How was General Relativity tested? ||The Mystery of Spacetime Relativity|| Part 6 || Unboxing Physics
Unboxing Physics
2018-07-21
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Tests of general relativity serve to establish observational evidence for the theory of general relativity. The first three tests, proposed by Einstein in 1915, concerned the "anomalous" precession of the perihelion of Mercury, the bending of light in gravitational fields, and the gravitational redshift.
Videos of the series---
1. All about gravity--- https://youtu.be/7CeNjYzpmgM
2. Space-Time Mystery explained--- https://youtu.be/s7VbXhD73bQ
3. How does special relativity works?--- https://youtu.be/fIQAHRw5mgg
4. General Theory of relativity, a myth or reality?--- https://youtu.be/y4Se7ld1ppc
5. Consequences of General Theory of Relativity---https://youtu.be/rFWdfHn6bJE
The precession of Mercury was already known; experiments showing light bending in line with the predictions of general relativity was found in 1919, with increasing precision measurements done in subsequent tests, and astrophysical measurement of the gravitational redshift was claimed to be measured in 1925, although measurements sensitive enough to actually confirm the theory were not done until 1954. A program of more accurate tests starting in 1959 tested the various predictions of general relativity with a further degree of accuracy in the weak gravitational field limit, severely limiting possible deviations from the theory.
In the 1970s, additional tests began to be made, starting with Irwin Shapiro's measurement of the relativistic time delay in radar signal travel time near the sun. Beginning in 1974, Hulse, Taylor and others have studied the behaviour of binary pulsars experiencing much stronger gravitational fields than those found in the Solar System. Both in the weak field limit (as in the Solar System) and with the stronger fields present in systems of binary pulsars the predictions of general relativity have been extremely well tested locally.
In February 2016, the Advanced LIGO team announced that they had directly detected gravitational waves from a black hole merger.[1] This discovery, along with additional detections announced in June 2016 and June 2017,[2] tested general relativity in the very strong field limit, observing to date no deviations from theory.
Videos of the series---
1. All about gravity--- https://youtu.be/7CeNjYzpmgM
2. Space-Time Mystery explained--- https://youtu.be/s7VbXhD73bQ
3. How does special relativity works?--- https://youtu.be/fIQAHRw5mgg
4. General Theory of relativity, a myth or reality?--- https://youtu.be/y4Se7ld1ppc
5. Consequences of General Theory of Relativity---https://youtu.be/rFWdfHn6bJE
The precession of Mercury was already known; experiments showing light bending in line with the predictions of general relativity was found in 1919, with increasing precision measurements done in subsequent tests, and astrophysical measurement of the gravitational redshift was claimed to be measured in 1925, although measurements sensitive enough to actually confirm the theory were not done until 1954. A program of more accurate tests starting in 1959 tested the various predictions of general relativity with a further degree of accuracy in the weak gravitational field limit, severely limiting possible deviations from the theory.
In the 1970s, additional tests began to be made, starting with Irwin Shapiro's measurement of the relativistic time delay in radar signal travel time near the sun. Beginning in 1974, Hulse, Taylor and others have studied the behaviour of binary pulsars experiencing much stronger gravitational fields than those found in the Solar System. Both in the weak field limit (as in the Solar System) and with the stronger fields present in systems of binary pulsars the predictions of general relativity have been extremely well tested locally.
In February 2016, the Advanced LIGO team announced that they had directly detected gravitational waves from a black hole merger.[1] This discovery, along with additional detections announced in June 2016 and June 2017,[2] tested general relativity in the very strong field limit, observing to date no deviations from theory.
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