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אחרי הרצאה באסטרופיסיקה בה הוזכרה אנרגיה שלילית של הואקום כמקור אפשרי להאצת התפשטות היקום, עלי לתקן ולומר, כסטודנט פישר אל רעהו, שאני לא יודע מספיק כדי להתייחס ברצינות לדברים שהעלית. יום טוב. |
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Well - you're taking an Astrophysics course. So maybe you could clear something up for me:
They say that distant galaxies are moving faster than closer galaxies, which makes people think that galaxies are accelerating in time. But we can't see how distant galaxies are acting now, but, rather, we see how they were at the time -D/c, where D is their distance from us. So, basically, we see that galaxies in the very distant past, and that are far away move faster - but couldn't that mean the exact opposite, that is, that the galaxies are decelerating? From one humble Undergrad to another, of course. |
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זאת, למעשה, שאלה מעניינת מאוד. לא חשבתי על זה כך מעולם, אבל הטיעון שלך נשמע מאוד הגיוני. ליאור, אני מאוד מאוד אשמח אם תוכל לענות על השאלה, או לפחות לשאול מישהו שכן יכול לענות, אם אתה לא. |
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כבר הפנתי את השאלה לפיסיקאי נבון ממני, אם כי איני בטוח שהאימייל נשלח. אין לי תשובה אינטליגנטית לשלוף מהמותן, אך אם תפנו למדען המשוגע (1), מובטחת תשובה תוך ~שבועיים. |
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The higher velocity of distant objects is not related in the standard cosmoligical models to acceleration, but rather to the Hubble expansion law of the universe.
the hubble expansion law states that the velocity of an object expanding with the universe (i.e. no peculiar speed) usually called a comoving observer, from any other commoving observer is lieary proportional to the comoving distance between the two. V = H*r ; with H standing for the Hubble constant at said time, H = H(t). hubble law has been observationaly verified to a good extent (in astrophysics an order of magnitude is usually acceptable), and is also a direct result of assuming a non-static homogenous (and thus isotropic) univerese. the hubble constant changes with time, or so the standard cosmological models say, and different models predict a different behaviour of H(t). these are tightly connected to specific solution of the einstine equation, and to the metrics the solution enables (a homogenous universer results in one of three metrics- flat, positivly eccentric, and negativly accentric). according to the standrd model today, the "lamda-CDM" model, which consists of a cold dark matter big-bang universe with a cosmological constant, the univeres' expansion rate should actually be increasing, thus u can say that the univerese is accelerating. as far as i know it's not iron cast yet. i can check with an astronomer in the huji astro-group for more detail on said observations. |
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Sorry if I'm being thick, (and you can write in Hebrew, if you wish, I'm writing in English only due to technical constraints) but how could they measure consequences of the Hubble law, if all one can do is check how galaxies behaved in the past, when it's not even the same time for all the other galaxies, since they're at different distances?
By the way: the Hubble constant changes with time? That reminds me of someone asking me about using different coefficients for his polynomial at different points. |
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English is preferable, i might be making some spelling mistakes, and i apologize for them, but the technical terms are all english, i hate to try and find translations...
first about the hubble "constant" changing - the constant is constant in space, but not in time. now, i'm about to step into a subject i'm no expert about, i apologize for any mistakes i might make - the way to build a metric one can work with to describe the universe, in a GR way, is to "slice" it to equal-time three dimensional "planes". the simplest way is to assume that the universe is euclidean at short ranges (observations of near space confirm that, near meaning as far as we can see, if i'm not mistaken), and then define a metric from a point of view of a "all-knowing" observer, that is one that can measure distances on the plane, between any two points. now, for every two points on said metric, in every plane, the same hubble law holds, that is - the velocity between the two is proportional to a constant that is the same one in all space at that time. the relation between said constant and the expansion rate of the universe is H(t) = a*/a (with a* being the time derivative of a, a "dot") where a is the expansion factor of the universe (has to be normalized to some a_0 if u want it to mean anything). as for measuring galaxies at different times, i think that compensation can be done. one way is to measure "near" galaxies, where time differences are small in cosmological orders of magnitude. another, i believe, is measuring relative velocities of objects about on a line of sight (seems tricky to me, i don't know if it's actually done). this is an interesting point, i think i've heard an answer to it once, and am sure i've asked it once, which make my not knowing it now somewhat dissapointing (and depressing, considering the implication about my memory), so i will check with my sources for the answer, and be back. an important point, i think, is that predicitons can be made, according to the standard model, regarding what the hubble expansion should look like, if the modle's assumptions and derivations are correct, including "looking into the past" effects, and as far as i know the observations match those to a good degree. be back with more precise answers soon, i hope |
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עודד נועץ במנחה שלו, וזה מוסר כי תצפיות ממקורות מרוחקים משוקללות אמנם בהתאם למרחקם מכדה''א, כדי לפצות על פרק הזמן שלוקח לאור להגיע מן המקור המרוחק. מודלים קוסמולוגיים שונים נותנים אומדנים שונים למרחק זה, כך שמידת ההתאמה בין התצפיות לתיאוריה תלויה במודל הקוסמולוגי לפיו משקללים את התצפיות. זהו מדד נוסף לטיב המודל המוצע - עדיף מודל קוסמולוגי המניב התאמה טובה יותר בין התצפיות לתיאוריה. כרגיל באסטרופיסיקה, הבעיה פתוחה והספקולציות רבות. |
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תשובת MadSci: http://www.madsci.org/posts/1013049337.As.q.html
Your question was answered by: Benjamin Monreal Grad student, Physics, MIT Hello Dubi, I think that your reasoning is mostly correct; the light we see today (in, say, a Hubble Deep Field image) was actually emitted by the galaxies billions of years ago; and, indeed, billions of years ago the galaxies could have had different velocities than they do now. The Supernova Cosmology Project, indeed, saw exactly this effect! They observed supernovae up to seven billion light-years away, and showed that the Universe was expanding faster at that time. That's exactly the importance of these measurements: we can find a relationship between the Hubble constant (how fast the Universe is expanding, i.e. the redshift) at various times in its evolutions (i.e. the distance to the supernova, measured by its brightness). The light-travel time is an important feature of this measurement. It's not just a simple model, though, asking "does it slow down or does it speed up?" We have to predict how the Hubble constant would change under various circumstances (gravity, a cosmological constant, dark matter, etc.) and see whether these predictions agree or disagree with the data. With the new supernova data, you cannot model the Universe as a bunch of mass under the influence of only gravity. If gravity is the only force acting on all of these galaxies and supernovae, then we cannot explain how the Hubble constant (i.e. the expansion rate) has gotten from its old value (measured by the distant supernovae) to its modern value (measured by the nearby supernovae. Basically, in the past 7 billion years, things have not slowed down as much as we expected them to. Observationally, we saw that extremely redshifted supernova (SN1997ff was a good one) that were unusually bright. Redshifted means fast expansion. Bright means nearby. Combining the two, this supernovae is so nearby, that it can't have been moving so fast for the whole lifetime of the Universe (taking into account gravity, etc.) Therefore, the Universe must have started out with a slower expansion, and accelerated. (Imagine that you throw a baseball, wait one second, and open your eyes. If the baseball is moving at 10 meters per second when you measure it, you would expect it to be 10 meters away! If it is only 5 meters away, you can explain it by saying that it started out slowly, and sped up to 10 m/s.) Lots of good information on this topic can be found by going to http://xxx.lanl.gov/find/astro-ph/ the Physics preprint archives and searching for papers with "accelerating universe" in the title. You'll find a mix of gritty-detail-technical papers, and a few easy-to-read articles. -Ben |
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Dubi, Lior and Oded.
I feel much more informed, though I am probably, not much wiser. Processing will resume this Wednesday, when I have some free time. |
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