Dec
13
Thu
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
11
Fri
âš« New Moon
Jan 11 @ 12:44 pm – 1:44 pm
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
26
Sat
⚪ Full Moon
Jan 26 @ 9:39 pm – 10:39 pm

January’s Full Moon is the “Old Moon”, “Wolf Moon”, “Ice Moon”, “Moon after Yule”, or “Paush Poornima”

Feb
10
Sun
âš« New Moon
Feb 10 @ 12:21 am – 1:21 am
Feb
11
Mon
Monthly Meeting @ George Mason University
Feb 11 @ 12:00 am – 2:00 am
Monthly Meeting @ George Mason University

Our next speaker is Eric Douglass and he will be speaking on Types of Observable Lunar Craters NOTE: This meeting will be held in the “Showcase Room” which is the meeting room at the base of the Research Hall Observatory instead of the normal location.

 

 

Feb
23
Sat
Mercury Retrograde Begins
Feb 23 all-day

see http://cantonbecker.com/retrograde for details…