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Principal quantum number

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This discrete energy spectrum resulted from the solution of the quantum mechanical problem on the electron motion in the Coulomb field, coincides with the spectrum that was obtained with the help application of the Bohr–Sommerfeld quantization rules to the classical equations. The radial quantum
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reduces to the three equations that when solved lead to the first three quantum numbers. Therefore, the equations for the first three quantum numbers are all interrelated. The principal quantum number arose in the solution of the radial part of the wave equation as shown below.
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represents the relative overall energy of each orbital. The energy level of each orbital increases as its distance from the nucleus increases. The sets of orbitals with the same
630: 205:, distinguishing between different energy levels. With the development of modern quantum mechanics, the simple Bohr model was replaced with a more complex theory of 854: 1075: 150:
In a simplistic one-electron model described below, the total energy of an electron is a negative inverse quadratic function of the principal quantum number
1182: 424: 1068: 1177: 1048: 1012: 1203: 1061: 410:. Schrödinger's equation developed the idea from a flat two-dimensional Bohr atom to the three-dimensional wavefunction model. 995: 112: 17: 1110: 1029: 933: 590: 822:{\displaystyle E_{n}=-{\frac {Z^{2}\hbar ^{2}}{2m_{0}a_{0}^{2}n^{2}}}=-{\frac {Z^{2}e^{4}m_{0}}{2\hbar ^{2}n^{2}}},} 107:
increases, the electron is also at a higher energy and is, therefore, less tightly bound to the nucleus. For higher
251:. Two electrons belonging to the same atom cannot have the same values for all four quantum numbers, due to the 406:
can take only positive integer values. The concept of energy levels and notation were taken from the earlier
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There is a set of quantum numbers associated with the energy states of the atom. The four quantum numbers
1295: 1198: 393:{\displaystyle E_{n}={\frac {E_{1}}{n^{2}}}={\frac {-13.6{\text{ eV}}}{n^{2}}},\quad n=1,2,3,\ldots } 252: 1305: 1139: 494: 155: 72: 1300: 1148: 897: 79: 983: 256: 162: > 1. In more complex systems—those having forces other than the nucleus–electron 1084: 1021: 413:
In the Bohr model, the allowed orbits were derived from quantized (discrete) values of orbital
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The minimum energy exchanged during any wave–matter interaction is the product of the wave
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Periodic Table Applet: showing principal and azimuthal quantum number for each element
1260: 1229: 1105: 1025: 991: 657: 540: 61: 31: 1274: 1245: 1208: 498: 497:, but the energy levels are accurate and classically they correspond to the sum of 490: 414: 917: 546:
In the notation of the periodic table, the main shells of electrons are labeled:
528: 486: 170:. For multielectron atoms this splitting results in "subshells" parametrized by 1122: 1100: 1095: 969: 901: 889: 646: 517: 502: 248: 206: 140: 57: 45: 481:= 1, 2, 3, ... and is called the principal quantum number, and 1289: 1250: 1224: 909: 244: 240: 183: 163: 175: 135:
electron states are more numerous. Accounting for two states of spin, each
209:. However, the modern theory still requires the principal quantum number. 1053: 857: 531:. This causes the wave to display particle-like packets of energy called 282: 68: 1269: 407: 202: 67:
Apart from the principal quantum number, the other quantum numbers for
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The principal quantum number is related to the radial quantum number,
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Atomic spectroscopy. Introduction of theory to Hyperfine Structure
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number determines the number of nodes of the radial wave function
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The principal quantum number was first created for use in the
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The definite total energy for a particle motion in a common
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energies of the electron in the hydrogen atom are given by:
535:. The difference between energy levels that have different 53: 489:. This formula is not correct in quantum mechanics as the 888: = 1, 2, 3, 4, 5, 6, 7 are used in relation to the 924:
on order of hundreds; values up to 766 were detected.
470:{\displaystyle L=n\cdot \hbar =n\cdot {h \over 2\pi }} 896: = 8 (and possibly 9) for yet-undiscovered 835: 666: 593: 427: 291: 1183:
Electron configurations of the elements (data page)
848: 821: 624: 469: 392: 56:to describe that electron's state. Its values are 1287: 975: 263:The Schrödinger wave equation describes energy 968:) is degenerate, assuming absence of external 1069: 243:of a single electron in an atom, called its 27:Number assigned to each electron in an atom 1083: 1076: 1062: 274:and a definite total energy, the value of 111:the electron is farther from the nucleus, 131: âˆ’ 1 inclusively, hence higher- 1178:Periodic table (electron configurations) 1010: 1004: 575:based on the principal quantum number. 182:alone gradually becomes inadequate for 98: 14: 1288: 981: 1057: 127:(azimuthal) values ranging from 0 to 952:Here we ignore spin. Accounting for 636:is the azimuthal quantum number and 203:semiclassical Bohr model of the atom 946: 908:sometimes occur for description of 892:theory, with expected inclusion of 24: 516:value are often referred to as an 25: 1317: 1111:Introduction to quantum mechanics 1042: 934:Introduction to quantum mechanics 440: 198: = 19) and afterwards. 267:with corresponding real numbers 239:specify the complete and unique 625:{\displaystyle n=n_{r}+\ell +1} 362: 493:magnitude is described by the 13: 1: 939: 508:The principal quantum number 212: 649:in the radial wavefunction. 7: 1171:Ground-state configurations 1011:Tennyson, Jonathan (2005). 927: 10: 1322: 1140:Azimuthal quantum number ( 1131:Principal quantum number ( 982:Andrew, A. V. (2006). "2. 645:is equal to the number of 421:according to the equation 216: 190:) and fails completely on 1259: 1238: 1217: 1199:Pauli exclusion principle 1191: 1170: 1149:Magnetic quantum number ( 1121: 1091: 1014:Astronomical Spectroscopy 920:spectral lines involving 875: 257:Schrödinger wave equation 253:Pauli exclusion principle 495:azimuthal quantum number 156:degenerate energy levels 73:azimuthal quantum number 36:principal quantum number 960:orbital (determined by 143:can accommodate up to 2 80:magnetic quantum number 60:(from one) making it a 1085:Electron configuration 1022:Imperial College Press 912:. Observations of the 850: 823: 626: 471: 408:Bohr model of the atom 394: 1239:Bonding participation 1158:Spin quantum number ( 851: 849:{\displaystyle a_{0}} 824: 627: 472: 395: 18:Radial quantum number 984:Schrödinger equation 833: 664: 591: 425: 289: 115:. For each value of 99:Overview and history 914:interstellar medium 735: 90:spin quantum number 846: 819: 721: 622: 527:multiplied by the 467: 390: 219:Hydrogen-like atom 71:electrons are the 1296:Quantum chemistry 1283: 1282: 1261:Electron counting 1230:Unpaired electron 1106:Quantum mechanics 997:978-0-387-25573-6 898:period 8 elements 814: 747: 658:discrete spectrum 541:emission spectrum 505:of the electron. 465: 357: 344: 327: 186:starting from 5 ( 174:. Description of 62:discrete variable 48:assigned to each 44:) is one of four 32:quantum mechanics 16:(Redirected from 1313: 1275:18-electron rule 1246:Valence electron 1218:Electron pairing 1209:Aufbau principle 1192:Electron filling 1161: 1152: 1143: 1134: 1078: 1071: 1064: 1055: 1054: 1036: 1035: 1019: 1008: 1002: 1001: 979: 973: 950: 855: 853: 852: 847: 845: 844: 828: 826: 825: 820: 815: 813: 812: 811: 802: 801: 788: 787: 786: 777: 776: 767: 766: 756: 748: 746: 745: 744: 734: 729: 720: 719: 706: 705: 704: 695: 694: 684: 676: 675: 631: 629: 628: 623: 609: 608: 543:of the element. 491:angular momentum 476: 474: 473: 468: 466: 464: 453: 415:angular momentum 399: 397: 396: 391: 358: 356: 355: 346: 345: 342: 333: 328: 326: 325: 316: 315: 306: 301: 300: 21: 1321: 1320: 1316: 1315: 1314: 1312: 1311: 1310: 1306:Quantum numbers 1286: 1285: 1284: 1279: 1255: 1234: 1213: 1187: 1166: 1159: 1150: 1141: 1132: 1123:Quantum numbers 1117: 1087: 1082: 1045: 1040: 1039: 1032: 1017: 1009: 1005: 998: 990:. p. 274. 980: 976: 951: 947: 942: 930: 918:atomic hydrogen 878: 840: 836: 834: 831: 830: 807: 803: 797: 793: 789: 782: 778: 772: 768: 762: 758: 757: 755: 740: 736: 730: 725: 715: 711: 707: 700: 696: 690: 686: 685: 683: 671: 667: 665: 662: 661: 660:, is given by: 644: 604: 600: 592: 589: 588: 586: 573: 529:Planck constant 487:Planck constant 457: 452: 426: 423: 422: 351: 347: 341: 334: 332: 321: 317: 311: 307: 305: 296: 292: 290: 287: 286: 279: 272: 221: 215: 207:atomic orbitals 101: 86: 58:natural numbers 46:quantum numbers 28: 23: 22: 15: 12: 11: 5: 1319: 1309: 1308: 1303: 1301:Atomic physics 1298: 1281: 1280: 1278: 1277: 1272: 1266: 1264: 1257: 1256: 1254: 1253: 1248: 1242: 1240: 1236: 1235: 1233: 1232: 1227: 1221: 1219: 1215: 1214: 1212: 1211: 1206: 1201: 1195: 1193: 1189: 1188: 1186: 1185: 1180: 1174: 1172: 1168: 1167: 1165: 1164: 1155: 1146: 1137: 1127: 1125: 1119: 1118: 1116: 1115: 1114: 1113: 1103: 1101:Atomic orbital 1098: 1096:Electron shell 1092: 1089: 1088: 1081: 1080: 1073: 1066: 1058: 1052: 1051: 1044: 1043:External links 1041: 1038: 1037: 1030: 1024:. p. 39. 1003: 996: 974: 970:magnetic field 944: 943: 941: 938: 937: 936: 929: 926: 910:excited states 902:atomic physics 890:electron shell 877: 874: 843: 839: 818: 810: 806: 800: 796: 792: 785: 781: 775: 771: 765: 761: 754: 751: 743: 739: 733: 728: 724: 718: 714: 710: 703: 699: 693: 689: 682: 679: 674: 670: 640: 621: 618: 615: 612: 607: 603: 599: 596: 582: 548: 539:determine the 518:electron shell 503:kinetic energy 463: 460: 456: 451: 448: 445: 442: 439: 436: 433: 430: 402:The parameter 389: 386: 383: 380: 377: 374: 371: 368: 365: 361: 354: 350: 340: 337: 331: 324: 320: 314: 310: 304: 299: 295: 277: 270: 217:Main article: 214: 211: 184:atomic numbers 166:—these levels 100: 97: 84: 26: 9: 6: 4: 3: 2: 1318: 1307: 1304: 1302: 1299: 1297: 1294: 1293: 1291: 1276: 1273: 1271: 1268: 1267: 1265: 1262: 1258: 1252: 1251:Core electron 1249: 1247: 1244: 1243: 1241: 1237: 1231: 1228: 1226: 1225:Electron pair 1223: 1222: 1220: 1216: 1210: 1207: 1205: 1202: 1200: 1197: 1196: 1194: 1190: 1184: 1181: 1179: 1176: 1175: 1173: 1169: 1163: 1156: 1154: 1147: 1145: 1138: 1136: 1129: 1128: 1126: 1124: 1120: 1112: 1109: 1108: 1107: 1104: 1102: 1099: 1097: 1094: 1093: 1090: 1086: 1079: 1074: 1072: 1067: 1065: 1060: 1059: 1056: 1050: 1047: 1046: 1033: 1031:1-86094-513-9 1027: 1023: 1016: 1015: 1007: 999: 993: 989: 985: 978: 971: 967: 963: 959: 955: 949: 945: 935: 932: 931: 925: 923: 919: 915: 911: 907: 903: 899: 895: 891: 887: 883: 873: 871: 867: 861: 859: 841: 837: 816: 808: 804: 798: 794: 790: 783: 779: 773: 769: 763: 759: 752: 749: 741: 737: 731: 726: 722: 716: 712: 708: 701: 697: 691: 687: 680: 677: 672: 668: 659: 655: 654:Coulomb field 650: 648: 643: 639: 635: 619: 616: 613: 610: 605: 601: 597: 594: 585: 581: 576: 571: 567: 563: 559: 555: 551: 547: 544: 542: 538: 534: 530: 526: 521: 519: 515: 511: 506: 504: 500: 496: 492: 488: 484: 480: 461: 458: 454: 449: 446: 443: 437: 434: 431: 428: 420: 416: 411: 409: 405: 400: 387: 384: 381: 378: 375: 372: 369: 366: 363: 359: 352: 348: 338: 335: 329: 322: 318: 312: 308: 302: 297: 293: 284: 280: 273: 266: 261: 258: 254: 250: 246: 245:wave function 242: 241:quantum state 238: 234: 230: 226: 220: 210: 208: 204: 199: 197: 193: 189: 185: 181: 177: 176:energy levels 173: 169: 165: 164:Coulomb force 161: 157: 154:, leading to 153: 148: 146: 142: 138: 134: 130: 126: 122: 118: 114: 110: 106: 96: 94: 91: 87: 81: 77: 74: 70: 65: 63: 59: 55: 51: 47: 43: 42: 37: 33: 19: 1130: 1013: 1006: 987: 977: 965: 961: 957: 953: 948: 921: 905: 893: 885: 879: 869: 865: 862: 651: 641: 637: 633: 583: 579: 577: 574: 569: 565: 561: 557: 553: 549: 545: 536: 522: 513: 509: 507: 482: 478: 418: 412: 403: 401: 275: 268: 262: 236: 232: 228: 224: 222: 200: 195: 179: 171: 159: 151: 149: 144: 136: 132: 128: 124: 120: 116: 108: 104: 102: 92: 82: 75: 66: 40: 39: 38:(symbolized 35: 29: 1204:Hund's rule 858:Bohr radius 656:and with a 283:bound state 265:eigenstates 147:electrons. 1290:Categories 1270:Octet rule 1020:. London: 940:References 572:= 3), etc. 213:Derivation 119:there are 113:on average 88:, and the 904:, higher 884:, values 882:chemistry 795:ℏ 753:− 698:ℏ 681:− 614:ℓ 525:frequency 499:potential 462:π 450:⋅ 441:ℏ 438:⋅ 388:… 336:− 192:potassium 178:based on 158:for each 123:accepted 928:See also 343: eV 50:electron 916:reveal 856:is the 485:is the 255:. The 249:orbital 1028:  994:  876:Values 829:where 632:where 587:, by: 564:= 2), 556:= 1), 533:quanta 477:where 281:. The 235:, and 78:, the 52:in an 34:, the 1263:rules 1018:(PDF) 958:every 900:. In 647:nodes 188:boron 168:split 141:shell 69:bound 1026:ISBN 992:ISBN 964:and 501:and 339:13.6 54:atom 986:". 880:In 872:). 247:or 103:As 30:In 1292:: 956:, 860:. 520:. 417:, 231:, 227:, 95:. 64:. 1162:) 1160:s 1153:) 1151:m 1144:) 1142:ℓ 1135:) 1133:n 1077:e 1070:t 1063:v 1034:. 1000:. 972:. 966:ℓ 962:n 954:s 922:n 906:n 894:n 886:n 870:r 868:( 866:R 842:0 838:a 817:, 809:2 805:n 799:2 791:2 784:0 780:m 774:4 770:e 764:2 760:Z 750:= 742:2 738:n 732:2 727:0 723:a 717:0 713:m 709:2 702:2 692:2 688:Z 678:= 673:n 669:E 642:r 638:n 634:ℓ 620:1 617:+ 611:+ 606:r 602:n 598:= 595:n 584:r 580:n 570:n 568:( 566:M 562:n 560:( 558:L 554:n 552:( 550:K 537:n 514:n 510:n 483:h 479:n 459:2 455:h 447:n 444:= 435:n 432:= 429:L 419:L 404:n 385:, 382:3 379:, 376:2 373:, 370:1 367:= 364:n 360:, 353:2 349:n 330:= 323:2 319:n 313:1 309:E 303:= 298:n 294:E 278:n 276:E 271:n 269:E 237:s 233:m 229:ℓ 225:n 196:Z 194:( 180:n 172:ℓ 160:n 152:n 145:n 139:- 137:n 133:n 129:n 125:ℓ 121:n 117:n 109:n 105:n 93:s 85:l 83:m 76:ℓ 41:n 20:)

Index

Radial quantum number
quantum mechanics
quantum numbers
electron
atom
natural numbers
discrete variable
bound
azimuthal quantum number
magnetic quantum number
spin quantum number
on average
shell
degenerate energy levels
Coulomb force
split
energy levels
atomic numbers
boron
potassium
semiclassical Bohr model of the atom
atomic orbitals
Hydrogen-like atom
quantum state
wave function
orbital
Pauli exclusion principle
Schrödinger wave equation
eigenstates
bound state

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