- #1
nomather1471
- 19
- 1
Can we show orthogonality of timelike and null vector?
Last edited:
WannabeNewton said:Finally, let ##\{e_i \}## be an orthonormal basis
I think you have to show that:WannabeNewton said:I just want to expand upon what George said. Let ##(M,g)## be a space-time and ##p\in M##. Furthermore, let ##X## be a time-like vector in ##T_p M## and ##Y## a non-zero vector in ##T_p M## such that ##g_p(X,Y) = 0##. Finally, let ##\{e_i \}## be an orthonormal basis for ##T_p M## so that ##X = X^i e_i## and ##Y = Y^i e_i##.
Then ##(X^2)^2 + (X^3)^2 + (X^4)^2 < (X^1)^2## and ##X^1 Y^1 = X^2 Y^2 + X^3Y^3 + X^4Y^4##.
Note this immediately implies that ##(X^1)^2 > 0## and that ##(Y^2)^2 + (Y^3)^2 + (Y^4)^2 > 0##.
Therefore [tex](X^1 Y^1)^2 \leq ((X^2)^2 + (X^3)^2 + (X^4)^2)((Y^2)^2 + (Y^3)^2 + (Y^4)^2)< (X^1)^2((Y^2)^2 + (Y^3)^2 + (Y^4)^2)[/tex] thus ##(Y^1)^2 < (Y^2)^2 + (Y^3)^2 + (Y^4)^2## i.e. ##Y## is space-like.
nomather1471 said:I think you have to show that:
[tex](X^1 Y^1)^2 \leq ((X^2)^2 + (X^3)^2 + (X^4)^2)((Y^2)^2 + (Y^3)^2 + (Y^4)^2)[/tex]
The concept of orthogonality refers to the perpendicularity or independence of two vectors in a vector space. In the context of timelike and null vectors, it means that these two types of vectors are perpendicular or independent of each other in a four-dimensional spacetime.
A timelike vector is a vector with a positive squared length in a four-dimensional spacetime. It represents the direction of movement through time. In terms of orthogonality, timelike vectors are always orthogonal to null vectors, meaning they are perpendicular and do not share any components or directions.
A null vector has a squared length of zero in a four-dimensional spacetime and represents a direction that is neither purely spatial nor purely temporal. In the context of orthogonality, null vectors are always orthogonal to timelike vectors, meaning they are perpendicular and do not share any components or directions.
The concept of orthogonality is important in relativity and spacetime because it helps to define the relationship between timelike and null vectors, which are fundamental in describing the dynamics of particles and fields in a four-dimensional spacetime. It also plays a crucial role in understanding the geometry of spacetime and how it is affected by the presence of matter and energy.
In relativity, the principle of causality states that the cause of an event must precede the effect in time. This is directly related to the orthogonality of timelike and null vectors, as it ensures that events cannot occur simultaneously or in reverse order in a four-dimensional spacetime. The orthogonality of these vectors also helps to define the light cone structure, which is essential in understanding causality in relativity.