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Tests of General Relativity: Equivalence Principle and Experimental Verification, Study notes of Astronomy

The tests of general relativity through the equivalence principle, discussing its components, solar system tests, and weak equivalence principle formulism. It also covers experiments like eotvos, michelson & morley, and pound-rebka-snider, which aim to verify the principle.

Typology: Study notes

Pre 2010

Uploaded on 02/13/2009

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Download Tests of General Relativity: Equivalence Principle and Experimental Verification and more Study notes Astronomy in PDF only on Docsity! 1 Tests of the Equivalence Principle and the “Classic” Weak Field Tests  Compartmentalizing General Relativity into testable components  Tests of the Equivalence Principle  Post-Newtonian Parameterization  The classic solar system tests  Deflection of light  Precession of perihelion of Mercury  Shapiro delay 2 The Metric Tensor  Definition of (3d) metric tensor gij … the distance between points (x1, x2, x3) and (x1+δx1,x2+δx2,x3+δx3)  Can simply generalize this to 4-d spacetime  Geodesics are those paths which minimize the distance between two points A and B  For a given matter distribution, metric is determined by Einstein’s equation (ten coupled partial differential equations) 5 III.5 : Tests of the Einstein Equivalence Principle (EEP)  Weak Equivalence Principle (WEP)  Dates back to Galileo (or earlier!)  Statement: the acceleration experienced by an object in a given gravitational field is independent of the objects mass or composition.  Inertial and gravitational mass are equivalent  To test this, we need a formulism for describing deviations from the WEP. 6  Weak Equivalence Principle formulism  Consider an object as a collection of masses bound together by various interactions (weak, strong, electromagnetic)  Suppose that some part of the binding energy associated with these interactions violates the WEP  If we measure the acceleration of two bodies with different composition, we can define 7  Classic Experiment of Eotvos…  Used torsional balance to determine that η<10-8  Roll, Krotkov, Dicke (Princeton)…  Improved Eotvos method and obtained tighter limit η<10-11 The confrontation between GR and Experiment; C.M.Will 10  Classic experiment of Michelson & Morley using interferometry  Hughes-Drever experiments probe “c” through effect on energy levels in atomic nucleus  Can now directly time “one-way” trips of light signal The confrontation between GR and Experiment; C.M.Will 11  Local Positional Invariance  Is physics independent of location?  Test through gravitational redshift  Suppose two identical clocks are placed at different locations in gravitational field… we’ve seen that there is a fractional shift of frequency  But if the physics governing the clocks depends on position, then we can write 12  Pound-Rebka-Snider tower experiment (Harvard)…  frequency shift of gamma-ray emission line from Fe-57  Null redshift experiment…  Synchronization of three H-maser clocks (used changes in solar grav. potential) The confrontation between GR and Experiment; C.M.Will 15  Classic expedition by Eddington to observe solar eclipse…  First confirmation of GR  Made Einstein instantly famous!  Modern measurements of light-bending possible from VLBI observations of quasars… get GR result to 0.2%. The confrontation between GR and Experiment; C.M.Will 16 III.8: Shapiro delay  Spacetime curvature increase time taken for a photon to propagate from point A to B  Within our solar system, spacetime curvature from Sun dominates… so events that occur on far side of Sun are “late” THE PARAMETER (1+4)/2 DEFLECTION ‘OF LIGHT VLBI Y , i Hipparcos _| PSR 1937421 5s | Voyager wPir ey Radio Optical ° 1.05 | Pot | 1.00 e a s 095-- es 4 xs ly 1.05 SHAPIRO TIME DELAY | i 1.00 I" o9s|- i i 1 Lt 1920 1940 1960 1970 1980 1990 2000 YEAR OF EXPERIMENT 17