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 Consequently, I worry that its source might have been an unpublished manuscript that was rejected(?).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. —
2040:
723:
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.--
702:
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") —
891:
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
944:
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
722:
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
678:
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
825:
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,
673:
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
701:
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
922:
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
2310:
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
430:
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.
606:
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 -
2873:
2302:
1005:
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
1762:
1249:
1635:
2529:
1679:
2927:
1716:
1206:
1169:
2226:
1984:
2772:
2375:
797:
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. —
757:
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
885:
859:
2618:
2033:
1328:
841:
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. —
44:
3222:
327:
2685:
3127:
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
2623:
3130:
3044:
3212:
168:
1254:
135:
2944:
984:
956:
903:
99:
30:
1721:
1211:
104:
20:
1590:
266:
227:
74:
2400:
1640:
2868:{\displaystyle \mathbf {\dot {x}} _{1}=\mathbf {f} _{1}\left(\mathbf {x} _{1},S_{0}\left(\mathbf {x} _{1}\right)\right)}
202:
2885:
644:
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) -
2948:
988:
960:
907:
129:
65:
2297:{\displaystyle {\frac {\partial \phi \left(\mathbf {x} \right)}{\partial \mathbf {x} }}\mathbf {B} \left(x\right)=0.}
1684:
1174:
1137:
3194:
2198:
1956:
2341:
125:
3190:
367:
386:
that will be enough to satisfy most people. It would be great if an expert could make things more precise. —
175:
109:
508:
258:
208:
2534:
359:
24:
378:
I'm not an expert in sliding mode control, but I've gone through and added comments that the system
190:
3106:
2940:
1031:
980:
952:
899:
804:
772:
709:
633:
571:
525:
474:
442:
413:
393:
161:
55:
141:
2319:
1989:
1767:
1764:. The system, where the dimension of the lower equation coincides with that of the control input
1035:
1007:
930:
831:
687:
70:
1798:
864:
670:
504:
51:
1123:{\displaystyle \mathbf {{\dot {x}}=f} \left(x\right)\mathbf {+B} \left(x\right)\mathbf {u} }
1011:
934:
844:
758:
754:
666:
3034:{\displaystyle {\mathcal {S}}=\{\mathbb {x} \in \mathbb {R} ^{n}|\sigma (\mathbf {x} )=0\}}
2591:
2011:
1301:
649:
612:
318:
275:
457:
The set in
Theorem 2 is empty. This definition clearly is incorrect. Is a dot missing? --
793:
I just made a change that changes the order so that my request (about the bottom of the
242:
221:
2935:
975:
947:
894:
799:
767:
728:
704:
628:
623:
585:
566:
555:
520:
469:
458:
437:
408:
388:
2571:
2380:
1333:
550:
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
3198:
2952:
1015:
992:
964:
938:
911:
835:
808:
776:
732:
713:
691:
653:
637:
616:
589:
575:
559:
529:
512:
478:
461:
446:
417:
397:
382:
reach the surface in finite time because the control need not be continuous. I
371:
645:
608:
248:
762:
724:
581:
551:
1868:
be a vector of new state variables defined by the nonlinear transformation
1030:
I removed the following section on an SMC regular form which was added by
1364:
537:
The state-feedback control law is not a continuous function of time; it
698:
467:
Someone fixed this sometime. I tried to make it a little better now. —
2929:
which takes part of the reduced order system dynamics(\ref{BCPFM06}).
271:
2675:{\displaystyle \mathbf {x} _{2}=S_{0}\left(\mathbf {x} _{1}\right)}
1795:
The idea of transformation is formulated in the following way: Let
926:
I suggest to formulate this remark somewhere in this introduction.
350:
1 is required for the finite time entrance to the sliding surface.
3182:{\displaystyle {\dot {\sigma }}(x)=0\;\forall x\in {\mathcal {S}}}
3096:{\displaystyle {\dot {\sigma }}(x)=0\;\forall x\in {\mathcal {S}}}
2338:
is a discontinuous control enforcing sliding mode in the manifold
1986:
is continuous and continuously differentiable with respect to
184:
15:
2588:
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.
2228:
is a solution to the matrix partial differential equation
2195:
will be independent of the control if the vector function
1052:
In this section a particular canonical for, the so-called
1757:{\displaystyle \det \left(\mathbf {B} _{2}\right)\neq 0}
1244:{\displaystyle \mathbf {B} \in \mathbb {R} ^{n\times m}}
665:
Sliding mode control is sometimes critiqued as being a
1630:{\displaystyle \mathbf {x} _{1}\in \mathbb {R} ^{n-m}}
160:
3133:
3109:
3047:
2969:
2888:
2775:
2688:
2626:
2594:
2574:
2537:
2403:
2383:
2344:
2322:
2236:
2201:
2043:
2014:
1992:
1959:
1876:
1801:
1770:
1724:
1687:
1643:
1593:
1358:
1336:
1304:
1257:
1214:
1177:
1140:
1064:
867:
847:
489:
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:. The equations with respect to
1994:
1968:
1926:
1898:
1772:
1734:
1689:
1646:
1596:
1562:
1552:
1548:
1544:
1539:
1535:
1518:
1498:
1495:
1483:
1466:
1449:
1446:
1423:
1420:
1408:
1391:
1374:
1371:
1268:
1216:
1179:
1142:
1116:
1100:
1097:
1081:
1078:
1072:
1069:
669:when compared to other forms of
251:
241:
220:
189:
45:Click here to start a new topic.
3218:Mid-importance Systems articles
2531:. 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? Welcome!
3244:
1953:where the vector function
310:project's importance scale
3199:02:31, 23 June 2020 (UTC)
929:What are your opinions ?
880:{\displaystyle \sigma =0}
692:07:40, 6 April 2009 (UTC)
682:Correct me if I'm wrong.
602:Add phase portrait figure
325:
303:
236:
215:
80:Be welcoming to newcomers
3213:C-Class Systems articles
1016:08:56, 27 May 2011 (UTC)
993:17:43, 26 May 2011 (UTC)
965:17:06, 26 May 2011 (UTC)
939:10:04, 26 May 2011 (UTC)
912:13:41, 3 July 2009 (UTC)
836:07:11, 3 July 2009 (UTC)
809:21:24, 9 June 2009 (UTC)
777:15:05, 9 June 2009 (UTC)
733:14:28, 9 June 2009 (UTC)
590:14:40, 10 May 2009 (UTC)
462:19:58, 25 May 2007 (UTC)
418:16:28, 5 June 2009 (UTC)
345:Existence is not correct
854:{\displaystyle \sigma }
763:10.1109/MCS.2008.931718
714:20:27, 8 May 2009 (UTC)
576:20:42, 8 May 2009 (UTC)
560:19:58, 8 May 2009 (UTC)
3183:
3121:
3097:
3035:
2923:
2869:
2761:
2676:
2614:
2582:
2562:
2525:
2391:
2371:
2332:
2298:
2222:
2185:
2029:
2002:
1980:
1943:
1862:
1780:
1758:
1712:
1675:
1631:
1577:
1344:
1324:
1292:
1245:
1202:
1165:
1124:
881:
855:
322:
259:Systems science portal
197:This article is rated
75:avoid personal attacks
3184:
3122:
3098:
3036:
2924:
2870:
2762:
2677:
2615:
2613:{\displaystyle (n-m)}
2583:
2563:
2526:
2392:
2372:
2333:
2299:
2223:
2186:
2030:
2028:{\displaystyle y_{1}}
2003:
1981:
1944:
1863:
1790:\cite{Loukyanov1981}.
1781:
1759:
1713:
1676:
1632:
1578:
1345:
1325:
1323:{\displaystyle (n-m)}
1293:
1246:
1203:
1166:
1125:
882:
856:
453:Region of attraction?
321:
100:Neutral point of view
3131:
3107:
3103:. For any choice of
3045:
2967:
2886:
2773:
2686:
2624:
2592:
2572:
2535:
2401:
2381:
2342:
2320:
2234:
2199:
2041:
2012:
1990:
1957:
1874:
1799:
1768:
1722:
1685:
1641:
1591:
1356:
1334:
1302:
1255:
1212:
1175:
1138:
1062:
865:
845:
356:Marco Tulio Angulo
105:No original research
25:Sliding mode control
3191:Random wiki drifter
1852:
1834:
267:WikiProject Systems
3179:
3162:
3117:
3093:
3076:
3031:
2919:
2865:
2757:
2672:
2610:
2578:
2558:
2521:
2387:
2367:
2328:
2294:
2218:
2181:
2025:
1998:
1976:
1939:
1910:
1858:
1838:
1820:
1776:
1754:
1708:
1671:
1627:
1573:
1568:
1340:
1320:
1288:
1241:
1198:
1161:
1120:
877:
851:
747:not as susceptible
679:article, however.
323:
203:content assessment
86:dispute resolution
47:
3143:
3057:
2786:
2581:{\displaystyle m}
2390:{\displaystyle m}
2270:
2153:
2099:
2054:
1452:
1377:
1343:{\displaystyle m}
1261:
1075:
671:nonlinear control
362:comment added by
342:
341:
338:
337:
334:
333:
183:
182:
66:Assume good faith
43:
3235:
3188:
3186:
3185:
3180:
3178:
3177:
3145:
3144:
3136:
3126:
3124:
3123:
3118:
3116:
3115:
3102:
3100:
3099:
3094:
3092:
3091:
3059:
3058:
3050:
3040:
3038:
3037:
3032:
3018:
3007:
3002:
3001:
2996:
2987:
2976:
2975:
2928:
2926:
2925:
2920:
2918:
2914:
2913:
2908:
2898:
2897:
2874:
2872:
2871:
2866:
2864:
2860:
2859:
2855:
2854:
2849:
2839:
2838:
2826:
2825:
2820:
2809:
2808:
2803:
2794:
2793:
2788:
2787:
2779:
2766:
2764:
2763:
2758:
2750:
2746:
2745:
2740:
2730:
2729:
2717:
2716:
2711:
2699:
2681:
2679:
2678:
2673:
2671:
2667:
2666:
2661:
2651:
2650:
2638:
2637:
2632:
2619:
2617:
2616:
2611:
2587:
2585:
2584:
2579:
2567:
2565:
2564:
2559:
2548:
2530:
2528:
2527:
2522:
2520:
2519:
2514:
2510:
2509:
2505:
2496:
2495:
2477:
2473:
2464:
2463:
2451:
2447:
2438:
2437:
2419:
2415:
2396:
2394:
2393:
2388:
2376:
2374:
2373:
2368:
2360:
2356:
2337:
2335:
2334:
2329:
2327:
2303:
2301:
2300:
2295:
2287:
2276:
2271:
2269:
2268:
2259:
2258:
2254:
2238:
2227:
2225:
2224:
2219:
2217:
2213:
2190:
2188:
2187:
2182:
2180:
2172:
2168:
2159:
2154:
2152:
2151:
2142:
2141:
2137:
2121:
2116:
2112:
2100:
2098:
2097:
2088:
2087:
2083:
2067:
2062:
2061:
2056:
2055:
2047:
2034:
2032:
2031:
2026:
2024:
2023:
2007:
2005:
2004:
1999:
1997:
1985:
1983:
1982:
1977:
1975:
1971:
1948:
1946:
1945:
1940:
1935:
1934:
1929:
1920:
1919:
1905:
1901:
1886:
1885:
1867:
1865:
1864:
1859:
1857:
1853:
1851:
1846:
1833:
1828:
1811:
1810:
1785:
1783:
1782:
1777:
1775:
1763:
1761:
1760:
1755:
1747:
1743:
1742:
1737:
1717:
1715:
1714:
1709:
1707:
1706:
1701:
1692:
1680:
1678:
1677:
1672:
1670:
1669:
1664:
1655:
1654:
1649:
1636:
1634:
1633:
1628:
1626:
1625:
1614:
1605:
1604:
1599:
1582:
1580:
1579:
1574:
1572:
1569:
1565:
1561:
1557:
1556:
1555:
1543:
1542:
1527:
1526:
1521:
1512:
1508:
1507:
1506:
1501:
1492:
1491:
1486:
1475:
1474:
1469:
1460:
1459:
1454:
1453:
1445:
1437:
1433:
1432:
1431:
1426:
1417:
1416:
1411:
1400:
1399:
1394:
1385:
1384:
1379:
1378:
1370:
1349:
1347:
1346:
1341:
1329:
1327:
1326:
1321:
1297:
1295:
1294:
1289:
1275:
1271:
1262:
1259:
1250:
1248:
1247:
1242:
1240:
1239:
1228:
1219:
1207:
1205:
1204:
1199:
1197:
1196:
1191:
1182:
1170:
1168:
1167:
1162:
1160:
1159:
1154:
1145:
1129:
1127:
1126:
1121:
1119:
1114:
1103:
1095:
1084:
1077:
1076:
1068:
886:
884:
883:
878:
860:
858:
857:
852:
755:blunt instrument
667:blunt instrument
534:Quite good, but
374:
292:
291:
290:Systems articles
288:
285:
282:
261:
256:
255:
254:
245:
238:
237:
232:
224:
217:
200:
194:
193:
185:
179:
178:
164:
95:Article policies
16:
3243:
3242:
3238:
3237:
3236:
3234:
3233:
3232:
3203:
3202:
3129:
3128:
3105:
3104:
3043:
3042:
2991:
2965:
2964:
2960:
2903:
2899:
2889:
2884:
2883:
2844:
2840:
2830:
2815:
2814:
2810:
2798:
2776:
2771:
2770:
2735:
2731:
2721:
2706:
2684:
2683:
2656:
2652:
2642:
2627:
2622:
2621:
2590:
2589:
2570:
2569:
2533:
2532:
2497:
2487:
2465:
2455:
2439:
2429:
2428:
2424:
2423:
2407:
2399:
2398:
2379:
2378:
2348:
2340:
2339:
2318:
2317:
2277:
2260:
2246:
2239:
2232:
2231:
2205:
2197:
2196:
2160:
2143:
2129:
2122:
2104:
2089:
2075:
2068:
2044:
2039:
2038:
2015:
2010:
2009:
1988:
1987:
1963:
1955:
1954:
1924:
1911:
1893:
1877:
1872:
1871:
1819:
1815:
1802:
1797:
1796:
1766:
1765:
1732:
1728:
1720:
1719:
1696:
1683:
1682:
1659:
1644:
1639:
1638:
1609:
1594:
1589:
1588:
1567:
1566:
1547:
1534:
1533:
1529:
1516:
1493:
1481:
1480:
1476:
1464:
1442:
1439:
1438:
1418:
1406:
1405:
1401:
1389:
1367:
1359:
1354:
1353:
1332:
1331:
1300:
1299:
1263:
1253:
1252:
1223:
1210:
1209:
1186:
1173:
1172:
1149:
1136:
1135:
1104:
1085:
1060:
1059:
1028:
920:
863:
862:
843:
842:
823:
662:
604:
487:
455:
428:
357:
347:
289:
286:
283:
280:
279:
276:systems science
257:
252:
250:
230:
201:on Knowledge's
198:
121:
116:
115:
114:
91:
61:
12:
11:
5:
3241:
3239:
3231:
3230:
3225:
3220:
3215:
3205:
3204:
3176:
3171:
3168:
3165:
3160:
3157:
3154:
3151:
3148:
3142:
3139:
3114:
3090:
3085:
3082:
3079:
3074:
3071:
3068:
3065:
3062:
3056:
3053:
3041:that somehow
3030:
3027:
3024:
3021:
3017:
3013:
3010:
3006:
3000:
2995:
2990:
2986:
2982:
2979:
2974:
2959:
2956:
2931:
2930:
2917:
2912:
2907:
2902:
2896:
2892:
2879:
2877:
2876:
2875:
2863:
2858:
2853:
2848:
2843:
2837:
2833:
2829:
2824:
2819:
2813:
2807:
2802:
2797:
2792:
2785:
2782:
2756:
2753:
2749:
2744:
2739:
2734:
2728:
2724:
2720:
2715:
2710:
2705:
2702:
2698:
2694:
2691:
2670:
2665:
2660:
2655:
2649:
2645:
2641:
2636:
2631:
2609:
2606:
2603:
2600:
2597:
2577:
2557:
2554:
2551:
2547:
2543:
2540:
2518:
2513:
2508:
2504:
2500:
2494:
2490:
2486:
2483:
2480:
2476:
2472:
2468:
2462:
2458:
2454:
2450:
2446:
2442:
2436:
2432:
2427:
2422:
2418:
2414:
2410:
2406:
2386:
2366:
2363:
2359:
2355:
2351:
2347:
2326:
2314:
2312:
2308:
2306:
2305:
2304:
2293:
2290:
2286:
2283:
2280:
2275:
2267:
2263:
2257:
2253:
2249:
2245:
2242:
2216:
2212:
2208:
2204:
2193:
2192:
2191:
2179:
2176:
2171:
2167:
2163:
2158:
2150:
2146:
2140:
2136:
2132:
2128:
2125:
2119:
2115:
2111:
2107:
2103:
2096:
2092:
2086:
2082:
2078:
2074:
2071:
2065:
2060:
2053:
2050:
2022:
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:
916:
915:
914:
876:
873:
870:
850:
822:
819:
818:
817:
816:
815:
814:
813:
812:
811:
784:
783:
782:
781:
780:
779:
738:
737:
736:
735:
717:
716:
661:
658:
657:
656:
641:
640:
603:
600:
599:
598:
597:
596:
595:
594:
593:
592:
548:
547:
546:
486:
483:
482:
481:
454:
451:
450:
449:
427:
424:
423:
422:
421:
420:
401:
400:
364:189.136.148.79
346:
343:
340:
339:
336:
335:
332:
331:
328:Control theory
324:
314:
313:
306:Mid-importance
302:
296:
295:
293:
263:
262:
246:
234:
233:
231:Mid‑importance
225:
213:
212:
206:
195:
181:
180:
118:
117:
113:
112:
107:
102:
93:
92:
90:
89:
82:
77:
68:
62:
60:
59:
48:
39:
38:
35:
34:
28:
13:
10:
9:
6:
4:
3:
2:
3240:
3229:
3226:
3224:
3221:
3219:
3216:
3214:
3211:
3210:
3208:
3201:
3200:
3196:
3192:
3169:
3166:
3158:
3155:
3149:
3140:
3137:
3083:
3080:
3072:
3069:
3063:
3054:
3051:
3025:
3022:
3008:
2998:
2988:
2977:
2957:
2955:
2954:
2950:
2946:
2942:
2938:
2937:
2915:
2910:
2900:
2894:
2890:
2880:
2878:
2861:
2856:
2851:
2841:
2835:
2831:
2827:
2822:
2811:
2805:
2795:
2790:
2769:
2768:
2754:
2751:
2747:
2742:
2732:
2726:
2722:
2718:
2713:
2703:
2689:
2668:
2663:
2653:
2647:
2643:
2639:
2634:
2604:
2601:
2598:
2575:
2555:
2552:
2538:
2516:
2511:
2506:
2498:
2492:
2488:
2484:
2481:
2478:
2474:
2466:
2460:
2456:
2452:
2448:
2440:
2434:
2430:
2425:
2420:
2416:
2408:
2404:
2384:
2364:
2361:
2357:
2349:
2345:
2315:
2313:
2309:
2307:
2291:
2288:
2284:
2281:
2278:
2255:
2247:
2243:
2230:
2229:
2214:
2206:
2202:
2194:
2169:
2161:
2138:
2130:
2126:
2117:
2113:
2105:
2101:
2084:
2076:
2072:
2063:
2058:
2051:
2048:
2037:
2036:
2020:
2016:
1972:
1964:
1960:
1952:
1936:
1931:
1921:
1916:
1912:
1906:
1902:
1894:
1890:
1887:
1882:
1878:
1870:
1869:
1854:
1848:
1843:
1839:
1835:
1830:
1825:
1821:
1816:
1812:
1807:
1803:
1794:
1792:
1789:
1751:
1748:
1744:
1739:
1729:
1703:
1693:
1666:
1656:
1651:
1622:
1619:
1616:
1606:
1601:
1586:
1558:
1530:
1523:
1513:
1509:
1503:
1488:
1477:
1471:
1461:
1456:
1434:
1428:
1413:
1402:
1396:
1386:
1381:
1360:
1352:
1351:
1337:
1314:
1311:
1308:
1285:
1282:
1279:
1276:
1272:
1264:
1236:
1233:
1230:
1220:
1193:
1183:
1156:
1146:
1133:
1111:
1108:
1105:
1092:
1089:
1086:
1058:
1057:
1055:
1051:
1047:
1043:
1042:
1041:
1040:
1039:
1037:
1033:
1032:User:jdsanch1
1025:
1017:
1013:
1009:
1004:
1003:
1002:
1001:
1000:
999:
994:
990:
986:
982:
978:
977:
972:
971:
970:
969:
966:
962:
958:
954:
950:
949:
943:
942:
941:
940:
936:
932:
927:
924:
917:
913:
909:
905:
901:
897:
896:
890:
874:
871:
868:
848:
840:
839:
838:
837:
833:
829:
828:User:Nillerdk
820:
810:
806:
802:
801:
796:
792:
791:
790:
789:
788:
787:
786:
785:
778:
774:
770:
769:
764:
760:
756:
752:
748:
744:
743:
742:
741:
740:
739:
734:
730:
726:
721:
720:
719:
718:
715:
711:
707:
706:
700:
696:
695:
694:
693:
689:
685:
684:User:Nillerdk
680:
676:
675:
672:
668:
659:
655:
651:
647:
643:
642:
639:
635:
631:
630:
625:
621:
620:
619:
618:
614:
610:
601:
591:
587:
583:
579:
578:
577:
573:
569:
568:
564:Better now? —
563:
562:
561:
557:
553:
549:
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:)
3064:x
3061:(
3029:}
3026:0
3023:=
3020:)
3016:x
3012:(
3005:|
2999:n
2994:R
2985:x
2981:{
2978:=
2973:S
2949:@
2947:/
2943:/
2939:(
2933:—
2916:)
2911:1
2906:x
2901:(
2895:0
2891:S
2862:)
2857:)
2852:1
2847:x
2842:(
2836:0
2832:S
2828:,
2823:1
2818:x
2812:(
2806:1
2801:f
2796:=
2791:1
2781:x
2755:0
2752:=
2748:)
2743:1
2738:x
2733:(
2727:0
2723:S
2714:2
2709:x
2704:=
2701:)
2697:x
2693:(
2690:S
2669:)
2664:1
2659:x
2654:(
2648:0
2644:S
2640:=
2635:2
2630:x
2608:)
2605:m
2599:n
2596:(
2576:m
2556:0
2553:=
2550:)
2546:x
2542:(
2539:S
2517:T
2512:]
2507:)
2503:x
2499:(
2493:m
2489:s
2485:,
2479:,
2475:)
2471:x
2467:(
2461:2
2457:s
2453:,
2449:)
2445:x
2441:(
2435:1
2431:s
2426:[
2421:=
2417:)
2413:x
2409:(
2405:S
2385:m
2365:0
2362:=
2358:)
2354:x
2350:(
2346:S
2325:u
2289:=
2285:)
2282:x
2279:(
2274:B
2266:x
2256:)
2252:x
2248:(
2215:)
2211:x
2207:(
2178:,
2175:u
2170:)
2166:x
2162:(
2157:B
2149:x
2139:)
2135:x
2131:(
2118:+
2114:)
2110:x
2106:(
2102:f
2095:x
2085:)
2081:x
2077:(
2064:=
2059:1
2049:y
2021:1
2017:y
1995:x
1973:)
1969:x
1965:(
1937:,
1932:2
1927:x
1922:=
1917:2
1913:y
1907:,
1903:)
1899:x
1895:(
1888:=
1883:1
1879:y
1855:]
1849:T
1844:2
1840:y
1836:,
1831:T
1826:1
1822:y
1817:[
1813:=
1808:T
1804:y
1773:u
1752:0
1745:)
1740:2
1735:B
1730:(
1704:m
1699:R
1690:u
1667:m
1662:R
1652:2
1647:x
1623:m
1617:n
1612:R
1602:1
1597:x
1563:u
1559:)
1553:2
1549:x
1545:,
1540:1
1536:x
1531:(
1524:2
1519:B
1514:+
1510:)
1504:2
1499:x
1496:,
1489:1
1484:x
1478:(
1472:2
1467:f
1462:=
1457:2
1447:x
1435:)
1429:2
1424:x
1421:,
1414:1
1409:x
1403:(
1397:1
1392:f
1387:=
1382:1
1372:x
1361:{
1338:m
1318:)
1315:m
1309:n
1306:(
1286:n
1280:m
1277:=
1273:)
1269:B
1265:(
1237:m
1231:n
1226:R
1217:B
1194:m
1189:R
1180:u
1157:n
1152:R
1143:x
1117:u
1112:)
1109:x
1106:(
1101:B
1098:+
1093:)
1090:x
1087:(
1082:f
1079:=
1070:x
1034:(
1010:(
989:@
987:/
983:/
979:(
961:@
959:/
955:/
951:(
933:(
908:@
906:/
902:/
898:(
875:0
872:=
830:(
803:(
771:(
761::
727:(
708:(
686:(
648:(
632:(
611:(
584:(
570:(
554:(
545:.
507:(
412:(
366:(
330:.
312:.
278:.
211::
172:·
166:·
158:·
151:·
145:·
139:·
133:·
128:(
58:.
Text is available under the Creative Commons Attribution-ShareAlike License. Additional terms may apply.