Gutman Bespal Ko Space Covariant NP Tetrad

Exact Solutions of Einstein's Field Equations

Description

Covariant NP tetrad for Gutman Bespal ko space

References

Gutman, Sbornik Sovrem. Probl. Grav. Tbilissi, p201, (1967)
Wesson, J. Math. Phys., v19, p2283, (1978)
Lake, Gen. Rel. Grav., v15, p357, (1983)
Kramer et al. (14.67) p173

Object definitions

Coframe

Coframe of Gutman Bespal Ko Space Covariant NP Tetrad
\left\{e_1\to r^2 d(t)-\frac{r d(r)}{\sqrt{1-k r^2}},e_2\to \frac{d(r)}{2 r \sqrt{1-k r^2}}+\frac{d(t)}{2},e_3\to -\frac{r d(\phi ) \sqrt{f(t)} \sin (\theta )}{\sqrt{2}}-\frac{i r d(\theta ) \sqrt{f(t)}}{\sqrt{2}},e_4\to -\frac{r d(\phi ) \sqrt{f(t)} \sin (\theta )}{\sqrt{2}}+\frac{i r d(\theta ) \sqrt{f(t)}}{\sqrt{2}}\right\}
<math> <mrow> <mo>{</mo> <mrow> <mrow> <msub> <mi>e</mi> <mn>1</mn> </msub> <semantics> <mo>&#8594;</mo> <annotation encoding='Mathematica'>&quot;\[Rule]&quot;</annotation> </semantics> <mrow> <mrow> <msup> <mi>r</mi> <mn>2</mn> </msup> <mo>&#8290;</mo> <mrow> <mi>d</mi> <mo>&#8289;</mo> <mo>(</mo> <mi>t</mi> <mo>)</mo> </mrow> </mrow> <mo>-</mo> <mfrac> <mrow> <mi>r</mi> <mo>&#8290;</mo> <mrow> <mi>d</mi> <mo>&#8289;</mo> <mo>(</mo> <mi>r</mi> <mo>)</mo> </mrow> </mrow> <msqrt> <mrow> <mn>1</mn> <mo>-</mo> <mrow> <mi>k</mi> <mo>&#8290;</mo> <msup> <mi>r</mi> <mn>2</mn> </msup> </mrow> </mrow> </msqrt> </mfrac> </mrow> </mrow> <mo>,</mo> <mrow> <msub> <mi>e</mi> <mn>2</mn> </msub> <semantics> <mo>&#8594;</mo> <annotation encoding='Mathematica'>&quot;\[Rule]&quot;</annotation> </semantics> <mrow> <mfrac> <mrow> <mi>d</mi> <mo>&#8289;</mo> <mo>(</mo> <mi>r</mi> <mo>)</mo> </mrow> <mrow> <mn>2</mn> <mo>&#8290;</mo> <mi>r</mi> <mo>&#8290;</mo> <msqrt> <mrow> <mn>1</mn> <mo>-</mo> <mrow> <mi>k</mi> <mo>&#8290;</mo> <msup> <mi>r</mi> <mn>2</mn> </msup> </mrow> </mrow> </msqrt> </mrow> </mfrac> <mo>+</mo> <mfrac> <mrow> <mi>d</mi> <mo>&#8289;</mo> <mo>(</mo> <mi>t</mi> <mo>)</mo> </mrow> <mn>2</mn> </mfrac> </mrow> </mrow> <mo>,</mo> <mrow> <msub> <mi>e</mi> <mn>3</mn> </msub> <semantics> <mo>&#8594;</mo> <annotation encoding='Mathematica'>&quot;\[Rule]&quot;</annotation> </semantics> <mrow> <mrow> <mo>-</mo> <mfrac> <mrow> <mi>r</mi> <mo>&#8290;</mo> <mrow> <mi>d</mi> <mo>&#8289;</mo> <mo>(</mo> <mi>&#981;</mi> <mo>)</mo> </mrow> <mo>&#8290;</mo> <msqrt> <mrow> <mi>f</mi> <mo>&#8289;</mo> <mo>(</mo> <mi>t</mi> <mo>)</mo> </mrow> </msqrt> <mo>&#8290;</mo> <mrow> <mi>sin</mi> <mo>&#8289;</mo> <mo>(</mo> <mi>&#952;</mi> <mo>)</mo> </mrow> </mrow> <msqrt> <mn>2</mn> </msqrt> </mfrac> </mrow> <mo>-</mo> <mrow> <mfrac> <mrow> <mi>&#8520;</mi> <mo>&#8290;</mo> <mi>r</mi> <mo>&#8290;</mo> <mrow> <mi>d</mi> <mo>&#8289;</mo> <mo>(</mo> <mi>&#952;</mi> <mo>)</mo> </mrow> <mo>&#8290;</mo> <msqrt> <mrow> <mi>f</mi> <mo>&#8289;</mo> <mo>(</mo> <mi>t</mi> <mo>)</mo> </mrow> </msqrt> </mrow> <msqrt> <mn>2</mn> </msqrt> </mfrac> </mrow> </mrow> </mrow> <mo>,</mo> <mrow> <msub> <mi>e</mi> <mn>4</mn> </msub> <semantics> <mo>&#8594;</mo> <annotation encoding='Mathematica'>&quot;\[Rule]&quot;</annotation> </semantics> <mrow> <mrow> <mo>-</mo> <mfrac> <mrow> <mi>r</mi> <mo>&#8290;</mo> <mrow> <mi>d</mi> <mo>&#8289;</mo> <mo>(</mo> <mi>&#981;</mi> <mo>)</mo> </mrow> <mo>&#8290;</mo> <msqrt> <mrow> <mi>f</mi> <mo>&#8289;</mo> <mo>(</mo> <mi>t</mi> <mo>)</mo> </mrow> </msqrt> <mo>&#8290;</mo> <mrow> <mi>sin</mi> <mo>&#8289;</mo> <mo>(</mo> <mi>&#952;</mi> <mo>)</mo> </mrow> </mrow> <msqrt> <mn>2</mn> </msqrt> </mfrac> </mrow> <mo>+</mo> <mfrac> <mrow> <mi>&#8520;</mi> <mo>&#8290;</mo> <mi>r</mi> <mo>&#8290;</mo> <mrow> <mi>d</mi> <mo>&#8289;</mo> <mo>(</mo> <mi>&#952;</mi> <mo>)</mo> </mrow> <mo>&#8290;</mo> <msqrt> <mrow> <mi>f</mi> <mo>&#8289;</mo> <mo>(</mo> <mi>t</mi> <mo>)</mo> </mrow> </msqrt> </mrow> <msqrt> <mn>2</mn> </msqrt> </mfrac> </mrow> </mrow> </mrow> <mo>}</mo> </mrow> </math>
{Subscript[e, 1] -> -((r*d[r])/Sqrt[1 - k*r^2]) + r^2*d[t], Subscript[e, 2] -> d[r]/(2*r*Sqrt[1 - k*r^2]) + d[t]/2, Subscript[e, 3] -> ((-I)*r*d[\[Theta]]*Sqrt[f[t]])/Sqrt[2] - (r*d[\[Phi]]*Sqrt[f[t]]*Sin[\[Theta]])/Sqrt[2], Subscript[e, 4] -> (I*r*d[\[Theta]]*Sqrt[f[t]])/Sqrt[2] - (r*d[\[Phi]]*Sqrt[f[t]]*Sin[\[Theta]])/Sqrt[2]}
[e[1] = -r/(1-k*r^2)^(1/2)*d(r)+r^2*d(t), e[2] = 1/2/r/(1-k*r^2)^(1/2)*d(r)+1/2*d(t), e[3] = -1/2*I*2^(1/2)*r*d(theta)*f(t)^(1/2)-1/2*2^(1/2)*r*d(phi)*f(t)^(1/2)*sin(theta), e[4] = 1/2*I*2^(1/2)*r*d(theta)*f(t)^(1/2)-1/2*2^(1/2)*r*d(phi)*f(t)^(1/2)*sin(theta)]

Metric

Metric of Gutman Bespal Ko Space Covariant NP Tetrad
\left\{g\to e_1\otimes e_2+e_2\otimes e_1-e_3\otimes e_4-e_4\otimes e_3\right\}
<math> <mrow> <mo>{</mo> <mrow> <mi>g</mi> <semantics> <mo>&#8594;</mo> <annotation encoding='Mathematica'>&quot;\[Rule]&quot;</annotation> </semantics> <mrow> <mrow> <msub> <mi>e</mi> <mn>1</mn> </msub> <mo>&#8855;</mo> <msub> <mi>e</mi> <mn>2</mn> </msub> </mrow> <mo>+</mo> <mrow> <msub> <mi>e</mi> <mn>2</mn> </msub> <mo>&#8855;</mo> <msub> <mi>e</mi> <mn>1</mn> </msub> </mrow> <mo>-</mo> <mrow> <msub> <mi>e</mi> <mn>3</mn> </msub> <mo>&#8855;</mo> <msub> <mi>e</mi> <mn>4</mn> </msub> </mrow> <mo>-</mo> <mrow> <msub> <mi>e</mi> <mn>4</mn> </msub> <mo>&#8855;</mo> <msub> <mi>e</mi> <mn>3</mn> </msub> </mrow> </mrow> </mrow> <mo>}</mo> </mrow> </math>
{g -> Subscript[e, 1] \[CircleTimes] Subscript[e, 2] + Subscript[e, 2] \[CircleTimes] Subscript[e, 1] - Subscript[e, 3] \[CircleTimes] Subscript[e, 4] - Subscript[e, 4] \[CircleTimes] Subscript[e, 3]}
[g = `&.`(e[1],e[2])+`&.`(e[2],e[1])-`&.`(e[3],e[4])-`&.`(e[4],e[3])]

Constraints

Constraints of Gutman Bespal Ko Space Covariant NP Tetrad
\left\{f(t)\to \frac{1}{2} G e^{2 t}+\frac{1}{2} H e^{-2 t}+\frac{1}{2}\right\}
<math> <mrow> <mo>{</mo> <mrow> <mrow> <mi>f</mi> <mo>&#8289;</mo> <mo>(</mo> <mi>t</mi> <mo>)</mo> </mrow> <semantics> <mo>&#8594;</mo> <annotation encoding='Mathematica'>&quot;\[Rule]&quot;</annotation> </semantics> <mrow> <mrow> <mfrac> <mn>1</mn> <mn>2</mn> </mfrac> <mo>&#8290;</mo> <mi>G</mi> <mo>&#8290;</mo> <msup> <mi>&#8519;</mi> <mrow> <mn>2</mn> <mo>&#8290;</mo> <mi>t</mi> </mrow> </msup> </mrow> <mo>+</mo> <mrow> <mfrac> <mn>1</mn> <mn>2</mn> </mfrac> <mo>&#8290;</mo> <mi>H</mi> <mo>&#8290;</mo> <msup> <mi>&#8519;</mi> <mrow> <mrow> <mo>-</mo> <mn>2</mn> </mrow> <mo>&#8290;</mo> <mi>t</mi> </mrow> </msup> </mrow> <mo>+</mo> <mfrac> <mn>1</mn> <mn>2</mn> </mfrac> </mrow> </mrow> <mo>}</mo> </mrow> </math>
{f[t] -> 1/2 + (E^(2*t)*G)/2 + H/(2*E^(2*t))}
[f(t) = 1/2+1/2*exp(2*t)*G+1/2*exp(-2*t)*H]

Constants

Constants of Gutman Bespal Ko Space Covariant NP Tetrad
\{G,H,k\}
<math> <mrow> <mo>{</mo> <mrow> <mi>G</mi> <mo>,</mo> <mi>H</mi> <mo>,</mo> <mi>k</mi> </mrow> <mo>}</mo> </mrow> </math>
{G, H, k}
[G, H, k]

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Exact Solutions of Einstein's Field Equations: Gutman Bespal Ko Space Covariant NP Tetrad from Differential Geometry Library. http://digi-area.com/DifferentialGeometryLibrary/ExactSolutionsofEinsteinsFieldEquations/Gutman-Bespal-Ko-Space-Covariant-NP-Tetrad.php

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