Surfaces of infinite red-shift around a uniformly accelerating and rotating particle
The structure of the surfaces of infinite red-shift that are formed about an accelerating Kerr-type particle is studied. It is shown that for nonzero acceleration and rotation there exist three relevant surfaces of infinite red-shift. One of these surfaces is analogous to the Schwarzschild surface a...
Gespeichert in:
Veröffentlicht in: | Phys. Rev., D; (United States) D; (United States), 1980-01, Vol.21 (8), p.2064-2074 |
---|---|
Hauptverfasser: | , |
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
Online-Zugang: | Volltext |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
container_end_page | 2074 |
---|---|
container_issue | 8 |
container_start_page | 2064 |
container_title | Phys. Rev., D; (United States) |
container_volume | 21 |
creator | Farhoosh, Hamid Zimmerman, Robert L. |
description | The structure of the surfaces of infinite red-shift that are formed about an accelerating Kerr-type particle is studied. It is shown that for nonzero acceleration and rotation there exist three relevant surfaces of infinite red-shift. One of these surfaces is analogous to the Schwarzschild surface and is mainly a consequence of the mass. The acceleration causes this surface to expand in the forward direction and contract in the backward direction. In addition, the rotation causes the Schwarzschild surface to contract both in the forward and backward directions. The second surface is mainly due to the acceleration and is called the Rindler surface. It has a shape similar to a parabola of revolution. As the acceleration increases, the Rindler surface moves inward, approaching the Schwarzschild surface. Rotation causes the Rindler surface to contract slightly in the equatorial plane. As the acceleration increases to a critical value the Rindler and the Schwarzschild surfaces coincide on the equatorial plane. As the acceleration is increased further, the points of coincidence spread towards the poles. The third surface is produced mainly by the rotation and is a shape similar to the interior Kerr surface. This surface is called the Kerr surface. By increasing the rotation this surface expands in the polar regions, approaching the Schwarzschild surface. Acceleration causes this surface to distort and become elongated in the forward direction and contracted in the backward direction. |
doi_str_mv | 10.1103/PhysRevD.21.2064 |
format | Article |
fullrecord | <record><control><sourceid>crossref_osti_</sourceid><recordid>TN_cdi_crossref_primary_10_1103_PhysRevD_21_2064</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>10_1103_PhysRevD_21_2064</sourcerecordid><originalsourceid>FETCH-LOGICAL-c315t-b7032c4b9a9ea95452a0e6d216ebf8d520c4cbd74a7b312c194985777d9dfdca3</originalsourceid><addsrcrecordid>eNo1kE1LAzEQhnNQsFbvHoP3rfncbY5SPyoUFK3nkJ0kNrJNSpIK_fduqb6X4WUehuFB6IaSGaWE371tDuXd_TzMGJ0x0oozNCFStg2bM3qBLkv5JmNYyydo_bHP3oArOHkcog8xVIezs03ZBF-xyWkfLTZ4H4NPeTscsAFwg8umhviFzbjMqZ7KzuQaYHBX6NybobjrvzlFn0-P68WyWb0-vyzuVw1wKmvTd4QzEL0yyhklhWSGuNYy2rrez61kBAT0thOm6zllQJVQc9l1nVXWWzB8im5Pd1OpQRcYX4cNpBgdVC2FkKpVI0ROEORUSnZe73LYmnzQlOijLv2vSzOqj7r4L3YFYtk</addsrcrecordid><sourcetype>Open Access Repository</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype></control><display><type>article</type><title>Surfaces of infinite red-shift around a uniformly accelerating and rotating particle</title><source>American Physical Society Journals</source><creator>Farhoosh, Hamid ; Zimmerman, Robert L.</creator><creatorcontrib>Farhoosh, Hamid ; Zimmerman, Robert L. ; Department of Physics and Institute of Theoretical Science, University of Oregon, Eugene, Oregon 97403</creatorcontrib><description>The structure of the surfaces of infinite red-shift that are formed about an accelerating Kerr-type particle is studied. It is shown that for nonzero acceleration and rotation there exist three relevant surfaces of infinite red-shift. One of these surfaces is analogous to the Schwarzschild surface and is mainly a consequence of the mass. The acceleration causes this surface to expand in the forward direction and contract in the backward direction. In addition, the rotation causes the Schwarzschild surface to contract both in the forward and backward directions. The second surface is mainly due to the acceleration and is called the Rindler surface. It has a shape similar to a parabola of revolution. As the acceleration increases, the Rindler surface moves inward, approaching the Schwarzschild surface. Rotation causes the Rindler surface to contract slightly in the equatorial plane. As the acceleration increases to a critical value the Rindler and the Schwarzschild surfaces coincide on the equatorial plane. As the acceleration is increased further, the points of coincidence spread towards the poles. The third surface is produced mainly by the rotation and is a shape similar to the interior Kerr surface. This surface is called the Kerr surface. By increasing the rotation this surface expands in the polar regions, approaching the Schwarzschild surface. Acceleration causes this surface to distort and become elongated in the forward direction and contracted in the backward direction.</description><identifier>ISSN: 0556-2821</identifier><identifier>DOI: 10.1103/PhysRevD.21.2064</identifier><language>eng</language><publisher>United States</publisher><subject>657003 - Theoretical & Mathematical Physics- Relativity & Gravitation ; ACCELERATION ; CLASSICAL AND QUANTUM MECHANICS, GENERAL PHYSICS ; EINSTEIN FIELD EQUATIONS ; EQUATIONS ; EQUIVALENCE PRINCIPLE ; FIELD EQUATIONS ; KERR METRIC ; METRICS ; MOTION ; RED SHIFT ; ROTATION ; SCHWARZSCHILD METRIC ; VACUUM STATES</subject><ispartof>Phys. Rev., D; (United States), 1980-01, Vol.21 (8), p.2064-2074</ispartof><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c315t-b7032c4b9a9ea95452a0e6d216ebf8d520c4cbd74a7b312c194985777d9dfdca3</citedby><cites>FETCH-LOGICAL-c315t-b7032c4b9a9ea95452a0e6d216ebf8d520c4cbd74a7b312c194985777d9dfdca3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,885,2874,2875,27923,27924</link.rule.ids><backlink>$$Uhttps://www.osti.gov/biblio/5445969$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Farhoosh, Hamid</creatorcontrib><creatorcontrib>Zimmerman, Robert L.</creatorcontrib><creatorcontrib>Department of Physics and Institute of Theoretical Science, University of Oregon, Eugene, Oregon 97403</creatorcontrib><title>Surfaces of infinite red-shift around a uniformly accelerating and rotating particle</title><title>Phys. Rev., D; (United States)</title><description>The structure of the surfaces of infinite red-shift that are formed about an accelerating Kerr-type particle is studied. It is shown that for nonzero acceleration and rotation there exist three relevant surfaces of infinite red-shift. One of these surfaces is analogous to the Schwarzschild surface and is mainly a consequence of the mass. The acceleration causes this surface to expand in the forward direction and contract in the backward direction. In addition, the rotation causes the Schwarzschild surface to contract both in the forward and backward directions. The second surface is mainly due to the acceleration and is called the Rindler surface. It has a shape similar to a parabola of revolution. As the acceleration increases, the Rindler surface moves inward, approaching the Schwarzschild surface. Rotation causes the Rindler surface to contract slightly in the equatorial plane. As the acceleration increases to a critical value the Rindler and the Schwarzschild surfaces coincide on the equatorial plane. As the acceleration is increased further, the points of coincidence spread towards the poles. The third surface is produced mainly by the rotation and is a shape similar to the interior Kerr surface. This surface is called the Kerr surface. By increasing the rotation this surface expands in the polar regions, approaching the Schwarzschild surface. Acceleration causes this surface to distort and become elongated in the forward direction and contracted in the backward direction.</description><subject>657003 - Theoretical & Mathematical Physics- Relativity & Gravitation</subject><subject>ACCELERATION</subject><subject>CLASSICAL AND QUANTUM MECHANICS, GENERAL PHYSICS</subject><subject>EINSTEIN FIELD EQUATIONS</subject><subject>EQUATIONS</subject><subject>EQUIVALENCE PRINCIPLE</subject><subject>FIELD EQUATIONS</subject><subject>KERR METRIC</subject><subject>METRICS</subject><subject>MOTION</subject><subject>RED SHIFT</subject><subject>ROTATION</subject><subject>SCHWARZSCHILD METRIC</subject><subject>VACUUM STATES</subject><issn>0556-2821</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1980</creationdate><recordtype>article</recordtype><recordid>eNo1kE1LAzEQhnNQsFbvHoP3rfncbY5SPyoUFK3nkJ0kNrJNSpIK_fduqb6X4WUehuFB6IaSGaWE371tDuXd_TzMGJ0x0oozNCFStg2bM3qBLkv5JmNYyydo_bHP3oArOHkcog8xVIezs03ZBF-xyWkfLTZ4H4NPeTscsAFwg8umhviFzbjMqZ7KzuQaYHBX6NybobjrvzlFn0-P68WyWb0-vyzuVw1wKmvTd4QzEL0yyhklhWSGuNYy2rrez61kBAT0thOm6zllQJVQc9l1nVXWWzB8im5Pd1OpQRcYX4cNpBgdVC2FkKpVI0ROEORUSnZe73LYmnzQlOijLv2vSzOqj7r4L3YFYtk</recordid><startdate>19800101</startdate><enddate>19800101</enddate><creator>Farhoosh, Hamid</creator><creator>Zimmerman, Robert L.</creator><scope>AAYXX</scope><scope>CITATION</scope><scope>OTOTI</scope></search><sort><creationdate>19800101</creationdate><title>Surfaces of infinite red-shift around a uniformly accelerating and rotating particle</title><author>Farhoosh, Hamid ; Zimmerman, Robert L.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c315t-b7032c4b9a9ea95452a0e6d216ebf8d520c4cbd74a7b312c194985777d9dfdca3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1980</creationdate><topic>657003 - Theoretical & Mathematical Physics- Relativity & Gravitation</topic><topic>ACCELERATION</topic><topic>CLASSICAL AND QUANTUM MECHANICS, GENERAL PHYSICS</topic><topic>EINSTEIN FIELD EQUATIONS</topic><topic>EQUATIONS</topic><topic>EQUIVALENCE PRINCIPLE</topic><topic>FIELD EQUATIONS</topic><topic>KERR METRIC</topic><topic>METRICS</topic><topic>MOTION</topic><topic>RED SHIFT</topic><topic>ROTATION</topic><topic>SCHWARZSCHILD METRIC</topic><topic>VACUUM STATES</topic><toplevel>online_resources</toplevel><creatorcontrib>Farhoosh, Hamid</creatorcontrib><creatorcontrib>Zimmerman, Robert L.</creatorcontrib><creatorcontrib>Department of Physics and Institute of Theoretical Science, University of Oregon, Eugene, Oregon 97403</creatorcontrib><collection>CrossRef</collection><collection>OSTI.GOV</collection><jtitle>Phys. Rev., D; (United States)</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Farhoosh, Hamid</au><au>Zimmerman, Robert L.</au><aucorp>Department of Physics and Institute of Theoretical Science, University of Oregon, Eugene, Oregon 97403</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Surfaces of infinite red-shift around a uniformly accelerating and rotating particle</atitle><jtitle>Phys. Rev., D; (United States)</jtitle><date>1980-01-01</date><risdate>1980</risdate><volume>21</volume><issue>8</issue><spage>2064</spage><epage>2074</epage><pages>2064-2074</pages><issn>0556-2821</issn><abstract>The structure of the surfaces of infinite red-shift that are formed about an accelerating Kerr-type particle is studied. It is shown that for nonzero acceleration and rotation there exist three relevant surfaces of infinite red-shift. One of these surfaces is analogous to the Schwarzschild surface and is mainly a consequence of the mass. The acceleration causes this surface to expand in the forward direction and contract in the backward direction. In addition, the rotation causes the Schwarzschild surface to contract both in the forward and backward directions. The second surface is mainly due to the acceleration and is called the Rindler surface. It has a shape similar to a parabola of revolution. As the acceleration increases, the Rindler surface moves inward, approaching the Schwarzschild surface. Rotation causes the Rindler surface to contract slightly in the equatorial plane. As the acceleration increases to a critical value the Rindler and the Schwarzschild surfaces coincide on the equatorial plane. As the acceleration is increased further, the points of coincidence spread towards the poles. The third surface is produced mainly by the rotation and is a shape similar to the interior Kerr surface. This surface is called the Kerr surface. By increasing the rotation this surface expands in the polar regions, approaching the Schwarzschild surface. Acceleration causes this surface to distort and become elongated in the forward direction and contracted in the backward direction.</abstract><cop>United States</cop><doi>10.1103/PhysRevD.21.2064</doi><tpages>11</tpages></addata></record> |
fulltext | fulltext |
identifier | ISSN: 0556-2821 |
ispartof | Phys. Rev., D; (United States), 1980-01, Vol.21 (8), p.2064-2074 |
issn | 0556-2821 |
language | eng |
recordid | cdi_crossref_primary_10_1103_PhysRevD_21_2064 |
source | American Physical Society Journals |
subjects | 657003 - Theoretical & Mathematical Physics- Relativity & Gravitation ACCELERATION CLASSICAL AND QUANTUM MECHANICS, GENERAL PHYSICS EINSTEIN FIELD EQUATIONS EQUATIONS EQUIVALENCE PRINCIPLE FIELD EQUATIONS KERR METRIC METRICS MOTION RED SHIFT ROTATION SCHWARZSCHILD METRIC VACUUM STATES |
title | Surfaces of infinite red-shift around a uniformly accelerating and rotating particle |
url | https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-12T02%3A40%3A22IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-crossref_osti_&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Surfaces%20of%20infinite%20red-shift%20around%20a%20uniformly%20accelerating%20and%20rotating%20particle&rft.jtitle=Phys.%20Rev.,%20D;%20(United%20States)&rft.au=Farhoosh,%20Hamid&rft.aucorp=Department%20of%20Physics%20and%20Institute%20of%20Theoretical%20Science,%20University%20of%20Oregon,%20Eugene,%20Oregon%2097403&rft.date=1980-01-01&rft.volume=21&rft.issue=8&rft.spage=2064&rft.epage=2074&rft.pages=2064-2074&rft.issn=0556-2821&rft_id=info:doi/10.1103/PhysRevD.21.2064&rft_dat=%3Ccrossref_osti_%3E10_1103_PhysRevD_21_2064%3C/crossref_osti_%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_id=info:pmid/&rfr_iscdi=true |