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Talk:Solenoidal vector field

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211: 100: 90: 69: 36: 201: 174: 27: 332:. Now, what is this page trying to achieve? Is it going to state the lemma, in effect, in vector calculus terms, so as not to frighten the horses? Is it going to state some valid special case? Is it going to try to prove (better, sketch a proof of) something? Anyway these points seem bound up with trying to get our necessary and our sufficient conditions clearer. 1024:
think "combing pipes so they're always connected". I'm guessing this is a 19th century idea. If you read James Clerk Maxwell's diaries, they're filled with these esoteric thoughts of mechanistic fluids sloshing around in cycles. The concept of a vector field, clearly popular in the 19th cent, its hard to imagine that its much older than that.
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It's "solenoidal" because of the curl. You can imagine each vector in the field as being a tiny pipe, and the pipes must always be connected so that there's just as much coming in as there is going out: the pipes don't leak. So instead of the conventional "combing hair without flat spots or peaks",
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These fields are almost certainly called solenoidal because of their relationship to solenoidal magnetic fields (i.e. magnetic fields generated from pipe-like coils of current-carrying wires). This seems to me to be a folk etymology (and a quite bizarre one at that), it definitely needs a source.
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As far as I understand the definition of a vector field that is solenoidal on a domain Omega (using the term domain loosely here) is that there is no net flow through any closed surface (again using that term loosely) contained in Omega. For many types of domains, such as e.g. simply connected or
850:. Michiel Hazewinkel "Encyclopaedia of Mathematics" vol. 9 p402 (viewable in Google Books) gives a stronger surface-integral definition, and notes that divergencelessness does not imply solenoidality in domains with holes. I can't immediately find any other book giving this stronger definition. 16:
Is there any reason at all not to edit this down so that it just says (1) solenoidal means zero divergence and (2) this is equivalent to having a vector potential? I don't think there's any other content on this page that isn't either incorrect or irrelevant. Perhaps it's worth adding that
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However, this analogy does not hold in all cases. A typical example, that has some relevance e.g. in the Earth Sciences, are annuli and thick spherical shells. For such domains a field can by divergence-free, but non-solenoidal. An example is given by the field
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an anon contribution, and hit "Return" before finishing my comment. I meant to say that the proof in the article is rigurious. Even if the curl is not the same as the cross-product, they obey the same laws.
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in a number of articles. It's clearly incorrect in this case (I reckon), so I've reverted it. Please discuss the matter here if you disagree. Also, it'd be helpful if you registered a user name. Thanks,
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F such that f = curl F is only supposed be true on specific domains (I'm not sure whether it's star-like or simply connected one implying the other anyway). Don't you think it should be added ?
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Actually B is now considered the Magnetic Field by physicists, so please never use Magnetic Field to mean H. Special Contributions 83.131.29.96 is totally correct on that one!
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True, most of the article seems to go on and on and the essence of the subject gets lost. What I find odd is that the article starts by saying that a solenoidal vector field
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confirms that such a word was used in Ancient Greek. How it came to be applied to the vector field I don't know, though your explanation does seem rather more plausible. -
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We should follow the sources; start with the 'elementary' definition, then follow with the 'advanced' definition, noting how they differ. --
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does only constitute one part of the boundary of the volume enclosed by it, the other one being the inner boundary of the domain itself.
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G. Backus, Poloidal and Torroidal Fields in Geomagnetic Field Modelling, Reviews of Geophysics, no. 1, vol. 24, 1986, pp. 75-109
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most commonly defined as divergenceless - however theses are largely elementary texts which confine their attention to
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star-shaped this is the case (for a continuously differentiable field) if and only if the field is divergence-free.
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a common way of expressing the property of a vector field's having zero divergence. It is not a way at all. It is
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This field can be shown to be divergence-free on this domain. However, the net flow through a sphere
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but that's too much for me. A rewrite (leaving out the talk of cars highways and gears) would be
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A common way of expressing this property is to say that the field has no sources or sinks.
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There is no way solenoidal comes from Greek "constrained as if in a pipe"
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This does not contradict the divergence theorem, since the sphere
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While here - there is certainly a connection with the
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The term 1061:Knowledge vital articles in Mathematics 1001:says the word comes from Ancient Greek 962:What counter-examples had you in mind? 686: 677: 170: 65: 18:a velocity field with zero divergence. 842:Flicking through a few books, I find 7: 222:This article is within the scope of 111:This article is within the scope of 1106:Start-Class fluid dynamics articles 54:It is of interest to the following 1066:Start-Class level-5 vital articles 750: 628: 393:What does "divless" mean? Just as 372:Special:Contributions/83.131.29.96 310:div v = 0. Maybe mathematics is a 14: 1086:Mid-priority mathematics articles 444:of an field is the field itself ( 440:is not itself an electric field. 131:Knowledge:WikiProject Mathematics 1081:Start-Class mathematics articles 1056:Knowledge level-5 vital articles 1007:Liddell & Scott's dictionary 947:, as the simplest examples show. 429:is just an magnetic analogue of 209: 199: 172: 134:Template:WikiProject Mathematics 98: 88: 67: 34: 25: 17:incompressible fluid flow =: --> 1096:Mid-importance physics articles 820:Lecture Notes in Geomathematics 262:This article has been rated as 151:This article has been rated as 766: 754: 709: 701: 644: 632: 593: 584: 571: 565: 512:13:46, 12 September 2007 (UTC) 1: 993:21:24, 20 February 2023 (UTC) 972:13:08, 31 December 2019 (UTC) 957:10:35, 31 December 2019 (UTC) 920:15:36, 20 February 2014 (UTC) 865:17:53, 28 December 2009 (UTC) 837:11:05, 28 December 2009 (UTC) 361:22:55, 13 November 2005 (UTC) 318:. --12:27, 16 Mar 2005 (UTC) 298:Much of it should go methinks 277:This article is supported by 242:Knowledge:WikiProject Physics 236:and see a list of open tasks. 125:and see a list of open tasks. 1091:Start-Class physics articles 939:No, that is most definitely 245:Template:WikiProject Physics 431:electric displacement field 321:OK: done, rather brutally. 1127: 1051:Start-Class vital articles 1034:16:23, 22 March 2024 (UTC) 1019:00:18, 23 March 2023 (UTC) 544:Correctness of definition? 409:over an area, and just as 268:project's importance scale 492:00:34, 17 June 2014 (UTC) 338:17:03, 20 Mar 2005 (UTC) 325:14:11, 2005 Mar 20 (UTC) 276: 261: 194: 150: 83: 62: 538:08:48, 21 May 2008 (UTC) 465:10:46, 8 July 2007 (UTC) 388:17:04, 7 July 2007 (UTC) 280:Fluid Dynamics Taskforce 157:project's priority scale 1111:Fluid dynamics articles 517:Simply connected domain 114:WikiProject Mathematics 798: 775: 730: 610: 925:Terrible introduction 799: 797:{\displaystyle 4\pi } 776: 731: 611: 450:magnetic flux density 376:magnetic flux density 41:level-5 vital article 785: 746: 624: 559: 401:over an area, so is 137:mathematics articles 342:My recent reversion 225:WikiProject Physics 794: 771: 726: 687: 678: 606: 366:B is divless not H 106:Mathematics portal 50:content assessment 604: 540: 528:comment added by 503:Why is it called 495: 478:comment added by 295: 294: 291: 290: 287: 286: 167: 166: 163: 162: 1118: 888:vector potential 803: 801: 800: 795: 780: 778: 777: 772: 770: 769: 735: 733: 732: 727: 725: 724: 712: 704: 685: 684: 676: 675: 670: 658: 657: 648: 647: 615: 613: 612: 607: 605: 603: 602: 601: 596: 587: 578: 523: 521:div f = 0 =: --> 494: 472: 458:more than a year 336:Charles Matthews 323:Gareth McCaughan 250: 249: 248:physics articles 246: 243: 240: 219: 214: 213: 203: 196: 195: 190: 187: 176: 169: 139: 138: 135: 132: 129: 108: 103: 102: 92: 85: 84: 79: 71: 64: 47: 38: 37: 30: 29: 21: 1126: 1125: 1121: 1120: 1119: 1117: 1116: 1115: 1041: 1040: 1005:"pipe-shaped"; 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