| | #Increasingly precise measurements of the advance of the perihelion of Mercury show a shift greater than predicted by Relativity, well beyond the margin of error.<ref>In a complicated or contrived series of calculations that most physics majors cannot duplicate even after learning them, the theory of general relativity's fundamental formula, <math>G_{\mu\nu} = 8 \pi K T_{\mu\nu}\,</math>, was conformed to match Mercury's then-observed precession of 5600.0 arc-seconds per century. Subsequently, however, more sophisticated technology has measured a different value of this precession (5599.7 arc-seconds per century, with a margin of error of only 0.01), and leading promoters of Relativity (such as Professor Clifford Will) have omitted this in listing tests confirming Relativity.</ref> | | #Increasingly precise measurements of the advance of the perihelion of Mercury show a shift greater than predicted by Relativity, well beyond the margin of error.<ref>In a complicated or contrived series of calculations that most physics majors cannot duplicate even after learning them, the theory of general relativity's fundamental formula, <math>G_{\mu\nu} = 8 \pi K T_{\mu\nu}\,</math>, was conformed to match Mercury's then-observed precession of 5600.0 arc-seconds per century. Subsequently, however, more sophisticated technology has measured a different value of this precession (5599.7 arc-seconds per century, with a margin of error of only 0.01), and leading promoters of Relativity (such as Professor Clifford Will) have omitted this in listing tests confirming Relativity.</ref> |
| | #The discontinuity in momentum as velocity approaches "c" for infinitesimal mass, compared to the momentum of light. | | #The discontinuity in momentum as velocity approaches "c" for infinitesimal mass, compared to the momentum of light. |
| − | #The logical problem of a force which is applied at a right angle to the velocity of a relativistic mass - does this act on the rest mass or the relativistic mass?<ref>The distinction between "rest mass" and "relativistic mass" is archaic. Modern textbooks use just "mass", which is the same as the old "rest mass". Problems of force applied at various angles to a particle's motion are solved (reasonably) straightforwardly in a formulation involving 4-momentum in spacetime.</ref> | + | #The logical problem of a force which is applied at a right angle to the velocity of a relativistic mass - does this act on the rest mass or the relativistic mass? |
| | #The observed lack of curvature in overall space.<ref>If space were curved, one would never expect the universe as a whole to be almost precisely flat. Yet it is.</ref> | | #The observed lack of curvature in overall space.<ref>If space were curved, one would never expect the universe as a whole to be almost precisely flat. Yet it is.</ref> |
| | #The universe shortly after its creation, when quantum effects dominated and contradicted Relativity. | | #The universe shortly after its creation, when quantum effects dominated and contradicted Relativity. |