The linearization of the metric of curved space-time

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Discussion Overview

The discussion revolves around the linearization of the metric of curved space-time, specifically addressing the mathematical expressions and expansions involved in relating the curved metric to a flat metric. Participants explore the implications of different terms in the expansion and the nature of the components involved.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • One participant questions why the second order term in the expansion is expressed as HacHcb instead of Haccb.
  • Another participant asserts that the second order term is indeed HacHcb.
  • A different participant references a matrix identity to support their view on the expansion.
  • Some participants challenge the interpretation of the expansion, suggesting that the objects involved are components rather than matrices.
  • A participant expresses confusion regarding the absence of a factor of 1/2 in the Taylor series expansion of κ compared to the expansion of (I + H)-1.
  • Another participant proposes that the expansion of gik as the inverse metric aligns with the expression for (I + H)-1, suggesting a similarity in the expansions.

Areas of Agreement / Disagreement

Participants express differing views on the correct formulation of the expansion terms and the nature of the components involved, indicating that multiple competing perspectives remain without a clear consensus.

Contextual Notes

There are unresolved questions regarding the assumptions behind the expansions and the definitions of the components, particularly in relation to the Taylor series and the treatment of the metric components.

maica
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Why Yab=Xab-kHab+k2HacHcb-... and not Yab=Xab-kHab+(1/2)k2Haccb-...?
Y is the curved space-time metric
X is the planespace-time metric
 
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The second order term in k is HacHcb and not Haccb
 
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Because of the matrix identity (I + H)-1 = I - H + HH - ...
 
but this expansion is not an expansion matrix. these objects are components, numbers
 
maica said:
but this expansion is not an expansion matrix. these objects are components, numbers

How do you calculate the value of (HH)ab, given the components of H?
 
I'm a little lost. The expression (I+H)-1 = I - H + HH - ... is the Taylor series in powers of "H", but gij = ηij + κhij + (1/2)κ2hilhlj, is a series in powers of "κ", and doesn't have the expoent "-1", which is responsible for the absence of the factor 1/2 in the Taylor series of "H". I can't see why the factor 1/2 is absent, in Taylor series of "κ" powers. I think that the expansion of (HH)ab is identical of the gij expansion, because of de tensor rank.
 
I think that I understood. If we consider the equation gikgkj = δij and if gkj = ηkj + κ hkj then gik is the inverse and its expansion is gik = ηik - κ hik + κ2 hil hlk - ... identical to the expression (I + H)-1.
 
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