- #1
Jonny_trigonometry
- 452
- 0
It is true that [tex] \frac{\partial}{\partial x^\beta} T^{0 \beta} = \gamma^2 c \left( \frac{\partial \rho}{\partial t} + \vec{\nabla} \bullet \left[ \rho \vec{v} \right] \right) = 0 [/tex]
but, how do we arrive at this point?
What is in [tex] T^{ \alpha \beta} [/tex]
and how do we compute it for any alpha? I'm sorry if this is a no brainer. I missed some critical lectures.
but, how do we arrive at this point?
What is in [tex] T^{ \alpha \beta} [/tex]
and how do we compute it for any alpha? I'm sorry if this is a no brainer. I missed some critical lectures.