Sunday, May 22, 2011

GRAVITATIONAL RADIATION: TESTING RELATIVITY THEORY


GRAVITATIONAL RADIATION: TESTING RELATIVITY THEORY 
One of Einstein's predictions lay idle for nearly half a century as too difficult to verify: Extremely weak gravitational waves are radiated into space with the velocity of light by rap­idly accelerated or orbiting bodies. These waves might be detectable with sensitive apparatus, and large astro­nomical objects undergoing violent activity, such as supernova outbursts or the nucleus of an active galaxy, may be the best places from which to detect them. Any gravitational wave passing through an object momen­tarily deforms its space and causes
the object to vibrate slightly.
More than a decade ago experi­ments tried to pick up, inside large, suspended, aluminum cylinders, infinitesimal oscillations that would be produced by gravitational waves striking the cylinders. At first it seemed that they had succeeded in detecting gravity waves simulta­neously in a Maryland laboratory and at the Argonne National Laboratory near Chicago. Most of these were re­ported to be coming from the Galaxy's center in Sagittarius. It now appears that the observed oscillations were much too large to be consistent with current physical theory. So far, other and far more sensitive gravity­wave detectors, which can detect de­formations as small as 10.,7 centi­meter, have failed to find any evidence of gravitational radiation coming from the center of our Galaxy or anywhere else. However, indirect evidence of gravitational radiation has been found in the radio observations of a binary pulsar (see page 377). The
gravitational interaction between the pulsar and its close companion, per­haps a neutron star or white dwarf, results in part of the orbital kinetic energy's being radiated away in the form of gravity waves. The loss in en­ergy decreases the orbital separation between the components. Radio monitoring during the period 1974 to 1979, covering some 1000 orbital revo­lutions, shows a decrease in the or­bital period of about 101 micro­seconds per year. Allowing for the uncertainties in the mass of each component and the inclination of their orbital plane, the result is in rea­sonable agreement with general relativity's prediction of 76 micro­seconds per year.