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Laplace pressure

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838: 419: 833:{\displaystyle \Delta P=\Delta P_{i}+\Delta P_{o}=2\gamma \left({\frac {1}{R_{i}}}+{\frac {1}{R_{i}+d}}\right)={\frac {2\gamma }{R_{i}}}\left(1+{\frac {R_{i}}{R_{i}+d}}\right)={\frac {2\gamma }{R_{i}}}\left(1+{\frac {R_{i}+d}{R_{i}+d}}-{\frac {d}{R_{i}+d}}\right)={\frac {4\gamma }{R_{i}}}\left(1-{\frac {1}{2}}{\frac {d}{R_{i}+d}}\right)\approx {\frac {4\gamma }{R_{i}}}+{\mathcal {O}}(d).} 20: 366:
For a gas bubble within a liquid, there is only one surface. For a gas bubble with a liquid wall, beyond which is again gas, there are two surfaces, each contributing to the total pressure difference. If the bubble is spherical and the outer radius differs from the inner radius by a small distance,
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A 1 mm bubble has negligible extra pressure. Yet when the diameter is ~3 ÎĽm, the bubble has an extra atmosphere inside than outside. When the bubble is only several hundred nanometers, the pressure inside can be several atmospheres. One should bear in mind that the surface tension in the
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numerator can be much smaller in the presence of surfactants or contaminants. The same calculation can be done for small oil droplets in water, where even in the presence of surfactants and a fairly low interfacial tension
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difference between the inside and the outside of a curved surface that forms the boundary between two fluid regions. The pressure difference is caused by the
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The Laplace pressure is commonly used to determine the pressure difference in spherical shapes such as bubbles or droplets. In this case,
156:{\displaystyle \Delta P\equiv P_{\text{inside}}-P_{\text{outside}}=\gamma \left({\frac {1}{R_{1}}}+{\frac {1}{R_{2}}}\right),} 868:= 72 mN/m at 25 Â°C (298 K). The extra pressure inside the bubble is given here for three bubble sizes: 52: 327: 1132: 1065: 988:= 5–10 mN/m, the pressure inside 100 nm diameter droplets can reach several atmospheres. 1127: 1012: 1037: 1095: 1032:
Butt, Hans-JĂĽrgen; Graf, Karlheinz; Kappl, Michael (2006). "Physics and Chemistry of Interfaces": 9.
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A common example of use is finding the pressure inside an air bubble in pure water, where
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of the interface between liquid and gas, or between two immiscible liquids.
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Pressure difference between the inside and the outside of a curved surface
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Gennes, Pierre-Gilles de; Francoise Brochard-Wyart; David Quere (2004).
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Experimental demonstration of Laplace pressure with soap bubbles.
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Springer. pp. 7–8. 921:{\displaystyle \Delta P} 896:{\displaystyle \Delta P} 981:{\displaystyle \gamma } 861:{\displaystyle \gamma } 257:{\displaystyle \sigma } 237:{\displaystyle \gamma } 1045:Cite journal requires 1013:Two balloon experiment 982: 922: 897: 862: 834: 407: 357: 315: 288: 258: 238: 214: 187: 157: 53:Young–Laplace equation 33: 983: 923: 898: 863: 835: 408: 358: 316: 314:{\displaystyle R_{2}} 289: 287:{\displaystyle R_{1}} 259: 239: 215: 213:{\displaystyle R_{2}} 188: 186:{\displaystyle R_{1}} 158: 31: 972: 909: 884: 852: 420: 371: 328: 298: 271: 248: 228: 197: 170: 62: 978: 918: 893: 874:Bubble diameter (2 858: 830: 403: 353: 311: 284: 254: 234: 210: 183: 153: 34: 1133:Bubbles (physics) 1077:978-0-387-00592-8 965: 964: 806: 776: 751: 730: 700: 672: 621: 591: 548: 518: 490: 351: 244:(also denoted as 143: 123: 94: 81: 29: 1140: 1107: 1106: 1104: 1103: 1094:. Archived from 1088: 1082: 1081: 1061: 1055: 1054: 1048: 1043: 1041: 1033: 1029: 998:Ostwald ripening 987: 985: 984: 979: 927: 925: 924: 919: 902: 900: 899: 894: 871: 867: 865: 864: 859: 839: 837: 836: 831: 817: 816: 807: 805: 804: 795: 787: 782: 778: 777: 775: 768: 767: 754: 752: 744: 731: 729: 728: 719: 711: 706: 702: 701: 699: 692: 691: 678: 673: 671: 664: 663: 653: 646: 645: 635: 622: 620: 619: 610: 602: 597: 593: 592: 590: 583: 582: 572: 571: 562: 549: 547: 546: 537: 529: 524: 520: 519: 517: 510: 509: 496: 491: 489: 488: 476: 460: 459: 444: 443: 412: 410: 409: 404: 396: 395: 383: 382: 362: 360: 359: 354: 352: 344: 320: 318: 317: 312: 310: 309: 293: 291: 290: 285: 283: 282: 263: 261: 260: 255: 243: 241: 240: 235: 219: 217: 216: 211: 209: 208: 192: 190: 189: 184: 182: 181: 162: 160: 159: 154: 149: 145: 144: 142: 141: 129: 124: 122: 121: 109: 96: 95: 92: 83: 82: 79: 38:Laplace pressure 30: 1148: 1147: 1143: 1142: 1141: 1139: 1138: 1137: 1113: 1112: 1111: 1110: 1101: 1099: 1090: 1089: 1085: 1078: 1063: 1062: 1058: 1044: 1034: 1031: 1030: 1026: 1021: 1003:Kelvin equation 994: 970: 969: 907: 906: 882: 881: 850: 849: 846: 796: 788: 759: 758: 736: 732: 720: 712: 683: 682: 655: 654: 637: 636: 627: 623: 611: 603: 574: 573: 563: 554: 550: 538: 530: 501: 500: 480: 474: 470: 451: 435: 418: 417: 387: 374: 369: 368: 326: 325: 301: 296: 295: 274: 269: 268: 246: 245: 226: 225: 200: 195: 194: 173: 168: 167: 133: 113: 107: 103: 87: 74: 60: 59: 46:surface tension 19: 17: 12: 11: 5: 1146: 1144: 1136: 1135: 1130: 1128:Fluid dynamics 1125: 1115: 1114: 1109: 1108: 1083: 1076: 1056: 1047:|journal= 1023: 1022: 1020: 1017: 1016: 1015: 1010: 1008:Laplace number 1005: 1000: 993: 990: 977: 963: 962: 959: 956: 952: 951: 948: 945: 941: 940: 937: 934: 930: 929: 917: 914: 904: 892: 889: 879: 857: 845: 842: 841: 840: 829: 826: 823: 820: 815: 810: 803: 799: 794: 791: 785: 781: 774: 771: 766: 762: 757: 750: 747: 742: 739: 735: 727: 723: 718: 715: 709: 705: 698: 695: 690: 686: 681: 676: 670: 667: 662: 658: 652: 649: 644: 640: 633: 630: 626: 618: 614: 609: 606: 600: 596: 589: 586: 581: 577: 570: 566: 560: 557: 553: 545: 541: 536: 533: 527: 523: 516: 513: 508: 504: 499: 494: 487: 483: 479: 473: 469: 466: 463: 458: 454: 450: 447: 442: 438: 434: 431: 428: 425: 402: 399: 394: 390: 386: 381: 377: 364: 363: 350: 347: 342: 339: 336: 333: 308: 304: 281: 277: 253: 233: 207: 203: 180: 176: 164: 163: 152: 148: 140: 136: 132: 127: 120: 116: 112: 106: 102: 99: 90: 86: 77: 73: 70: 67: 15: 13: 10: 9: 6: 4: 3: 2: 1145: 1134: 1131: 1129: 1126: 1124: 1121: 1120: 1118: 1098:on 2010-04-17 1097: 1093: 1087: 1084: 1079: 1073: 1069: 1068: 1060: 1057: 1052: 1039: 1028: 1025: 1018: 1014: 1011: 1009: 1006: 1004: 1001: 999: 996: 995: 991: 989: 975: 960: 957: 954: 953: 949: 946: 943: 942: 938: 935: 932: 931: 915: 905: 890: 880: 877: 873: 872: 869: 855: 843: 827: 821: 808: 801: 797: 792: 789: 783: 779: 772: 769: 764: 760: 755: 748: 745: 740: 737: 733: 725: 721: 716: 713: 707: 703: 696: 693: 688: 684: 679: 674: 668: 665: 660: 656: 650: 647: 642: 638: 631: 628: 624: 616: 612: 607: 604: 598: 594: 587: 584: 579: 575: 568: 564: 558: 555: 551: 543: 539: 534: 531: 525: 521: 514: 511: 506: 502: 497: 492: 485: 481: 477: 471: 467: 464: 461: 456: 452: 445: 440: 436: 429: 426: 416: 415: 414: 400: 397: 392: 388: 384: 379: 375: 348: 345: 340: 337: 334: 324: 323: 322: 306: 302: 279: 275: 265: 251: 231: 223: 205: 201: 178: 174: 150: 146: 138: 134: 130: 125: 118: 114: 110: 104: 100: 97: 88: 84: 75: 71: 68: 58: 57: 56: 54: 49: 47: 43: 39: 1100:. Retrieved 1096:the original 1086: 1066: 1059: 1038:cite journal 1027: 966: 875: 847: 365: 266: 165: 50: 37: 35: 1117:Categories 1102:2010-04-03 1019:References 413:, we find 976:γ 913:Δ 888:Δ 856:γ 793:γ 784:≈ 741:− 717:γ 675:− 608:γ 535:γ 468:γ 449:Δ 433:Δ 424:Δ 341:γ 332:Δ 252:σ 232:γ 101:γ 85:− 72:≡ 66:Δ 55:given as 1123:Pressure 992:See also 939:0.00284 844:Examples 220:are the 42:pressure 958:960000 878:) (ÎĽm) 93:outside 40:is the 1074:  961:9.474 950:0.947 947:96000 928:(atm) 166:where 80:inside 933:1000 903:(Pa) 1072:ISBN 1051:help 955:0.3 944:3.0 936:288 224:and 193:and 36:The 1119:: 1042:: 1040:}} 1036:{{ 321:: 294:= 1105:. 1080:. 1053:) 1049:( 916:P 891:P 876:r 828:. 825:) 822:d 819:( 814:O 809:+ 802:i 798:R 790:4 780:) 773:d 770:+ 765:i 761:R 756:d 749:2 746:1 738:1 734:( 726:i 722:R 714:4 708:= 704:) 697:d 694:+ 689:i 685:R 680:d 669:d 666:+ 661:i 657:R 651:d 648:+ 643:i 639:R 632:+ 629:1 625:( 617:i 613:R 605:2 599:= 595:) 588:d 585:+ 580:i 576:R 569:i 565:R 559:+ 556:1 552:( 544:i 540:R 532:2 526:= 522:) 515:d 512:+ 507:i 503:R 498:1 493:+ 486:i 482:R 478:1 472:( 465:2 462:= 457:o 453:P 446:+ 441:i 437:P 430:= 427:P 401:d 398:+ 393:i 389:R 385:= 380:o 376:R 349:R 346:2 338:= 335:P 307:2 303:R 280:1 276:R 206:2 202:R 179:1 175:R 151:, 147:) 139:2 135:R 131:1 126:+ 119:1 115:R 111:1 105:( 98:= 89:P 76:P 69:P

Index

pressure
surface tension
Young–Laplace equation
principal radii of curvature
Ostwald ripening
Kelvin equation
Laplace number
Two balloon experiment
cite journal
help
Capillarity and Wetting Phenomena
ISBN
978-0-387-00592-8
"Antimicrobial Nanoemulsions"
the original
Categories
Pressure
Fluid dynamics
Bubbles (physics)

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