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Talk:Counterexamples to Relativity (view source)
Revision as of 17:58, August 10, 2010
, 17:58, August 10, 2010→Wormholes: new section
:: Are you sure that this is true? What are you fixing? One formula for relativistic momentum is <math>dp=\gamma v\left( dm \right)</math>. This remains a differential quantity in <math>m</math> as velocity becomes infinite: <math>\frac{dp}{dm}=\gamma v</math>. Fixing energy gives the correct momentum result in the limit as velocity becomes infinite. Maybe the misunderstanding results from taking two limits at once -- the prefactor that depends on velocity becomes infinite while the rest-mass dependence remains linear. [[User:TylerGD|TylerGD]] 13:28, 10 August 2010 (EDT)
:: Are you sure that this is true? What are you fixing? One formula for relativistic momentum is <math>dp=\gamma v\left( dm \right)</math>. This remains a differential quantity in <math>m</math> as velocity becomes infinite: <math>\frac{dp}{dm}=\gamma v</math>. Fixing energy gives the correct momentum result in the limit as velocity becomes infinite. Maybe the misunderstanding results from taking two limits at once -- the prefactor that depends on velocity becomes infinite while the rest-mass dependence remains linear. [[User:TylerGD|TylerGD]] 13:28, 10 August 2010 (EDT)
== Wormholes ==
There seems to be some confusion on the difference between predicting and allowing. General relativity allows wormholes under some conditions. But a lack of observed wormholes or even a lack of wormholes would not be inconsistent with the theory.