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Monodomain model

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780: 502: 1446: 775:{\displaystyle {\begin{aligned}\nabla \cdot \left(\mathbf {\Sigma } _{i}\nabla v\right)+\nabla \cdot \left(\mathbf {\Sigma } _{i}\nabla v_{e}\right)&=\chi \left(C_{m}{\frac {\partial v}{\partial t}}+I_{\text{ion}}\right)\\\nabla \cdot \left(\mathbf {\Sigma } _{i}\nabla v\right)+\nabla \cdot \left(\left(\mathbf {\Sigma } _{i}+\mathbf {\Sigma } _{e}\right)\nabla v_{e}\right)&=0\end{aligned}}} 22: 340: 1081: 184: 948: 1090:
Differently from the bidomain model, the monodomain model is usually equipped with an isolated boundary condition, which means that it is assumed that there is not current that can flow from or to the domain (usually the heart). Mathematically, this is done imposing a zero transmembrane potential
1188: 955: 834: 335:{\displaystyle {\frac {\lambda }{1+\lambda }}\nabla \cdot \left(\mathbf {\Sigma } _{i}\nabla v\right)=\chi \left(C_{m}{\frac {\partial v}{\partial t}}+I_{\text{ion}}\right)\quad \quad {\text{in }}\mathbb {T} \times (0,T),} 829: 126:
of the electrical propagation in myocardial tissue. The reduction comes from assuming that the intra- and extracellular domains have equal anisotropy ratios. Although not as physiologically accurate as the
1105: 507: 371: 1238: 1076:{\displaystyle {\frac {\lambda }{1+\lambda }}\nabla \cdot \left(\mathbf {\Sigma } _{i}\nabla v\right)=\chi \left(C_{m}{\frac {\partial v}{\partial t}}+I_{\text{ion}}\right).} 418: 1213: 159: 465: 485: 445: 391: 179: 943:{\displaystyle \nabla \cdot \left(\mathbf {\Sigma } _{i}\nabla v_{e}\right)=-{\frac {1}{1+\lambda }}\nabla \cdot \left(\mathbf {\Sigma } _{i}\nabla v\right).} 1487: 1521: 1317: 1254: 787: 1531: 1506: 1292: 105: 39: 1511: 1480: 86: 1183:{\displaystyle (\mathbf {\Sigma } _{i}\nabla v)\cdot \mathbf {n} =0\quad \quad {\text{on }}\partial \mathbb {T} \times (0,T)} 58: 43: 1526: 65: 1516: 1473: 1092: 1393:
Boulakia, Muriel; Cazeau, Serge; Fernández, Miguel A.; Gerbeau, Jean-Frédéric; Zemzemi, Nejib (24 December 2009).
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Mathematically modelling the electrical activity of the heart : from cell to body surface and back again
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Then, inserting this into the first bidomain equation gives the unique equation of the monodomain model
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the final time, the monodomain model can be formulated as follows
131:, it is still adequate in some cases, and has reduced complexity. 1395:"Mathematical Modeling of Electrocardiograms: A Numerical Study" 15: 1283:
Pullan, Andrew J.; Buist, Martin L.; Cheng, Leo K. (2005).
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is the membrane surface area per unit volume (of tissue).
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Chaos: An Interdisciplinary Journal of Nonlinear Science
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is the intra- to extracellular conductivity ratio, and
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Rossi, Simone; Griffith, Boyce E. (1 September 2017).
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The monodomain model can be easily derived from the
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Unsourced material may be challenged and removed. 1232: 1207: 1182: 1075: 942: 823: 774: 479: 459: 439: 420:is the transmembrane ionic current per unit area, 412: 385: 365: 334: 173: 153: 1388: 1386: 1310:Mathematical Physiology II: Systems Physiology 1481: 1278: 1276: 1274: 1272: 1270: 1215:is the unit outward normal of the domain and 8: 447:is the membrane capacitance per unit area, 1488: 1474: 373:is the intracellular conductivity tensor, 1366: 1226: 1225: 1220: 1200: 1198: 1158: 1157: 1149: 1136: 1118: 1113: 1107: 1059: 1032: 1026: 994: 989: 959: 957: 920: 915: 885: 868: 855: 850: 836: 815: 810: 797: 792: 789: 747: 729: 724: 714: 709: 672: 667: 640: 613: 607: 577: 564: 559: 527: 522: 506: 504: 472: 452: 431: 425: 404: 398: 378: 357: 352: 349: 307: 306: 301: 288: 261: 255: 223: 218: 188: 186: 166: 147: 146: 144: 106:Learn how and when to remove this message 831:, the second equation can be written as 1266: 784:Assuming equal anisotropy ratios, i.e. 366:{\displaystyle \mathbf {\Sigma } _{i}} 1233:{\displaystyle \partial \mathbb {T} } 7: 1442: 1440: 1255:Forward problem of electrocardiology 44:adding citations to reliable sources 1460:. You can help Knowledge (XXG) by 1222: 1154: 1124: 1043: 1035: 1000: 977: 926: 903: 861: 838: 740: 692: 678: 655: 624: 616: 570: 547: 533: 510: 499:. This last one can be written as 272: 264: 229: 206: 14: 1444: 1402:Annals of Biomedical Engineering 1201: 1137: 1114: 990: 916: 851: 811: 793: 725: 710: 668: 560: 523: 393:is the transmembrane potential, 353: 219: 20: 1148: 1147: 300: 299: 31:needs additional citations for 1522:Partial differential equations 1177: 1165: 1130: 1109: 413:{\displaystyle I_{\text{ion}}} 326: 314: 1: 1208:{\displaystyle \mathbf {n} } 154:{\displaystyle \mathbb {T} } 1548: 1439: 1312:(2nd ed.). Springer. 1308:Keener J, Sneyd J (2009). 1093:Neumann boundary condition 1532:Applied mathematics stubs 1507:Cardiac electrophysiology 1414:10.1007/s10439-009-9873-0 1240:is the domain boundary. 460:{\displaystyle \lambda } 161:the spatial domain, and 1512:Differential equations 1456:-related article is a 1234: 1209: 1184: 1077: 944: 825: 776: 481: 461: 441: 414: 387: 367: 336: 175: 155: 122:is a reduction of the 1235: 1210: 1185: 1078: 945: 826: 777: 482: 480:{\displaystyle \chi } 462: 442: 440:{\displaystyle C_{m}} 415: 388: 368: 337: 176: 156: 1287:. World Scientific. 1219: 1197: 1106: 956: 835: 788: 503: 471: 451: 424: 397: 377: 348: 185: 165: 143: 40:improve this article 1527:Biological theorems 1454:applied mathematics 1086:Boundary conditions 1230: 1205: 1180: 1091:flux (homogeneous 1073: 940: 821: 772: 770: 477: 457: 437: 410: 383: 363: 332: 171: 151: 55:"Monodomain model" 1517:Electrophysiology 1469: 1468: 1351:10.1063/1.5000706 1319:978-0-387-79387-0 1152: 1062: 1050: 975: 901: 643: 631: 407: 386:{\displaystyle v} 304: 291: 279: 204: 174:{\displaystyle T} 116: 115: 108: 90: 1539: 1490: 1483: 1476: 1448: 1441: 1434: 1433: 1408:(3): 1071–1097. 1399: 1390: 1381: 1380: 1370: 1330: 1324: 1323: 1305: 1299: 1298: 1280: 1239: 1237: 1236: 1231: 1229: 1214: 1212: 1211: 1206: 1204: 1189: 1187: 1186: 1181: 1161: 1153: 1150: 1140: 1123: 1122: 1117: 1082: 1080: 1079: 1074: 1069: 1065: 1064: 1063: 1060: 1051: 1049: 1041: 1033: 1031: 1030: 1010: 1006: 999: 998: 993: 976: 974: 960: 949: 947: 946: 941: 936: 932: 925: 924: 919: 902: 900: 886: 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107: 99: 88: 85: 81: 78: 74: 71: 67: 64: 60: 57: –  56: 52: 51:Find sources: 45: 41: 35: 34: 29:This article 27: 23: 18: 17: 1462:expanding it 1451: 1405: 1401: 1342: 1338: 1328: 1309: 1303: 1284: 1192: 1096: 1089: 951: 783: 494: 343: 138: 119: 117: 102: 93: 83: 76: 69: 62: 50: 38:Please help 33:verification 30: 135:Formulation 1501:Categories 1261:References 491:Derivation 96:April 2014 66:newspapers 1359:1054-1500 1223:∂ 1163:× 1155:∂ 1134:⋅ 1125:∇ 1115:Σ 1044:∂ 1036:∂ 1015:χ 1001:∇ 991:Σ 981:⋅ 978:∇ 972:λ 962:λ 927:∇ 917:Σ 907:⋅ 904:∇ 898:λ 883:− 862:∇ 852:Σ 842:⋅ 839:∇ 812:Σ 807:λ 794:Σ 741:∇ 726:Σ 711:Σ 696:⋅ 693:∇ 679:∇ 669:Σ 659:⋅ 656:∇ 625:∂ 617:∂ 596:χ 571:∇ 561:Σ 551:⋅ 548:∇ 534:∇ 524:Σ 514:⋅ 511:∇ 475:χ 455:λ 354:Σ 312:× 273:∂ 265:∂ 244:χ 230:∇ 220:Σ 210:⋅ 207:∇ 201:λ 191:λ 1430:10114284 1422:20033779 1377:28964127 1244:See also 1151:on  303:in  1368:5585078 80:scholar 1428:  1420:  1375:  1365:  1357:  1316:  1291:  1193:where 344:where 139:Being 82:  75:  68:  61:  53:  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Index


verification
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adding citations to reliable sources
"Monodomain model"
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bidomain model
bidomain model
bidomain model
Neumann boundary condition
Bidomain model
Forward problem of electrocardiology





ISBN
978-9812563736
ISBN
978-0-387-79387-0
"Incorporating inductances in tissue-scale models of cardiac electrophysiology"
doi
10.1063/1.5000706
ISSN

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