Norman Albers
- 21
- 0
How do we express the Minkowski field tensor for circular currents?
The Minkowski field tensor represents the flat space-time metric, typically expressed in Cartesian coordinates as diag(-1,1,1,1) or in spherical coordinates. When charge-carrying objects are introduced, the space-time metric transitions from Minkowski to a curved metric, necessitating the use of the Lorentzian space-time metric. Understanding this transition requires knowledge of general relativity (GR) and applied differential geometry, as well as the ability to solve the Einstein Field Equations for specific configurations, such as circular currents.
PREREQUISITESPhysicists, students of general relativity, and anyone interested in the mathematical formulation of space-time metrics and their applications in theoretical physics.
Why? Wouldn't it be better just to ignore him rather than give him the feeling that he'll get a response from someone whenever he posts non-sensical questions?AlphaNumeric said:Albers, though you're now banned, I'll take this opportunity to explain to you why your question doesn't even make sense.