Proof - epsilon permutation and metric tensor relation

Hence the summary is - In summary, the equation given can be simplified to g^{ij}\epsilon_{ipt}\epsilon_{jrs}\, = \, g_{pr}g_{ts} \, - \, g_{ps}g_{tr}, by using the given notation and the value of the determinant formed by the metric components of the space. This can be shown by expanding the expression and simplifying it using the Kronecker delta notation.
  • #1
symmetric
9
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Homework Statement



[tex]\mbox{Prove that}\,g^{ij} \epsilon_{ipt}\epsilon_{jrs}\,=\, g_{pr}g_{ts}\,-\,g_{ps}g_{tr}[/tex]
Notation :
[tex]e_{ijk}\,=\,e^{ijk}\,=\,\left\{\begin{array}{cc}1,&\mbox{ if ijk is even permutation of integers 123...n }\\-1, & \mbox{if ijk is odd permutation of integers 123...n}\\0&\mbox{in all other cases} \end{array}\right[/tex]

[tex] \epsilon_{ijk}\,=\,\sqrt{g}e_{ijk} [/tex]
[tex] \epsilon^{ijk}\,=\,\frac{1}{\sqrt{g}}e^{ijk} [/tex]

[tex] \mbox{where}\,g\, = | g_{ij}| \mbox{ value of determinant formed by metric components of space }[/tex]


Homework Equations


The Attempt at a Solution



[tex] \epsilon_{ipt}\epsilon_{jrs}\,=\,ge_{ipt}e_{jrs} [/tex]

[tex]g^{ij}\epsilon_{ipt}\epsilon_{jrs}\,=\,g^{ij}ge_{ipt}e_{jrs}\,=\,g^{ij}\,g\left| \begin{array}{ccc}\delta_{ij}&\delta_{ir}&\delta_{is}\\ \delta_{pj}&\delta_{pr}&\delta_{ps}\\ \delta_{tj}&\delta_{tr}&\delta_{ts}\end{array}\right|[/tex]

[tex] = g^{ij}\,\left| \begin{array}{ccc}g_{ij}&g_{ir}&g_{is}\\ g_{pj}&g_{pr}&g_{ps}\\ g_{tj}&g_{tr}&g_{ts}\end{array}\right|[/tex][tex] = g^{ij}g_{ij} ( g_{pr}g_{ts} \, - \, g_{ps}g_{tr} ) \, - \, g^{ij}g_{ir} ( g_{pj}g_{ts} \, - \, g_{ps}g_{tj} ) \, + \, g^{ij}g_{is} ( g_{pj}g_{tr} \, - \, g_{pr}g_{tj} )[/tex]

[tex] = ( g_{pr}g_{ts} \, - \, g_{ps}g_{tr} ) \, - \, \delta_r^j ( g_{pj}g_{ts} \, - \, g_{ps}g_{tj} ) \, + \, \delta_s^j ( g_{pj}g_{tr} \, - \, g_{pr}g_{tj} )[/tex]

[tex] = g_{pr}g_{ts} \, - \, g_{ps}g_{tr} \, - \, g_{pr}g_{ts} \, + \, g_{ps}g_{tr} \, + \, g_{ps}g_{tr} \, - \, g_{pr}g_{ts} [/tex]

[tex]g^{ij}\epsilon_{ipt}\epsilon_{jrs}\, = \, g_{ps}g_{tr} \, - \, g_{pr}g_{ts}[/tex]

[tex]g^{ij}\epsilon_{ipt}\epsilon_{jrs}\, = \, - ( g_{pr}g_{ts} \, - \, g_{ps}g_{tr} )[/tex]

Why am I getting unexpected -ve sign ?
 
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  • #2
Got the correction ! The modified solution is as follows -

From above solution continuing up to step -

[tex] g^{ij}\epsilon_{ipt}\epsilon_{jrs}\,=\, g^{ij}g_{ij} ( g_{pr}g_{ts} \, - \, g_{ps}g_{tr} ) \, - \, g^{ij}g_{ir} ( g_{pj}g_{ts} \, - \, g_{ps}g_{tj} ) \, + \, g^{ij}g_{is} ( g_{pj}g_{tr} \, - \, g_{pr}g_{tj} )[/tex]

then -

[tex]g^{ij}\epsilon_{ipt}\epsilon_{jrs}\,=\delta_j^j( g_{pr}g_{ts} \, - \, g_{ps}g_{tr} ) \, - \, \delta_r^j ( g_{pj}g_{ts} \, - \, g_{ps}g_{tj} ) \, + \, \delta_s^j ( g_{pj}g_{tr} \, - \, g_{pr}g_{tj} ) [/tex]

[tex]= 3 ( g_{pr}g_{ts} \, - \, g_{ps}g_{tr} ) \, - \, \delta_r^j ( g_{pj}g_{ts} \, - \, g_{ps}g_{tj} ) \, + \, \delta_s^j ( g_{pj}g_{tr} \, - \, g_{pr}g_{tj} )[/tex]

[tex]= 3( g_{pr}g_{ts} ) \, - \,3( g_{ps}g_{tr} ) \, - \, g_{pr}g_{ts} \, + \, g_{ps}g_{tr} \, + \, g_{ps}g_{tr} \, - \, g_{pr}g_{ts}[/tex]

[tex]g^{ij}\epsilon_{ipt}\epsilon_{jrs}\, = \, g_{pr}g_{ts} \, - \, g_{ps}g_{tr} [/tex]

which is same as required !
 

Related to Proof - epsilon permutation and metric tensor relation

1. What is the proof for the relationship between epsilon permutation and metric tensor?

The proof for the relationship between epsilon permutation and metric tensor is based on the properties of the Levi-Civita symbol, which is a mathematical tool used to describe the behavior of rotation and reflection in three-dimensional space. It is also based on the properties of the metric tensor, which is a mathematical object that describes the geometry of a space.

2. What is the significance of the epsilon permutation and metric tensor relationship?

The relationship between epsilon permutation and metric tensor is significant because it allows us to express geometric quantities in terms of algebraic quantities, making calculations and equations easier to work with. It also helps us understand the geometric interpretation of tensors and how they are related to transformations in space.

3. How is the epsilon permutation related to the metric tensor in Einstein's field equations?

In Einstein's field equations, the epsilon permutation is used to define the structure of spacetime, while the metric tensor is used to describe the curvature of spacetime. The relationship between these two concepts is crucial in understanding the behavior of gravity and its effects on the curvature of spacetime.

4. Can the proof for the relationship between epsilon permutation and metric tensor be applied to other dimensions?

Yes, the proof for the relationship between epsilon permutation and metric tensor can be extended to any number of dimensions. However, the specific form of the equations may vary depending on the dimensionality of the space being studied.

5. How does the relationship between epsilon permutation and metric tensor impact theoretical physics?

The relationship between epsilon permutation and metric tensor is crucial in theoretical physics, particularly in the development of theories such as general relativity and string theory. It allows us to understand the underlying geometric structure of space and time, and how it is affected by various forces and interactions. This relationship also plays a role in the development of mathematical models and predictions for phenomena in the universe.

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