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Euler's pump and turbine equation

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Euler’s pump and turbine equations can be used to predict the effect that changing the impeller geometry has on the head. Qualitative estimations can be made from the impeller geometry about the performance of the turbine/pump.
891: 256: 724: 55:(or the “moment of momentum”) which is fundamental to all turbomachines. Accordingly, the change of the angular momentum is equal to the sum of the external moments. The variation of angular momentum 998: 382: 318: 98: 1065: 148: 604: 580: 552: 520: 492: 460: 432: 1087: 118: 741: 31:. These equations govern the power, efficiencies and other factors that contribute to the design of turbomachines. With the help of these equations the 1142: : 185-232. Here, Euler presents his results for maximizing the outputs of windmills and water wheels, among other means of powering pumps. 35:
developed by a pump and the head utilised by a turbine can be easily determined. As the name suggests these equations were formulated by
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in the eighteenth century. These equations can be derived from the moment of momentum equation when applied for a pump or a turbine.
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Since no pressure forces are created on cylindrical surfaces in the circumferential direction, it is possible to write:
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are the relative velocities of the fluid with respect to the blade at the inlet and outlet respectively.
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Based on Eq.(1.13), Euler developed the equation for the pressure head created by an impeller:
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Figures 'a' and 'b' show impellers with backward and forward-curved vanes respectively.
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are the absolute velocities of the fluid at the inlet and outlet respectively.
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the static component of the head is zero, hence the equation reduces to:
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Mémoires de l'Académie Royale des Sciences et des Belles Lettres à Berlin
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Mémoires de l'Académie Royale des Sciences et des Belles Lettres à Berlin
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Mémoires de l'Académie Royale des Sciences et des Belles Lettres à Berlin
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are the velocities of the blade at the inlet and outlet respectively.
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The color triangles formed by velocity vectors u,c and w are called
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equations are the most fundamental equations in the field of
719:{\displaystyle Y_{th}=H_{t}\cdot g=c_{2u}u_{2}-c_{1u}u_{1}} 20: 1166:"Recherches plus exactes sur l'effect des moulins Ă  vent" 993:{\displaystyle H={1 \over {2g}}(V_{1}^{2}-V_{2}^{2}).\,} 1187: 1075: 1024: 925: 744: 631: 592: 560: 532: 500: 472: 440: 412: 327: 266: 166: 129: 106: 61: 1168:(More exact research on the effect of windmills), 42: 1081: 1059: 992: 885: 718: 598: 574: 546: 514: 486: 454: 426: 376: 312: 250: 142: 112: 92: 1403: 377:{\displaystyle c_{1u}=c_{1}\cos \alpha _{1}.\,} 403:and are helpful in explaining how pumps work. 313:{\displaystyle c_{2u}=c_{2}\cos \alpha _{2}\,} 93:{\displaystyle \rho \cdot Q\cdot r\cdot c_{u}} 1229: 1236: 1222: 1104:List of topics named after Leonhard Euler 989: 571: 543: 511: 483: 451: 423: 373: 309: 247: 16:Turbomachinery Equation in Fluid Dynamics 613: 100:at inlet and outlet, an external torque 51:of mechanics is the conservation of the 1404: 905: : theoretical specific supply; H 1217: 387: 1089:is constant across the rotor blade. 13: 1296:Euler's continued fraction formula 1243: 1157: : 227-295. An analysis of 14: 1448: 1321:Euler's pump and turbine equation 1384: 1383: 1341:Euler equations (fluid dynamics) 1331:Euler's sum of powers conjecture 1188:Johann Friedrich GĂĽlich (2010). 1099:Euler equations (fluid dynamics) 1012:This equation can be written as 392: 43:Conservation of angular momentum 1281:Euler–Poisson–Darboux equation 1181: 1121: 1060:{\displaystyle I=h_{0}-uc_{u}} 983: 947: 880: 772: 225: 173: 1: 1114: 1311:Euler's four-square identity 120:and friction moments due to 7: 1366:Euler–Bernoulli beam theory 1092: 10: 1453: 1379: 1276:Euler–Mascheroni constant 1251: 143:{\displaystyle M_{\tau }} 1326:Euler's rotation theorem 1192:(2nd ed.). Berlin: 1003: 1286:Euler–Rodrigues formula 1266:Euler–Maclaurin formula 1256:Euler–Lagrange equation 599:{\displaystyle \omega } 575:{\displaystyle u_{2}\,} 547:{\displaystyle u_{1}\,} 515:{\displaystyle w_{2}\,} 487:{\displaystyle w_{1}\,} 455:{\displaystyle c_{2}\,} 427:{\displaystyle c_{1}\,} 1361:Euler number (physics) 1291:Euler–Tricomi equation 1083: 1061: 994: 887: 720: 600: 576: 548: 516: 488: 456: 428: 378: 314: 252: 144: 114: 94: 1301:Euler's critical load 1271:Euler–Maruyama method 1084: 1062: 995: 888: 721: 614:Euler's pump equation 601: 577: 549: 517: 489: 457: 429: 379: 315: 253: 145: 115: 95: 1261:Euler–Lotka equation 1073: 1022: 923: 742: 629: 606:is angular velocity. 590: 558: 530: 498: 470: 438: 410: 325: 264: 164: 127: 104: 59: 982: 964: 879: 861: 843: 825: 807: 789: 49:Newton's second law 1079: 1057: 990: 968: 950: 912:For the case of a 883: 865: 847: 829: 811: 793: 775: 716: 596: 572: 544: 512: 484: 452: 424: 401:velocity triangles 388:Velocity triangles 374: 310: 248: 140: 110: 90: 1399: 1398: 1203:978-3-642-12823-3 1190:Centrifugal Pumps 1176: : 166-234. 1082:{\displaystyle I} 945: 113:{\displaystyle M} 47:A consequence of 1444: 1427:Ventilation fans 1387: 1386: 1316:Euler's identity 1238: 1231: 1224: 1215: 1214: 1208: 1207: 1185: 1179: 1125: 1088: 1086: 1085: 1080: 1066: 1064: 1063: 1058: 1056: 1055: 1040: 1039: 999: 997: 996: 991: 981: 976: 963: 958: 946: 944: 933: 892: 890: 889: 884: 878: 873: 860: 855: 842: 837: 824: 819: 806: 801: 788: 783: 768: 757: 756: 725: 723: 722: 717: 715: 714: 705: 704: 689: 688: 679: 678: 657: 656: 644: 643: 605: 603: 602: 597: 581: 579: 578: 573: 570: 569: 553: 551: 550: 545: 542: 541: 521: 519: 518: 513: 510: 509: 493: 491: 490: 485: 482: 481: 461: 459: 458: 453: 450: 449: 433: 431: 430: 425: 422: 421: 396: 383: 381: 380: 375: 369: 368: 353: 352: 340: 339: 319: 317: 316: 311: 308: 307: 292: 291: 279: 278: 257: 255: 254: 249: 246: 245: 224: 223: 214: 213: 198: 197: 188: 187: 149: 147: 146: 141: 139: 138: 119: 117: 116: 111: 99: 97: 96: 91: 89: 88: 53:angular momentum 1452: 1451: 1447: 1446: 1445: 1443: 1442: 1441: 1422:Gas compressors 1402: 1401: 1400: 1395: 1375: 1336:Euler's theorem 1306:Euler's formula 1247: 1242: 1212: 1211: 1204: 1194:Springer-Verlag 1186: 1182: 1126: 1122: 1117: 1095: 1074: 1071: 1070: 1051: 1047: 1035: 1031: 1023: 1020: 1019: 1006: 977: 972: 959: 954: 937: 932: 924: 921: 920: 908: 904: 874: 869: 856: 851: 838: 833: 820: 815: 802: 797: 784: 779: 764: 749: 745: 743: 740: 739: 710: 706: 697: 693: 684: 680: 671: 667: 652: 648: 636: 632: 630: 627: 626: 616: 591: 588: 587: 565: 561: 559: 556: 555: 537: 533: 531: 528: 527: 505: 501: 499: 496: 495: 477: 473: 471: 468: 467: 445: 441: 439: 436: 435: 417: 413: 411: 408: 407: 390: 364: 360: 348: 344: 332: 328: 326: 323: 322: 303: 299: 287: 283: 271: 267: 265: 262: 261: 241: 237: 219: 215: 206: 202: 193: 189: 180: 176: 165: 162: 161: 154:or a diffuser. 134: 130: 128: 125: 124: 105: 102: 101: 84: 80: 60: 57: 56: 45: 17: 12: 11: 5: 1450: 1440: 1439: 1437:Leonhard Euler 1434: 1432:Fluid dynamics 1429: 1424: 1419: 1414: 1397: 1396: 1394: 1393: 1380: 1377: 1376: 1374: 1373: 1368: 1363: 1358: 1353: 1348: 1346:Euler function 1343: 1338: 1333: 1328: 1323: 1318: 1313: 1308: 1303: 1298: 1293: 1288: 1283: 1278: 1273: 1268: 1263: 1258: 1252: 1249: 1248: 1245:Leonhard Euler 1241: 1240: 1233: 1226: 1218: 1210: 1209: 1202: 1180: 1178: 1177: 1162: 1159:Segner's wheel 1143: 1119: 1118: 1116: 1113: 1112: 1111: 1106: 1101: 1094: 1091: 1078: 1054: 1050: 1046: 1043: 1038: 1034: 1030: 1027: 1005: 1002: 1001: 1000: 988: 985: 980: 975: 971: 967: 962: 957: 953: 949: 943: 940: 936: 931: 928: 914:Pelton turbine 906: 902: 899: 898: 897: 896: 895: 894: 882: 877: 872: 868: 864: 859: 854: 850: 846: 841: 836: 832: 828: 823: 818: 814: 810: 805: 800: 796: 792: 787: 782: 778: 774: 771: 767: 763: 760: 755: 752: 748: 732: 731: 730: 729: 728: 727: 713: 709: 703: 700: 696: 692: 687: 683: 677: 674: 670: 666: 663: 660: 655: 651: 647: 642: 639: 635: 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1184: 1175: 1171: 1167: 1164:Euler (1756) 1163: 1160: 1156: 1152: 1148: 1145:Euler (1754) 1144: 1141: 1137: 1133: 1130:Euler (1752) 1129: 1128: 1124: 1120: 1110: 1107: 1105: 1102: 1100: 1097: 1096: 1090: 1076: 1067: 1052: 1048: 1044: 1041: 1036: 1032: 1028: 1025: 1017: 1015: 1010: 986: 978: 973: 969: 965: 960: 955: 951: 941: 938: 934: 929: 926: 919: 918: 917: 915: 910: 875: 870: 866: 862: 857: 852: 848: 844: 839: 834: 830: 826: 821: 816: 812: 808: 803: 798: 794: 790: 785: 780: 776: 769: 765: 761: 758: 753: 750: 746: 738: 737: 736: 735: 734: 733: 711: 707: 701: 698: 694: 690: 685: 681: 675: 672: 668: 664: 661: 658: 653: 649: 645: 640: 637: 633: 625: 624: 623: 622: 621: 620: 619: 611: 593: 586: 585: 566: 562: 538: 534: 526: 525: 506: 502: 478: 474: 466: 465: 446: 442: 418: 414: 406: 405: 404: 402: 397: 395: 370: 365: 361: 357: 354: 349: 345: 341: 336: 333: 329: 321: 304: 300: 296: 293: 288: 284: 280: 275: 272: 268: 260: 242: 238: 234: 231: 228: 220: 216: 210: 207: 203: 199: 194: 190: 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871:1 867:c 858:2 853:2 849:c 845:+ 840:2 835:2 831:w 822:2 817:1 813:w 809:+ 804:2 799:1 795:u 786:2 781:2 777:u 773:( 770:2 766:/ 762:1 759:= 754:h 751:t 747:Y 712:1 708:u 702:u 699:1 695:c 686:2 682:u 676:u 673:2 669:c 665:= 662:g 654:t 650:H 646:= 641:h 638:t 634:Y 567:2 563:u 539:1 535:u 507:2 503:w 479:1 475:w 447:2 443:c 419:1 415:c 371:. 366:1 350:1 346:c 342:= 337:u 334:1 330:c 305:2 289:2 285:c 281:= 276:u 273:2 269:c 239:M 235:+ 232:M 229:= 226:) 221:1 217:r 211:u 208:1 204:c 195:2 191:r 185:u 182:2 178:c 174:( 171:Q 132:M 108:M 86:u 82:c 75:r 69:Q

Index

pump
turbine
turbomachinery
head
Leonhard Euler
Newton's second law
angular momentum
shear stresses
impeller

velocity triangles
Pelton turbine
rothalpy
Euler equations (fluid dynamics)
List of topics named after Leonhard Euler
Rothalpy
"Maximes pour arranger le plus avantageusement les machines destinées à élever de l'eau par moyen des pompes"
"Théorie plus complette des machines qui sont mises en mouvement par la réaction de l'eau"
Segner's wheel
"Recherches plus exactes sur l'effect des moulins Ă  vent"
Springer-Verlag
ISBN
978-3-642-12823-3
v
t
e
Leonhard Euler
Euler–Lagrange equation
Euler–Lotka equation
Euler–Maclaurin formula

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