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Talk:Sliding mode control

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945:
should be added about implementation details... or realizations of sliding mode controllers. Perhaps all of this could be added to the first sentence or two of the article and the rest could remain. If you have a suggestion on new wording, you should give it. I think changes should be made with great care though; there is danger that the discussion can actually add more ambiguity for the casual reader (and face it, most people who use SMC in industry are going to view it as a switching control... or perhaps the asymptotic limit of very high gain control with the understanding that real-world effects lead to chattering). —
923:
Filippov is not an highly swithing signal. Since the state is on the sliding surface, the control has the same regularity as the external input. In a discrete implementation, when an explicit Euler method or an explicit ZOH is used, we get a high frequency switching signal. This is not inherent to the sliding mode control but to an poor disctrization scheme or to the actuator's technology. When an implicit discretization is performed and the actuators is able to deliver the whole convex hull of the systems right-hand-side, the control does not switch anymore.
1038:). It's a mess. It was apparently lifted from someone's LaTeX manuscript (notice all of the \ref's and \cite's). Consequently, I worry that its source might have been an unpublished manuscript that was rejected(?). Regardless, if it is to be added here, all of the LaTeX \refs and \cites must be replaced with the equivalent Knowledge versions. Moreover, the \cite targets must actually be added to the references. Finally, it should be proof read to remove typos (e.g., change "for" to "form" in the first sentence). 243: 222: 319: 253: 1581: 2189: 2311:\cite{Loukyanov1981} authors have investigated this problem and proposed a design regularization algorithm. It has been established that the regularization problem is solvable only for one class of systems which fulfills the Frobenius' theorem conditions. The reader is referred to \cite{Utkin1992} for a complete overview of this approach applied to both single-input and multiple-input. 749:. Of course, chattering can occur. In fact, in real systems, even when there is no delay, unmodeled nonlinearities from quantization error and friction produce the same discontinuities you'd see in a sliding mode controller. Hence, chattering is just a fact of life. However, a sliding mode controller nearly depends on it; it's not a maybe, it's a given. Sliding mode control 191: 1355: 892:
in the vector field) precisely where the zero-switching surface is. We need to be cognizant that it may be impossible to create a sliding mode along our sliding hypersurface, but I don't think we need to gild the lily. That being said, it's certainly fine to make things more precise. This article still needs a lot of work. —
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from the article. However, he does not discuss the topic "low-pass behaviour of the system" which makes in my opinion the problem negletable in sytems with order higher as lets say 2 or 3. However I do not agree to the words above, because chattering also happens under ideal conditions unless you have a zero-band.--
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applied with care and should not be a hammer applied to every nail. This is not a new criticism. It's just that VSC has become the PID of industrial nonlinear control; it evolves on its own without any informed help. (All of that being said, I'll revert your change and massage it to not be as "brutal") —
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the sliding mode exists, then it is totally appropriate to substitute one term for the other. The reason why "mode" and "surface" are so easily swapped is that systems in which they do not match are of no interest to us. That is, we're building a control that generates a sliding mode (i.e., a crease
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These are minor technicalities that bridge into the realm of interpretation. I concede your point that switching is more an artifact of the real world than of the idealization of the control method. Perhaps the control method should be presented in a more pure form for motivation and then something
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When I learned about sliding mode control about 2000 chattering (high frequency switching) was a topic although I cannot recall the correct bibliographical data of that utkin-paper. Without mentioning sliding mode control "Föllinger, Nichtlineare Regelung I & II" described the effect as deleted
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Reason: Unsourced that the apparant "brutality" of the control algoritm is a disadvantage. If used with switching power converters the choice of sliding mode controller seems very natural. (Source an further explanation added to the article). The socalled chattering problem should be treated in the
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I think the article is a good introduction to SMC. Thanks for correcting my corrections. I have a terminology question. I am thinking of the "sliding surface" as the supspace/place where the motion - the "sliding mode" - takes place. I think the article confuses the place and the (kind of) motion,
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that have more moderate control action. In particular, because actuators have delays and other imperfections, the hard sliding-mode-control action can lead to chatter, energy loss, plant damage, and excitation of unmodeled dynamics. Continuous control design methods are not as susceptible to these
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in industrial control (often using the same justification that you use -- the future is in switching). However, the mathematics needed to justify comments about the robustness (and safety) of the control method are far more sophisticated than what you need with continuous control. VSC needs to be
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From my point of view, the sentence in the introduction " ... is a nonlinear control method that alters the dynamics of a nonlinear system by application of a high-frequency switching control" is really ambiguous. In continuous time, the sliding mode control given by the solution in the sense of
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Necessary and sufficient conditions for solving the equation (\ref{BCPFM05}) may be found based on the theory of Pfaffian's form in the text book of Rashevskii \cite{Rashevskii1947}. It should be noticed that partial differential equations of this type need strong solvability conditions. In
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The best perfomance of idea in sliding mode controll achieved prof. Feldbaum. The main idea of his method is finding the optimal phase curves. And after some modification we are may find hyperplane - sliding hyperplane. This is the best knowing method for the controlling of the object.
1576:{\displaystyle \left\{{\begin{array}{l}\mathbf {\dot {x}} _{1}=\mathbf {f} _{1}\left(\mathbf {x} _{1}\mathbf {,x} _{2}\right)\\\mathbf {\dot {x}} _{2}=\mathbf {f} _{2}\left(\mathbf {x} _{1}\mathbf {,x} _{2}\right)+\mathbf {B} _{2}\mathbf {\left(x_{1},x_{2}\right)u} \end{array}}\right.} 826:
but I might be wrong. For example, I can say "the system trajectories cross the sliding surface, but sliding mode does not occur" but if I swap "sliding surface" and "sliding mode" the sentance makes no sense anymore. Do I have a point? I'll look for some sources myself too.
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Could I suggest adding a phase portrait to the introduction to illustrate a sliding action? I find these really help when you are first learning about sliding mode (even if it can only apply to second order systems). If nobody objects then I could provide an image -
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It is fine for me. I agree that the introduction should keep its generality. I will work on a new section on the realization/discretization of sliding modes controllers if I have some time to show how the infinitely switching control is not mandatory.
2962:
The article goes at length to describe reaching laws and talks about keeping the motion on the sliding surface, but says nothing about how to actually do that, including in the examples. It merely says something like suppose that on the sliding surface
2184:{\displaystyle {\dot {y}}_{1}={\frac {\partial \phi \left(\mathbf {x} \right)}{\partial \mathbf {x} }}f\left(\mathbf {x} \right)+{\frac {\partial \phi \left(\mathbf {x} \right)}{\partial \mathbf {x} }}\mathbf {B} \left(\mathbf {x} \right)\mathbf {u,} } 1128: 3039: 2765: 1947: 153: 2680: 3187: 3101: 1296: 2881:
In other words, the evolution of the upper subsystem in (\ref{BCPFM02}) is determined by equation (\ref{BCPFM06}). The desired dynamics of sliding mode can be designed by a proper choice of the function
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paragraph) makes no sense. See the last three paragraphs in the introduction. See if that's satisfactory. They now include a note about the optimality of sliding mode in certain contexts. —
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that gains its robustness from its brutality. It's also primitive when you consider all of the recent work in hybrid systems (see, for example, the terrific review from IEEE CSM this year:
2233: 765:). All of that being said, please review the bottom of the second paragraph and the third paragraph. I think they're a good unbiased summary of the state of the art in SMC application. — 2566: 1056:
is presented to obtain a convenient interpretation of the reduced order dynamics provided by sliding mode control, decoupling the system into two subsystems of lower dimensions.
541:. That is, the structure of the control law changes based on the position of the state trajectory; hence, sliding mode control is a variable structure control method because it 3125: 147: 2336: 2006: 1784: 1866: 622:
I think that's a great idea. It might be a good idea to use a phase portrait for one of the commonly-used examples already given on the page. Go ahead and provide one. Be
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I'm going to argue that it's sloppy to say that a "sliding mode does not occur." However, I concede your point. The issue is that I can create a switching function
1298:. Following the regular form design approach, a nonlinear transformation should be found such that the system is decoupled into two subsystems of lower dimensions 2586: 2395: 1348: 1061: 2966: 435:
Then add a reference. It's common to discuss sliding mode control schemes in optimal control classes. In fact, this topic may need its OWN Knowledge article. —
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and any dynamics it is not automatically guaranteed that this will hold. Shouldn't something be said about this and an example given where one does have
79: 1873: 3217: 309: 299: 349:\dot V < 0 only implies asymtotic movement to the sliding surface. A more strong condition like \dot V \leq \alpha o \dot V \leq V^{1/p}, p: --> 3227: 85: 887:. However, that surface is not necessarily a sliding mode of the system – I have no guarantee that a sliding mode exists. That being said, 363: 697:
If I recall correctly, Khalil has an entire section devoted to continuous alternatives to sliding mode control. SMC has been treated as a
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I've generated a plot but it seems that I have to make ten edits before I can upload images (so will upload it asap) -
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that will be enough to satisfy most people. It would be great if an expert could make things more precise. —
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I'm not an expert in sliding mode control, but I've gone through and added comments that the system
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The set in Theorem 2 is empty. This definition clearly is incorrect. Is a dot missing? --
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I just made a change that changes the order so that my request (about the bottom of the
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seems to be redundant. However I am not sure and therefore cannot solve the problem.--
3206: 2760:{\displaystyle S(\mathbf {x} )=\mathbf {x} _{2}-S_{0}\left(\mathbf {x} _{1}\right)=0} 827: 683: 2316:
According to system (\ref{BCPFM02}), the sliding mode control approach assumes that
1942:{\displaystyle y_{1}=\phi \left(\mathbf {x} \right),\quad y_{2}=\mathbf {x} _{2},} 1786:
and the upper equation does not depend on the real control, is referred to as a
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reach the surface in finite time because the control need not be continuous. I
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be a vector of new state variables defined by the nonlinear transformation
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I removed the following section on an SMC regular form which was added by
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The state-feedback control law is not a continuous function of time; it
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Someone fixed this sometime. I tried to make it a little better now. —
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which takes part of the reduced order system dynamics(\ref{BCPFM06}).
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The idea of transformation is formulated in the following way: Let
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I suggest to formulate this remark somewhere in this introduction.
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1 is required for the finite time entrance to the sliding surface.
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is a discontinuous control enforcing sliding mode in the manifold
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is continuous and continuously differentiable with respect to
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components of the state vector are function of the remaining
1291:{\displaystyle {\text{rank}}\left(\mathbf {B} \right)=m<n} 3174: 3112: 3088: 2972: 2682:. As a result, the sliding mode equation along the manifold 317: 1570: 674:
problems and can be made to mimic sliding-mode controllers.
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is a solution to the matrix partial differential equation
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will be independent of the control if the vector function
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In this section a particular canonical for, the so-called
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Sliding mode control is sometimes critiqued as being a
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Anyone care to add an introduction in plain English?
2524:{\displaystyle S\left(\mathbf {x} \right)=\left^{T}} 1674:{\displaystyle \mathbf {x} _{2}\in \mathbb {R} ^{m}} 3181: 3119: 3095: 3033: 2922:{\displaystyle S_{0}\left(\mathbf {x} _{1}\right)} 2921: 2867: 2759: 2674: 2612: 2580: 2560: 2523: 2397:selected switching surfaces denoted by the vector 2389: 2369: 2330: 2296: 2220: 2183: 2027: 2000: 1978: 1941: 1860: 1778: 1756: 1710: 1673: 1629: 1575: 1342: 1322: 1290: 1243: 1200: 1163: 1122: 879: 853: 406:Just about to add a section making this precise. — 2958:Guaranteeing desired dynamics on sliding surface? 1725: 1711:{\displaystyle \mathbf {u} \in \mathbb {R} ^{m}} 1201:{\displaystyle \mathbf {u} \in \mathbb {R} ^{m}} 1164:{\displaystyle \mathbf {x} \in \mathbb {R} ^{n}} 33:for general discussion of the article's subject. 745:I think that's why the original statement says 543:switches from one smooth control law to another 2221:{\displaystyle \phi \left(\mathbf {x} \right)} 1979:{\displaystyle \phi \left(\mathbf {x} \right)} 539:switches from one smooth condition to another 174: 8: 3028: 2980: 2370:{\displaystyle S\left(\mathbf {x} \right)=0} 270:, which collaborates on articles related to 861:, and there is a surface corresponding to 660:Moved away from article on April 6th, 2009 495:- How does Sliding mode solve the problem 216: 3173: 3172: 3135: 3134: 3132: 3111: 3110: 3108: 3087: 3086: 3049: 3048: 3046: 3014: 3003: 2997: 2993: 2992: 2984: 2983: 2971: 2970: 2968: 2909: 2904: 2893: 2887: 2850: 2845: 2834: 2821: 2816: 2804: 2799: 2789: 2778: 2777: 2774: 2741: 2736: 2725: 2712: 2707: 2695: 2687: 2662: 2657: 2646: 2633: 2628: 2625: 2593: 2573: 2544: 2536: 2515: 2501: 2491: 2469: 2459: 2443: 2433: 2411: 2402: 2382: 2352: 2343: 2323: 2321: 2272: 2264: 2250: 2237: 2235: 2209: 2200: 2173: 2164: 2155: 2147: 2133: 2120: 2108: 2093: 2079: 2066: 2057: 2046: 2045: 2042: 2019: 2013: 1993: 1991: 1967: 1958: 1930: 1925: 1915: 1897: 1881: 1875: 1847: 1842: 1829: 1824: 1806: 1800: 1771: 1769: 1738: 1733: 1723: 1702: 1698: 1697: 1688: 1686: 1665: 1661: 1660: 1650: 1645: 1642: 1615: 1611: 1610: 1600: 1595: 1592: 1551: 1538: 1528: 1522: 1517: 1502: 1494: 1487: 1482: 1470: 1465: 1455: 1444: 1443: 1427: 1419: 1412: 1407: 1395: 1390: 1380: 1369: 1368: 1363: 1357: 1335: 1303: 1267: 1258: 1256: 1229: 1225: 1224: 1215: 1213: 1192: 1188: 1187: 1178: 1176: 1155: 1151: 1150: 1141: 1139: 1115: 1096: 1067: 1066: 1065: 1063: 866: 846: 3161: 3075: 518:Better? If not, what more would help? — 218: 188: 973:I've made some changes. How is that? — 580:I think the answer is "Yes". Thanks.-- 7: 498:- Possibly an analogy or an example 326:This article is within the field of 264:This article is within the scope of 1026:Removed new section on regular form 918:High frequency switching control  ? 492:- What is the problem to be solved 207:It is of interest to the following 23:for discussing improvements to the 3223:Systems articles in control theory 3163: 3077: 2261: 2240: 2144: 2123: 2090: 2069: 1044:Sliding mode control based on the 14: 2561:{\displaystyle S(\mathbf {x} )=0} 3015: 2905: 2846: 2817: 2800: 2783: 2780: 2737: 2708: 2696: 2658: 2629: 2545: 2502: 2470: 2444: 2412: 2353: 2324: 2273: 2265: 2251: 2210: 2177: 2174: 2165: 2156: 2148: 2134: 2109: 2094: 2080: 2008:. 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After sliding mode occurs on 304:This article has been rated as 3152: 3146: 3120:{\displaystyle {\mathcal {S}}} 3066: 3060: 3019: 3011: 3004: 2700: 2692: 2607: 2595: 2549: 2541: 1317: 1305: 1: 1909: 530:18:31, 29 November 2008 (UTC) 513:00:45, 22 February 2008 (UTC) 479:18:31, 29 November 2008 (UTC) 447:18:30, 29 November 2008 (UTC) 398:18:29, 29 November 2008 (UTC) 284:Knowledge:WikiProject Systems 42:Put new text under old text. 3228:WikiProject Systems articles 2953:16:28, 2 November 2011 (UTC) 2331:{\displaystyle \mathbf {u} } 2001:{\displaystyle \mathbf {x} } 1779:{\displaystyle \mathbf {u} } 654:17:29, 19 January 2009 (UTC) 638:22:27, 15 January 2009 (UTC) 617:17:29, 15 January 2009 (UTC) 372:15:38, 4 November 2008 (UTC) 287:Template:WikiProject Systems 1861:{\displaystyle y^{T}=\left} 50:New to Knowledge? 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2018: 1996: 1974: 1970: 1966: 1962: 1951: 1950: 1949: 1938: 1933: 1928: 1923: 1918: 1914: 1908: 1904: 1900: 1896: 1892: 1889: 1884: 1880: 1856: 1850: 1845: 1841: 1837: 1832: 1827: 1823: 1818: 1814: 1809: 1805: 1793: 1791: 1774: 1753: 1750: 1746: 1741: 1736: 1731: 1727: 1705: 1700: 1695: 1691: 1668: 1663: 1658: 1653: 1648: 1624: 1621: 1618: 1613: 1608: 1603: 1598: 1585: 1584: 1583: 1571: 1564: 1560: 1554: 1550: 1546: 1541: 1537: 1532: 1525: 1520: 1515: 1511: 1505: 1500: 1497: 1490: 1485: 1479: 1473: 1468: 1463: 1458: 1451: 1448: 1441: 1440: 1436: 1430: 1425: 1422: 1415: 1410: 1404: 1398: 1393: 1388: 1383: 1376: 1373: 1366: 1365: 1362: 1339: 1319: 1316: 1313: 1310: 1307: 1287: 1284: 1281: 1278: 1274: 1270: 1266: 1238: 1235: 1232: 1227: 1222: 1218: 1195: 1190: 1185: 1181: 1158: 1153: 1148: 1144: 1132: 1131: 1130: 1118: 1113: 1110: 1107: 1102: 1099: 1094: 1091: 1088: 1083: 1080: 1074: 1071: 1050: 1049: 1048: 1027: 1024: 1023: 1022: 1021: 1020: 1019: 1018: 998: 997: 996: 995: 968: 967: 919: 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544: 540: 536: 535: 533: 532: 531: 527: 523: 522: 517: 516: 515: 514: 510: 506: 505:Davide Andrea 502: 499: 496: 493: 490: 485:Plain English 484: 480: 476: 472: 471: 466: 465: 464: 463: 460: 452: 448: 444: 440: 439: 434: 433: 432: 425: 419: 415: 411: 410: 405: 404: 403: 402: 399: 395: 391: 390: 385: 381: 377: 376: 375: 373: 369: 365: 361: 354: 351: 344: 329: 320: 316: 315: 311: 307: 301: 298: 297: 294: 277: 273: 269: 268: 260: 249: 247: 244: 240: 239: 235: 229: 226: 223: 219: 214: 210: 204: 196: 192: 187: 186: 177: 173: 170: 167: 163: 159: 155: 152: 149: 146: 143: 140: 137: 134: 131: 127: 124: 123:Find sources: 120: 119: 111: 110:Verifiability 108: 106: 103: 101: 98: 97: 96: 87: 83: 81: 78: 76: 72: 69: 67: 64: 63: 57: 53: 52:Learn to edit 49: 46: 41: 40: 37: 36: 32: 26: 22: 18: 17: 2961: 2934: 2932: 1788:Regular Form 1787: 1054:Regular Form 1053: 1046:Regular Form 1045: 1029: 974: 946: 928: 925: 921: 893: 888: 824: 821:Good article 798: 794: 766: 750: 746: 703: 681: 677: 664: 663: 627: 605: 565: 542: 538: 519: 503: 500: 497: 494: 491: 488: 468: 456: 436: 429: 407: 387: 383: 379: 355: 352: 348: 305: 265: 209:WikiProjects 171: 165: 157: 150: 144: 138: 132: 122: 94: 19:This is the 358:—Preceding 148:free images 31:not a forum 3207:Categories 2936:TedPavlic 976:TedPavlic 948:TedPavlic 895:TedPavlic 800:TedPavlic 768:TedPavlic 705:TedPavlic 629:TedPavlic 567:TedPavlic 521:TedPavlic 470:TedPavlic 459:TedPavlic 438:TedPavlic 409:TedPavlic 389:TedPavlic 88:if needed 71:Be polite 21:talk page 426:Feldbaum 360:unsigned 353:Cheers. 56:get help 29:This is 27:article. 2945:contrib 985:contrib 957:contrib 904:contrib 699:panacea 624:WP:BOLD 501:Thanks 308:on the 281:Systems 272:systems 228:Systems 199:C-class 154:WP refs 142:scholar 2620:ones: 1587:where 1251:, and 1134:where 1008:Vacary 931:Vacary 795:second 205:scale. 126:Google 2377:with 646:Adlab 609:Adlab 384:think 169:JSTOR 130:books 84:Seek 3195:talk 3189:? -- 2941:talk 1718:and 1330:and 1283:< 1260:rank 1036:talk 1012:talk 981:talk 953:talk 935:talk 900:talk 832:talk 805:talk 773:talk 729:talk 725:Hfst 710:talk 688:talk 650:talk 634:talk 613:talk 586:talk 582:Hfst 572:talk 556:talk 552:Hfst 526:talk 509:talk 475:talk 443:talk 414:talk 394:talk 368:talk 274:and 162:FENS 136:news 73:and 2767:is 1726:det 759:doi 626:. — 524:| ( 473:| ( 441:| ( 392:| ( 380:CAN 300:Mid 176:TWL 3209:: 3197:) 3170:∈ 3164:∀ 3141:˙ 3138:σ 3084:∈ 3078:∀ 3055:˙ 3052:σ 3009:σ 2989:∈ 2951:) 2784:˙ 2719:− 2602:− 2568:, 2482:… 2292:0. 2262:∂ 2244:ϕ 2241:∂ 2203:ϕ 2145:∂ 2127:ϕ 2124:∂ 2091:∂ 2073:ϕ 2070:∂ 2052:˙ 2035:, 1961:ϕ 1891:ϕ 1749:≠ 1694:∈ 1681:, 1657:∈ 1637:, 1620:− 1607:∈ 1450:˙ 1375:˙ 1350:: 1312:− 1234:× 1221:∈ 1208:, 1184:∈ 1171:, 1147:∈ 1073:˙ 1014:) 991:) 963:) 937:) 910:) 889:if 869:σ 849:σ 834:) 807:) 775:) 753:a 751:is 731:) 712:) 690:) 652:) 636:) 615:) 588:) 574:) 558:) 528:) 511:) 477:) 445:) 416:) 396:) 370:) 156:) 54:; 3193:( 3175:S 3167:x 3159:0 3156:= 3153:) 3150:x 3147:( 3113:S 3089:S 3081:x 3073:0 3070:= 3067:) 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