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Spaghettification

From Wikipedia, the free encyclopedia
Phenomenon in astrophysics
For the computer programming term, seeSpaghetti code.

Astronaut falling into a black hole (schematic illustration of the spaghettification effect)
Tidal forces acting on a spherical body in a non-homogeneousgravitational field. In this diagram, the gravitational force originates from a source to the right. It shows both the tidal field (thick red arrows) and the gravity field (thin blue arrows) exerted on the body's surface and center (label O) by a source (label S).

Inastrophysics,spaghettification,[1] ornoodle effect[2] is the vertical stretching and horizontal compression of objects into long thin shapes in a very strong, non-homogeneousgravitational field. The term was popularized byStephen Hawking who described the flight of a fictionalastronaut who, passing within a black hole'sevent horizon, is "stretched like spaghetti".[3][4] It is caused by extremetidal forces. In the most extreme cases, near ablack hole, the stretching and compression are so powerful that no object can resist it. Within a small region, the horizontal compression balances the vertical stretching so that a small object being spaghettified experiences no net change in volume. If one were to fall into a black hole feet first, the gravity at their feet would be much stronger than at their head, causing the person to be vertically stretched. Along with that, the right side of the body will be pulled to the left, and the left side of the body will be pulled to the right, horizontally compressing the person.[5]

A simple example

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The spaghettification of four objects falling towards a planet

The concept can be illustrated with four objects in space above a planet, positioned in a diamond formation. The force on each object is directed towards the planets center. In accordance with theinverse-square law, the lowest of the four objects experiences the biggest gravitational acceleration, and two objects on each side are pulled towards each other, so that the whole formation becomes stretched along the line to the planet and compressed transversely.[3]

If these four objects are connected parts of a larger rigid object, then it will resist distortion. Internal elastic forces develop as the body distorts to balance the tidal forces, to maintainmechanical equilibrium. If the tidal forces become too large, the body may yield creating a narrow line of broken pieces.

The forces responsible for spaghettification are calledtidal forces. The radial tidal force across an object of massm and sizeΔr{\displaystyle \Delta r} at a distancer from an object of massM can be estimated withNewton's law of gravity:ΔF=Δr2GmMr3{\displaystyle \Delta F=\Delta r{\frac {2GmM}{r^{3}}}}whereG is thegravitational constant.[3]

Relation to the event horizon

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Spaghettification of a star by a supermassive black hole[6]

The point at which tidal forces destroy an object or kill a person is proportional to the black hole's mass. This point is not the event horizon. For asupermassive black hole, such as those found at a galaxy's center, this point lies within theevent horizon, so an astronaut may cross the event horizon without noticing any squashing and pulling, although it remains only a matter of time, as once inside an event horizon, falling towards the center is inevitable.[7] Stellar black holes have much higher spacetime curvature at their event horizon, so the tidal forces would spaghettify the astronaut before the event horizon.[8][9]

References

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  1. ^Calder, Nigel (1977).The Key to the Universe: A Report on the New Physics.Viking Press. p. 143.ISBN 978-0-67041270-9. RetrievedJuly 10, 2022. Published as a companion to theBBC TV documentaryThe Key to the Universe.
  2. ^Wheeler, J. Craig (2007).Cosmic catastrophes: exploding stars, black holes, and mapping the universe (2nd ed.). Cambridge; New York: Cambridge University Press. p. 182.ISBN 978-0-521-85714-7.OCLC 73954922.
  3. ^abcPinochet, Jorge (July 1, 2022)."The little robot, black holes, and spaghettification".Physics Education.57 (4): 045008.arXiv:2203.04759.doi:10.1088/1361-6552/ac5727.ISSN 0031-9120.
  4. ^Hawking, Stephen (1988).A Brief History of Time. Bantam Dell Publishing Group. p. 256.ISBN 978-0-553-10953-5.
  5. ^Fraknoi, Andrew;Morrison, David;C. Wolff, Sidney (2016).Astronomy. OpenStax. p. 862.ISBN 9781938168284.
  6. ^Price, Daniel J.; Liptai, David; Mandel, Ilya; Shepherd, Joanna; Lodato, Giuseppe; Levin, Yuri (2024)."Eddington Envelopes: The Fate of Stars on Parabolic Orbits Tidally Disrupted by Supermassive Black Holes".The Astrophysical Journal Letters.971 (2): L46.arXiv:2404.09381.Bibcode:2024ApJ...971L..46P.doi:10.3847/2041-8213/ad6862.
  7. ^Hawley, John Frederick; Holcomb, Katherine A. (2005).Foundations of modern cosmology (2nd ed.). Oxford; New York: Oxford University Press. p. 253.ISBN 978-0-19-853096-1.
  8. ^Hobson, Michael Paul; Efstathiou, Georges; Lasenby, Anthony N. (2006).General relativity: an introduction for physicists. Cambridge: Cambridge University Press. p. 265.ISBN 978-0-521-82951-9.
  9. ^Kutner, Marc L. (2003).Astronomy: a physical perspective (2nd ed.). Cambridge: Cambridge University Press. p. 150.ISBN 978-0-521-52927-3.

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