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ACGRG5 Meeting Christchurch New Zealand 18 XII 2009
Measuring solar diameter with Baily beads: from Watts to Kaguya's lunar profiles Costantino Sigismondi, Mitsuru Soma, Dave Herald icra.it ACGRG5 Meeting Christchurch New Zealand 18 XII 2009
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Solar astronomy in Rome
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to Sapienza University
Capitol Observatory (until 1937) Leo XII in 1823 to Sapienza University Roma turrita, di Emma Amadei. Fratelli Palombi Editori, 1943, pag. 145.
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Ertel Meridian Circle (1853) for DRIFT-SCAN METHOD
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Dotted line: Capitol; continuous line data from Greenwich
Seeing influence From P.J.D. Gething, 1955 Greenwich observations of the horizontal and vertical diameters of the Sun MNRAS 115, 558.
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Annular eclipse of 1567 in Rome
relinquebatur in Sole circulus quidam exilis undique totam lunam ambiens (Annular) Clavius, Commentarium in Sphaeram, Roma 1581
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Contribution from D. Herald, Australia Occult 4 Baily’s Beads
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Contribution from M. Soma, Japan: Kaguya lunar probe Analysis of old and new data
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Method of Eclipses
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Lunar and Earth’s Orbital motions are precisely known e. g
Lunar and Earth’s Orbital motions are precisely known e.g. LLR, tropical year
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Lunar Limb: profiles accuracy
Chester Watts (1962) published the atlas of lunar limbs at all libration phases
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Digitized Watts Atlas
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Kaguya completed its mission this year: the crash looking for water
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Kaguya LALT Accuracy ± 1m, sampling each 1.5 to 10 km
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Observational strategy: Grazing Eclipse
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Geographical location
Referred to permanent landscape features GPS / Satellite image
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UTC timing Has to be precise (0.01 s) Has to be portable
(2 temperature calibrated quartz watches)
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Imaging the eclipse Naked eye (1567-1715-1925)
Video + high density filters Video + projection
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Signal to Noise ratio To determine the faintest bead or its limiting magnitude
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Sky background If the projection is not made in a camera obscura there are different background levels, ranging over more than 1000 in intensity Total eclipse, Egypt Zawyet al Mahtallah march 29, 2006 Southern Limit
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Sunset /Sunrise Ostia (Rome) September 5: horizon extinction
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High Clouds Roma, October 18
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Atmosphere extinction
Deviation starts at ~2° above horizon
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Solar Limb Darkening Function
From Rogerson, 1959
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+ + + Our equipment White Projection Screen
Camcorder and 2 quartz calibrated watches
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Our Measurements Spain, 2005 (clouded) Data from IOTA (2005-on)
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Egypt, 2006 published in Solar Phys 257, 237
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Corona at the shadow limit
Before totality (± 4 minutes of visibility at naked eye) Video dr. Fady Morcos Zawayet al Mahtallah
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At maximum eclipse At naked eye the irregular structure of the corona was well visible. Does exists a Circular Inner Corona?
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French Guyana, Sept. 2006 Eclipse at sunrise, high extinction and seeing 16 beads identified Preliminary ΔR= 0.04±0.04 arcsec
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And planetary transits?
Venus 1769: Discovery of Black Drop effect by Captain James Cook at Tahiti
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Explanation of Black drop
due to instrumental optical distortions
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Transit of Venus 2004, also Mercury 1999, 2003 and 2006
Chord method
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Solar Diameter measurement at Venus’ Transit in Hα
50 images (A. Ayomamitis, Athens, Greece) Internal contacts: 7 am ± 8 s (low Sun, high atmospheric turbulence) 1 pm ± 1 s D. Herald’s Occult4 software: ΔR=+0.34±0.38 arcseconds (in agreement with Neckel, So Phys 153, )
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publications Solar Physics 257, 237 (2009) Kilcik, Sigismondi, Rozelot and Guhl Analysis with Watts profile of 2006 total eclipse Synopsis of eclipse data historical and recent Diameter vs solar activity
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Real lunar limb vs Watts profile
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δR=-0.41” on 29 march 2006
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Solar Physics 258, 191 Sigismondi et al.
Atlas of Baily Beads Observational data from 25 observing stations; 600 beads Standard of blocking filters Limovie video analysis
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standard filter’s transmittance
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Video analysis with Limovie (Japan)
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Works in progress: at Locarno Observatory Switzerland
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DRIFT-SCAN Method: transits on fixed hourly circles
Transit timing is proportional to solar diameter Atmospheric seeing affects measurements Space data (eclipses and PICARD satellite) for calibration
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Diameter and seeing monitor
Time [1 frame] Quicktime 7.0 Window video setup
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The solar image drifts on the screen along this direction
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ρ”=15”·σ·cos(δ) Seeing formula
Without seeing the time intervals tn+1-tn are all equal. The standard deviation σ of time intervals is related to the seeing ρ by the formula ρ”=15”·σ·cos(δ) where δ is the solar declination
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Eclipses and PICARD (launch 15.2.2010) for absolute calibrations
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Perspectives Eclipses observations: international coordinated IOTA champaigns, collaboration with PICARD satellite Drift-scan with Seeing monitor at IRSOL Application of Kaguya profiles to old and new eclipses
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