File:Kerr-surfaces.png
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Kerr-surfaces.png
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Contents
Summary
DescriptionKerr-surfaces.png |
English: Event horizons and ergospheres of a rotating black hole (spin parameter a=Jc/G/M²=0.99); the ring-singularity is located at the equatorial kink of the inner ergosphere at R=a.
Deutsch: Ereignishorizonte und Ergosphären eines mit dem Spinparameter a=Jc/G/M²=0.99 rotierenden schwarzen Lochs. Die Ringsingularität liegt an der äquatorialen Ausbuchtung der inneren Ergosphäre bei R=a. |
Date | |
Source | Own work (source) |
Author | Yukterez (Simon Tyran, Vienna) |
Other versions |
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Code
rE=1+Sqrt[1-a^2 Cos[θ]^2]; RE[A_]:={Sqrt[rE^2+A^2] Sin[θ]Cos[φ],Sqrt[rE^2+A^2] Sin[θ]Sin[φ],rE Cos[θ]}; (* outer ergosphere *) rG=1-Sqrt[1-a^2 Cos[θ]^2]; RG[A_]:={Sqrt[rG^2+A^2] Sin[θ]Cos[φ],Sqrt[rG^2+A^2] Sin[θ]Sin[φ],rG Cos[θ]}; (* inner ergosphere *) rA=1+Sqrt[1-a^2]; RA[A_]:={Sqrt[rA^2+A^2] Sin[θ]Cos[φ],Sqrt[rA^2+A^2] Sin[θ]Sin[φ],rA Cos[θ]}; (* outer horizon *) rI=1-Sqrt[1-a^2]; RI[A_]:={Sqrt[rI^2+A^2] Sin[θ]Cos[φ],Sqrt[rI^2+A^2] Sin[θ]Sin[φ],rI Cos[θ]}; (* inner horizon *) p[f_, c_]:=ParametricPlot3D[f, {φ, 0, 2 π}, {θ, 0, π}, PlotStyle -> Directive[c, Opacity[0.15]]] (* plotfunction *) Do[Print[Show[p[RE[a], Blue], p[RA[a], Cyan], p[RI[a], Orange], p[RG[a], Red]], {a,0,1,0.1}]] (* cartesian, x,y,z *) Do[Print[Show[p[RE[0], Blue], p[RA[0], Cyan], p[RI[0], Orange], p[RG[0], Red]], {a,0,1,0.1}]] (* pseudospherical, r,θ,Ф *)
Comparison
- Boyer-Lindquist: doi:10.1139/p81-086 Nigel Sharp: On embeddings of the Kerr geometry; page 3, figure 3
- Kerr-Schild: Matt Visser: The Kerr spacetime, A brief introduction; page 35, figure 3
- Source: kerr.yukterez.net / kerr.newman.yukterez.net
Licensing
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25 June 2017
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588 pixel
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df5780df94d1245cf657e8a89dec646c7abc5bbe
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Date/Time | Thumbnail | Dimensions | User | Comment | |
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current | 08:18, 29 August 2021 | 800 × 588 (60 KB) | wikimediacommons>Yukterez | pointing the arrows to the outer edges of the surfaces to avoid 2D/3D confusions |
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