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Sauerbrey equation

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is the nominal frequency shift of that mode divided by its mode number (most software outputs normalized frequency shift by default). Because the film is treated as an extension of thickness, Sauerbrey’s equation only applies to systems in which the following three conditions are met: the deposited
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The equation is derived by treating the deposited mass as though it were an extension of the thickness of the underlying quartz. Because of this, the mass to frequency correlation (as determined by Sauerbrey’s equation) is largely independent of electrode geometry. This has the benefit of allowing
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with the mass deposited on it. He simultaneously developed a method for measuring the characteristic frequency and its changes by using the crystal as the frequency determining component of an oscillator circuit. His method continues to be used as the primary tool in
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The Sauerbrey equation was developed for oscillation in air and only applies to rigid masses attached to the crystal. It has been shown that quartz crystal microbalance measurements can be performed in liquid, in which case a
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Kanazawa, K. Keiji; Gordon II, Joseph G. (July 1985). "Frequency of a quartz microbalance in contact with liquid".
475:> 0.05, the Z-match method must be used to determine the change in mass. The formula for the Z-match method is: 1397: 1313: 55:
mass determination without calibration, making the set-up desirable from a cost and time investment standpoint.
1513: 1439: 1326: 259: 1301: 32: 1350: 183: 447: 413: 1240: 1213: 952: 817: 790: 298: 267: 51:(QCM) experiments for conversion of frequency to mass and is valid in nearly all applications. 1342: 1037: 1008: 981: 743: 389: 358: 327: 216: 191: 1484: 1447: 1334: 714: 685: 656: 640:{\displaystyle {\frac {\Delta m}{A}}\ ={\frac {N_{q}\rho _{q}}{\pi Zf_{L}}}\tan ^{-1}\left} 410:
mass must be rigid, the deposited mass must be distributed evenly and the frequency change
158: 1322: 1200:{\displaystyle \Delta f={-\ f_{0}^{3/2}(\eta _{l}\rho _{l}/\pi \rho _{q}\mu _{q}n)^{1/2}}} 1443: 1426:"Quartz-crystal microbalance study for characterizing atomic oxygen in plasma ash tools" 1330: 941:{\displaystyle ={\sqrt {\left({\frac {\rho _{q}\mu _{q}}{\rho _{f}\mu _{f}}}\ \right)}}} 1267: 846: 768: 241: 1502: 1425: 1354: 352: 40: 142:{\displaystyle \Delta f=-{\frac {2f_{0}^{2}}{A{\sqrt {\rho _{q}\mu _{q}}}}}\Delta m} 39:, Germany. It is a method for correlating changes in the oscillation frequency of a 1373:(NB. This was partially presented at Physikertagung in Heidelberg in October 1957.) 17: 1306:"Verwendung von Schwingquarzen zur Wägung dünner Schichten und zur Mikrowägung" 1305: 1346: 1072: 1424:
Srivastava, Aseem Kumar; Sakthivel, Palanikumaran (January–February 2001).
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Journal of Vacuum Science & Technology A: Vacuum, Surfaces, and Films
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related decrease in the resonant frequency will be observed:
738:– Frequency constant for AT-cut quartz crystal (1.668x10Hz·Å) 709:– Frequency of unloaded crystal, i.e. Resonant frequency (Hz) 1390:
QCM100 – Quartz Crystal Microbalance Theory and Calibration
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If the change in frequency is greater than 5%, that is,
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as: 1383: 1381: 1379: 7: 1264:is the viscosity of the liquid, and 1085: 747: 680:– Frequency of loaded crystal (Hz) 488: 451: 417: 393: 220: 211:– normalized frequency change (Hz) 195: 133: 68: 25: 1407:from the original on 2019-02-27 1400:/ Lambda Photometrics Limited, 1364:from the original on 2019-02-26 1237:is the density of the liquid, 1179: 1124: 355:of quartz for AT-cut crystal ( 37:TTechnische Universität Berlin 1: 863:– Z-Factor of film material 650:Equation 2 – Z-match method 186:of the fundamental mode (Hz) 31:was developed by the German 1005:– Shear modulus of quartz ( 49:quartz crystal microbalance 1535: 468:{\displaystyle \Delta f/f} 434:{\displaystyle \Delta f/f} 1398:Stanford Research Systems 1257:{\displaystyle \eta _{l}} 1230:{\displaystyle \rho _{l}} 969:{\displaystyle \rho _{f}} 834:{\displaystyle \rho _{q}} 807:{\displaystyle \rho _{q}} 386:The normalized frequency 315:{\displaystyle \rho _{q}} 284:{\displaystyle \rho _{q}} 1054:{\displaystyle \mu _{f}} 1025:{\displaystyle \mu _{q}} 998:{\displaystyle \mu _{q}} 756:{\displaystyle \Delta m} 402:{\displaystyle \Delta f} 375:{\displaystyle \mu _{q}} 344:{\displaystyle \mu _{q}} 229:{\displaystyle \Delta m} 204:{\displaystyle \Delta f} 1314:Zeitschrift für Physik 1302:Sauerbrey, Günter Hans 1278: 1258: 1231: 1201: 1055: 1026: 999: 970: 942: 857: 835: 808: 779: 757: 732: 703: 674: 641: 469: 435: 403: 376: 345: 316: 285: 252: 230: 205: 176: 143: 1279: 1259: 1232: 1202: 1056: 1027: 1000: 971: 943: 858: 836: 814:– Density of quartz ( 809: 780: 758: 733: 731:{\displaystyle N_{q}} 704: 702:{\displaystyle f_{U}} 675: 673:{\displaystyle f_{L}} 642: 470: 436: 404: 377: 346: 317: 286: 253: 231: 206: 177: 175:{\displaystyle f_{0}} 144: 1519:Weighing instruments 1509:Electrical phenomena 1476:Analytical Chemistry 1284:is the mode number. 1268: 1241: 1214: 1082: 1038: 1009: 982: 953: 867: 847: 818: 791: 769: 744: 715: 686: 657: 482: 448: 414: 390: 359: 328: 299: 268: 242: 217: 192: 159: 65: 1489:10.1021/ac00285a062 1444:2001JVSTA..19...97S 1331:1959ZPhy..155..206S 1123: 100: 1339:10.1007/BF01337937 1274: 1254: 1227: 1197: 1101: 1051: 1032:= 2.947x10 g·cm·s) 1022: 995: 966: 938: 853: 831: 804: 775: 753: 728: 699: 670: 637: 465: 431: 399: 382:= 2.947x10 g·cm·s) 372: 341: 312: 281: 248: 226: 201: 184:Resonant frequency 172: 139: 86: 29:Sauerbrey equation 18:Sauerbrey constant 1453:10.1116/1.1335681 1277:{\displaystyle n} 1100: 936: 930: 926: 856:{\displaystyle Z} 778:{\displaystyle A} 763:– Mass change (g) 625: 548: 502: 498: 260:Piezoelectrically 251:{\displaystyle A} 236:– Mass change (g) 131: 128: 16:(Redirected from 1526: 1493: 1492: 1483:(8): 1770–1771. 1470: 1464: 1463: 1461: 1460: 1455: 1421: 1415: 1414: 1413: 1412: 1406: 1395: 1385: 1374: 1372: 1370: 1369: 1363: 1310: 1298: 1283: 1281: 1280: 1275: 1263: 1261: 1260: 1255: 1253: 1252: 1236: 1234: 1233: 1228: 1226: 1225: 1206: 1204: 1203: 1198: 1196: 1195: 1194: 1190: 1174: 1173: 1164: 1163: 1151: 1146: 1145: 1136: 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81: 33:Günter Sauerbrey 21: 1534: 1533: 1529: 1528: 1527: 1525: 1524: 1523: 1499: 1498: 1497: 1496: 1472: 1471: 1467: 1458: 1456: 1423: 1422: 1418: 1410: 1408: 1404: 1393: 1387: 1386: 1377: 1367: 1365: 1361: 1323:Springer-Verlag 1308: 1304:(April 1959) . 1300: 1299: 1295: 1290: 1266: 1265: 1244: 1239: 1238: 1217: 1212: 1211: 1178: 1165: 1155: 1137: 1127: 1080: 1079: 1068: 1041: 1036: 1035: 1012: 1007: 1006: 985: 980: 979: 956: 951: 950: 915: 905: 904: 893: 883: 882: 879: 875: 865: 864: 845: 844: 821: 816: 815: 794: 789: 788: 767: 766: 742: 741: 718: 713: 712: 689: 684: 683: 660: 655: 654: 615: 604: 591: 590: 584: 580: 570: 566: 550: 537: 530: 519: 509: 508: 487: 480: 479: 446: 445: 412: 411: 388: 387: 362: 357: 356: 331: 326: 325: 302: 297: 296: 271: 266: 265: 240: 239: 215: 214: 190: 189: 162: 157: 156: 118: 108: 102: 82: 63: 62: 23: 22: 15: 12: 11: 5: 1532: 1530: 1522: 1521: 1516: 1511: 1501: 1500: 1495: 1494: 1465: 1416: 1375: 1292: 1291: 1289: 1286: 1273: 1251: 1247: 1224: 1220: 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1420: 1417: 1403: 1399: 1392: 1391: 1384: 1382: 1380: 1376: 1360: 1356: 1352: 1348: 1344: 1340: 1336: 1332: 1328: 1324: 1320: 1317:(in German). 1316: 1315: 1307: 1303: 1297: 1294: 1287: 1285: 1271: 1249: 1245: 1222: 1218: 1191: 1187: 1183: 1175: 1170: 1166: 1160: 1156: 1152: 1148: 1142: 1138: 1132: 1128: 1119: 1115: 1111: 1106: 1102: 1095: 1091: 1088: 1078: 1077: 1076: 1074: 1065: 1046: 1042: 1034: 1017: 1013: 990: 986: 978: 961: 957: 949: 932: 920: 916: 910: 906: 898: 894: 888: 884: 876: 870: 850: 843: 841:= 2.648 g/cm) 826: 822: 799: 795: 787: 772: 765: 750: 740: 723: 719: 711: 694: 690: 682: 665: 661: 653: 652: 651: 633: 628: 620: 616: 609: 605: 601: 596: 592: 585: 581: 577: 574: 571: 567: 563: 558: 555: 551: 542: 538: 534: 531: 524: 520: 514: 510: 503: 495: 491: 478: 477: 476: 462: 458: 454: 442: 428: 424: 420: 396: 367: 363: 354: 353:Shear modulus 336: 332: 324: 322:= 2.648 g/cm) 307: 303: 294: 276: 272: 264: 261: 245: 238: 223: 213: 198: 188: 185: 167: 163: 155: 154: 153: 136: 123: 119: 113: 109: 103: 96: 91: 87: 83: 77: 74: 71: 61: 60: 59: 56: 52: 50: 45: 42: 41:piezoelectric 38: 34: 30: 19: 1480: 1474: 1468: 1457:. Retrieved 1435: 1429: 1419: 1409:, retrieved 1389: 1366:. Retrieved 1318: 1312: 1296: 1209: 1069: 649: 443: 385: 151: 57: 53: 28: 26: 1514:Transducers 1325:: 206–222. 1066:Limitations 441:< 0.05. 295:of quartz ( 1503:Categories 1459:2019-02-27 1411:2019-02-27 1368:2019-02-26 1288:References 1355:122855173 1347:0044-3328 1246:η 1219:ρ 1167:μ 1157:ρ 1153:π 1139:ρ 1129:η 1096:− 1086:Δ 1073:viscosity 1043:μ 1014:μ 987:μ 958:ρ 917:μ 907:ρ 895:μ 885:ρ 823:ρ 796:ρ 748:Δ 602:− 586:π 578:⁡ 564:⁡ 556:− 532:π 521:ρ 489:Δ 452:Δ 418:Δ 394:Δ 364:μ 333:μ 304:ρ 273:ρ 221:Δ 196:Δ 134:Δ 120:μ 110:ρ 78:− 69:Δ 1402:archived 1359:Archived 1440:Bibcode 1327:Bibcode 293:Density 152:where: 44:crystal 1353:  1345:  1210:where 1099:  929:  501:  1405:(PDF) 1394:(PDF) 1362:(PDF) 1351:S2CID 1321:(2). 1309:(PDF) 1343:ISSN 27:The 1485:doi 1448:doi 1335:doi 1319:155 575:tan 552:tan 1505:: 1481:57 1479:. 1446:. 1436:19 1434:. 1428:. 1396:, 1378:^ 1357:. 1349:. 1341:. 1333:. 1311:. 351:– 291:– 258:– 182:– 1491:. 1487:: 1462:. 1450:: 1442:: 1371:. 1337:: 1329:: 1272:n 1250:l 1223:l 1192:2 1188:/ 1184:1 1180:) 1176:n 1171:q 1161:q 1149:/ 1143:l 1133:l 1125:( 1120:2 1116:/ 1112:3 1107:0 1103:f 1092:= 1089:f 1047:f 1018:q 991:q 962:f 933:) 921:f 911:f 899:q 889:q 877:( 871:= 851:Z 827:q 800:q 773:A 751:m 724:q 720:N 695:U 691:f 666:L 662:f 634:] 629:) 621:U 617:f 610:L 606:f 597:U 593:f 582:( 572:Z 568:[ 559:1 543:L 539:f 535:Z 525:q 515:q 511:N 504:= 496:A 492:m 463:f 459:/ 455:f 429:f 425:/ 421:f 397:f 368:q 337:q 308:q 277:q 246:A 224:m 199:f 168:0 164:f 137:m 124:q 114:q 104:A 97:2 92:0 88:f 84:2 75:= 72:f 20:)

Index

Sauerbrey constant
Günter Sauerbrey
TTechnische Universität Berlin
piezoelectric
crystal
quartz crystal microbalance
Resonant frequency
Piezoelectrically
Density
Shear modulus
viscosity
Sauerbrey, Günter Hans
"Verwendung von Schwingquarzen zur Wägung dünner Schichten und zur Mikrowägung"
Zeitschrift für Physik
Springer-Verlag
Bibcode
1959ZPhy..155..206S
doi
10.1007/BF01337937
ISSN
0044-3328
S2CID
122855173
Archived



QCM100 – Quartz Crystal Microbalance Theory and Calibration
Stanford Research Systems
archived

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