Posted on 06/23/2003 9:25:12 AM PDT by RightWhale
Berkeley Lab Physicist Challenges Speed of Gravity Claim
Berkeley - Jun 22, 2003
Albert Einstein may have been right that gravity travels at the same speed as light but, contrary to a claim made earlier this year, the theory has not yet been proven. A scientist at Lawrence Berkeley National Laboratory (Berkeley Lab) says the announcement by two scientists, widely reported this past January, about the speed of gravity was wrong.
Stuart Samuel, a participating scientist with the Theory Group of Berkeley Lab's Physics Division, in a paper published in Physical Review Letters, has demonstrated that an "ill-advised" assumption made in the earlier claim led to an unwarranted conclusion. "Einstein may be correct about the speed of gravity but the experiment in question neither confirms nor refutes this," says Samuel. "In effect, the experiment was measuring effects associated with the propagation of light, not the speed of gravity."
According to Einstein's General Theory of Relativity, light and gravity travel at the same speed, about 186,000 miles (300,000 kilometers) per second. Most scientists believe this is true, but the assumption was that it could only be proven through the detection of gravity waves. Sergei Kopeikin, a University of Missouri physicist, and Edward Fomalont, an astronomer at the National Radio Astronomy Observatory (NRAO), believed there was an alternative.
On September 8, 2002, the planet Jupiter passed almost directly in front of the radio waves coming from a quasar, a star-like object in the center of a galaxy billions of light-years away. When this happened, Jupiter's gravity bent the quasar's radio waves, causing a slight delay in their arrival on Earth. Kopeikin believed the length of time that the radio waves would be delayed would depend upon the speed at which gravity propagates from Jupiter. To measure the delay, Fomalont set up an interferometry system using the NRAO's Very Long Baseline Array, a group of ten 25-meter radio telescopes distributed across the continental United States, Hawaii, and the Virgin Islands, plus the 100-meter Effelsberg radio telescope in Germany. Kopeikin then took the data and calculated velocity-dependent effects. His calculations appeared to show that the speed at which gravity was being propagated from Jupiter matched the speed of light to within 20 percent. The scientists announced their findings in January at the annual meeting of the American Astronomical Society.
Samuel argues that Kopeikin erred when he based his calculations on Jupiter's position at the time the quasar's radio waves reached Earth rather than the position of Jupiter when the radio waves passed by that planet. "The original idea behind the experiment was to use the effects of Jupiter's motion on quasar-signal time-delays to measure the propagation of gravity," he says. "If gravity acts instantly, then the gravitational force would be determined by the position of Jupiter at the time when the quasar's signal passed by the planet. If, on the other hand, the speed of gravity were finite, then the strength of gravity would be determined by the position of Jupiter at a slightly earlier time so as to allow for the propagation of gravitational effects."
Samuel was able to simplify the calculations of the velocity-dependent effects by shifting from a reference frame in which Jupiter is moving, as was used by Kopeikin, to a reference frame in which Jupiter is stationary and Earth is moving. When he did this, Samuel found a formula that differed from the one used by Kopeikin to analyze the data. Under this new formula, the velocity-dependent effects were considerably smaller. Even though Fomalont was able to measure a time delay of about 5 trillionths of a second, this was not nearly sensitive enough to measure the actual gravitational influence of Jupiter. "With the correct formula, the effects of the motion of Jupiter on the quasar-signal time-delay are at least 100 times and perhaps even a thousand times smaller than could have been measured by the array of radio telescopes that Fomalont used," Samuel says. "There's a reasonable chance that such measurements might one day be used to define the speed of gravity, but they just aren't doable with our current technology."
I think your question is probably on the mark: they are so weak we cannot measure them.
Heck, two black holes waltzing around once per minute 100 LY away we can't detect...
--Boris
You know, the standard answer to "how do gravitons get out of a black hole?" is that the field is a "fossil" left over from when the hole was a star.
So the obvious question is: if stuff is falling into the hole, how can its gravity increase?
I've seen answers but have a hard time grasping them.
Evidently the integral of the mass/position of the inflow at the moment it crosses the event horizon averages out and the field intensifies that way. I dunno.
--Boris
P.S. Everything radiates EM (light) unless it is at absolute zero...right?
Per Wien's law [yet another law,] the peak wavelength is inversely proportional to temperature [as always, measured relative to absolute zero] so as the temperature approaches absolute zero, the wavelength of the emitted light approaches infinitely large values. At the same time the energy of the wavelength falls rapidly as the wavelength increases, so the intensity of the light emitted near absolute zero is very low. This radiation is probably not going to be called light except on FR since it is way outside the visible spectrum. It's not even in the radio spectrum.
V e r y, . v e r y . l o w . f r e q u e n c y. Even lower than that.
I don't quite understand the question.
From LIM: "Glad you cleared that up."
ROFLMAO! RA, you've got more brains than are decent. Would you please explain this in layman's terms? :^)
Oh, you're just fishin' for a compliment, aren't you? :^)
Actually, I know RA quite well, and yes...he does talk and think just like that. Which is why I told him he has more brains than are decent and asked him for a translation. I'm just a lowly geochemist and have postively NO clue what he was talking about either, but it sounded legit.
Indeed he does, but in this instance he's quoting "Physicist," so it's a safe bet it wasn't uttered in jest.
Well it most certainly was legit. What you are all talking about was the addition that Physicist freepmailed me for a post I was making. (If you note: I added this caveat in front of that paragraph with this statement: " An addition by Physicist")
It was a paragraph he added to my description of the Standard Model for a post I made a while back. I had originally only included the (Pion and others) as an exchange force and he made the addition that the others needed to be a bit clearer. I should have added my two cents to this to make that paragraph more understandable from the beginning.
My apologies for not doing this from the beginning. So here goes:
BTW This is all mine, so any mistakes are mine as well:
First, lets take a look at Van der Waals Forces:
(I am attempting this without a complete lecture on chemical bonding so please be kind) Atom and molecules are attracted to each other by two classes of bonds. The Intramolecular bond and the Intermolecular bond.
The Intermolecular bond is divided into these categories; Van der Waals Forces, Hydrogen Bonds, and molecule-ion attractions.
The Intramolecular bond (which are much stronger than the Intermolecular bond) is divided into these categories; Ionic bonding, covalent bonding, and metallic bonds.
We will only concentrate on the Van der Waals Forces.
Van der Waals Forces arise from the interaction of the electrons and nuclei of electrically neutral atoms and molecules. How is this possible if these are considered electrically neutral I hear you ask. What is going on here is that the electrons and nuclei of atoms and molecules (for this description: from here out called particles) are not at rest, but are in a constant motion. Since this is the case, there arises an electrical imbalance (called an instantaneous dipole [another term is a temporary polarity]) in this electrically neutral particle. Two particles in this dipole state will attract. Also this dipole action in one particle can cause a dipole in an adjoining (nearby) particle. So the dipole-dipole attraction is what is known as Van der Waals Forces. If these particles kinetic energies are low enough (anc close enough together), the repeated actions of the instantaneous dipoles will keep them attracted together.
One of the interesting things about this that the more electrons are in play the greater the Van der Waals Force. This is why the noble gas Krypton liquefies at a higher temperature than the noble gas Neon.
Whewwwwww!!!!!! Half done!:
Back to the Standard Model.
Again trying to keep this at an understandable level I may mess this up So if I did not explain this quite right, please correct me!.
A brief background: How does a nucleus stay together when it is packed with positively charged protons? Since like charges repel, you would think that the nucleus would fly apart. The force that keeps this from happening is the Strong Force. One of the things that was discovered is that the mass of any nucleus is always less than the sum of the individual particles (called nucleons) that make it up. The difference (residual) is due to the Binding Energy of the nucleus. This binding energy is directly related to the strength of the strong force. Note: This is why there is a release of energy when an atom is split. (nuclear fission).
So just what is this Strong Force anyway? The Strong force has an effect on quarks, anti quarks and gluons. Oh my, another term, QUARKS! After much research, it was discovered that the protons and neutrons in the nucleus were made up of smaller particles called quarks. It turned out that two types of quarks were needed to produce a proton or a neutron. However, there are six types of quarks in normal matter. The strong force binds these quarks together to form a family of particles called hadrons which include both protons and neutrons. (SORRY IF THIS IS GETTING COMPLEX) To simplify this discussion, quarks have a color charge (red, green, and blue). BTW, this was a convenient way of describing the charge, it is not referring to color as we commonly use it). Like colors repel and unlike colors attract. There are also antiquarks. The attraction between the quark and antiquark is stronger than between just quarks. If it is a quark/antiquark (same color) it is called a meson. If its between quarks it is called a baryon (protons and neutrons fall in this category). Here is the rub, baryonic particles can exist if their total color is neutral; i.e. have a red green and blue charge altogether.
Without getting into too much more detail, quarks can interact, changing color, etc. so long as the total charge is conserved.
The quark interactions are cause by exchanging particles called gluons. There are eight kinds of gluons each having a specific color charge.
So back to the original paragraph. Neutral (all three colors) hadrons (which include protons and neutrons) can interact with the strong force similarly to the way atoms an molecules react via the Van der Waals forces.
Physicist? Anything you want to add or change if I "stuffed it up" so to speak?
Oh, so I'm a humorless cipher then, am I? Guess I'll just go eat worms...
;^)
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