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Coupling (physics)

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656: 530: 1031: 166: 632:—or how strongly the electric force of each atom holds the plasma together. Plasmas can therefore be categorized into weakly- and strongly-coupled plasmas depending upon the value of this ratio. Many of the typical classical plasmas, such as the plasma in the 1112: 374: 758: 963: 346: 265: 1020: 475:
are the inductances of the primary and secondary circuits, respectively. If the flux lines of the primary inductor thread every line of the secondary one, then the coefficient of coupling is 1 and
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to each other, then these waves are said to be "coupled." This normally occurs when the waves share a common component. An example of this is two pendulums connected by a
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which interact with each other are said to be coupled. This interaction is caused by one of the fundamental forces, whose strengths are usually given by a dimensionless
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Forces which have a coupling constant greater than 1 are said to be "strongly coupled" while those with constants less than 1 are said to be "weakly coupled."
665: 916: 54: 872: 980:. As they are both forms of angular momentum, they must be conserved. Even if energy is transferred between the two, the total angular momentum, 1237: 269: 188: 1262: 1207: 1179: 1151: 586:. For instance, the Earth is coupled to both the Sun and the Moon, as it is under the gravitational influence of both. Common in space are 36: 615: 405:
of an inductor in an unconnected LC circuit, the circuits are said to be coupled. The coefficient of coupling k defines how closely the
412: 1096: 968:(also known as spin-orbit coupling) is a special case of angular momentum coupling. Specifically, it is the interaction between the 906: 649: 987: 90: 97: 354:
of the pendulum with an added coupling factor of the spring. This behavior is also seen in certain molecules (such as
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which is the addition of the two Hamiltonians in isolation with an added interaction factor. In most simple systems,
559: 602:. When smaller particles, such as dust, which are coupled together over time accumulate into much larger objects, 1288: 910: 894: 888: 547: 69: 603: 566:, known as a doublet, representing the individual atoms. If coupling is present, then there will be a triplet, 655: 529: 1050: 1046: 149: 1054: 351: 594:
which circle each other. Multiple objects may also be coupled to each other simultaneously, such as with
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from two separate sources interact with each other, they are said to be coupled. For example, two
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Objects in space which are coupled to each other are under the mutual influence of each other's
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connected by a spring. The connection affects the oscillatory pattern of both objects. In
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Dispersion relations for non-coupled, weakly-coupled, and strongly-coupled particles
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O), wherein two of the atoms will vibrate around a central one in a similar manner.
633: 599: 74: 637: 591: 130: 1140: 402: 382: 185:. If the pendulums are identical, then their equations of motion are given by 78: 1030: 875:. If the two systems have similar total energy, then the system may undergo 386: 590:, two objects gravitationally coupled to each other. Examples of this are 1038: 898: 606:
is occurring. This is the major process by which stars and planets form.
390: 134: 753:{\displaystyle {\hat {H}}={\hat {H}}_{a}+{\hat {H}}_{b}+{\hat {V}}_{ab}} 373: 583: 393:
and can therefore be modeled as a simple harmonic oscillator. When the
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Two systems are coupled if they are interacting with each other
958:{\displaystyle \mathbf {J} =\mathbf {J_{1}} +\mathbf {J_{2}} } 558:
magnetic field of another nearby atom. This is very common in
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Hagelstein, Peter; Senturia, Stephen; Orlando, Terry (2004).
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to be coupled when they are interacting with each other. In
341:{\displaystyle m{\ddot {y}}=-mg{\frac {y}{l_{2}}}+k(x-y)} 260:{\displaystyle m{\ddot {x}}=-mg{\frac {x}{l_{1}}}-k(x-y)} 1200:
Introductory Applied Quantum and Statistical Mechanics
1015:{\displaystyle \mathbf {J} =\mathbf {L} +\mathbf {S} } 481: 990: 919: 838: 802: 766: 668: 415: 272: 191: 562:. If the atoms are not coupled, then there will be 1139: 1014: 957: 863: 824: 788: 752: 514: 453: 340: 259: 640:star is an example of a strongly coupled plasma. 454:{\displaystyle {\frac {M}{\sqrt {L_{p}L_{s}}}}=k} 1091:(Fourth ed.). West Sussex, England: Wiley. 648:Two coupled quantum systems can be modeled by a 574:of the individual atoms oscillating in tandem. 905:may have coupled angular momenta. Due to the 98: 8: 636:, are weakly coupled, while the plasma in a 526:, so most systems are not perfectly coupled. 1255:Elementary Particle-Second, Revised Edition 105: 91: 18: 1026:Particle physics and quantum field theory 1007: 999: 991: 989: 948: 943: 933: 928: 920: 918: 852: 841: 840: 837: 816: 805: 804: 801: 780: 769: 768: 765: 741: 730: 729: 719: 708: 707: 697: 686: 685: 670: 669: 667: 568:one larger peak with two smaller ones to 504: 494: 488: 480: 436: 426: 416: 414: 309: 300: 277: 276: 271: 228: 219: 196: 195: 190: 1072: 533:Peaks in an NMR image of Ethyl Acetate. 169:Coupled pendulums connected by a spring 129:, coupling is a connection between two 44: 28: 21: 1053:α, approximately equal to 1/137. For 624:is given by the ratio of its average 7: 1223: 1221: 1219: 1193: 1191: 1165: 1163: 1082: 1080: 1078: 1076: 976:, and its orbital angular momentum, 570:either side. This occurs due to the 1089:The Physics of Vibrations and Waves 616:Frequency classification of plasmas 515:{\textstyle M={\sqrt {L_{p}L_{s}}}} 984:, of the system must be constant, 14: 522:In practice, however, there is of 377:Two LC circuits coupled together. 1008: 1000: 992: 949: 945: 934: 930: 921: 907:conservation of angular momentum 385:, charge oscillates between the 864:{\displaystyle {\hat {V}}_{ab}} 37:Rotational–vibrational coupling 1202:. Hoboken, New Jersey: Wiley. 846: 825:{\displaystyle {\hat {H}}_{b}} 810: 789:{\displaystyle {\hat {H}}_{a}} 774: 735: 713: 691: 675: 350:These equations represent the 335: 323: 254: 242: 1: 1049:, this value is known as the 409:and is given by the equation 1146:. W.H. Freeman and Company. 832:can be solved exactly while 1228:Merzbacher, Eugene (1998). 620:The coupling constant of a 161:Coupled harmonic oscillator 55:Ro–vibrational spectroscopy 1305: 1138:Kaufmann, William (1988). 1034:Examples of gluon coupling 886: 613: 143:two particles are coupled 1253:Griffiths, David (2010). 1232:(Third ed.). Wiley. 1170:Ichimaru, Setsuo (1986). 911:angular momentum operator 901:orbiting around the same 889:Angular momentum coupling 883:Angular momentum coupling 145:if they are connected by 70:Angular momentum coupling 1142:Universe, Second Edition 1113:"5.5 Spin-Spin Coupling" 407:two circuits are coupled 1051:fine-structure constant 1047:quantum electrodynamics 1055:quantum chromodynamics 1035: 1016: 966:Spin-Orbit interaction 959: 909:and the nature of the 871:can be solved through 865: 826: 790: 754: 660: 628:energy to its average 534: 516: 455: 378: 352:simple harmonic motion 342: 261: 170: 1033: 1017: 960: 866: 827: 791: 755: 658: 556:one atom affects the 532: 517: 467:of the circuits and L 456: 399:one inductor is able 376: 343: 262: 177:are able to transmit 168: 123:two objects are said 1117:Chemistry Libretexts 988: 917: 836: 800: 764: 666: 564:two individual peaks 479: 413: 270: 189: 1087:Pain, H.J. (1993). 873:perturbation theory 626:Coulomb-interaction 369:Coupled LC circuits 127:classical mechanics 65:Rovibronic coupling 23:Coupling in science 1239:978-0-471--88702-7 1060:asymptotic freedom 1036: 1012: 955: 861: 822: 786: 750: 661: 548:Spin-spin coupling 543:Spin-spin coupling 535: 512: 451: 379: 338: 257: 171: 150:fundamental forces 29:Classical coupling 1264:978-3-527-40601-2 1230:Quantum Mechanics 1209:978-0-471-20276-9 1181:978-0-8053-8754-4 1153:978-0-7167-1927-4 1043:coupling constant 849: 813: 777: 738: 716: 694: 678: 644:Quantum mechanics 596:globular clusters 510: 465:mutual inductance 443: 442: 315: 285: 234: 204: 133:systems, such as 115: 114: 60:Vibronic coupling 1296: 1289:Particle physics 1269: 1268: 1250: 1244: 1243: 1225: 1214: 1213: 1195: 1186: 1185: 1167: 1158: 1157: 1145: 1135: 1129: 1128: 1126: 1124: 1109: 1103: 1102: 1084: 1021: 1019: 1018: 1013: 1011: 1003: 995: 964: 962: 961: 956: 954: 953: 952: 939: 938: 937: 924: 877:Rabi oscillation 870: 868: 867: 862: 860: 859: 851: 850: 842: 831: 829: 828: 823: 821: 820: 815: 814: 806: 795: 793: 792: 787: 785: 784: 779: 778: 770: 759: 757: 756: 751: 749: 748: 740: 739: 731: 724: 723: 718: 717: 709: 702: 701: 696: 695: 687: 680: 679: 671: 550:occurs when the 521: 519: 518: 513: 511: 509: 508: 499: 498: 489: 460: 458: 457: 452: 444: 441: 440: 431: 430: 421: 417: 347: 345: 344: 339: 316: 314: 313: 301: 287: 286: 278: 266: 264: 263: 258: 235: 233: 232: 220: 206: 205: 197: 147:one of the four 139:particle physics 107: 100: 93: 46:Quantum coupling 19: 1304: 1303: 1299: 1298: 1297: 1295: 1294: 1293: 1274: 1273: 1272: 1265: 1252: 1251: 1247: 1240: 1227: 1226: 1217: 1210: 1197: 1196: 1189: 1182: 1169: 1168: 1161: 1154: 1137: 1136: 1132: 1122: 1120: 1111: 1110: 1106: 1099: 1086: 1085: 1074: 1070: 1028: 986: 985: 972:of a particle, 944: 929: 915: 914: 895:angular momenta 891: 885: 839: 834: 833: 803: 798: 797: 767: 762: 761: 728: 706: 684: 664: 663: 646: 618: 612: 580: 569: 565: 557: 545: 540: 525: 500: 490: 477: 476: 474: 470: 463:where M is the 432: 422: 411: 410: 408: 400: 371: 364: 359: 305: 268: 267: 224: 187: 186: 163: 158: 148: 144: 124: 111: 17: 12: 11: 5: 1302: 1300: 1292: 1291: 1286: 1276: 1275: 1271: 1270: 1263: 1245: 1238: 1215: 1208: 1187: 1180: 1172:Plasma Physics 1159: 1152: 1130: 1104: 1097: 1071: 1069: 1066: 1027: 1024: 1010: 1006: 1002: 998: 994: 970:intrinsic spin 951: 947: 942: 936: 932: 927: 923: 887:Main article: 884: 881: 858: 855: 848: 845: 819: 812: 809: 783: 776: 773: 747: 744: 737: 734: 727: 722: 715: 712: 705: 700: 693: 690: 683: 677: 674: 645: 642: 630:kinetic energy 614:Main article: 611: 608: 588:binary systems 579: 576: 567: 563: 555: 552:magnetic field 544: 541: 539: 536: 523: 507: 503: 497: 493: 487: 484: 472: 468: 450: 447: 439: 435: 429: 425: 420: 406: 401:to affect the 398: 370: 367: 362: 357: 337: 334: 331: 328: 325: 322: 319: 312: 308: 304: 299: 296: 293: 290: 284: 281: 275: 256: 253: 250: 247: 244: 241: 238: 231: 227: 223: 218: 215: 212: 209: 203: 200: 194: 162: 159: 157: 156:Wave mechanics 154: 146: 142: 122: 113: 112: 110: 109: 102: 95: 87: 84: 83: 82: 81: 72: 67: 62: 57: 49: 48: 42: 41: 40: 39: 31: 30: 26: 25: 15: 13: 10: 9: 6: 4: 3: 2: 1301: 1290: 1287: 1285: 1282: 1281: 1279: 1266: 1260: 1257:. Wiley-VCH. 1256: 1249: 1246: 1241: 1235: 1231: 1224: 1222: 1220: 1216: 1211: 1205: 1201: 1194: 1192: 1188: 1183: 1177: 1173: 1166: 1164: 1160: 1155: 1149: 1144: 1143: 1134: 1131: 1118: 1114: 1108: 1105: 1100: 1098:0-471-93742-8 1094: 1090: 1083: 1081: 1079: 1077: 1073: 1067: 1065: 1063: 1061: 1056: 1052: 1048: 1044: 1040: 1032: 1025: 1023: 1004: 996: 983: 979: 975: 971: 967: 940: 925: 912: 908: 904: 900: 896: 890: 882: 880: 878: 874: 856: 853: 843: 817: 807: 781: 771: 745: 742: 732: 725: 720: 710: 703: 698: 688: 681: 672: 657: 653: 651: 643: 641: 639: 635: 631: 627: 623: 617: 609: 607: 605: 601: 600:galaxy groups 597: 593: 589: 585: 577: 575: 573: 561: 553: 549: 542: 537: 531: 527: 505: 501: 495: 491: 485: 482: 466: 461: 448: 445: 437: 433: 427: 423: 418: 404: 396: 395:magnetic flux 392: 388: 384: 375: 368: 366: 360: 353: 348: 332: 329: 326: 320: 317: 310: 306: 302: 297: 294: 291: 288: 282: 279: 273: 251: 248: 245: 239: 236: 229: 225: 221: 216: 213: 210: 207: 201: 198: 192: 184: 180: 176: 167: 160: 155: 153: 151: 140: 136: 132: 128: 120: 108: 103: 101: 96: 94: 89: 88: 86: 85: 80: 76: 73: 71: 68: 66: 63: 61: 58: 56: 53: 52: 51: 50: 47: 43: 38: 35: 34: 33: 32: 27: 24: 20: 1254: 1248: 1229: 1199: 1171: 1141: 1133: 1121:. Retrieved 1119:. 2015-07-21 1116: 1107: 1088: 1058: 1037: 981: 977: 973: 892: 662: 647: 634:solar corona 619: 592:binary stars 581: 578:Astrophysics 546: 462: 380: 349: 172: 116: 75:NMR coupling 22: 652:of the form 650:Hamiltonian 638:white dwarf 560:NMR imaging 524:ten leakage 383:LC circuits 131:oscillating 1278:Categories 1068:References 403:inductance 79:J-coupling 1039:Particles 899:electrons 847:^ 811:^ 775:^ 736:^ 714:^ 692:^ 676:^ 604:accretion 538:Chemistry 387:capacitor 330:− 292:− 283:¨ 249:− 237:− 211:− 202:¨ 135:pendulums 391:inductor 389:and the 903:nucleus 584:gravity 173:If two 119:physics 1261:  1236:  1206:  1178:  1150:  1123:13 Apr 1095:  622:plasma 610:Plasma 183:spring 179:energy 1284:Force 1045:. In 893:When 572:spins 471:and L 397:from 361:and H 175:waves 1259:ISBN 1234:ISBN 1204:ISBN 1176:ISBN 1148:ISBN 1125:2017 1093:ISBN 796:and 598:and 554:of 381:In 117:In 77:or 1280:: 1218:^ 1190:^ 1162:^ 1115:. 1075:^ 1022:. 879:. 356:CO 152:. 141:, 121:, 1267:. 1242:. 1212:. 1184:. 1156:. 1127:. 1101:. 1062:. 1009:S 1005:+ 1001:L 997:= 993:J 982:J 978:L 974:S 950:2 946:J 941:+ 935:1 931:J 926:= 922:J 857:b 854:a 844:V 818:b 808:H 782:a 772:H 746:b 743:a 733:V 726:+ 721:b 711:H 704:+ 699:a 689:H 682:= 673:H 506:s 502:L 496:p 492:L 486:= 483:M 473:s 469:p 449:k 446:= 438:s 434:L 428:p 424:L 419:M 363:2 358:2 336:) 333:y 327:x 324:( 321:k 318:+ 311:2 307:l 303:y 298:g 295:m 289:= 280:y 274:m 255:) 252:y 246:x 243:( 240:k 230:1 226:l 222:x 217:g 214:m 208:= 199:x 193:m 106:e 99:t 92:v

Index

Coupling in science
Rotational–vibrational coupling
Quantum coupling
Ro–vibrational spectroscopy
Vibronic coupling
Rovibronic coupling
Angular momentum coupling
NMR coupling
J-coupling
v
t
e
physics
classical mechanics
oscillating
pendulums
particle physics
fundamental forces

waves
energy
spring
simple harmonic motion
CO2

LC circuits
capacitor
inductor
magnetic flux
inductance

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