NOVEMBER NEWSLETTER 2008
INDEX: MEETINGS, OTHER NEWS, CONTACTS
MEETINGS OCTOBER MEETING
The October meeting was introduced
by our Chairman, John Vale-Taylor who explained that this month we were viewing
two lectures from an astronomical course as an introduction to Einstein’s
Theories of Relativity.
We would like to thank Alex and
Cameron Brown for providing a laptop to replay the DVD at short notice after
we developed an unexpected problem.
Astro Lectures
Einstein’s General Theory of
Relativity
In the first video,
We were introduced to the idea of General Relativity and how time and space in
reality are not linear when in the vicinity of gravitational fields, messing
up the measurement of time and distances.
To begin the video talk, the lecturer
talked about Newton’s laws of gravity and how they had served well for
three hundred years but then Einstein believed that Newton’s laws begin
to break down when speeds approach that of light.
Einstein claimed that acceleration
produced the same effect on a body as uniform gravity did and using the idea
of a man in a windowless elevator when looking at a torch shining light horizontally
across the elevator he would see the light bend if they were accelerating close
to the speed of light. Einstein postulated that the same effect would
occur if instead of accelerating, a source of gravity appeared beneath the
elevator. The man could not tell the difference.
This effect of warping space was
likened to an ant walking in a straight line across a flat rubber sheet. Placing
a weight in the centre of this sheet would cause it to distort and now the
ant would take a very different path if trying to walk in a straight line. If
the sheet was considered to be time and space coordinates then their distortion
would suggest the bending of time and space.
In this analogy, the two dimensional
sheet would be distorted, not by the earth’s gravity but by some fourth
dimensional effect that man cannot visualise.
In 1919 Arthur Eddington observed
an eclipse of the Sun and during total darkness measured the position of certain
stars close to the Sun as they became visible. He found that their position
had been affected by the Sun’s gravity. (Today radio astronomy
is used to measure the Sun’s gravitational effect during daylight) The
displacement was in line with Einstein’s predictions.
An interesting experiment took place
in 1963 in the Jefferson Tower at Harvard University. A source of iron
Fe 57 was placed at the bottom and radiated gamma rays at a precise wavelength. This
was to be detected by an absorber at the top of the tower, but because of gravity,
the rays were red shifted and so were not absorbed. By blue shifting
the source by a calculated amount, the radiation was then able to be absorbed,
so suggesting that Einstein was correct.
The experiment was carried out with
the source at the top of the tower. This time the gamma rays were blue
shifted and so by red shifting the source the wavelength was brought back so
that it was again absorbed.
Finally in this lecture, the lecturer
described how the atomic clocks aboard the Global Position Satellites (GPS)
had to be corrected by calculated amounts to correct for their speed and the
effects of gravity. Without these very tiny corrections, errors of many
kilometres would appear on Earth.
Warping of Space and Time
In the second video we looked more
closely at the importance of correcting for errors in GPS navigation. Special
Relativity, which states that the speed of light is relatively the same whatever
speed one is travelling at, causes the clocks in the GPS satellites to run
7 micro-seconds fast, whilst General Relativity, which states that gravity
warps space, causes the clocks to run slower by 43 micro-seconds. So
the clocks have to be compensated for by correcting them by 38 micro-seconds.
Since light travels by about a foot
in a billionth of a second, in just a day, the GPS would create an error of
several miles and be useless without the precise correction.
The lecturer noted that this was
the most obvious result of both the Special and General theories of Relativity.
Looking again at the General Theory
of Relativity, we looked at the precession of two orbiting pulsars whose orbits
are very elliptical. The warping of space and time meant that the point
of aphelion precessed during time, but because the effect of gravity precession
appeared at a different rate expected and could only be accounted for by applying
the theory of general relativity.
Gravity waves are being radiated
by the orbiting pair and this takes energy out of the system, therefore as
time passes, the pair’s orbit speeds up and the distance of the pulsars’ orbit
has been calculated to be reducing by about 7 millimetres a year.
This means that the precession is
also changing and the angle at which it is speeding up can only be accounted
for by general relativity.
The video then led the discussion
to the effect of gravity on the path of light, using the effect of a star’s
gravity to bend light from a distant quasar that is in line but behind the
star. This causes the light to curve. Many examples have been photographed
in many parts of the sky. The effect is called gravitational lensing.
If the quasar is precisely in line
behind the star, then a ring is seen around the star. This is called
an Einstein Ring because Einstein had predicted the effect, although he never
thought it would ever be seen.
Another effect is called micro-lensing
where the gravity of a star “focuses” the light from a more distant
star behind it, producing a brightening as the two come into line. In
fact quite recently a star was seen to produce this brightening and then shortly
afterwards there was another short burst. This was caused by a newly
discovered huge planet orbiting the nearer star.
These are just some of the ways in which the
predicted effects have helped to confirm the theories of both General and Special
Relativity.
NOVEMBER MEETING
Wednesday 19th November 2008 During our meeting, we will be having a talk by John Murrell who is a very active member of the Croydon Astronomical Society. His talk is on “Gamma Ray Bursts”. These are the most luminous electromagnetic events occurring in space since the Big Bang.
The meeting begins at 1930 although members are invited to arrive anytime after 1900 as this is a good time to exchange ideas and discuss problems.
The venue as always is in the Upper Room of the Methodist Church at the east end of Wadhurst Lower High Street, opposite the entrance to Uplands College. (For those with SatNav – the post code is TN5 6AX)
FUTURE MEETINGS
Wednesday 10th December 2008. Please note that as it is December, the Society meets on the Second Wednesday instead of the third as in other months.
Paul Treadaway, who is a well known member of the Society gives a talk about “How Stars Work”.
Members will remember the talk Paul gave us last year and will recall the intriguing scenarios he posed.
Christmas is with us at the end of the month so there will be plenty of mince pies to be eaten during the meeting.
Wednesday 21st January 2009 This is the Annual General Meeting. That should not take too long and then Phil Berry gives a fascinating talk, bringing us up to date with the impressive progress he has achieved with his observatory following on from his previous talk earlier in the year. This time Phil calls his talk “The Further Trials and Tribulations of an Amateur Astronomer”.
OTHER NEWS AND INFORMATION
WEB-SITE WINS SAGAS PRAISE
SAGAS, the Southern Area Group of Astronomical Societies, have awarded our web-site, administered by Michael Harte with a top score of 5 stars for promoting and providing links to the SAGAS website. Only one other group managed the full score.
Congratulations to Michael.
SKY NOTES FOR NOVEMBER
Planets
Mercury will be visible as a morning object for the early part of the month when it rises about one hour before the Sun. It is at superior conjunction on the 25th when it is around the far side of the Sun.
Venus is brightening as an evening object in the south west. By the middle of the month it will be at magnitude -4.0 when it will set two hours after the Sun.
Mars is not suitably placed for observation this month.
Jupiter is still in Sagittarius and low down in the south at magnitude -2.0. It becomes more difficult to observe during November despite setting two and a half hours after the Sun by the end of the month.
Saturn is a morning object at magnitude 1.1 rising some six hours ahead of the Sun by mid-month (that’s just after 01.00) so it will soon be an evening object. The ring system is moving towards an edge-on view as seen from Earth, which will occur during September 2009. Because of this Saturn’s satellite Titan will be visible in transit across the face of the planet and will also be seen to be occulted.
Lunar Occultations
On the evening of November 13th
the Moon’s passage across the sky takes it once again “through” the
Pleiades star cluster. On the down side the Moon is just past full but on the
plus side there are some bright re-appearances to see. The brightest is Alcyone
at magnitude 2.8 which might be observed to disappear at the bright limb first.
Next year Alcyone will be the subject of a graze occultation visible from the
south east of England.
As usual in the table I’ve
only included events for stars down to around magnitude 7.5 that occur before
midnight. DD = disappearance at the dark limb, DB = disappearance
at the bright limb and RD = re-appearance at the dark
limb. Although there are many re-appearances, only the very brightest are included
here.
Times are all GMT.
| Nov | Time |
Star |
Magnitude | Ph |
PAo |
| 2nd | 18:11 |
SAO 186505 |
7.2 |
DD |
95 |
| 3rd | 18:59 |
SAO 187710 |
7.4 |
DD |
84 |
| 4th | 17:35 |
SAO 188737 |
7.6 |
DD |
72 |
| 4th | 20:42 |
SAO 188829 |
6.0 |
DD |
119 |
| 5th | 16.27 |
SAO 163833 |
7.4 |
DD |
27 |
| 5th | 18.10 |
SAO 163869 |
7.6 |
DD |
130 |
| 6th | 21.21 |
SAO 164548 |
7.3 |
DD |
82 |
| 8th | 21.42 |
SAO 146580 |
7.2 |
DD |
111 |
| 9th | 18.15 |
SAO 128489 |
7.2 |
DD |
11 |
| 9th | 18.17 |
SAO 128494 |
7.6 |
DD |
28 |
| 9th | 18.23 |
SAO 128492 |
7.6 |
DD |
2 |
| 11th | 16.30 |
SAO 92556 |
6.7 |
DD |
117 |
| 12th | 18.29 |
Mu Arietis |
5.7 |
DD |
101 |
| 13th | 19.05 |
Electra |
3.7 |
RD |
293 |
| 13th | 19.12 |
Alcyone |
2.8 |
DB |
2.8 |
| 13th | 19.37 |
Merope |
4.1 |
RD |
236 |
| 13th | 20.09 |
Alcyone |
2.8 |
RD |
249 |
| 13th | 20.39 |
Atlas |
3.6 |
RD |
211 |
| 13th | 20.47 |
Pleione |
5.1 |
RD |
230 |
| 15th | 18.48 |
139 Tauri |
4.8 |
RD |
243 |
Phases of the Moon for November
| New | First Quarter | Full | Last Qaurter |
| 27th | 6th | 13th | 19th |
Meteors
The Taurids.
The Taurid meteor shower comes to maximum on the 3rd of this month and although
the ZHR (zenithal hourly rate) is only 10 there are usually a high proportion
of bright and slow meteors plus some fireballs. The maximum is known to be
rather flat and extended unlike showers such as the Leonids or Perseids that
show a sudden but brief period of increased activity. In 2005 the Taurids
displayed unusually high activity and it is suggested that this could be
repeated again this year. This shower which is known to have a double radiant
in Taurus is associated with the comet 2P/Encke. It is well worth observing
partly because the crescent Moon will be out of the way, having set before
20.00 on the night of maximum, and also because there is a chance of seeing
something rather special.
The Leonids.
The Leonid meteor shower is active from November 15th to the 20th with maximum
occurring on the 17th. Unfortunately a gibbous Moon will interfere with a
ZHR of around 20 at maximum. The radiant does not rise until 23.00 which
is only a few hours after the Moon. In the past this shower has seen some
spectacular outbursts but unfortunately the predictions from those who model
the shower’s activity suggest that this year will not be one of them.
ISS
There are a large number of passes of the ISS this month as seen from Wadhurst
but many are low in the sky or occur in the early hours of the morning. I
have only included those that are the brightest, attain reasonable altitude
and occur before midnight. The information given is for when the ISS is at maximum
altitude, so it is best to look some minutes before this time. Full
details of all passes can be found at: - www.heavens-above.com
Times are all GMT.
| November | Time | Magnitude | Altitude | Azimuth |
23rd |
18.16 |
-0.9 |
32 |
SSW |
24th |
17.07 |
-0.6 |
22 |
SSE |
25th |
17.32 |
-1.7 |
45 |
SSE |
26th |
17.58 |
-2.4 |
81 |
SSE |
27th |
16.48 |
-1.7 |
48 |
SSE |
27th |
18.22 |
-0.9 |
38 |
W |
28th |
17.13 |
-2.4 |
83 |
SSE |
29th |
17.39 |
-2.4 |
77 |
N |
30th |
18.04 |
-2.1 |
68 |
WNW |
Iridium Flares
I thought I would include a few of these events because although they are of
no scientific value, they can be quite spectacular with the very brightest
reaching beyond magnitude -8. They are caused when an Iridium satellite briefly
reflects sunlight from one of its 3 antennae onto a small area of the Earth’s
surface. The name “Iridium” was used because there were originally
going to be 77 of them (forming a communications network to cover the globe)
and Iridium has the atomic number 77 in the periodic table. The predictions
are specifically for the Wadhurst area because although the time, altitude
and azimuth elements change very little (compared with my home in Hildenborough
for example) the magnitude of the flare can vary considerably. I’ve
only included the brightest and most easily visible – a full list is
available at:
www.heavens-above.com
It is possible to see flares in daylight if you know exactly where to look
for them.
| November | Time | Magnitude | Altitude | Azimuth |
2nd |
17.39 |
-4 |
42 |
S |
3rd |
17.33 |
-4 |
41 |
S |
7th |
17.18 |
-6 |
37 |
S |
9th |
18.42 |
-5 |
40 |
SE |
14th |
18.21 |
-6 |
40 |
SSE |
18th |
18.06 |
-8 |
39 |
SSE |
19th |
18.00 |
-7 |
38 |
SSE |
25th |
17.36 |
-5 |
35 |
S |
27th |
17.30 |
-4 |
32 |
S |
Advance Warning for December
Lunar Occultation of Venus
In the afternoon of December 1st Venus will be occulted by the dark limb of
a thin crescent Moon and will later emerge on the bright limb. The disappearance
should be a fairly easy event as Venus will be at magnitude -4.1 and the
Sun will be setting around the time that the planet is occulted. One thing
to bear in mind is that the Moon will be quite low in the sky (only 14° high
at disappearance) so a good south western horizon is required.
| December | Object | Time | Phase |
1st |
Venus |
15.47 |
DD |
1st |
Venus |
17.17 |
RB |
Meteors
The Geminid meteor shower reaches maximum on December 13th although moonlight
will interfere.
The Ursid meteor shower reaches maximum on December 20th but is more favourable
as the Moon is between last quarter and new and doesn’t rise until 03.20
NASA SPACE PLACE
The Chemical Weather Report
“Sunny tomorrow with highs
in the mid-70s. There’s going to be some carbon monoxide blowing in from
forest fires, and all that sunshine is predicted to bring a surge in ground-level
ozone by afternoon. Old and young people and anyone with lung conditions are
advised to stay indoors between 3 and 5 p.m.”
Whoever heard of a weather report
like that?
Get used to it. Weather reports
of the future are going to tell you a lot more about the atmosphere than just
how warm and rainy it is. In the same way that satellite observations
of Earth revolutionized basic weather forecasting in the 1970s and 80s, satellite
tracking of air pollution is about to revolutionize the forecasting of air
quality. Such forecasts could help people plan around high levels of
ground-level ozone—a dangerous lung irritant—just as they now plan
around bad storms.
“The phrase that people have
used is chemical weather forecasting,” says Kevin Bowman of NASA’s
Jet Propulsion Laboratory. Bowman is a senior member of the technical staff
for the Tropospheric Emission Spectrometer, one of four scientific sensors
on NASA’s Aura satellite.
Aura and other NASA satellites track
pollution in the same way that astronomers know the chemical composition of
stars and distant planetary atmospheres: using spectrometry. By breaking the
light from a planet or star into its spectrum of colours, scientists can read
off the atmosphere’s gases by looking at the “fingerprint” of
wavelengths absorbed or emitted by those chemicals. From Earth orbit, pollution-watching
satellites use this trick to measure trace gases such as carbon monoxide, nitrogen
oxide, and ozone.
However, as Bowman explains, “Polar
sun-synchronous satellites such as Aura are limited at best to two overpasses
per day.” A recent report by the National Research Council recommends
putting a pollution-watching satellite into geosynchronous orbit—a special
very high-altitude orbit above the equator in which satellites make only one
orbit per day, thus seeming to hover over the same spot on the equator below. There,
this new satellite, called GEOCAPE (Geostationary Coastal and Air Pollution
Events), would give scientists a continuous eye in the sky, allowing them to
predict daily pollution levels just as meteorologists predict storms.
“NASA is beginning to investigate
what it would take to build an instrument like this,” Bowman says. Such
a chemical weather satellite could be in orbit as soon as 2013, according to
the NRC report. Weather forecasts might never be the same.
Learn more about the Tropospheric
Emission Spectrometer at: tes.jpl.nasa.gov
Kids can learn some elementary smog chemistry while making “Gummy Greenhouse Gases” out of gumdrops at: spaceplace.nasa.gov/en/kids/tes/gumdrops
This article was provided by the Jet Propulsion Laboratory, California Institute of Technology, under a contract with the National Aeronautics and Space Administration.
Any material for inclusion in the December Newsletter should be with the Editor by 28th November 2008
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