Dec
13
Thu
Geminids Meteor Shower
Dec 13 all-day

Geminids
The final major meteor shower of every year (unless one surprises us!) is always the December Geminid shower, often producing 50 or more meteors per hour. It is a beloved shower, because, as a general rule, it’s either the August Perseids or the December Geminids that give us the most prolific display of the year. Best of all, the new moon guarantees a dark sky on the peak night of the Geminid shower (mid-evening December 13 until dawn December 14). But the nights on either side of the peak date should be good as well. Unlike many meteor showers, you can start watching the Geminids by 9 or 10 p.m. local time. The peak might be around 2 a.m. local time on these nights, because that’s when the shower’s radiant point is highest in the sky as seen around the world. With no moon to ruin the show, 2012 presents a most favorable year for watching the grand finale of the meteor showers. Best viewing of the Geminids will probably be from about 1 a.m. to 3 a.m. on December 14.

âš« New Moon
Dec 13 @ 1:42 am – 2:42 am
Dec
21
Fri
Winter Solstice
Dec 21 @ 6:12 am – 7:12 am

The winter solstice is the shortest day of the year, respectively, in the sense that the length of time elapsed between sunrise and sunset on this day is a minimum for the year. Of course, daylight saving time means that the first Sunday in April has 23 hours and the last Sunday in October has 25 hours, but these human meddlings with the calendar and do not correspond to the actual number of daylight hours.

http://scienceworld.wolfram.com/astronomy/WinterSolstice.html

Dec
28
Fri
⚪ Full Moon
Dec 28 @ 3:21 am – 4:21 am
Jan
3
Thu
Quadrantids Meteor Shower
Jan 3 all-day

Don’t Miss This! In 2013, this is the only one of six major (and predictable) meteor showers that won’t be significantly washed out by a bright moon. Look for meteors radiating from the constellation Bootes. The Quadrantid meteor shower will reach its maximum rate of activity. Some meteors will be visible each night from 1 Jan to 6 Jan, but the best show will be on this evening. The maximum number of meteors expected to be visible from a dark location is around 80 per hour (ZHR). The Moon will be 22 days old at the time of peak activity, and so will present minimal interference.

Jan
5
Sat
Great Meadow Public Night @ Great Meadow
Jan 5 @ 11:30 pm – Jan 6 @ 4:00 am
Jan
11
Fri
âš« New Moon
Jan 11 @ 12:44 pm – 1:44 pm
Jan
12
Sat
Cancelled – C.M. Crockett Public Night @ C.M. Crockett
Jan 12 @ 11:00 pm – Jan 13 @ 4:00 am

 

NOVAC’s C.M. Crockett Site Page

 

Jan
14
Mon
Monthly Meeting @ George Mason University
Jan 14 @ 12:00 am – 2:00 am

Our next speaker is Gideon Bass and he will be speaking on Kepler Studies of Low-Mass Eclipsing

Summary of Upcoming Lecture

KIC 6131659 is a long-period (17.5 days) eclipsing binary discovered by the Kepler mission.  We analyzed six quarters of Kepler data along with supporting ground-based photometric and spectroscopic data to obtain accurate values for the mass and radius of both stars, namely M1=0.922 ± 0.007Msun, R1=0.8800 ± 0.0028Rsun, and M2=0.685 ± 0.005Msun, R2=0.6395 ± 0.0061Rsun.  There is a well-known issue with low mass (M <<0.8Msun) stars (in cases where the mass and radius measurement uncertainties are smaller than two or three percent) where the measured radii are almost always 5 to 15 percent larger than expected from evolutionary models, i.e. the measured radii are all above the model isochrones in a mass-radius plane.  In contrast, the two stars in KIC 6131659 were found to sit on the same theoretical isochrone in the mass-radius plane.  Until recently, all of the well-studied eclipsing binaries with low-mass stars had periods less than about three days.  The stars in such systems may have been inflated by high levels of stellar activity induced by tidal effects in these close binaries.  KIC 6131659 shows essentially no evidence of enhanced stellar activity, and our measurements support the hypothesis that the unusual mass-radius relationship observed in most low-mass stars is influenced by strong magnetic activity created by the rapid rotation of the stars in tidally-locked, short-period systems.  Finally, using short cadence data, we show that KIC 6131657 has one of the smallest measured non-zero eccentricities of a binary with two main sequence stars, where e cos ω = (4.57 ± 0.02) × 10-5.

 

Jan
19
Sat
Join NASA for a Star Party @ David M. Brown Planetarium
Jan 19 @ 10:30 pm – Jan 20 @ 2:30 am

Join NASA for a Star Party at the David. M. Brown Planetarium. They are looking for NOVAC to bring there scopes if you want to help out.