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The Paczynski-Wiita potential: A step-by-step "derivation"
High Energy Astrophysical Phenomena · Submitted 6 Apr 2009
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim The gravitational part differs from the Paczynski-Wiita potential only by a constant.
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The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
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The abstract, sentence by sentence
Paczynski realized that a properly chosen gravitational potential may accurately model (in a "pseudo Newtonian" theory) general relativistic effects that determine motion of matter near a non-rotating black hole. Paczynski's choice, known today as the "Paczynski-Wiita potential", proved to be very practical. It was used by numerous researchers in the black hole accretion theory, and became a standard tool in relativistic astrophysics. The model is an example of Paczynski's admired ability to invent "out of nowhere" simple ideas that were brilliant, deep and useful. Paczynski has guessed intuitively the form of the potential. However, it could be also derived by a a step-by-step formal procedure. I show the derivation here. My derivation is based on a standard definition of the relativistic "effective potential" in the Schwarzschild spacetime. The relativistic effective potential may be uniquely divided into its "gravitational" and "centrifugal" part. The gravitational part differs from the Paczynski-Wiita potential only by a constant.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Paczynski realized that a properly chosen gravitational potential may accurately model (in a "pseudo Newtonian" theory) general relativistic effects that determine motion of matter near a non-rotating black hole. | background 1.00 | 0.04 | 0.13 | hedged possibility 0.94 |
| s1 | Paczynski's choice, known today as the "Paczynski-Wiita potential", proved to be very practical. | background 0.97 | 0.05 | 0.09 | asserted 1.00 |
| s2 | It was used by numerous researchers in the black hole accretion theory, and became a standard tool in relativistic astrophysics. | background 1.00 | 0.04 | 0.07 | asserted 1.00 |
| s3 | The model is an example of Paczynski's admired ability to invent "out of nowhere" simple ideas that were brilliant, deep and useful. | background 0.68 | 0.06 | 0.06 | asserted 1.00 |
| s4 | Paczynski has guessed intuitively the form of the potential. | background 0.92 | 0.06 | 0.07 | asserted 0.99 |
| s5 | However, it could be also derived by a a step-by-step formal procedure. | contribution 0.47 | 0.29 | 0.17 | hedged possibility 0.99 |
| s6 | I show the derivation here. | contribution 0.97 | 0.94 | 0.07 | asserted 0.99 |
| s7 | My derivation is based on a standard definition of the relativistic "effective potential" in the Schwarzschild spacetime. | method 0.99 | 0.68 | 0.08 | asserted 0.99 |
| s8 | The relativistic effective potential may be uniquely divided into its "gravitational" and "centrifugal" part. | method 0.84 | 0.35 | 0.13 | hedged possibility 0.94 |
| s9 | The gravitational part differs from the Paczynski-Wiita potential only by a constant. | result 0.97 | 0.73 | 0.53 | asserted 1.00 |
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The paper
Original abstract
Paczynski realized that a properly chosen gravitational potential may accurately model (in a "pseudo Newtonian" theory) general relativistic effects that determine motion of matter near a non-rotating black hole. Paczynski's choice, known today as the "Paczynski-Wiita potential", proved to be very practical. It was used by numerous researchers in the black hole accretion theory, and became a standard tool in relativistic astrophysics. The model is an example of Paczynski's admired ability to invent "out of nowhere" simple ideas that were brilliant, deep and useful. Paczynski has guessed intuitively the form of the potential. However, it could be also derived by a a step-by-step formal procedure. I show the derivation here. My derivation is based on a standard definition of the relativistic "effective potential" in the Schwarzschild spacetime. The relativistic effective potential may be uniquely divided into its "gravitational" and "centrifugal" part. The gravitational part differs from the Paczynski-Wiita potential only by a constant.
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How the literature uses it
1 arXiv paper cite this in 4 sentences
Papers citing it · 3 sentences without a confident label
Cites it as background 1 paper
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Since these motions can be quite complicated, pseudo-Newtonian potentials have been introduced that give an effective simplified description of timelike geodesics around Schwarzschild and Kerr black holes [ref] .
Spherical inhomogeneous solutions of Einstein and scalar-tensor gravity: a map of the land · Introduction · 0.90
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