Fasciculus:Kerr.black.hole.shadow.and.horizons.gif

Kerr.black.hole.shadow.and.horizons.gif(408 × 332 elementa imaginalia, magnitudo fasciculi: 695 chiliocteti, typus MIME: image/gif, looped, 200 repla, 13 s)

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Summarium

Descriptio
English: Shadow (black) & horizons and ergospheres (white) of a rotating black hole. The dimensionless spin parameter a/M=Jc/G/M² is running from 0 to 1. Units: G=M=c=1 (lengths are in GM/c²). The observer is assumed to be far away from the black hole and stationary with respect to the fixed stars.[1][2][3][4][5][6]
Datum
Fons Opus proprium, Code
Auctor Yukterez (Simon Tyran, Vienna)
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Equations

Natural dimensionless units:

Inner (-) and outer (+) ergospheres:

Inner (-) and outer (+) horizons:

Shadow contours:

Limaςon parameter series expansion:

Fourier transformation for the observer's inclination angle θ:

Code: Source (Mathematica Syntax)

References

  1. Andreas de Vries: Shadows of rotating black holes
  2. Hung-Yi Pu, Kiyun Yun, Ziri Younsi, Suk Jin Yoon: Odyssey
  3. Max Planck Institute: Scientists to image event horizon of black hole
  4. Claudio Paganini, Blazej Ruba, Marius Oancea: Null Geodesics on Kerr Spacetimes
  5. Naoki Tsukamoto: Kerr-Newman and rotating regular black hole shadows in flat spacetime
  6. Grenzebach, Perlick & Lämmerzahl: Photon Regions and Shadows of Kerr–Newman–NUT Black Holes

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Captions

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Contours of the observed shadow and the invisible surfaces of a rotating black hole

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2 Novembris 2017

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