Timelike and lightlike/null vectors

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SUMMARY

A timelike vector cannot be orthogonal to a null vector in Minkowski space-time due to the properties of their respective metrics. A timelike vector satisfies the condition \(X^{2} = g_{ab}X^{a}X^{b} > 0\), while a null vector satisfies \(Y^{2} = g_{ab}Y^{a}Y^{b} = 0\). The orthogonality condition \(g_{ab}X^{a}Y^{a} = 0\) leads to a contradiction when substituting the components of the vectors, confirming that such orthogonality is impossible.

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  • Understanding of Minkowski space-time and its line element \(ds^{2} = dt^{2} - dx^{2} - dy^{2} - dz^{2}\)
  • Familiarity with the concepts of timelike and null vectors in the context of general relativity
  • Knowledge of tensor notation and the Einstein summation convention
  • Basic understanding of Euclidean vector operations and dot products
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  • Study the properties of 4-vectors in special relativity
  • Learn about the implications of orthogonality in the context of Lorentz transformations
  • Explore the geometric interpretation of timelike and null vectors in spacetime diagrams
  • Investigate the role of metrics in defining vector relationships in general relativity
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purakanui
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I have another problem that I am stuck on.

Show that a timelike vector cannot be orthogonal to a null vector.

Timelike:
X[tex]^{2}[/tex] = g(sub a b)X[tex]^{a}[/tex]X[tex]^{b}[/tex] > 0

Null:
X[tex]^{2}[/tex] = g(sub a b)X[tex]^{a}[/tex]X[tex]^{b}[/tex] = 0

In order for them to be orthogonal...

g(sub a b)X[tex]^{a}[/tex]Y[tex]^{a}[/tex] = 0

I know from the line element of Minkowski space-time you have

ds[tex]^{2}[/tex] = dt[tex]^{2}[/tex] - dx[tex]^{2}[/tex] - dy[tex]^{2}[/tex] - dz[tex]^{2}[/tex]

I have played around with substituting the line element into the equation that specifies if it is orthogonal, but to no success. Any help would be great!

Sorry for the bad writting, I couldn't get latex to do subscripts, it only did them in superscripts...

Thanks,

Chris
 
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Here's a possible argument. Treat each 4 vector as e.g. (x0, r) where r is a 3 vector, x0 the timelike component. Let Y be a null vector, X be timelike vector. Then we have:

(1) Y0^2 - ry dot ry = 0, where dot is euclidean 3 dot product.

(2) X0 Y0 - rx dot ry = 0

(3) X0^2 - rx dot rx > 0

From which:

x0 > norm(rx) , 3 norm, euclidean, by (3)

Y0 = norm (ry) by (1)

X0 Y0 > norm(rx) norm(ry) >= rx dot ry

which contradicts (2).
 
thanks =)
 

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