Saturday, May 2, 2015



Diagram of comet C/2014 Q2 (Lovejoy) for May 1, 2015 at 21:00 UT. This is based on image posted by Fritz Helmut Hemmerich on Facebook

In this diagram North is up and east is left. Position angles are measured from north counterclockwise.

The comet displays a radial dust fan tail, an ion tail, and large coma with light reflected by dust plus gas emission from CN and C2 Swan bands which give the coma the characteristic blue green glow. The ion tail points away from the sun and this fact makes it simple to rotate a comet image to align with calculated position angle of extended sun-comet radius vector or the parameter PsAng in JPL Horizons ephemeris. The dust fan is short in length because of the small plane angle between earth and the comet plane (22 degrees). and small sun-comet-earth phase angle (29 degrees). If the earth was directly above or below the comet, we would be able to see the full extent of its dust and ion tails. Instead we see an approximate sin theta projection. The plane angle will continue to decrease and reach zero on June 27, 2015 when the earth passes through the comet orbit plane. At that time, the comet's tails and trail if it can be seen will be edge on, the dust tail will be thicker than a trail. The tail/trail could wrap around and appear to be emating from the comet head as an apparent anti tail, depending on the viewing geometry. A trail consists of larger dust particles which are affected the least by solar radiation pressure. The dust tail shows that there is a wide range of dust particle sizes. The affect of solar radiation pressure on dust particles is inversely proportional to particle radius. That may seem counter intuitive since small particles have smaller cross sectional area. In the fan, the largest particles lie closest to the position angle of the negative velocity vector or parameter PsAMV. The smaller particles curve away from the anti solar direction in the sky. This is difficult to understand and may seem counter intuitive when the position angles of the -v vector (PsAMV) and anti solar radius vector (PsAng) are so far apart. A Finson-Probstein analyis or model could be fit to comet images to show these characteristics.

The green glow from C2 emission has been diminishing and is expected to fade when the comet recedes from the sun beyond 2 AU. This comet was 1.858 AU from the sun on date/time of observation image. CN emission will decrease and is not expected beyond 3 AU. In SOHO/Swan images, the comet's hydrogen coma has decreased in size but still visible. SWAN images capture Lyman-alpha hydrogen emission in the far ultraviolet at 121.6 nm wavelength. That is emission from the first excited state of hydrogen atoms predicted by Quantum Mechanics over a 100 years ago and very well understood in physics today. You have to have a spacecraft above earth atmosphere to see that deep into far ultraviolet spectrum. The SOHO spacecraft is in a halo orbit about the earth-sun L1 Lagrangian point.

Thursday, April 30, 2015

Comet C/2013 US10 (Catalina) Development


Charles Bell, Neil Norman, and Taras Prystavski  (April 30, 2015)

There is a report on comets-ml by Paul Camilleri, Warners Bay Australia, that comet C/2013 US10 (Catalina)  shows no enhancement with a Swan filter. That is what I expect at the comet's current heliocentric distance, 3.142 AU.  C2 generally starts to show emission when a comet reaches 2 AU (or July 30, 2015 for C/2013 US10 (Catalina)). If we could see CN emission at at 3880 Å or 388 nm, we should start to pick it up as the comet passes inward at 3 AU (or May 11, 2015 for C/2013 US10 (Catalina)). The lower end of the visible spectrum is 3900  Å or 390 nm.

Lack of SWAN filter enhancement to me does not mean lack of gas but lack of sufficient gas emission. Gas emission and in particular SWAN band or C2 emission is not yet apparent.

The solar UV flux at the comet's heliocentric distance is not yet sufficient to produce photo dissociation of the parent molecular species of C2 and cause sufficient photon excitation and emission with the common blue green glow we associate with comets.  Theoretically it is the energy of a UV photon that does all these interactions. Flux is different, in that it is the number of photons passing through a unit area with time. As comets approach perihelion, the solar UV flux increases inversely proportional to r squared

We are currently seeing reflected sunlight from dust emitted by this comet. The light reflected may be slightly reddened. The light we see should have nearly the same color indices as sunlight. Photometrically that means the values of B-V, V-R, should be close to standard values of sunlight.  The Johnson V band filter is centered on the C2 emission band at 515 nm wavelength.  Use of such filters have in the past been used to detect gas emission.

Solar color indices:
(B-V) 0.65 
(V-R) 0.35 
(R-I) 0.28
See Section 4.4 in The Sizes, Shapes, Albedos, and Colors of Cometary Nuclei by Philippe L. Lamy, Imre Toth, Yanga R. Fernández, Harold A. Weaver in Comets II

Dust is lifted from the nucleus of the comet by lifting forces as volatile solids sublimate to gaseous phase. There has to be gas flow to cause the drag force to lift the dust.
Comet Spectra by C. Arpigny in Comets: Scientific data and missionsKuiper, G. P. [editor] (Arizona Univ.; Tucson, AZ, United States);Roemer, E. [editor] (Arizona Univ.; Tucson, AZ, United States)Abstract: Proceedings of conference on comets, University of Arizona - Apr. 1970 Publication Date: Jul 01, 1972 NASA-CR-129110; LC-72-619613  Distribution Limits: Unclassified; Publicly available; Unlimited

Wednesday, April 29, 2015

Fluffy dust grains from comet 67P/Churyumov-Gerasimenko

Fluffy dust grains gathered by the ESA Rosetta spacecraft COSIMA instrument from comet 67P/Churyumov-Gerasimenko between October 25 -31, 2014 when the comet was between 3.113 and 3.074 AU from the sun and before the comet was predicted to shed its dusty mantle. Dust particle "a" on the left crumbled into a rubble pile when collected. Dust particle "b" on the right shattered. Each particle is shown with two illumination views which project different shadow lengths becuase of their size.

During the comet's 2008 return, the comet's dust production doubled when it was between 2.7 and 2.5 AU from the Sun (July 2008), indicating that this was when the nucleus shed its mantle. The authors of a paper in Nature publised on in Feb 2015 suggests that these particles are agglomerates of entities in the size range of interplanetary dust particles and probably represent parent material of interplanetary dust particles.

Reference:
Schulz, Rita; Hilchenbach, Martin; Langevin, Yves; Kissel, Jochen; Silen, Johan; Briois, Christelle; Engrand, Cecile; Hornung, Klaus; Baklouti, Donia; Bardyn, Anaïs; Cottin, Hervé; Fischer, Henning; Fray, Nicolas; Godard, Marie; Lehto, Harry; Le Roy, Léna; Merouane, Sihane; Orthous-Daunay, François-Régis; Paquette, John; Rynö, Jouni; Siljeström, Sandra; Stenzel, Oliver; Thirkell, Laurent; Varmuza, Kurt; Zaprudin, Boris, Comet 67P/Churyumov-Gerasimenko sheds dust coat accumulated over the past four years (02/2015), Nature, Volume 518, Issue 7538, pp. 216-218
http://adsabs.harvard.edu/abs/2015Natur.518..216S

Image credit: ESA/Rosetta/MPS for COSIMA Team MPS / CSNSM / UNIBW / TUORLA / IWF/ IAS / ESA BUW / MPE / LPC2E / LCM / FMI / UTU / LISA / UOFC / vH&S
http://www.esa.int/spaceinimages/Images/2015/01/Fluffy_dust_grains

Thursday, April 2, 2015

Heliocentric magnitude of comet C/2014 Q2 (Lovejoy)

Comet C/2014 Q2 (Lovejoy) Heliocentric magnitude versus log r 

This plot of the heliocentric magnitude versus log r shows that a large difference in the brightening of comet C/2014 Q2 (Lovejoy) pre perihelion compared to post perihelion The comet is expected to fade at a slower rate departing the sun than it brightened as it approached the sun. The general shape of this plot is similar to the plot of logarithmic slope of Afrho. R band photometry data from the Cometas-Obs group observers was reduced and normalized to zero phase by the relation:

mH = m - 5 log delta + 2.5 log phi
mH is heliocentric magnitude
m is R band magnitude at aperture of 10,000 km
where delta is earth distance
2.5 log phi is magnitude of the phase function


Thanks to the following observers for their data contributions who are credited as follows: 213 Montcabrer, Ramon Naves y Montse Campas; 232 Masquefa, Esteban Reina; 939 Rodeno, Julio Castellano; A02 Cal Maciarol Mòdul 8, Josep Lluís Salto; A06 Mataro, Esteve Cortés y Fernando García; B20 Observatori Carmelità, Josep María Aymamí; B74 Santa Maria de Montmagastrell, Josep María Bosch; B96 Brixiis Observatory, Erik Bryssinck; C23 Olmen, Alfons Diepvens; C35 Terrassa, José Aledo; C86 Blanes, Josep Gaitan; C90 Vinyols, Luís Tremosa; D90 GRAS - Moorook observatory; G39 ROAD, San Pedro de Atacama; G68 Sierra Stars Observatory, Markleeville; H06 GRAS remote telescope; H47 Vicksburg, Charles Bell; I72 Carpe-Noctem, José Luís Martín Velasco; I88 Fuensanta, José Carrillo; I99 Blanquita, Fernando Limón; J01 Cielo Profundo, Juan José González Díaz; J24 Altamira, José Francisco Hernández; J38 Faustino García Cuesta; J67 La Puebla de Vallbona, Enrique Arce; K14 Sencelles, Mario Morales; Q62 Siding Spring; V03 Carlos Labordena Barceló; X18 CArlos Perelló; Z73 Nuevos Horizontes, Jesús Delgado y Josefa Peña; Z74 Francisco Soldán; Z77 Osuna, José María Fernández

References:

A’Hearn M.F., Schleicher D.G., Feldman P.D., Millis R.L., and Thompson D.T., 1984. Comet
Bowell 1980b. The Astronomical Journal 89:579-591.

Blaauw, Rhiannon C.; Suggs, Robert M.; Cooke, William J., Dust Production of Comet 21P/Giacobini-Zinner using Broadband Photometry, Meteoritics & Planetary Science, Volume 49, Issue 1, pp. 45-51 (2014)

Marcus J.N. 2007. Forward-Scattering Enhancement of Comet Brightness. II. The Light Curve of
C/2006 P1. International Comet Quarterly 29:119-130.

Raab, H., 2005, Astrometrica Software, Shareware for research grade CCD photometry: http://www.astrometrica.at/

Roig, J.C., Nogues, R.N., Lorenz, E.S., & Gonzalez, J.L.S., 2011. Fotometrica Con Astrometrica, a software tool: http://www.astrosurf.com/cometas-obs/

Schleicher, D. , Composite Dust Phase Function for Comets (2010 May)

Wednesday, April 1, 2015

Comet C/2014 Q2 (Lovejoy)  Ion and Dust Tail Image credit: NASA/JPL-Caltech
Comet C/2014 Q2 (Lovejoy) imaged in the infrared by the NEOWISE spacecraft on January 30, 2015 when the comet was at perihelion at solar distance of 1.29 AU.

Blue = 3.4-micron wavelength (infrared)
Orange = 4.6-micron wavelength. (infrared)

Image has been rotated so that position angle of ion tail matches JPL Horizons position angle of the sun-comet extended radius vector = 72.2 degrees. North is up and east is left. In the infrared, the comet's dust tail can be seen as indicated and expected between PsAng and PsAMV.

2015-Jan-30
delta = 0.73 AU
r = q = 1.29 AU
Phase = 49.4 deg
PsAng = 72.2 deg
PsAMV = 156.732
Image credit: NASA/JPL-Caltech

Logarithmic slope of Afrho and Dust production of comet C/2014 Q2 (Lovejoy) pre and post perihelion

Comet C/2014 Q2 (Lovejoy)  Logarithmic slope pre and post perihelion

Dust production of comet C/2014 Q2 followed a logarithmic slope (gamma ) of 4.695 with respect to heliocentric distance prior to perihelion. After perihelion the logarithmic slope changed and is smaller. I expect  that with additional data points post perihelion value of logarithmic slope will be better determined.  
The logarithmic slope can be used to estimate value at perihelion as was done on comet comet 21P/Giacobini-Zinner for a study to better constrain mete
or stream forecasts for the Draconids. (Blaauw, Suggs, and Cooke 2012) This study found a similar value of logarithmic slope for comet 21P. They note that a post perihelion value of logarithmic slope for 21P by Pittichova et. al, 2008 was also less. This reduction in the logarithmic slope post perihelion is also evident in photometry results. To determine logarithmic slope, Afrho measures need to be normalized to zero phase by dividing by the phase function. I used Dave Schleicher's phase function. I 
Thanks to the following observers for their data contributions who are credited as follows: 213 Montcabrer, Ramon Naves y Montse Campas; 232 Masquefa, Esteban Reina; 939 Rodeno, Julio Castellano; A02 Cal Maciarol Mòdul 8, Josep Lluís Salto; A06 Mataro, Esteve Cortés y Fernando García; B20 Observatori Carmelità, Josep María Aymamí; B74 Santa Maria de Montmagastrell, Josep María Bosch; B96 Brixiis Observatory, Erik Bryssinck; C23 Olmen, Alfons Diepvens; C35 Terrassa, José Aledo; C86 Blanes, Josep Gaitan; C90 Vinyols, Luís Tremosa; D90 GRAS - Moorook observatory; G39 ROAD, San Pedro de Atacama; G68 Sierra Stars Observatory, Markleeville; H06 GRAS remote telescope; H47 Vicksburg, Charles Bell; I72 Carpe-Noctem, José Luís Martín Velasco; I88 Fuensanta, José Carrillo; I99 Blanquita, Fernando Limón; J01 Cielo Profundo, Juan José González Díaz; J24 Altamira, José Francisco Hernández; J38 Faustino García Cuesta; J67 La Puebla de Vallbona, Enrique Arce; K14 Sencelles, Mario Morales; Q62 Siding Spring; V03 Carlos Labordena Barceló; X18 CArlos Perelló; Z73 Nuevos Horizontes, Jesús Delgado y Josefa Peña; Z74 Francisco Soldán; Z77 Osuna, José María Fernández

References:
Dust Production of Comet 21P/Giacobini-Zinner using Broadband Photometry by Rhiannon C. Blauuw, Robert M. Suggs and William J. Cooke, Meteoritics & Planetary Science 49, Nr 1, 45–51 (2014)
Blauuw- Dynetics Technical Services/MITS Huntsville, AL 35812
Suggs and Cooke - Meteoroid Environment Office/EV44/NASA Mar shall Space Flight Center, Huntsville, AL

The paper by Blauuw, Suggs and Cooke, who work at NASA Marshall Space Center, is open access in the public domain on the NASA technical report server at the following link;
http://ntrs.nasa.gov/…/n…/casi.ntrs.nasa.gov/20130013031.pdf