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Stationary spacetime

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arises for rotating sources due to the rotational kinetic energy which, because of mass–energy equivalence, can also act as the source of a gravitational field. The situation is analogous to a static electromagnetic field where one has two sets of potentials, electric and magnetic. In general
338: 684: 1555: 1291: 2154: 1884: 1615: 578: 1364: 756:. The twist vector measures the extent to which the Killing vector fails to be orthogonal to a family of 3-surfaces. A non-zero twist indicates the presence of rotation in the spacetime geometry. 754: 2268: 502: 907: 985: 2059: 1218: 1191: 607:
is a 3-vector, called the twist vector, which vanishes when the Killing vector is hypersurface orthogonal. The latter arises as the spatial components of the twist 4-vector
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and are consequently independent of time. Thus, the geometry of a stationary spacetime does not change in time. In the special case
1561: 527: 146:, may be chosen so that they are all independent of the time coordinate. The line element of a stationary spacetime has the form 1322: 2270:
the corresponding Ricci scalar. These equations form the starting point for investigating exact stationary vacuum metrics.
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it is more convenient to use the two Hansen potentials, the mass and angular momentum potentials,
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plays the role of the Newtonian gravitational potential. A nontrivial angular momentum potential
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The coordinate representation described above has an interesting geometrical interpretation. The
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is the metric tensor of 3-dimensional space. In this coordinate system the Killing vector field
333:{\displaystyle ds^{2}=\lambda (dt-\omega _{i}\,dy^{i})^{2}-\lambda ^{-1}h_{ij}\,dy^{i}\,dy^{j},} 1685: 1650: 1623: 1439: 1412: 679:{\displaystyle \omega _{\mu }=e_{\mu \nu \rho \sigma }\xi ^{\nu }\nabla ^{\rho }\xi ^{\sigma }} 50: 2302: 1372: 1010: 507: 1676: 1392: 1299: 1758: 1057: 393: 806: 366: 1785:. In terms of these quantities the Einstein vacuum field equations can be put in the form 8: 1712: 1738: 1087: 990: 932: 912: 860: 840: 786: 766: 346: 82: 2309: 2279: 1142: 1138: 760: 102: 1550:{\displaystyle \Phi _{M}={\frac {1}{4}}\lambda ^{-1}(\lambda ^{2}+\omega ^{2}-1),} 1682:
A stationary vacuum metric is thus expressible in terms of the Hansen potentials
98: 1286:{\displaystyle \nabla _{\mu }\omega _{\nu }-\nabla _{\nu }\omega _{\mu }=0,\,} 2354: 2149:{\displaystyle \Phi ^{2}=\Phi _{A}\Phi _{A}=(\Phi _{M}^{2}+\Phi _{J}^{2})} 686:(see, for example, p. 163) which is orthogonal to the Killing vector 1146: 524:
is a positive scalar representing the norm of the Killing vector, i.e.,
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Spacetime that admits a Killing vector that is asymptotically timelike
1879:{\displaystyle (h^{ij}\nabla _{i}\nabla _{j}-2R^{(3)})\Phi _{A}=0,\,} 90: 1157:
In a stationary spacetime satisfying the vacuum Einstein equations
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is stationary, but the converse is not generally true, as the
1610:{\displaystyle \Phi _{J}={\frac {1}{2}}\lambda ^{-1}\omega .} 2324:
Wald, R.M., (1984). General Relativity, (U. Chicago Press)
573:{\displaystyle \lambda =g_{\mu \nu }\xi ^{\mu }\xi ^{\nu }} 763:
Killing vector generates a one-parameter group of motion
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In a stationary spacetime, the metric tensor components,
1359:{\displaystyle \omega _{\mu }=\nabla _{\mu }\omega .\,} 877:. This identification, called a canonical projection, 2203: 2162: 2070: 1893: 1794: 1761: 1741: 1715: 1688: 1653: 1626: 1564: 1472: 1442: 1415: 1395: 1375: 1325: 1302: 1229: 1199: 1163: 1110: 1090: 1060: 1033: 1013: 993: 955: 935: 915: 883: 863: 843: 809: 789: 769: 719: 692: 613: 586: 530: 510: 453: 426: 396: 369: 349: 204: 152: 122: 2262: 2189: 2148: 2053: 1878: 1777: 1747: 1727: 1701: 1666: 1639: 1609: 1549: 1455: 1428: 1401: 1381: 1358: 1308: 1296:and is therefore locally the gradient of a scalar 1285: 1212: 1185: 1129: 1096: 1076: 1046: 1019: 999: 979: 941: 921: 901: 869: 849: 829: 795: 775: 748: 705: 678: 599: 572: 516: 496: 439: 412: 382: 355: 332: 188: 138: 2352: 1153:Use as starting point for vacuum field equations 2197:is the Ricci tensor of the spatial metric and 2345:Hansen, R.O. (1974). J. Math. Phys. 15, 46. 909:is a mapping that sends each trajectory in 749:{\displaystyle \omega _{\mu }\xi ^{\mu }=0} 111: 2333:Geroch, R., (1971). J. Math. Phys. 12, 918 2263:{\displaystyle R^{(3)}=h^{ij}R_{ij}^{(3)}} 857:represents a trajectory in the spacetime 1875: 1620:In general relativity the mass potential 1355: 1282: 313: 299: 246: 69:Learn how and when to remove this message 2341: 2339: 2305:General Relativity: A Geometric Approach 1193:outside the sources, the twist 4-vector 32:This article includes a list of general 1675:relativity, rotating sources produce a 2353: 390:are the three spatial coordinates and 2336: 837:, the quotient space. Each point of 497:{\displaystyle \xi ^{\mu }=(1,0,0,0)} 18: 902:{\displaystyle \pi :M\rightarrow V} 13: 2307:, Cambridge University Press, 1999 2129: 2111: 2095: 2085: 2072: 2036: 2026: 2016: 2006: 1983: 1958: 1948: 1938: 1928: 1857: 1822: 1812: 1690: 1655: 1628: 1566: 1474: 1444: 1417: 1340: 1254: 1231: 657: 38:it lacks sufficient corresponding 14: 2372: 980:{\displaystyle h=-\lambda \pi *g} 23: 2285:Spherically symmetric spacetime 2054:{\displaystyle R_{ij}^{(3)}=2,} 2327: 2318: 2296: 2255: 2249: 2215: 2209: 2182: 2176: 2143: 2107: 2045: 1993: 1970: 1924: 1913: 1907: 1853: 1848: 1842: 1795: 1679:that has no Newtonian analog. 1541: 1509: 1213:{\displaystyle \omega _{\mu }} 1186:{\displaystyle R_{\mu \nu }=0} 893: 491: 467: 261: 224: 183: 153: 1: 2290: 1130:{\displaystyle \omega _{i}=0} 1007:via pullback. The quantities 2190:{\displaystyle R_{ij}^{(3)}} 1137:the spacetime is said to be 139:{\displaystyle g_{\mu \nu }} 7: 2273: 1316:(called the twist scalar): 1149:provides a counterexample. 1047:{\displaystyle \omega _{i}} 706:{\displaystyle \xi ^{\mu }} 600:{\displaystyle \omega _{i}} 440:{\displaystyle \xi ^{\mu }} 189:{\displaystyle (i,j=1,2,3)} 10: 2377: 1702:{\displaystyle \Phi _{A}} 1667:{\displaystyle \Phi _{J}} 1640:{\displaystyle \Phi _{M}} 1456:{\displaystyle \Phi _{J}} 1429:{\displaystyle \Phi _{M}} 1382:{\displaystyle \lambda } 1020:{\displaystyle \lambda } 517:{\displaystyle \lambda } 363:is the time coordinate, 112:Description and analysis 87:Einstein field equations 1402:{\displaystyle \omega } 1369:Instead of the scalars 1309:{\displaystyle \omega } 1141:. By definition, every 53:more precise citations. 2264: 2191: 2150: 2055: 1880: 1779: 1778:{\displaystyle h_{ij}} 1749: 1729: 1703: 1668: 1641: 1611: 1551: 1457: 1430: 1403: 1383: 1360: 1310: 1287: 1214: 1187: 1131: 1098: 1078: 1077:{\displaystyle h_{ij}} 1048: 1021: 1001: 981: 943: 923: 903: 871: 851: 831: 797: 777: 750: 707: 680: 601: 574: 518: 498: 441: 414: 413:{\displaystyle h_{ij}} 384: 357: 334: 190: 140: 85:, specifically in the 2265: 2192: 2151: 2056: 1881: 1780: 1750: 1730: 1704: 1677:gravitomagnetic field 1669: 1642: 1612: 1552: 1458: 1431: 1404: 1384: 1361: 1311: 1288: 1215: 1188: 1132: 1099: 1079: 1049: 1022: 1002: 982: 949:and induces a metric 944: 924: 904: 872: 852: 832: 830:{\displaystyle V=M/G} 798: 778: 751: 708: 681: 602: 575: 519: 499: 442: 415: 385: 383:{\displaystyle y^{i}} 358: 335: 191: 141: 2361:Lorentzian manifolds 2201: 2160: 2068: 1891: 1792: 1759: 1739: 1713: 1686: 1651: 1624: 1562: 1470: 1440: 1413: 1393: 1373: 1323: 1300: 1227: 1197: 1161: 1108: 1088: 1058: 1031: 1011: 991: 953: 933: 913: 881: 861: 841: 807: 787: 767: 717: 690: 611: 584: 528: 508: 451: 424: 394: 367: 347: 202: 150: 120: 2259: 2186: 2142: 2124: 1917: 1755:) and the 3-metric 1728:{\displaystyle A=M} 447:has the components 2260: 2236: 2187: 2163: 2146: 2128: 2110: 2051: 1894: 1876: 1775: 1745: 1725: 1699: 1664: 1637: 1607: 1547: 1453: 1426: 1399: 1379: 1356: 1306: 1283: 1210: 1183: 1127: 1094: 1084:are all fields on 1074: 1044: 1017: 997: 977: 939: 919: 899: 867: 847: 827: 793: 773: 746: 713:, i.e., satisfies 703: 676: 597: 570: 514: 494: 437: 410: 380: 353: 330: 186: 136: 83:general relativity 1748:{\displaystyle J} 1586: 1494: 1097:{\displaystyle V} 1000:{\displaystyle V} 942:{\displaystyle V} 922:{\displaystyle M} 870:{\displaystyle M} 850:{\displaystyle V} 796:{\displaystyle M} 783:in the spacetime 776:{\displaystyle G} 356:{\displaystyle t} 79: 78: 71: 2368: 2346: 2343: 2334: 2331: 2325: 2322: 2316: 2300: 2280:Static spacetime 2269: 2267: 2266: 2261: 2258: 2247: 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1216: 1211: 1209: 1208: 1192: 1190: 1189: 1184: 1176: 1175: 1143:static spacetime 1136: 1134: 1133: 1128: 1120: 1119: 1103: 1101: 1100: 1095: 1083: 1081: 1080: 1075: 1073: 1072: 1053: 1051: 1050: 1045: 1043: 1042: 1026: 1024: 1023: 1018: 1006: 1004: 1003: 998: 986: 984: 983: 978: 948: 946: 945: 940: 929:onto a point in 928: 926: 925: 920: 908: 906: 905: 900: 876: 874: 873: 868: 856: 854: 853: 848: 836: 834: 833: 828: 823: 802: 800: 799: 794: 782: 780: 779: 774: 761:time translation 755: 753: 752: 747: 739: 738: 729: 728: 712: 710: 709: 704: 702: 701: 685: 683: 682: 677: 675: 674: 665: 664: 655: 654: 645: 644: 623: 622: 606: 604: 603: 598: 596: 595: 579: 577: 576: 571: 569: 568: 559: 558: 549: 548: 523: 521: 520: 515: 503: 501: 500: 495: 463: 462: 446: 444: 443: 438: 436: 435: 419: 417: 416: 411: 409: 408: 389: 387: 386: 381: 379: 378: 362: 360: 359: 354: 339: 337: 336: 331: 326: 325: 312: 311: 298: 297: 285: 284: 269: 268: 259: 258: 245: 244: 217: 216: 195: 193: 192: 187: 145: 143: 142: 137: 135: 134: 97:if it admits a 74: 67: 63: 60: 54: 49:this article by 40:inline citations 27: 26: 19: 2376: 2375: 2371: 2370: 2369: 2367: 2366: 2365: 2351: 2350: 2349: 2344: 2337: 2332: 2328: 2323: 2319: 2303:Ludvigsen, M., 2301: 2297: 2293: 2276: 2248: 2240: 2227: 2223: 2208: 2204: 2202: 2199: 2198: 2175: 2167: 2161: 2158: 2157: 2137: 2132: 2119: 2114: 2098: 2094: 2088: 2084: 2075: 2071: 2069: 2066: 2065: 2039: 2035: 2029: 2025: 2019: 2015: 2009: 2005: 1996: 1992: 1986: 1982: 1961: 1957: 1951: 1947: 1941: 1937: 1931: 1927: 1906: 1898: 1892: 1889: 1888: 1860: 1856: 1841: 1837: 1825: 1821: 1815: 1811: 1802: 1798: 1793: 1790: 1789: 1766: 1762: 1760: 1757: 1756: 1740: 1737: 1736: 1714: 1711: 1710: 1693: 1689: 1687: 1684: 1683: 1658: 1654: 1652: 1649: 1648: 1631: 1627: 1625: 1622: 1621: 1592: 1588: 1578: 1569: 1565: 1563: 1560: 1559: 1529: 1525: 1516: 1512: 1500: 1496: 1486: 1477: 1473: 1471: 1468: 1467: 1447: 1443: 1441: 1438: 1437: 1420: 1416: 1414: 1411: 1410: 1394: 1391: 1390: 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1367: 1366: 1354: 1351: 1346: 1342: 1338: 1333: 1329: 1305: 1294: 1293: 1281: 1278: 1275: 1270: 1266: 1260: 1256: 1252: 1247: 1243: 1237: 1233: 1220:is curl-free, 1207: 1203: 1182: 1179: 1174: 1171: 1167: 1154: 1151: 1126: 1123: 1118: 1114: 1093: 1071: 1068: 1064: 1041: 1037: 1016: 996: 976: 973: 970: 967: 964: 961: 958: 938: 918: 898: 895: 892: 889: 886: 866: 846: 826: 822: 818: 815: 812: 792: 772: 745: 742: 737: 733: 727: 723: 700: 696: 673: 669: 663: 659: 653: 649: 643: 640: 637: 634: 630: 626: 621: 617: 594: 590: 567: 563: 557: 553: 547: 544: 540: 536: 533: 513: 493: 490: 487: 484: 481: 478: 475: 472: 469: 466: 461: 457: 434: 430: 407: 404: 400: 377: 373: 352: 341: 340: 329: 324: 320: 316: 310: 306: 302: 296: 293: 289: 283: 280: 276: 272: 267: 263: 257: 253: 249: 243: 239: 235: 232: 229: 226: 223: 220: 215: 211: 207: 185: 182: 179: 176: 173: 170: 167: 164: 161: 158: 155: 133: 130: 126: 113: 110: 103:asymptotically 99:Killing vector 93:is said to be 77: 76: 31: 29: 22: 15: 9: 6: 4: 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1124: 1121: 1116: 1112: 1091: 1069: 1066: 1062: 1039: 1035: 1014: 994: 974: 971: 968: 965: 962: 959: 956: 936: 916: 896: 890: 887: 884: 864: 844: 824: 820: 816: 813: 810: 790: 770: 762: 757: 743: 740: 735: 731: 725: 721: 698: 694: 671: 667: 661: 651: 647: 641: 638: 635: 632: 628: 624: 619: 615: 592: 588: 565: 561: 555: 551: 545: 542: 538: 534: 531: 511: 488: 485: 482: 479: 476: 473: 470: 464: 459: 455: 432: 428: 405: 402: 398: 375: 371: 350: 327: 322: 318: 314: 308: 304: 300: 294: 291: 287: 281: 278: 274: 270: 265: 255: 251: 247: 241: 237: 233: 230: 227: 221: 218: 213: 209: 205: 198: 197: 196: 180: 177: 174: 171: 168: 165: 162: 159: 156: 131: 128: 124: 109: 107: 104: 100: 96: 92: 88: 84: 73: 70: 62: 52: 48: 42: 41: 35: 30: 21: 20: 2329: 2320: 2304: 2298: 2063: 1681: 1619: 1368: 1295: 1156: 758: 342: 115: 94: 80: 65: 56: 37: 1147:Kerr metric 51:introducing 2314:052163976X 2291:References 95:stationary 59:April 2021 34:references 2130:Φ 2112:Φ 2096:Φ 2086:Φ 2073:Φ 2037:Φ 2027:∇ 2017:Φ 2007:∇ 1998:− 1984:Φ 1968:− 1959:Φ 1949:∇ 1939:Φ 1929:∇ 1858:Φ 1832:− 1823:∇ 1813:∇ 1691:Φ 1656:Φ 1629:Φ 1602:ω 1594:− 1590:λ 1567:Φ 1536:− 1527:ω 1514:λ 1502:− 1498:λ 1475:Φ 1445:Φ 1418:Φ 1397:ω 1377:λ 1350:ω 1345:μ 1341:∇ 1332:μ 1328:ω 1304:ω 1269:μ 1265:ω 1259:ν 1255:∇ 1251:− 1246:ν 1242:ω 1236:μ 1232:∇ 1206:μ 1202:ω 1173:ν 1170:μ 1113:ω 1036:ω 1015:λ 972:∗ 969:π 966:λ 963:− 894:→ 885:π 736:μ 732:ξ 726:μ 722:ω 699:μ 695:ξ 672:σ 668:ξ 662:ρ 658:∇ 652:ν 648:ξ 642:σ 639:ρ 636:ν 633:μ 620:μ 616:ω 589:ω 566:ν 562:ξ 556:μ 552:ξ 546:ν 543:μ 532:λ 512:λ 460:μ 456:ξ 433:μ 429:ξ 279:− 275:λ 271:− 238:ω 234:− 222:λ 132:ν 129:μ 91:spacetime 2355:Category 2274:See also 106:timelike 101:that is 47:improve 2312:  2156:, and 2064:where 1139:static 580:, and 343:where 36:, but 2310:ISBN 1436:and 1389:and 1054:and 89:, a 987:on 81:In 2357:: 2338:^ 1735:, 1027:, 504:. 108:. 2256:) 2253:3 2250:( 2245:j 2242:i 2238:R 2232:j 2229:i 2225:h 2221:= 2216:) 2213:3 2210:( 2206:R 2183:) 2180:3 2177:( 2172:j 2169:i 2165:R 2144:) 2139:2 2134:J 2126:+ 2121:2 2116:M 2108:( 2105:= 2100:A 2090:A 2082:= 2077:2 2049:, 2046:] 2041:2 2031:j 2021:2 2011:i 2001:1 1994:) 1988:2 1980:4 1977:+ 1974:1 1971:( 1963:A 1953:j 1943:A 1933:i 1925:[ 1922:2 1919:= 1914:) 1911:3 1908:( 1903:j 1900:i 1896:R 1873:, 1870:0 1867:= 1862:A 1854:) 1849:) 1846:3 1843:( 1839:R 1835:2 1827:j 1817:i 1807:j 1804:i 1800:h 1796:( 1771:j 1768:i 1764:h 1743:J 1723:M 1720:= 1717:A 1709:( 1695:A 1660:J 1633:M 1605:. 1597:1 1584:2 1581:1 1576:= 1571:J 1545:, 1542:) 1539:1 1531:2 1523:+ 1518:2 1510:( 1505:1 1492:4 1489:1 1484:= 1479:M 1449:J 1422:M 1353:. 1337:= 1280:, 1277:0 1274:= 1181:0 1178:= 1166:R 1125:0 1122:= 1117:i 1092:V 1070:j 1067:i 1063:h 1040:i 995:V 975:g 960:= 957:h 937:V 917:M 897:V 891:M 888:: 865:M 845:V 825:G 821:/ 817:M 814:= 811:V 791:M 771:G 744:0 741:= 629:e 625:= 593:i 539:g 535:= 492:) 489:0 486:, 483:0 480:, 477:0 474:, 471:1 468:( 465:= 406:j 403:i 399:h 376:i 372:y 351:t 328:, 323:j 319:y 315:d 309:i 305:y 301:d 295:j 292:i 288:h 282:1 266:2 262:) 256:i 252:y 248:d 242:i 231:t 228:d 225:( 219:= 214:2 210:s 206:d 184:) 181:3 178:, 175:2 172:, 169:1 166:= 163:j 160:, 157:i 154:( 125:g 72:) 66:( 61:) 57:( 43:.

Index

references
inline citations
improve
introducing
Learn how and when to remove this message
general relativity
Einstein field equations
spacetime
Killing vector
asymptotically
timelike
time translation
static
static spacetime
Kerr metric
gravitomagnetic field
Static spacetime
Spherically symmetric spacetime
Ludvigsen, M., General Relativity: A Geometric Approach, Cambridge University Press, 1999
ISBN
052163976X


Category
Lorentzian manifolds

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