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| Dec27-03, 07:11 AM | #1 |
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Covariance
Greetings,
In some discussions about GR, I heard the term "covariance" and covariant form (eg, covariant form of Maxwell's equations) pop up often. I've been wondering for a while why the notion of covariance in GR is so important. I have some background in mathematical physics, so I know the difference between co- and contravariant components of a tensor a such. Cheers, |
| Dec27-03, 11:34 AM | #2 |
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[tex]f^i = \frac{dp^i}{dt}[/tex] and coordinate acceleration [tex]a^i = \frac{du^i}{dt}[/tex]. One observer may observe the instantaneous result from a force on a particle to relate the two as [tex]f^i = ma^i[/tex] for example if the particle is instantaneously at rest according to his frame. He then might propose this as a law of physics. In fact Newton did. The problem is that this equation is not frame invariant in form. Lets say another observer using a frame according to which the particle is instantaneously in motion perpendicular to the force describes the responce. He finds [tex]f^i = \gamma ma^i[/tex]. He descides to propose this for a law of physics. It still isn't general. Consider a third observer according to which the particle is instantaneously in motion in the direction of the force. He finds [tex]f^i = \gamma ^{3}ma^i[/tex]. All 3 are in disagreement. Lets say they finally arrive upon an equation that reduces to all 3 cases like equation 3.2.10 at http://www.geocities.com/zcphysicsms/chap3.htm#BM29 An accelerated frame observer would STILL dissagree with it. Tensors are frame covariant in the literal sense of the word which guarantees that the form of the equations involving only tensors and invariants will be invariant. So instead of going through all those rediculous itterations of the law you just state a tensor equation. For example start with a four vector force [tex]F^\lambda = \frac{DP^\lambda}{d\tau}[/tex] an invariant for mass m and a four vector acceleration [tex]A^\lambda = \frac{DU^\lambda}{d\tau}[/tex] and say [tex]F^\lambda = mA^\lambda[/tex] is your tensor equation law and automatically every frame observer will agree that it describes the physics according to every frame as long as it describes it according to any single one (with a hypothetical complete accuracy). Tensors are beautiful! To say "covariant form of Maxwell's equations" is kind of a strange way to fraise it because the everyday form is actually special relativistically covariant again in the literal sence of the word. What that form is not is "generally covariant" nor generally invariant in form. An accelerated frame observer will disagee that Maxwell's equations in old form describe the physics as he observes it. The generally covariant expressions for the electromagnetic field are the electromagnetic and electromagnetic duel tensors. The tensor equation given by equations 7.1.5 or 7.1.8 at http://www.geocities.com/zcphysicsms/chap7.htm#BM84 which you heard referred to as "covariant form of Maxwell's equations" have a frame invariant form. If even one observer finds that these equations describes physics (with a hypothetical complete accuracy) than every observer for every frame must agree whether inertial or accelerated whether in the depths of space or in considering a strong varying gravitational field. This expresses a general law. |
| Dec27-03, 12:43 PM | #3 |
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So as I understand it, it has little to do with the transformation behaviour of the 4-vectors involved? The forces and acceleration involved still have their components written in the uppercase, so they still represent contravariant components? Or am I seeing this wrong?
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| Dec27-03, 01:11 PM | #4 |
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Covariance |
| Dec27-03, 01:30 PM | #5 |
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Thank you. You have been most helpful.
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| Dec27-03, 03:33 PM | #6 |
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Arcon |
| Dec28-03, 01:56 AM | #7 |
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D'oh, I knew that! Not any four numbers is a 4-vector, they have to agree with a behaviour under transformation.
My main question was about the use of the term "covariance", and DW cleared that up quite nicely. |
| Dec28-03, 07:20 AM | #8 |
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The problem with DW's response is that he seems to imply that if an equation is not written explicitly as a tensor equation then it isn't covariant. However covariance means that an law of physics must be expressable in tensor form. DW is speaking specifically with regards to what is called manifestly covariant form which means its a tensor equation. |
| Dec28-03, 10:49 AM | #9 |
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By the way, instead of signing your post as pmb why don't you just post "as" pmb like you used to do in this forum instead of switching handles? |
| Dec28-03, 11:33 AM | #10 |
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The last time you posted in this forum, before this most recent incarnation, you (i.e. "DavidW") decided to start a flame war because you have this sick vendatta against me for proving you wrong so often. In your earlier incarnation it was because I corrected you on the meaning of "scalar." However it seems once more that you're less interested in physics and more interesed in causing trouble. Stop being so obsessed with me and stick to physics! |
| Dec28-03, 12:18 PM | #11 |
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Its not my fault if you didn't read all of what I wrote. What on Earth are you talking about? I highly respect David for the depth of work he did on his online text from which I have learned a lot so I chose his initials as my Nick name. You don't actually think someone posting here as say Britney Spears would actually be Britney Spears do you? If any such arguement occured between the two of you here based on these rude statements of yours I suspect it led to your dissmissal thus explaining why you no longer post "as" pmb. |
| Dec28-03, 01:21 PM | #12 |
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Guys, cut it out. I had a question, I got an answer, this thread has served it's purpose. If you want to argue do it by PM or e-mail, but don't clutter the board.
I just wish the creator of the thread could lock it, but alas. |
| Dec28-03, 01:33 PM | #13 |
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Dimitri - If you're happy then so am I. I have no intention of responding to DW in the future so don't worry about it.
Arcon |
| Dec29-03, 09:03 AM | #14 |
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