|
|
Thread Tools | Display Modes |
#21
|
|||
|
|||
Mike Williams wrote in message
Are you certain that your values for "proper motion" and "parallax" have the correct units for the equation you're using? I use a more direct method and get a vastly different answer. I started with the fact that the proper motion is RA: -7.54775 acsecs/year, Dec: +0.48180 arcsecs/year and the distance is 4.3 light years. A light year is 9.46e15 metres. -7.54775 arcsecs/year of RA is -0.000549399 radians/year 0.48180 arcsecs/year of Dec is 2.33583e-06 radians/year (Note a complete circle is 24h of RA but 360d of Dec) The transverse motions are Distance * sin(Angle), giving -2.23484e+13 and 9.5017e+10 metres/year. Divide by the number of seconds in a year and combine the two velocities by Pythagoras and I get the transverse motion to be 710 km/sec = 150 AU/year. My equation is from page 250, "Spherical Astronomy" by W.M. Smart (a very old book from the 1960s). On page 251, he gives an example using the star Capella, where the annual proper motion is 0.439 arc sec, parallax 0.075 arc sec, giving a transverse velocity of 27.7 km/sec. On that basis, I think I've got it right... unless the 3.7 arc sec/year total proper motion figure for Alpha Centauri I'm using is wrong? Considering also the Sun moves through space at roughly 20 km/sec, I think your number is a bit on the high side. Abdul |
#22
|
|||
|
|||
Mike Williams wrote:
Are you certain that your values for "proper motion" and "parallax" have the correct units for the equation you're using? I use a more direct method and get a vastly different answer. There are two errors in your calculation, both of which inflate the component of motion in right ascension. -7.54775 arcsecs/year of RA is -0.000549399 radians/year (Note a complete circle is 24h of RA but 360d of Dec) It isn't necessary to convert -7.54775 from hours:minutes:seconds to degrees:minutes:seconds. It's already expressed as arcseconds in the d:m:s system. But you do have to multiply it by the cosine of Alpha Centauri's declination. To see why, consider the surface of the Earth. Degrees latitude (north-south) always correspond to a surface distance of about 110 km, but the surface distance for a degree of longitude depends on the latitude. It's 110 km at the equator, where cos(lat) = 1, but smaller than 110 km by the factor cos(lat) at other latitudes. The declination of Alpha Centauri is -60° 50', and cos(-60° 50') is about 0.487. So your figure for radians/year in RA is too big by a factor of about 30: (360 / 24) * (1 / cos(-60° 50')). The formula Abdul used is pretty standard, and simpler to apply. You can divide by the parallax (in arcseconds) or multiply by the distance (in parsecs). 4.74 is just a constant of proportionality that converts between AU/year and km/s. An object at a distance of 1 parsec with a proper motion of 1 arcsecond/year has a transverse motion of 1 AU/year, or 150 million km/year, or 4.74 km/s. - Ernie http://home.comcast.net/~erniew |
#23
|
|||
|
|||
"Grimble Gromble" wrote in message ...
"AA Institute" wrote in message om... How can I precisely chart the *absolute* positions and ship-relative velocities of icy comets encountered on a forward pass... then try to re-intercept them on a reverse pass, having turned my ship around? That isn't necessary. Just plant a small transmitter on the comet; that will give you directional information. If the transmissions and receptions are accurately timed (pulsars make excellent clocks available to all) then the distance to the comet can be easily calculated. Grim Thanks! That's a sound idea, but I think we will be *certain* of a nice trail of comets stretching all the way to Alpha, long before the mission is due for launch... projected at round 2200 AD... by which time we will have filled all the interim experience gaps necessary with adventures on the Moon and Mars! Now, I was going to turn this thing into a cracking BIG SCREEN MOVIE, if only I could present my script to some 'movie' agency! Grim, you wouldn't happen to know of any contacts in the movie business by any chance would you? I'll share the royalties if it helps...! LOL.. Abdul |
#24
|
|||
|
|||
"AA Institute" wrote in message
m... Grim, you wouldn't happen to know of any contacts in the movie business by any chance would you? I'll share the royalties if it helps...! LOL.. I don't know anybody in anything. Grim |
#25
|
|||
|
|||
Ernie Wright wrote:
The formula Abdul used is pretty standard, and simpler to apply. You can divide by the parallax (in arcseconds) or multiply by the distance (in parsecs). 4.74 is just a constant of proportionality that converts between AU/year and km/s. An object at a distance of 1 parsec with a proper motion of 1 arcsecond/year has a transverse motion of 1 AU/year, or 150 million km/year, or 4.74 km/s. Oh, so that's where the 4.74 came from, I wasn't sure of its origins. So to depart toward Alpha Centauri on a hypothetical voyage, one has to leave the ecliptic plane of our solar system going south towards -60° 50' declination. Is there an easy calculation to work out how many degrees that direction is off the ecliptic plane of our solar system? Abdul |
#26
|
|||
|
|||
AA Institute wrote:
-60° 50' declination. Is there an easy calculation to work out how many degrees that direction is off the ecliptic plane of our solar system? Not quite as easy as the transverse motion calculation. What you'd be doing is converting from equatorial coordinates to ecliptic coordinates. The conversion involves a single rotation, but in three dimensions. The axis of the rotation is the intersection of the equatorial and ecliptic planes, and the amount of the rotation is the obliquity of the ecliptic (the tilt of the Earth). You'd start with both RA and Dec (you need both, since it's a 3D transformation) and end up with lamda and beta, ecliptic longitude and latitude. For more precise calculations, or calculations over long time frames, you'd have to account for various effects that cause the two planes to move with respect to each other. Nutation is a slight wobble of the equatorial system caused by the Moon. The Earth's axis also precesses slowly. A search would probably turn up online calculators to do the conversion for you, along with any number of pages on celestial coordinates, e.g. http://www.seds.org/~spider/spider/S....html#ecliptic Most star charting software is capable of displaying grid lines for several coordinate systems, and some can provide the location of specified objects in your choice of coordinate systems. Approximate current ecliptic coordinates for Alpha Centauri are beta = -42.6° lamda = 239.5° But don't take my word for it. I just did this on a calculator and may have gotten it wrong, and I haven't told you the epoch or whether I accounted for nutation. You'll get more satisfaction from understanding and doing the calculation yourself. - Ernie http://home.comcast.net/~erniew |
#27
|
|||
|
|||
BP wrote:
Right, okay that is the 26k year cycle. So, I guess really a stars movement would not really be noticeable on the scale of a star chart. I am referring to the Sky Atlas (Tirion,Sinnott).. The shift in coordinates due to precession is of the order of 1 degree every 70 years. The star with the largest proper motion, ie measured across the sky in a plane perpendicular to the line of site is Barnard's star, which moves approx 1 degree every 350 years, or about 6 times less than the motion due to precession. Most other stars would appear to move a far smaller angle. If you have a 1950 star chart, there are algorithms for calculating the position at another date. DaveL Bp The main reason for the changing Epochs is to account for precession of the earth's axis. The axis shifts by about an arcminute every year (plucked from memory, could be wrong). Because of this the coordinates of objects on the celestial sphere changes with time, by a small amount each year. DaveL |
#28
|
|||
|
|||
Ernie Wright wrote in message ...
AA Institute wrote: -60° 50' declination. Is there an easy calculation to work out how many degrees that direction is off the ecliptic plane of our solar system? snip Approximate current ecliptic coordinates for Alpha Centauri are beta = -42.6° lamda = 239.5° But don't take my word for it. I just did this on a calculator and may have gotten it wrong, and I haven't told you the epoch or whether I accounted for nutation. You'll get more satisfaction from understanding and doing the calculation yourself. - Ernie http://home.comcast.net/~erniew Thanks for confirming; yes I made it -42.6 degrees based on the obliquity, R.A. & Dec, for the current epoch around 2000.0-ish. The dynamics are quite complex and moving over time, hence if we're launching a hypothetical starship in a future era the variables are bound to be radically different by then. It just serves as an illustration for now. Abdul |
#29
|
|||
|
|||
"Grimble Gromble" wrote in message ...
"AA Institute" wrote in message om... Take our Sun for instance and the recent high levels of solar activity we've seen, sending massive amounts of charged particles toward the Earth. ... My god; it's shooting at us! So it is. Question is: would it shoot harder and more violently if the Sun had a binary companion of similar size and mass orbiting it at, say around where Saturn orbits the Sun? And if the orbit of that secondary star was highly elliptical, would the output vary along the orbital cycle in line with the distance separating the two stars? Do gravitational interactions between two stars in a binary system cause variability in the radiation output...through some kind of a 'tidal wave' inducement? AAI |
#30
|
|||
|
|||
Saul Levy wrote in message . ..
snip Space is plenty empty enough that most stars are isolated. Only occasionally will a star come close enough to perturb outlying objects in orbit around another star. F= G M m / r^2, the standard equation for interactive force between any two bodies in space, be they stars, planets, comets or any combination between them. A hypothetical comet of mass 1 x 10^5 kg orbiting the Sun at 50,000 AUs (7.5 x 10^15 metres) out in the direction of Alpha Centauri, would be tugged with a force of 2.4 x 10^-7 Newton by the Sun (of mass 2 x 10^30 kg). The same comet would be perturbed by Alpha Centauri's combined mass of 4 x 10^30 kg exerting a force of just 2.5 x 10^-8 Newton (from a distance of 222,000 AUs = 3.3 x 10^16 metres). Thus, the Sun will be 10 times more forceful on the body, compared to Alpha Centauri. Now, you could argue well 9/10th versus 1/10th... is that sufficiently strong a force to perturb the orbit of an outlying comet in the manner I describe he- http://uk.geocities.com/aa_spaceagen....html#midrange Back in the 1840s, French astronomer Urbain Jean Joseph Le Verrier made calculations along these lines to show that Uranus was being perturbed by an unseen body, which subsequently enabled him to predict the position of (then undiscovered) Neptune and guide astronomers at the Berlin observatory to discover this new planet. Now, Uranus of mass 8.7 x 10^25 kg orbits the Sun at a distance of 19.18 AUs on average (2.9 x 10^12 metres. The Sun exerts a force of 1.4 x 10^21 Newtons on Uranus. At their closest points in their respective mean orbits around the Sun, Uranus and Neptune (the latter of mass 1 x 10^26 kg) are separated by 1.6 x 10^12 metres. The maximum perturbational force between Uranus and Neptune during such (mean) close encounters in their orbits is 2.2 x 10^17 Newtons. Thus, the Sun's influence on Uranus is over 6,000 times as strong as the mutual perturbing forces between it and Neptune. Yet with this microscopic 1/6,000th as strong an influence, measurable positional shifts in the motion of Uranus were used to deduce the discovery of Neptune! The power of gravity, no matter how weak, no matter from what distance its influence, is not to be underestimated... AAI |
Thread Tools | |
Display Modes | |
|
|
Similar Threads | ||||
Thread | Thread Starter | Forum | Replies | Last Post |
Gravity as Falling Space | Henry Haapalainen | Science | 1 | September 4th 04 04:08 PM |
Further proof gravity is a push... | Rick Sobie | Astronomy Misc | 1 | March 16th 04 06:20 AM |
AMBER ALPHA STAR CESAM stellar model | harlod caufield | Space Shuttle | 0 | December 27th 03 08:12 PM |
AMBER ALPHA STAR CESAM stellar model | harlod caufield | Policy | 0 | December 27th 03 08:10 PM |