Difference between revisions of "On the Concept of Integrality in the Theory of Special Relativity"
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We assume that A moves at velocity <u>v</u> different from O with respect to B: hence we can say equivalently that B moves with respect to A at velocity -<u>v</u> because of the principle of relativity. In this case then the subject is of no importance. | We assume that A moves at velocity <u>v</u> different from O with respect to B: hence we can say equivalently that B moves with respect to A at velocity -<u>v</u> because of the principle of relativity. In this case then the subject is of no importance. | ||
| − | [[Category:Scientific Paper]] | + | [[Category:Scientific Paper|concept integrality theory special relativity]] |
| − | [[Category:Relativity]] | + | [[Category:Relativity|concept integrality theory special relativity]] |
Latest revision as of 19:46, 1 January 2017
| Scientific Paper | |
|---|---|
| Title | On the Concept of Integrality in the Theory of Special Relativity |
| Author(s) | Lorenzo Mencherini |
| Keywords | theory of special relativity, velocity, integrality |
| Published | 1989 |
| Journal | None |
| Pages | 179-182 |
Abstract
We say that a body is integral in a given reference frame if the coordinates of its points are constant in time.
Given any two bodies A and B, we ask what kinematic relationship there is between them.
We assume that A moves at velocity v different from O with respect to B: hence we can say equivalently that B moves with respect to A at velocity -v because of the principle of relativity. In this case then the subject is of no importance.
