al. (2008) young family asteroids and find that most space weathering color changes occur in ~1 million yrs.  Following a suggestion of Nesvorny et al. (2005), Binzel et al. (2010) find that frequent, distant tidal encounters with Earth by NEAs produce color changes (tidal rejuvenation of surfaces?). Few NEAs (or MBAs) are Q’s. [Can YORP spin-up help?]  Yet bright crater rays persist for 100s of m.y.  Rays from Tycho crater on the Moon (~100 m.y. old) dominate the full Moon  Copernicus rays are still prominent after 800 m.y.  Mercury is periodically bombarded by solar wind, yet rays from large, infrequent craters are vivid.
  • 9.
    Catalina Sky Survey 2008 TC3: Linking an Asteroid to a Bolide to a Meteorite! TC3 Reflectance Spectrum: Wm. Herschel Telescope (Fitzsimmons, Hsieh, Duddy & Ramsay) TC3 Lightcurve (Clay Center Observatory) TC3 asteroid moving (W. Boschin, TNG) TC3 atmospheric train (M. Mahir)  2008 TC3 was the 1st NEA ever discovered (Catalina Sky Survey, 7 Oct. 2008) that was then predicted, for sure, to impact Earth. Telescopic observations were made before impact: lightcurve, reflectance spectrum.  19 h after discovery, impact occurred and was recorded over Sudan; ~700 paired meteorites (named Almahata Sitta) have been collected so far. Almahata Sitta fragment on the ground in Sudan (P. Jenniskens)  This first-ever event was not a fluke: we must expect future (maybe annual) predictions of meteorite strikes, from existing and proposed modest telescopes, without waiting for “next generation” surveys.  But this meteorite is S T R A N G E !
  • 10.
    TC3 = AlmahataSitta = a Jumble!  Paolo and others have shown how small asteroids and meteorites are produced by collisional disruption of their “parent bodies,” drift into resonances by Yarkovsky, pumped-up e’s then deliver them to Earth.  Almahata Sitta was first thought to be an unusual ureilite.  But the 3-meter wide F-type asteroid is only 2/3rd ureilite; 1/3rd consists of 5 different E chondrite lithologies, 2 H chondrites, and anomalous achondrites (e.g. Bischoff, Horstmann, et al. “LPSC 41” & “Meteoroids 2010” ).  How did this conglomerate breccia come together in the asteroid belt? What would the spectrum of its parent asteroid look like? What held it together (spinning once every 97 sec!) on its way to Earth?  Other processes, not yet understood, must be at work!
  • 11.
    Non-Intuitive Processes onSmall Asteroids that May Yield Meteorites  Classical/cartoon model: chips from solid rocky asteroids.  1990s model: meteoroids dislodged by cratering events and catastrophic disruptions on “rubble pile” asteroids, drift by Yarkovsky Effect into orbital resonances, and are thereby converted into Earth-crossing orbits.  Very recent alternative (or additional) modes: landslides and equatorial escape after spin-up of “rubble pile” near-Earth asteroids by YORP… or distortion/disruption by planetary tides  Scheeres et al. (2010) propose that NEAs behave in microgravity with the non-intuitive physics that governs microscopic dust aggregates
  • 12.
    Once Upon aTime: Collisions Ruled… Now it’s mainly Sunlight and Tides Tidal Mass-  Interasteroidal collisions (both catastrophic Shedding disruptions and frequent, small cratering events) were invoked to explain everything that happened to Following a sug-sug- asteroids after early accretion and thermal gestion by Nes- Nes- processing: size distribution, spin rates and axis tilts, vorny et al., Bin- al., Bin- zel et al. (2010) al. liberation and delivery of smaller asteroids and show that tidal meteorite fragments into resonances, asteroid encounters with satellite formation, regolith properties, etc. Earth (perhaps even very distant  Yarkovsky Effect (reintroduced for 3rd time in the 20th ones) “freshen” century by D. Rubincam in 1980s) shown by Farinella, the colors of the Vokrouhlicky, Bottke and others to cause meteoroids space-weathered space- from anywhere in inner half of main asteroid belt to surfaces of NEAs. NEAs. drift into resonances, which deliver them to Earth.  YORP Effect (resurrected from mid-20th century by D. Rubincam in 1998) shown to be the major process shaping the axial tilts and spin rates of smaller asteroids. [Radzievskii 1954: “A mechanism for the disintegration of asteroids and meteorites.”]  These two Yarkovsky Effects may dominate the physical and dynamical behavior of smaller asteroids.
  • 13.
    YORP Spin-Up, BinaryFormation, and Mass Shedding…and Tides… Ostro et al. (2006) Ostro et al. (2006) Gravitational slope on KW4-α  Arecibo radar data on NEA 66391 (1999 KW4; Ostro et al.), and How do Small analyses/modeling by Scheeres, Fahnestock, Walsh, Michel, Richardson, et Asteroids Behave al. open a new paradigm for the evolution of small rubble piles: in Microgravity?  Asymmetric solar radiation spins some of them up, so mass moves to zero-G equatorial ridge, shedding mass, forming satellite/s, escape or What happened reimpact of satellites, and escape of meteoroids into interplanetary space. to Itokawa’s dust? What are  ~1/3 of NEAs are binaries, or have satellites or contact-binary shapes, porosities of implying a common evolutionary track. An NEA may undergo generations NEA’s? Are we NEA’s? of satellite formation during its dynamical life in the inner solar system. entering a  No modeling has yet been done on meteoroid production rates, but this microscopic could be a major source of meteorites. CRE ages may reflect such surficial world writ large? landslide processes rather than impact-churned regolith processes. Expect surprise! K. Walsh, P. Michel & D. Richardson (2008) K. Walsh, P. Michel & D. Richardson (2008)
  • 14.
    Conclusions…  Intuition fromour one-Earth- gravity environment fails us for small solar system bodies  They evolve in their physical traits very quickly…faster than we can understand  We’ve known that we have asteroid pieces (the meteorites) for more than 2 centuries, yet we still don’t understand asteroidal parent bodies  These are the kinds of puzzles Paolo would still be researching, were he still with us.
  • 15.
    Example: Rosetta and(21) Lutetia Lutetia/meteorite spectral comparisons Lutetia/meteorite  Rosetta flies by 100 km Lutetia in July  Arguments abound about meteorite Barucci et al. (2005) analog/s for this M(W)-type asteroid  “M” is mnemonic for “metal” but Rivkin (2000) showed that a subset of M’s have a 3µm hydration band (‘Wet’)  Also, I suggested (1970s) that M-like spectra might be enstatite chondrites  But Lutetia was selected as flyby target because of arguments that it may be a carbonaceous chondrite Vernazza et al. (2009)  Relevant data include polarization, visible and radar albedos, thermal IR emission spectra, UV/visible/near-IR reflectance spectra, mass+shape → bulk density  Truth table → “wet” enstatite chondrite  Rosetta may yield ambiguous results: We need a TC3-like-event for an M(W)!
  • 16.
    Short-Term Warnings: SpaceguardSurvey does Better than We Thought!  Was it a miracle that telescopes saw what was plausibly the largest NEA to impact Earth in 2008? No! Capability to see “final plungers” was overlooked.  Analyses in the 1990s of the “Spaceguard Survey” only considered cataloging of near-Earth asteroids (NEAs); short-term warning was evaluated only for rare comets.  Thus it was thought that there was only a tiny chance that a dangerous inbound 30-m NEA would be seen, let alone a 3-m “TC3”.  Short-term hazard warning was evaluated (NASA SDT 2003) for the “next generation” surveys, but not for small NEAs and meteorite recovery. “Consider a 30–40-m office-building-sized object striking at 100 times the speed of a jetliner…. Even with the proposed augmented Spaceguard Survey, it is unlikely that such a small object would be discovered in advance; impact would occur without warning.” – C. Chapman, EPSL (2004). “a short lead time for an NEO is extremely unlikely – we can expect either decades of warning or none at all” – Morrison, Harris, Sommer, Chapman & Carusi (“Asteroids III” 2002)