Fast Stars Near the Galactic Center (APOD 14 Jan 2007)
Fast Stars Near the Galactic Center (APOD 14 Jan 2007)
The APOD description says "over one million times the mass of our Sun is somehow confined to a region less than a fifth of a light-year across". How does the object (black hole or whatever) at the center of our galaxy compare in size to our Sun? I assume that our Sun is much, much smaller than a fifth of a light-year across.
Last edited by Confused on Fri Jan 19, 2007 8:36 pm, edited 1 time in total.
Well technically the BH has no size whatsoever, it is a singularity, however people usually define a BH as having the same size as its event horizon (its Schwarzchild radius), the radius at which nothing
not even light can escape.
Rs = 2 x G x m / c^2
So in this case
Rs = 2 x (6.67x10^(-11))x 10^6 x 2x10^30 / (3x10^8 )^2 = 3x10^9m according to Google calculator.
So if I have typed that in correctly its about 5 times bigger than the Sun, seems a bit small, ill check it when I have a calculator I can trust. Though of course we are not comparing apples with apples.
not even light can escape.
Rs = 2 x G x m / c^2
So in this case
Rs = 2 x (6.67x10^(-11))x 10^6 x 2x10^30 / (3x10^8 )^2 = 3x10^9m according to Google calculator.
So if I have typed that in correctly its about 5 times bigger than the Sun, seems a bit small, ill check it when I have a calculator I can trust. Though of course we are not comparing apples with apples.
Last edited by astro_uk on Sun Jan 14, 2007 9:47 pm, edited 1 time in total.
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When you say 5 times bigger, do you mean in diameter, or volume, or something else?astro_uk wrote:Well technically the BH has no size whatsoever, it is a singularity, however people usually define a BH as having the same size as its event horizon (its Schwarzchild radius), the radius at which nothing
not even light can escape.
Rs = 2 x G x m / c^2
So in this case
Rs = 2 x (6.67x10^(-11))x 10^6 x 2x10^30 / (3x10^8)^2 = 3x10^9m according to Google calculator.
So if I have typed that in correctly its about 5 times bigger than the Sun, seems a bit small, ill check it when I have a calculator I can trust. Though of course we are not comparing apples with apples.
Or would it be better described as say a radius from the centre of the sun to say, the orbit of Venus?
I need things explained in very simple terms if possible as, well, I'm very simple...
Regards,
Andy.
Andy.
I mean its radius is 5 times larger, the sun has a radius of about 7 x 10^8 m. Though I still have my doubts until I have a look at the numbers with a real calculator.
The gravitational force would still be huge at much greater distances than this number though, still plenty to keep those stars whizzing about.
The gravitational force would still be huge at much greater distances than this number though, still plenty to keep those stars whizzing about.
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http://antwrp.gsfc.nasa.gov/apod/ap070114.html
Now I'M confused. It takes sunlight about 8 min to reach the Earth. now a fifth of a light year would take light a little over two months to traverse. Or is that going back to the size of the event horizon?
Orin
Now I'M confused. It takes sunlight about 8 min to reach the Earth. now a fifth of a light year would take light a little over two months to traverse. Or is that going back to the size of the event horizon?
Orin
Orin
Smile today; tomorrow's another day!
Smile today; tomorrow's another day!
I wouldn't touch that with a ten foot sliderule !
The photo is about one light year wide (in the description), = 8-1/2" on my screen, the center star moving at the yellow cross is 3/8" dia. That's 1/22.6667 of the photo -- 1LY =6 trillion miles / 22.6667 = 264.7 billion miles. The photo's motion is over 8 years, the center star moves one diameter in the animation, that = 33 billion miles in one year, which = 1049 miles per second or 0.56% speed of light. Ball park of course, but do the stars really appear as 265 billion miles wide?? that doesn't make sense, but maybe the magnification and time exposure make the suns appear larger than life. Considering our solar system is 6 billion miles in diameter apx, that's 1/1000 th of a light year. (*1LY = 5.88 T miles oops ! This is thumb at arms length anyway) Our solar system is only 2.5% of the suns diameter in the photo, which again doesn't make sense.
Gravitational attraction of 1 million solar masses at 1/10 of a light year.
I'm having trouble finding an equation for this question, Wikipedia is not helping, and gravity is not my strong suit in math.
Gravitational attraction of 1 million solar masses at 1/10 of a light year.
I'm having trouble finding an equation for this question, Wikipedia is not helping, and gravity is not my strong suit in math.
The size they talk about is, I think, the size that can be inferred by the motion of the stars, this is not necessarily related to any physical scale of the BH, if there were stars that were closer to the BH, they could pin down its size more accurately.
F = (G x M1 x M2) / R^2
F = (6.67x10^(-11) * (10^6 * 2*10^30) * 1 / (0.1 x 9.4605284 × 10^15)^2
Giving a force of 1.5 x 10^(-4) N per kg at 1/10 lyr.
The stars are unresolved, they are not magnified, the size they appear on the image is due to the optics of the system. In reality they should appear as points, but due to the effect of the telescope optics and the Earths atmosphere the stars light gets smeared over several pixels making them seem much larger.Ball park of course, but do the stars really appear as 265 billion miles wide?? that doesn't make sense, but maybe the magnification
I think the equation you want is the standard Newtonian one, it should be good enough in this case.Gravitational attraction of 1 million solar masses at 1/10 of a light year.
I'm having trouble finding an equation for this question, Wikipedia is not helping, and gravity is not my strong suit in math.
F = (G x M1 x M2) / R^2
F = (6.67x10^(-11) * (10^6 * 2*10^30) * 1 / (0.1 x 9.4605284 × 10^15)^2
Giving a force of 1.5 x 10^(-4) N per kg at 1/10 lyr.
no can see
has that Jan 14, 2007 APOD been impounded ? Can't seem to get it displayed ?
Wolf Kotenberg
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If you log onto APOD and click on to January; Sunday; the 14th box. You should get it. even though the box don't show it. http://antwrp.gsfc.nasa.gov/apod/calendar/ca0701.html
try it!
Orin
try it!
Orin
Orin
Smile today; tomorrow's another day!
Smile today; tomorrow's another day!
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That sounds reasonable to me. Keep in mind that if a black hole with the mass of our sun would have a radius of only 3 km (so sayest the great Wikipedia). For a million times the mass you got a million times the radius, and indeed, the radius is linear with respect to the mass. Your math looks solid.astro_uk wrote:Well technically the BH has no size whatsoever, it is a singularity, however people usually define a BH as having the same size as its event horizon (its Schwarzchild radius), the radius at which nothing
not even light can escape.
Rs = 2 x G x m / c^2
So in this case
Rs = 2 x (6.67x10^(-11))x 10^6 x 2x10^30 / (3x10^8 )^2 = 3x10^9m according to Google calculator.
So if I have typed that in correctly its about 5 times bigger than the Sun, seems a bit small, ill check it when I have a calculator I can trust. Though of course we are not comparing apples with apples.
They may be in orbit around Sgr A, but they don't have to be. If the stars have enough velocity, they will simply fly by, with their trajectories being bent by the pull of the black hole. They probably are orbiting Sgr A, but you'd probably have to do quite a bit of modeling to be sure.StACase wrote:1. Are those stars following a standard orbital path?
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Thanks Orin for providing a link to the APOD of January 14th 2007, as I cannot find that APOD on the APOD archive list that I've seen. Odd that it does not appear, as the APOD for the 15th is in the archive!orin stepanek wrote:If you log onto APOD and click on to January; Sunday; the 14th box. You should get it. even though the box don't show it. http://antwrp.gsfc.nasa.gov/apod/calendar/ca0701.html
try it!
Orin
"For a million times the mass you got a million times the radius, and indeed, the radius is linear with respect to the mass. "
4/3 pi Radius ^3 = volume of a sphere , yes?
or, the cube root of one million times the radius, you mean?
or 100 times the radius of 3 kilometers = 300 km radius of the sphere of 1 million solar masses, would that equal the event horizon ??
I have some homework to do as the units of G (6.67 x 10 (-11)) aren't familiar.
4/3 pi Radius ^3 = volume of a sphere , yes?
or, the cube root of one million times the radius, you mean?
or 100 times the radius of 3 kilometers = 300 km radius of the sphere of 1 million solar masses, would that equal the event horizon ??
I have some homework to do as the units of G (6.67 x 10 (-11)) aren't familiar.
I could have missed something but I always thought that when a BH's mass is mentioned, that it is just a rough comparison to an observable star's mass. For a BH cannot have "mass" per say.
For example:
If we observe objects that are near enough to an alleged BH we can roughly calculate what the mass of the BH would be, if it were a star, in order to gravitationally interact with those objects from "that distance".
So, ultimately we cannot calculate mass for something that is unobservable. We can only calculate its gravitational effect on surrounding matter and compare it to the mass of what we can observe -like stars.
A crude laymen’s explanation I am sure -but is my understanding flawed?
For example:
If we observe objects that are near enough to an alleged BH we can roughly calculate what the mass of the BH would be, if it were a star, in order to gravitationally interact with those objects from "that distance".
So, ultimately we cannot calculate mass for something that is unobservable. We can only calculate its gravitational effect on surrounding matter and compare it to the mass of what we can observe -like stars.
A crude laymen’s explanation I am sure -but is my understanding flawed?
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That's for correlating the volume to the radius, yes. If it has a uniform density, the mass also. However, the Schwarzchild radius defines the event horizon, which is dependent on the strength of the gravitational field.kovil wrote:"For a million times the mass you got a million times the radius, and indeed, the radius is linear with respect to the mass. "
4/3 pi Radius ^3 = volume of a sphere , yes?
or, the cube root of one million times the radius, you mean?
or 100 times the radius of 3 kilometers = 300 km radius of the sphere of 1 million solar masses, would that equal the event horizon ??
I have some homework to do as the units of G (6.67 x 10 (-11)) aren't familiar.
Note that mass of a uniform volume of matter in normal space scales according to the radius-cubed, while gravitational acceleration falls off according to the radius-squared. If you divide, you're left with one factor of the radius. I've never gone through the steps of deriving the equation, but I suspect this fact shows up somewhere in the steps.
The units of the gravitational constant here are m^3 / (kg*s^2) or N*m^2 / kg^2
Martin, I think there's some confusion coming from methods of determining mass. With nothing to see for a black hole, you can't just measure it's radius. There's also no light intensity for you to measure and infer it's mass by the types of stars that radiate that much of various wavelengths. So you are correct that the mass has to be determined by the gravitational effect on nearby objects.
But, the black hole does have mass. Some quantity of matter went into the formation of the black hole (unless Sgr. A isn't really a black hole, but it is generally accepted to be), so at least in this sense it has mass, even if it's collapsed down to a singularity or some form of degenerate matter hidden behind the event horizon.
"Any man whose errors take ten years to correct is quite a man." ~J. Robert Oppenheimer (speaking about Albert Einstein)
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Is this not the projected orbit of the stars?
http://www.mpe.mpg.de/ir/GC/index.php
Also, curious... should we expect to see some (any?) lensing?
http://www.mpe.mpg.de/ir/GC/index.php
Also, curious... should we expect to see some (any?) lensing?
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Hey, that is a nifty animation you found Freebirds. Thanks.
If an object passes behind the black hole, there can be lensing, but I'm not sure how significant it would be unless it passed exactly behind. Given that we're talking about a volume of space ~10^18 times bigger than the black hole, that's probably very unlikely in the time spans we have the luxury of watching.
If an object passes behind the black hole, there can be lensing, but I'm not sure how significant it would be unless it passed exactly behind. Given that we're talking about a volume of space ~10^18 times bigger than the black hole, that's probably very unlikely in the time spans we have the luxury of watching.
"Any man whose errors take ten years to correct is quite a man." ~J. Robert Oppenheimer (speaking about Albert Einstein)
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Hello All
Hello Martin
You said
I fully agree with you.
Hello Martin
You said
If we observe objects that are near enough to an alleged BH we can roughly calculate what the mass of the BH would be, if it were a star, in order to gravitationally interact with those objects from "that distance".
So, ultimately we cannot calculate mass for something that is unobservable. We can only calculate its gravitational effect on surrounding matter and compare it to the mass of what we can observe -like stars.
I fully agree with you.
Harry : Smile and live another day.