Bin Wang, Bernard Brogliato, Vincent Acary, Ahcene Boubakir, Franck Plestan. HAL Id: hal
|
|
- Brandon Matthews
- 6 years ago
- Views:
Transcription
1 Experimental comparisons between implicit and explicit implementations of discrete-time sliding mode controllers: Towards cattering suppression in output and input signals Bin Wang, Bernard Brogliato, Vincent Acary, Acene Boubakir, Franck Plestan To cite tis version: Bin Wang, Bernard Brogliato, Vincent Acary, Acene Boubakir, Franck Plestan. Experimental comparisons between implicit and explicit implementations of discrete-time sliding mode controllers: Towards cattering suppression in output and input signals. VSS t IEEE International Worksop on Variable Structure Systems, Jun 214, Nantes, France. IEEE, Variable Structure Systems (VSS), t International Worksop on, pp.1-6, <1.119/VSS >. <al > HAL Id: al ttps://al.arcives-ouvertes.fr/al Submitted on 1 Nov 217 HAL is a multi-disciplinary open access arcive for te deposit and dissemination of scientific researc documents, weter tey are publised or not. Te documents may come from teacing and researc institutions in France or abroad, or from public or private researc centers. L arcive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recerce, publiés ou non, émanant des établissements d enseignement et de recerce français ou étrangers, des laboratoires publics ou privés.
2 Experimental comparisons between implicit and explicit implementations of discrete-time sliding mode controllers: towards cattering suppression in output and input signals B. Wang, B. Brogliato, V. Acary, A. Boubakir, F. Plestan Abstract Tis paper presents a set of experimental results concerning te sliding mode control of an electro-pneumatic system. Two discrete-time control strategies are considered for te implementation of te discontinuous part of te sliding mode controller: explicit and implicit discretizations. Wile te explicit implementation is known to generate numerical cattering [6], [7], [12], [13], te implicit one is expected to significantly reduce cattering wile keeping te accuracy. Te experimental results reported in tis work remarkably confirm tat te implicit discrete-time sliding mode supersedes te explicit ones, wit several important features: cattering in te control input is almost eliminated (wile te explicit and saturated controllers beave like ig-frequency bang-bang inputs), te input magnitude depends only on te perturbation size and is largely independent of te controller gain and sampling time. I. INTRODUCTION Consider te scalar system ẋ(t) =u(t)+d(t), wit u(t) sgn(x(t)), were sgn( ) is te set-valued signum function: sgn() = [ 1, 1], sgn(x) =1if x>, sgn(x) = 1 if x <. Let te disturbance d(t) satisfy d(t) δ < 1 for some δ. Using Filippov s matematical framework of differential inclusions, one deduces tat for any x(), te state x(t) reaces te sliding surface x =in a finite time t, and ten x(t) =for all t t. In te differential inclusions language, u(t) is a selection ξ(t) of te interval [ 1, 1] for t t, and it satisfies ξ(t) =u(t) = d(t) after t. In a sense, te set-valued controller acts as a disturbance observer once te sliding mode is attained. It is clear tat if one multiplies te signum by a gain a>, i.e. u(t) =a sgn(x(t)), ten one still as u(t) = d(t) in te sliding pase after t. However tis time te value of te selection ξ(t) inside te set-valued part of sgn(x(t)) is divided by a, i.e. ξ(t) = d(t) a. Let us now consider te Euler discretization of tis system. It reads: x k+1 = x k + u k + d k, were f k = f(t k ) for a Bin Wang was wit BIPOP team, INRIA Grenoble, 655 avenue de l Europe, Saint-ismier, France. Bernard Brogliato is wit BIPOP team, INRIA Grenoble, 655 avenue de l Europe, Saint-ismier, France. bernard.brogliato@inria.fr Vincent Acary is wit BIPOP team, INRIA Grenoble, 655 avenue de l Europe, Saint-ismier, France. vincent.acary@inria.fr Acene Boubakir is wit Laboratoire de Commande des Processus, Ecole Nationale Polytecnique d Alger, Algéria. Tis work was perfomed during a stay at IRCCyN, Nantes, France. a boubakir@yaoo.fr Franck Plestan is wit IRCCYN, Ecole Centrale de Nantes, 1 rue de la Noë, BP 9211, Nantes Cedex 3, France. franck.plestan@irccyn.ecnantes.fr Tis work as been performed wit te support of te Frenc National Researc Agency (ANR) project CaSliM (ANR 211 BS3 7 1). function f( ), and t k = t +k are te sampling times, > is te sampling period. In suc a simple case, te Euler and ZOH discretizations are te same, except for te disturbance d k = t k+1 t k d(t)dt for te ZOH metod. Our focus is on ow to coose u k. Te explicit metod yields u k sgn(x k ), yielding te closed-loop x k+1 x k d k sgn(x k ). As alluded to above, limit cycles exist wic create oscillations around te sliding surface (ere te origin), known as te numerical cattering in te output [6], [7], [12], [13]. One of te consequences is tat te explicit controller keeps switcing between te two values 1 and -1, and never attains any point inside ( 1, 1). In particular te explicit controller cannot approximate te continuous-time selection ξ( ) =u( ) wen te system evolves close to te sliding surface. If a gain a> premultiplies u( ) ten te explicit controller switces between two discrete values a and a, te switcing frequency being inversely proportional to te sampling period: tis is te numerical cattering in te input. It is noteworty tat te mere notion of a sliding surface does not exist in tis case, since te discrete trajectories cannot attain te origin, and te controller cannot take values in te set-valued part equal to ( 1, 1). One ten as to resort to so-called quasi-sliding surfaces [3], [11]. Te implicit metod is implemented as follows. Since d(t) is unknown, one first constructs a nominal unperturbed system wit state x k, from wic te input is computed: x k+1 = x k + u k, u k sgn( x k+1 ). Tis is a so-called generalized equation wit unknown x k+1. Its solution yields after few manipulations ( u k = proj [ 1, 1]; x k tat is te projection on te interval [ 1, 1], and is a causal input (not depending on future values of te state). Notice tat in te unperturbed case, x k and x k are te same. As proved in [1], [2], te implicit controller guarantees convergence of x k to te origin in a finite number of steps, and disturbance attenuation by a factor during te sliding mode. Most importantly, te control input takes values in ( 1, 1) once x k as reaced te origin, as may be seen from te generalized equation from wic it is calculated, and one as during tat pase u k = d k : u k is a selection ξ k of te discrete-time differential inclusion x k+1 = x k + u k, u k sgn( x k+1 ), and te discrete-time input observes te disturbance wen te sliding mode is attained. Similarly to te continuous-time case, if te controller is multiplied by a ) 1
3 gain a>, tenteselectionξ k = d k a. Terefore te implicit controller as te same features as its continuous-time counterpart. We may summarize tem as follows: (i) Wen tere is no perturbation, te sliding surface is reaced after a finite number of steps. Wen a perturbation acts on te system, te state of te nominal system reaces te sliding surface after a finite number of steps, wile te perturbation effect is attenuated by a factor on te system s state. (ii) Despite te system s state x k never attains its sliding surface due to te disturbance, te notion of discretetime sliding mode does exist, and corresponds to te nominal system s state x k vanising, or equivalently to te set-valued controller evolving strictly inside te interval [ 1, 1]. Intismodetecontrollercompensates for te disturbance, and is a copy of it. Its magnitude is terefore independent, in te sliding mode, of te controller gain, and tere is no need to adapt te gain (denoted as a above, and as G in te sequel) on-line. (iii) Teoretically tere is no numerical cattering during te sliding mode, neiter in te sliding variable, nor in te input. (iv) Te discrete-time controller keeps te simplicity of its continuous-time counterpart, wit no added gain to tune. (v) Computing te input at eac step boils down to solving asimplegeneralizedequation,equivalentlyaprojection on [ 1, 1], orsolvingaquadraticprogram.tisisquite easy to implement in a code. Te implicit algoritm extends to iger dimension systems, and wit sliding surfaces of codimension 2 [2]. Te main objective of tis note is to confirm tese features experimentally. II. DYNAMICS OF THE PLANT AND CONTROLLERS Te electropneumatic system used for te controllers evaluation consists in two actuators wic are controlled by two servodistributors (see Figure 1). Fig. 1: [1] te electropneumatic system - On te left and side is te main actuator wose its position is controlled. On te rigt and side is te perturbation actuator wose load force is controlled. Under some assumptions detailed in [1], te dynamic model of te pneumatic actuator can be written as a nonlinear system wic is affine in te control input [u P u N ] T, u P (resp. u N ) being te control input of te servodistributor connected to te P (resp. N) camber.temodelisdivided in two parts: two first equations concern te pressure dynamics in eac camber wereas te motion of te actuator is described by te two last equations. Ten te model of te electropneumatic experimental set-up reads as ṗ P = krt V P (y) [ϕ P + ψ P u P S rt p P v] ṗ N = krt V N (y) [ϕ N + ψ N u N + S rt p Nv] (1) v = 1 M [S (p P p N ) b v v F ] ẏ = v, wit p P (reps. p N ) te pressure in te P (resp. N) camber, y and v being te position and velocity of te actuator. Te force F is a disturbance. Note tat te previous system appears to ave two control inputs given tat tere is one servo distributor connected to eac camber. In te sequel, only te main actuator position is controlled: given tat tere is a single control objective, one states u = u P = u N. Te coice of sliding mode controller as been made because of its intrinsic features of robustness. Let us define te socalled sliding variable as σ(x, t) =ë + λ 1 ė + λ e (2) wit e = y y d (t), y d (t) being te desired trajectory, supposed to be sufficiently differentiable. As sown in [9], [8], te first time derivative of σ can be written as σ = Ψ(x, t)+φ(x)u = Ψ n (x, t)+ Ψ(t)+[ (x)+ Φ(t)] u suc tat Ψ n, are te nominal functions and Ψ, Φ are te uncertain terms. From [9], [8], functions Ψ and Φ are bounded in te pysical working domain (wic gives tat te uncertain terms are also bounded). Furtermore, one supposes tat Φ is sufficiently small wit respect to to ensure tat 1+ Φ >. Fromapracticalpointofview, tis assumption is not too strong: it simply means tat te uncertainties are small compared to te nominal values. Let us consider te control law 1 : u = 1 [ Ψ n + v]. (4) By applying (4) in (3), one gets σ = Φ Ψ n + Ψ+ (3) [ 1+ Φ ] v. (5) 1 As sown in [4], suc a control law allows to reduce te magnitude of te sliding mode controller by using te nominal informations in te controller. 2
4 Once u as been designed to linearize by feedback te system (1), te discontinuous part of te controller is defined as v Gsgn(σ) (6) wit G tuned sufficiently large. Te controller v as been implemented under its discrete forms as follows (wit k, σ k = σ(k), being te sampling period) Explicit sliding mode control (wit sgn( ) function) v k = Gsgn(σ k ), Implicit sliding mode control (wit sgn( ) multifunction) v k Gsgn(σ k+1 ) (implemented wit a projection as indicated in te introduction). III. EXPERIMENTAL RESULTS Te two controllers ave been implemented wit several feedback gains and sampling times. Te lengt of te interval of study is 2 seconds. Te comparisons are made mainly wit respect to: te input v magnitude and cattering, and te tracking error. A. Comparison of te tracking errors e Data in Tables I II and III V caracterize te position tracking error e obtained by te two different implementation metods, from te aspects of average, range, standard deviation and variation wit five different sampling periods. Te symbol Avg denotes te average of te tracking error over te duration of te test, abs is te absolute value of tracking error, Rge is te range. Te variation of a realvalued function f( ) defined on an interval [a, b] R is te quantity Var [a,b] (f) = N 1 i= f(t i+1 ) f(t i ) (9) were te set of time instants {t,t 1,,t N } is a partition of [a, b].intefollowing,tevariationsoftepositionerrore for te two implementation metods wit te different gains G, avebeencalculatedbycoosingtepartitiontimest i in (9), as te sampling times. Remark 3.1: Te variation in (9) as a quantity to caracterize te analyzed signals, is not common in Control Engineering. It is tougt ere in te context of sliding mode control, tat suc a quantity is useful to measure te cattering level of a signal, since it does represent ow muc te signal varies. However due to te partition tat as been cosen (te sampling times) te results are not comparable from one sampling period to te next, but only between te tree controllers for a fixed. In oter words, in Tables III Vdataavetobecomparedinsideasinglecolumn,butnot from one column to anoter one. All te data concerning e are reported in Tables I V and Figure 2. It is confirmed in Tables III V, tat te variation of te implicit input starts to be significantly smaller tan tat of te oter two, for 5 ms, te improvement being uge for =. Tese first data tend to indicate tat, in te case of te implicit input, its variation is drastically smaller for larger sampling periods (for = 15 ms: 1836 for te explicit metod, 8.1 for te implicit one wit G =1 4 ), confirming tat cattering on e is reduced wen te implicit controller is used. Te fact tat te output signal is smoot for te implicit metod, wile it catters for te explicit controller for large sampling time, is obvious in Figure 2. Similar conclusions were obtained for G =1 4 and are not reported ere because of lack of space. Tables I II concerns G =1 5.Tetwometodssow similar results in terms of average, range and standard deviation of e, te implicit one providing sligtly better results. Te variation values are given in Tables III V wit G =1 5,andisquitevisibleinFigure2:tevariationofe wit te implicit input is muc smaller tan wit te explicit controllers, except for =1ms were te obtained values are of same order. Tis indicates tat te cattering on e is drastically reduced wit te implicit input 2. A first conclusion, tat will be strengtened in te next paragrap, is tat te implicit control metod allows to take larger gains witout decreasing te performance (it means tat it is possible to reject/counteract larger perturbations/uncertainties witout more cattering). Te performance of implicit control is better wen G is larger, wile it is less good wit te explicit and saturation controllers. 1ms 2ms Avg(abs(e)) Rge e (-5.569, 5.627) ( , ) Stand. Dev. e (a) Explicit control 5ms 1ms Avg(abs(e)) Rge e ( , 4.61) ( , ) Stand. Dev. e (b) TABLE I: Comparisons of position error e wen G = Te results for too small sampling periods ( 2 ms) are not conclusive, because of te limited bandwidt of te filters used to compute ė and ë to construct σ. 3
5 Avg(abs(e)) Range of e ( , ) Standard Deviation of e (a) Explicit control Avg(abs(e)) Range of e ( , ) Standard Deviation of e (b) TABLE II: Comparisons of position error e wen G =1 5. 1ms 2ms Explicit control e e e e+3 (a) G =1 5 TABLE III: Variation of position error e. B. Comparison of discontinuous inputs v in and : Te features of te control inputs is a key-point in tis work, given tat one of te objectives is to sow te influence of implicit control to te cattering effect. Let us now pass to te control inputs comparisons, wit data reported in Tables VI VIII, Tables IX XI and Figure 3. Data given in Tables VI VIII and IX XI caracterize te switcing functions for tese tree metods. It includes te range and variation. Remark 3.1 applies also for te variation of te control, so tat in Tables VI VIII, data ave to be compared inside a single column, but not from one column to anoter one. Wat we call te switcing functions are sgn(σ k ) in, and sgn(σ k+1 ) in. For te implicit controller, tis is wat we called te selection ξ k in Introduction. Tis is not to be confused wit te discontinuous control v in (6). Comparisons of te inputs in te two metods are given in Tables VI VIII from range and variation aspects. In addition, te two controllers are depicted in Figure 3, for various time steps and gains. Globally, te experimental results sow tat te implicit metod drastically reduces te input cattering and magnitude compared wit te explicit metod. Te explicit switcing input keeps oscillating between te maximum and minimum values like a bang-bang controller (see data in Tables VI VIII, and Figure 3(a), wic is quite representative of all te switcing functions obtained wit explicit discretizations). In te tables, all te values used to caracterize te cattering in implicit metod are invariably muc less tan te explicit metod. Figures 3(b) 3(d), wic concerns te implicit controller switcing function for various sampling times, sow tat te implicit input v in is largely independent sampling time. From Table VI VIII, te data in te rows corresponding to te implicit controller allow to obtain a confirmation of tis fact. Te magnitudes of te switcing function for te implicit controller, for 6 different gains G and two different sampling periods, are reported in 5ms 1ms s Explicit control e e (a) G =1 5 TABLE IV: Variation of position error e. Explicit control 2.57e (a) G =1 5 TABLE V: Variation of position error e. Tables IX XI. It confirms tat te magnitude of te input v in (6), wic is te switcing function times te gain G, does not depend neiter on G nor on in tis range of sampling times. Tis insensitivity property is believed to be a fundamental property of te implicit metod introduced in [1], [2], compared to explicit implementations wic drastically differ wen and/or G are varied. Te results depicted in Figure 3 clearly demonstrate tat wereas te explicit controller tends to approximate a signal tat switces infinitely fast between two extreme values like bang-bang inputs, tis is not at all te case for te implicit controller tat beaves in a totally different way. Tis is a nice confirmation of bot teoretical and numerical predictions [1], [2], tat te implicit controller does represent te discrete-time approximation of te selection of te differential inclusion according to Filippov s matematical framework. Input cattering is also visible in Table VI VIII. Variation of te implicit switcing function is muc smaller tan te oter two. C. Summary Tese extensive experimental tests prove tat items (ii) (iii) (iv) and (v) in te Introduction, are not only teoretical and numerical predictions obtained in [1], [2], but significantly influence te discrete-time implemented slidingmode controller. Te implicit metod allows to drastically reduce te input cattering and magnitude, wile enancing te tracking capabilities (output cattering is almost entirely eliminated). It also allows te designer to coose larger sampling periods, wic may be of strong interest in practice. Peraps counter-intuitively for Control Engineers, te performance and robustness increase wen te gain G increases, wic is tougt to considerably simplify te controller gain tuning process. We ave also conducted extensive experiments wit a saturated explicit input. Te results we obtained are quite similar to te case witout saturation (te saturation seems to play a very tiny role in cattering effects), and are terefore not reported in tis note. 4
6 1ms 2ms s Explicit control (-1., 1.) (-1., 1.) (-.844,.973) (-.66,.545) ) (a) Range of te switcing function. 1ms 2ms Explicit control (b) Variation of te switcing function. TABLE VI: Switcing function, gain G =1 5. 5ms 1ms Explicit control (-1., 1.) (-1., 1.) (-.36,.417) (-.289,.349) (a) Range of te switcing function. 5ms 1ms Explicit control (b) Variation of te switcing function. TABLE VII: Switcing function, gain G =1 5. IV. CONCLUSION Experiments ave been conducted on an electropneumatic system, wit two different implementations of te sliding mode controller: explicit and implicit discretizations. Te results demonstrate tat te teoretical and numerical predictions of [1], [2] are true: te implicit implementation, wic consists merely of a projection on te interval [ 1, 1] and is tus very easy to implement in a code, drastically supersedes te oter one. Te output and input cattering are reduced in a significant way, witout canging te controller basic structure (i.e., no additional filter,observer, or dynamic controller is added compared to te original, basic sliding mode controller) and keeping its simplicity (in particular te gain tuning is easy, wic is a strong feature of te ECB-SMC metod). Te main feature of te implicit discretization, is tat it keeps, in discrete-time, te multivalued feature of te teoretical continuous-time sliding-mode controller, as it is matematically imposed in Filippov s framework. Te proposed implicit discretization metod is generic in te sense tat it could apply to any kind of sliding mode, set valued control. Future researc sould terefore concern similar experiments on te same and oter set-up, wit twisting and ig-order sliding-mode controllers. Explicit control (-1., 1.) (-.173,.247) (a) Range of te switcing function. Explicit control (b) Variation of te switcing function. TABLE VIII: Switcing function, gain G =1 5. G =5ms (.3,.35) (.5,.5) =1ms (.25,.3) (.5,.6) TABLE IX: Magnitude of implicit switcing function sgn(x k+1 ) for varying gains G and sampling period. REFERENCES [1] V. ACARY, B. BROGLIATO, Implicit Euler numerical sceme and cattering-free implementation of sliding mode systems, Systems and Control Letters, vol.59, pp , 21. [2] V. ACARY, B. BROGLIATO, Y. ORLOV, Cattering-free digital slidingmode control wit state observer and disturbance rejection,ieeetrans. Automatic Control, vol.57, no 5, pp , May 212. [3] BARTOSZEWICZ, A,Discrete-time quasi-sliding-mode control strategies, IEEE Transactions on Industrial Electronics, vol. 45, no 4, pp , [4] R. CASTRO-LINARÈS, S.LAGHROUCHE, A.GLUMINEAU, AND F. PLESTAN, Higer order sliding mode observer-based control, IFAC Symposium on System, Structure and Control, Oaxaca, Mexico, 24. [5] L. FRIDMAN, J.MORENO AND R. IRIARTE (EDITORS), Sliding Modes after te First Decade of te 21st Century. State of te Art, Lecture Notes in Control and Information Sciences, Volume 412, 212, DOI: 1.17/ , Springer Verlag Berlin Heidelberg. [6] Z. GALIAS, X. YU, Complex discretization beaviours of a simple sliding-mode control system, IEEE Transactions on Circuits and Systems II: Express Briefs, vol.53, no 8, pp , August 26. [7] Z. GALIAS, X.YU, Analysis of zero-order older discretization of two-dimensional sliding-mode control systems, IEEE Transactions on Circuits and Systems II: Express Briefs, vol.55, no 12, pp , December 28. [8] A. GIRIN, F. PLESTAN, X. BRUN, AND A. GLUMINEAU, Robust control of an electropneumatic actuator : application to an aeronautical bencmark, IEEE Transactions on Control Systems Tecnology, vol.17, no.3, pp , 29. [9] S. LAGHROUCHE, M.SMAOUI, F.PLESTAN, AND X. BRUN, Higer order sliding mode control based on optimal approac of an electropneumatic actuator, International Journal of Control, vol.79, no.2, pp , 26. [1] Y. SHTESSEL, M.TALEB, AND F. PLESTAN, A novel adaptive-gain supertwisting sliding mode controller: metodology and application, Automatica, vol.48, no.5, pp , 212. [11] SIRA RAMIREZ, H.,Non linear discrete variable structure systems in quasi sliding mode, Int,J.Control,vol.54,no.5,pp , [12] B. WANG, X. YU, G. CHEN, ZOH discretization effect on single-input sliding mode control systems wit matced uncertainties, Automatica, vol.45, pp , 29. [13] X. YU, B. WANG, Z. GALIAS, G. CHEN, Discretization effect on equivalent control-based multi-input sliding-mode control systems, IEEE Transactions on Automatic Control, vol.53, no 6, pp , July 28. 5
7 G =5ms (.3,.35) (.6,.63) =1ms (.25,.3) (.5,.6) TABLE X: Magnitude of implicit switcing function sgn(x k+1 ) for varying gains G and sampling period G =5ms (.3,.3) (.6,.65) =1ms (.25,.25) (.5,.5) TABLE XI: Magnitude of implicit switcing function sgn(x k+1 ) for varying gains G and sampling period (a) Explicit. sign(s k ). G =1 4, =5ms (a) =1ms. Explicit metod (b) Implicit. sign(s k+1 ). G =1 5, =5ms (b) =1ms. Implicit metod (c) Implicit. sign(s k+1 ). G =1 5, =1ms (c) =. Explicit metod (d) =. Implicit metod (d) Implicit. sign(s k+1 ). G =1 5, =. Fig. 3: Switcing function: Comparison between explicit metod (sign(s k ))andimplicitmetod(sign(s k+1 )). Fig. 2: Real position y (mm) in blue and y d (mm) in red, under =1ms and = for G =1 5. 6
A priori error indicator in the transformation method for problems with geometric uncertainties
A priori error indicator in te transformation metod for problems wit geometric uncertainties Duc Hung Mac, Stépane Clenet, Jean-Claude Mipo, Igor Tsukerman To cite tis version: Duc Hung Mac, Stépane Clenet,
More informationConsider a function f we ll specify which assumptions we need to make about it in a minute. Let us reformulate the integral. 1 f(x) dx.
Capter 2 Integrals as sums and derivatives as differences We now switc to te simplest metods for integrating or differentiating a function from its function samples. A careful study of Taylor expansions
More informationDigital Filter Structures
Digital Filter Structures Te convolution sum description of an LTI discrete-time system can, in principle, be used to implement te system For an IIR finite-dimensional system tis approac is not practical
More informationNew methodologies for adaptive sliding mode control
New methodologies for adaptive sliding mode control Franck Plestan, Yuri Shtessel, Vincent Bregeault, Alexander Poznyak To cite this version: Franck Plestan, Yuri Shtessel, Vincent Bregeault, Alexander
More informationNumerical Differentiation
Numerical Differentiation Finite Difference Formulas for te first derivative (Using Taylor Expansion tecnique) (section 8.3.) Suppose tat f() = g() is a function of te variable, and tat as 0 te function
More information1 The concept of limits (p.217 p.229, p.242 p.249, p.255 p.256) 1.1 Limits Consider the function determined by the formula 3. x since at this point
MA00 Capter 6 Calculus and Basic Linear Algebra I Limits, Continuity and Differentiability Te concept of its (p.7 p.9, p.4 p.49, p.55 p.56). Limits Consider te function determined by te formula f Note
More informationHigher order sliding mode control based on adaptive first order sliding mode controller
Preprints of the 19th World Congress The International Federation of Automatic Control Cape Town, South Africa. August 4-9, 14 Higher order sliding mode control based on adaptive first order sliding mode
More information2.8 The Derivative as a Function
.8 Te Derivative as a Function Typically, we can find te derivative of a function f at many points of its domain: Definition. Suppose tat f is a function wic is differentiable at every point of an open
More informationA = h w (1) Error Analysis Physics 141
Introduction In all brances of pysical science and engineering one deals constantly wit numbers wic results more or less directly from experimental observations. Experimental observations always ave inaccuracies.
More informationETNA Kent State University
Electronic Transactions on Numerical Analysis. Volume 34, pp. 14-19, 2008. Copyrigt 2008,. ISSN 1068-9613. ETNA A NOTE ON NUMERICALLY CONSISTENT INITIAL VALUES FOR HIGH INDEX DIFFERENTIAL-ALGEBRAIC EQUATIONS
More informationCombining functions: algebraic methods
Combining functions: algebraic metods Functions can be added, subtracted, multiplied, divided, and raised to a power, just like numbers or algebra expressions. If f(x) = x 2 and g(x) = x + 2, clearly f(x)
More informationNotes on wavefunctions II: momentum wavefunctions
Notes on wavefunctions II: momentum wavefunctions and uncertainty Te state of a particle at any time is described by a wavefunction ψ(x). Tese wavefunction must cange wit time, since we know tat particles
More informationQuaternion Dynamics, Part 1 Functions, Derivatives, and Integrals. Gary D. Simpson. rev 01 Aug 08, 2016.
Quaternion Dynamics, Part 1 Functions, Derivatives, and Integrals Gary D. Simpson gsim1887@aol.com rev 1 Aug 8, 216 Summary Definitions are presented for "quaternion functions" of a quaternion. Polynomial
More information2.11 That s So Derivative
2.11 Tat s So Derivative Introduction to Differential Calculus Just as one defines instantaneous velocity in terms of average velocity, we now define te instantaneous rate of cange of a function at a point
More informationHOW TO DEAL WITH FFT SAMPLING INFLUENCES ON ADEV CALCULATIONS
HOW TO DEAL WITH FFT SAMPLING INFLUENCES ON ADEV CALCULATIONS Po-Ceng Cang National Standard Time & Frequency Lab., TL, Taiwan 1, Lane 551, Min-Tsu Road, Sec. 5, Yang-Mei, Taoyuan, Taiwan 36 Tel: 886 3
More informationLIMITATIONS OF EULER S METHOD FOR NUMERICAL INTEGRATION
LIMITATIONS OF EULER S METHOD FOR NUMERICAL INTEGRATION LAURA EVANS.. Introduction Not all differential equations can be explicitly solved for y. Tis can be problematic if we need to know te value of y
More informationCopyright c 2008 Kevin Long
Lecture 4 Numerical solution of initial value problems Te metods you ve learned so far ave obtained closed-form solutions to initial value problems. A closedform solution is an explicit algebriac formula
More informationFinite Difference Methods Assignments
Finite Difference Metods Assignments Anders Söberg and Aay Saxena, Micael Tuné, and Maria Westermarck Revised: Jarmo Rantakokko June 6, 1999 Teknisk databeandling Assignment 1: A one-dimensional eat equation
More informationDissipative Systems Analysis and Control, Theory and Applications: Addendum/Erratum
Dissipative Systems Analysis and Control, Theory and Applications: Addendum/Erratum Bernard Brogliato To cite this version: Bernard Brogliato. Dissipative Systems Analysis and Control, Theory and Applications:
More informationDifferentiation in higher dimensions
Capter 2 Differentiation in iger dimensions 2.1 Te Total Derivative Recall tat if f : R R is a 1-variable function, and a R, we say tat f is differentiable at x = a if and only if te ratio f(a+) f(a) tends
More informationOrder of Accuracy. ũ h u Ch p, (1)
Order of Accuracy 1 Terminology We consider a numerical approximation of an exact value u. Te approximation depends on a small parameter, wic can be for instance te grid size or time step in a numerical
More information5 Ordinary Differential Equations: Finite Difference Methods for Boundary Problems
5 Ordinary Differential Equations: Finite Difference Metods for Boundary Problems Read sections 10.1, 10.2, 10.4 Review questions 10.1 10.4, 10.8 10.9, 10.13 5.1 Introduction In te previous capters we
More informationRobotic manipulation project
Robotic manipulation project Bin Nguyen December 5, 2006 Abstract Tis is te draft report for Robotic Manipulation s class project. Te cosen project aims to understand and implement Kevin Egan s non-convex
More informationTowards Perfectly Matched Layers for time-dependent space fractional PDEs
Towards Perfectly Matced Layers for time-dependent space fractional PDEs Xavier Antoine, Emmanuel Lorin To cite tis version: Xavier Antoine, Emmanuel Lorin. Towards Perfectly Matced Layers for time-dependent
More information4. The slope of the line 2x 7y = 8 is (a) 2/7 (b) 7/2 (c) 2 (d) 2/7 (e) None of these.
Mat 11. Test Form N Fall 016 Name. Instructions. Te first eleven problems are wort points eac. Te last six problems are wort 5 points eac. For te last six problems, you must use relevant metods of algebra
More informationSection 2.7 Derivatives and Rates of Change Part II Section 2.8 The Derivative as a Function. at the point a, to be. = at time t = a is
Mat 180 www.timetodare.com Section.7 Derivatives and Rates of Cange Part II Section.8 Te Derivative as a Function Derivatives ( ) In te previous section we defined te slope of te tangent to a curve wit
More informationThe Verlet Algorithm for Molecular Dynamics Simulations
Cemistry 380.37 Fall 2015 Dr. Jean M. Standard November 9, 2015 Te Verlet Algoritm for Molecular Dynamics Simulations Equations of motion For a many-body system consisting of N particles, Newton's classical
More informationarxiv: v1 [math.oc] 18 May 2018
Derivative-Free Optimization Algoritms based on Non-Commutative Maps * Jan Feiling,, Amelie Zeller, and Cristian Ebenbauer arxiv:805.0748v [mat.oc] 8 May 08 Institute for Systems Teory and Automatic Control,
More informationDerivation Of The Schwarzschild Radius Without General Relativity
Derivation Of Te Scwarzscild Radius Witout General Relativity In tis paper I present an alternative metod of deriving te Scwarzscild radius of a black ole. Te metod uses tree of te Planck units formulas:
More informationUniversity Mathematics 2
University Matematics 2 1 Differentiability In tis section, we discuss te differentiability of functions. Definition 1.1 Differentiable function). Let f) be a function. We say tat f is differentiable at
More informationThe derivative function
Roberto s Notes on Differential Calculus Capter : Definition of derivative Section Te derivative function Wat you need to know already: f is at a point on its grap and ow to compute it. Wat te derivative
More informationOn Discrete Time Optimal Control: A Closed-Form Solution
On Discrete Time Optimal Control: A Closed-Form Solution Ziqiang Gao Center for Advanced Control Tecnologies Cleveland State University, Cleveland, OH 445 z.gao@csuoio.edu Abstract: In tis paper, te matematical
More informationDedicated to the 70th birthday of Professor Lin Qun
Journal of Computational Matematics, Vol.4, No.3, 6, 4 44. ACCELERATION METHODS OF NONLINEAR ITERATION FOR NONLINEAR PARABOLIC EQUATIONS Guang-wei Yuan Xu-deng Hang Laboratory of Computational Pysics,
More informationHow to Find the Derivative of a Function: Calculus 1
Introduction How to Find te Derivative of a Function: Calculus 1 Calculus is not an easy matematics course Te fact tat you ave enrolled in suc a difficult subject indicates tat you are interested in te
More informationTime-Varying Gain Second Order Sliding Mode Differentiator,
Preprints of te 9t World Congress Te International Federation of Automatic Control Time-Varying Gain Second Order Sliding Mode Differentiator, Carlos Vázquez Stanislav Aranovskiy Leonid Freidovic Department
More informationComplete Quadratic Lyapunov functionals using Bessel-Legendre inequality
Complete Quadratic Lyapunov functionals using Bessel-Legendre inequality Alexandre Seuret Frédéric Gouaisbaut To cite tis version: Alexandre Seuret Frédéric Gouaisbaut Complete Quadratic Lyapunov functionals
More informationNew Streamfunction Approach for Magnetohydrodynamics
New Streamfunction Approac for Magnetoydrodynamics Kab Seo Kang Brooaven National Laboratory, Computational Science Center, Building 63, Room, Upton NY 973, USA. sang@bnl.gov Summary. We apply te finite
More informationROBUST REDUNDANCY RELATIONS FOR FAULT DIAGNOSIS IN NONLINEAR DESCRIPTOR SYSTEMS
Proceedings of te IASTED International Conference Modelling Identification and Control (AsiaMIC 23) April - 2 23 Puket Tailand ROBUST REDUNDANCY RELATIONS FOR FAULT DIAGNOSIS IN NONLINEAR DESCRIPTOR SYSTEMS
More informationQuasiperiodic phenomena in the Van der Pol - Mathieu equation
Quasiperiodic penomena in te Van der Pol - Matieu equation F. Veerman and F. Verulst Department of Matematics, Utrect University P.O. Box 80.010, 3508 TA Utrect Te Neterlands April 8, 009 Abstract Te Van
More informationNumerical modification of atmospheric models to include the feedback of oceanic currents on air-sea fluxes in ocean-atmosphere coupled models
Numerical modification of atmospheric models to include the feedback of oceanic currents on air-sea fluxes in ocean-atmosphere coupled models Florian Lemarié To cite this version: Florian Lemarié. Numerical
More informationControllability of a one-dimensional fractional heat equation: theoretical and numerical aspects
Controllability of a one-dimensional fractional eat equation: teoretical and numerical aspects Umberto Biccari, Víctor Hernández-Santamaría To cite tis version: Umberto Biccari, Víctor Hernández-Santamaría.
More information232 Calculus and Structures
3 Calculus and Structures CHAPTER 17 JUSTIFICATION OF THE AREA AND SLOPE METHODS FOR EVALUATING BEAMS Calculus and Structures 33 Copyrigt Capter 17 JUSTIFICATION OF THE AREA AND SLOPE METHODS 17.1 THE
More informationFunction Composition and Chain Rules
Function Composition and s James K. Peterson Department of Biological Sciences and Department of Matematical Sciences Clemson University Marc 8, 2017 Outline 1 Function Composition and Continuity 2 Function
More informationPolynomial Interpolation
Capter 4 Polynomial Interpolation In tis capter, we consider te important problem of approximatinga function fx, wose values at a set of distinct points x, x, x,, x n are known, by a polynomial P x suc
More informationNUMERICAL DIFFERENTIATION. James T. Smith San Francisco State University. In calculus classes, you compute derivatives algebraically: for example,
NUMERICAL DIFFERENTIATION James T Smit San Francisco State University In calculus classes, you compute derivatives algebraically: for example, f( x) = x + x f ( x) = x x Tis tecnique requires your knowing
More informationMath 102 TEST CHAPTERS 3 & 4 Solutions & Comments Fall 2006
Mat 102 TEST CHAPTERS 3 & 4 Solutions & Comments Fall 2006 f(x+) f(x) 10 1. For f(x) = x 2 + 2x 5, find ))))))))) and simplify completely. NOTE: **f(x+) is NOT f(x)+! f(x+) f(x) (x+) 2 + 2(x+) 5 ( x 2
More informationIEOR 165 Lecture 10 Distribution Estimation
IEOR 165 Lecture 10 Distribution Estimation 1 Motivating Problem Consider a situation were we ave iid data x i from some unknown distribution. One problem of interest is estimating te distribution tat
More informationParameter Fitted Scheme for Singularly Perturbed Delay Differential Equations
International Journal of Applied Science and Engineering 2013. 11, 4: 361-373 Parameter Fitted Sceme for Singularly Perturbed Delay Differential Equations Awoke Andargiea* and Y. N. Reddyb a b Department
More informationLIMITS AND DERIVATIVES CONDITIONS FOR THE EXISTENCE OF A LIMIT
LIMITS AND DERIVATIVES Te limit of a function is defined as te value of y tat te curve approaces, as x approaces a particular value. Te limit of f (x) as x approaces a is written as f (x) approaces, as
More informationFlavius Guiaş. X(t + h) = X(t) + F (X(s)) ds.
Numerical solvers for large systems of ordinary differential equations based on te stocastic direct simulation metod improved by te and Runge Kutta principles Flavius Guiaş Abstract We present a numerical
More informationChapter 5 FINITE DIFFERENCE METHOD (FDM)
MEE7 Computer Modeling Tecniques in Engineering Capter 5 FINITE DIFFERENCE METHOD (FDM) 5. Introduction to FDM Te finite difference tecniques are based upon approximations wic permit replacing differential
More informationEfficient algorithms for for clone items detection
Efficient algoritms for for clone items detection Raoul Medina, Caroline Noyer, and Olivier Raynaud Raoul Medina, Caroline Noyer and Olivier Raynaud LIMOS - Université Blaise Pascal, Campus universitaire
More informationPhysically Based Modeling: Principles and Practice Implicit Methods for Differential Equations
Pysically Based Modeling: Principles and Practice Implicit Metods for Differential Equations David Baraff Robotics Institute Carnegie Mellon University Please note: Tis document is 997 by David Baraff
More informationlecture 26: Richardson extrapolation
43 lecture 26: Ricardson extrapolation 35 Ricardson extrapolation, Romberg integration Trougout numerical analysis, one encounters procedures tat apply some simple approximation (eg, linear interpolation)
More informationJournal of Computational and Applied Mathematics
Journal of Computational and Applied Matematics 94 (6) 75 96 Contents lists available at ScienceDirect Journal of Computational and Applied Matematics journal omepage: www.elsevier.com/locate/cam Smootness-Increasing
More informationQuantum Mechanics Chapter 1.5: An illustration using measurements of particle spin.
I Introduction. Quantum Mecanics Capter.5: An illustration using measurements of particle spin. Quantum mecanics is a teory of pysics tat as been very successful in explaining and predicting many pysical
More informationNonparametric estimation of the average growth curve with general nonstationary error process
Nonparametric estimation of te average growt curve wit general nonstationary error process Karim Benenni, Mustapa Racdi To cite tis version: Karim Benenni, Mustapa Racdi. Nonparametric estimation of te
More information160 Chapter 3: Differentiation
3. Differentiation Rules 159 3. Differentiation Rules Tis section introuces a few rules tat allow us to ifferentiate a great variety of functions. By proving tese rules ere, we can ifferentiate functions
More informationMath 31A Discussion Notes Week 4 October 20 and October 22, 2015
Mat 3A Discussion Notes Week 4 October 20 and October 22, 205 To prepare for te first midterm, we ll spend tis week working eamples resembling te various problems you ve seen so far tis term. In tese notes
More informationMAT244 - Ordinary Di erential Equations - Summer 2016 Assignment 2 Due: July 20, 2016
MAT244 - Ordinary Di erential Equations - Summer 206 Assignment 2 Due: July 20, 206 Full Name: Student #: Last First Indicate wic Tutorial Section you attend by filling in te appropriate circle: Tut 0
More informationMAT 145. Type of Calculator Used TI-89 Titanium 100 points Score 100 possible points
MAT 15 Test #2 Name Solution Guide Type of Calculator Used TI-89 Titanium 100 points Score 100 possible points Use te grap of a function sown ere as you respond to questions 1 to 8. 1. lim f (x) 0 2. lim
More informationPolynomials 3: Powers of x 0 + h
near small binomial Capter 17 Polynomials 3: Powers of + Wile it is easy to compute wit powers of a counting-numerator, it is a lot more difficult to compute wit powers of a decimal-numerator. EXAMPLE
More informationPreface. Here are a couple of warnings to my students who may be here to get a copy of what happened on a day that you missed.
Preface Here are my online notes for my course tat I teac ere at Lamar University. Despite te fact tat tese are my class notes, tey sould be accessible to anyone wanting to learn or needing a refreser
More informationTime (hours) Morphine sulfate (mg)
Mat Xa Fall 2002 Review Notes Limits and Definition of Derivative Important Information: 1 According to te most recent information from te Registrar, te Xa final exam will be eld from 9:15 am to 12:15
More informationEaster bracelets for years
Easter bracelets for 5700000 years Denis Roegel To cite this version: Denis Roegel. Easter bracelets for 5700000 years. [Research Report] 2014. HAL Id: hal-01009457 https://hal.inria.fr/hal-01009457
More informationImplicit Euler Numerical Simulation of Sliding Mode Systems
Implicit Euler Numerical Simulation of Sliding Mode Systems Vincent Acary and Bernard Brogliato, INRIA Grenoble Rhône-Alpes Conference in honour of E. Hairer s 6th birthday Genève, 17-2 June 29 Objectives
More information1. Which one of the following expressions is not equal to all the others? 1 C. 1 D. 25x. 2. Simplify this expression as much as possible.
004 Algebra Pretest answers and scoring Part A. Multiple coice questions. Directions: Circle te letter ( A, B, C, D, or E ) net to te correct answer. points eac, no partial credit. Wic one of te following
More information, meant to remind us of the definition of f (x) as the limit of difference quotients: = lim
Mat 132 Differentiation Formulas Stewart 2.3 So far, we ave seen ow various real-world problems rate of cange and geometric problems tangent lines lead to derivatives. In tis section, we will see ow to
More information(a) At what number x = a does f have a removable discontinuity? What value f(a) should be assigned to f at x = a in order to make f continuous at a?
Solutions to Test 1 Fall 016 1pt 1. Te grap of a function f(x) is sown at rigt below. Part I. State te value of eac limit. If a limit is infinite, state weter it is or. If a limit does not exist (but is
More informationMathematics 5 Worksheet 11 Geometry, Tangency, and the Derivative
Matematics 5 Workseet 11 Geometry, Tangency, and te Derivative Problem 1. Find te equation of a line wit slope m tat intersects te point (3, 9). Solution. Te equation for a line passing troug a point (x
More informationResearch Article New Results on Multiple Solutions for Nth-Order Fuzzy Differential Equations under Generalized Differentiability
Hindawi Publising Corporation Boundary Value Problems Volume 009, Article ID 395714, 13 pages doi:10.1155/009/395714 Researc Article New Results on Multiple Solutions for Nt-Order Fuzzy Differential Equations
More informationPolynomial Interpolation
Capter 4 Polynomial Interpolation In tis capter, we consider te important problem of approximating a function f(x, wose values at a set of distinct points x, x, x 2,,x n are known, by a polynomial P (x
More informationLinear Quadratic Zero-Sum Two-Person Differential Games
Linear Quadratic Zero-Sum Two-Person Differential Games Pierre Bernhard To cite this version: Pierre Bernhard. Linear Quadratic Zero-Sum Two-Person Differential Games. Encyclopaedia of Systems and Control,
More informationThe Priestley-Chao Estimator
Te Priestley-Cao Estimator In tis section we will consider te Pristley-Cao estimator of te unknown regression function. It is assumed tat we ave a sample of observations (Y i, x i ), i = 1,..., n wic are
More informationDifferential equations. Differential equations
Differential equations A differential equation (DE) describes ow a quantity canges (as a function of time, position, ) d - A ball dropped from a building: t gt () dt d S qx - Uniformly loaded beam: wx
More informationA First-Order System Approach for Diffusion Equation. I. Second-Order Residual-Distribution Schemes
A First-Order System Approac for Diffusion Equation. I. Second-Order Residual-Distribution Scemes Hiroaki Nisikawa W. M. Keck Foundation Laboratory for Computational Fluid Dynamics, Department of Aerospace
More informationRobust Leader-follower Formation Control of Mobile Robots Based on a Second Order Kinematics Model
Vol. 33, No. 9 ACTA AUTOMATICA SINICA September, 27 Robust Leader-follower Formation Control of Mobile Robots Based on a Second Order Kinematics Model LIU Si-Cai 1, 2 TAN Da-Long 1 LIU Guang-Jun 3 Abstract
More informationDe-Coupler Design for an Interacting Tanks System
IOSR Journal of Electrical and Electronics Engineering (IOSR-JEEE) e-issn: 2278-1676,p-ISSN: 2320-3331, Volume 7, Issue 3 (Sep. - Oct. 2013), PP 77-81 De-Coupler Design for an Interacting Tanks System
More informationA SHORT INTRODUCTION TO BANACH LATTICES AND
CHAPTER A SHORT INTRODUCTION TO BANACH LATTICES AND POSITIVE OPERATORS In tis capter we give a brief introduction to Banac lattices and positive operators. Most results of tis capter can be found, e.g.,
More informationSECTION 3.2: DERIVATIVE FUNCTIONS and DIFFERENTIABILITY
(Section 3.2: Derivative Functions and Differentiability) 3.2.1 SECTION 3.2: DERIVATIVE FUNCTIONS and DIFFERENTIABILITY LEARNING OBJECTIVES Know, understand, and apply te Limit Definition of te Derivative
More informationch (for some fixed positive number c) reaching c
GSTF Journal of Matematics Statistics and Operations Researc (JMSOR) Vol. No. September 05 DOI 0.60/s4086-05-000-z Nonlinear Piecewise-defined Difference Equations wit Reciprocal and Cubic Terms Ramadan
More informationNumerical Experiments Using MATLAB: Superconvergence of Nonconforming Finite Element Approximation for Second-Order Elliptic Problems
Applied Matematics, 06, 7, 74-8 ttp://wwwscirporg/journal/am ISSN Online: 5-7393 ISSN Print: 5-7385 Numerical Experiments Using MATLAB: Superconvergence of Nonconforming Finite Element Approximation for
More informationEffect of the Dependent Paths in Linear Hull
1 Effect of te Dependent Pats in Linear Hull Zenli Dai, Meiqin Wang, Yue Sun Scool of Matematics, Sandong University, Jinan, 250100, Cina Key Laboratory of Cryptologic Tecnology and Information Security,
More informationSome Review Problems for First Midterm Mathematics 1300, Calculus 1
Some Review Problems for First Midterm Matematics 00, Calculus. Consider te trigonometric function f(t) wose grap is sown below. Write down a possible formula for f(t). Tis function appears to be an odd,
More informationRunge-Kutta methods. With orders of Taylor methods yet without derivatives of f (t, y(t))
Runge-Kutta metods Wit orders of Taylor metods yet witout derivatives of f (t, y(t)) First order Taylor expansion in two variables Teorem: Suppose tat f (t, y) and all its partial derivatives are continuous
More informationLecture XVII. Abstract We introduce the concept of directional derivative of a scalar function and discuss its relation with the gradient operator.
Lecture XVII Abstract We introduce te concept of directional derivative of a scalar function and discuss its relation wit te gradient operator. Directional derivative and gradient Te directional derivative
More informationMethylation-associated PHOX2B gene silencing is a rare event in human neuroblastoma.
Methylation-associated PHOX2B gene silencing is a rare event in human neuroblastoma. Loïc De Pontual, Delphine Trochet, Franck Bourdeaut, Sophie Thomas, Heather Etchevers, Agnes Chompret, Véronique Minard,
More informationThe Krewe of Caesar Problem. David Gurney. Southeastern Louisiana University. SLU 10541, 500 Western Avenue. Hammond, LA
Te Krewe of Caesar Problem David Gurney Souteastern Louisiana University SLU 10541, 500 Western Avenue Hammond, LA 7040 June 19, 00 Krewe of Caesar 1 ABSTRACT Tis paper provides an alternative to te usual
More informationCORRELATION TEST OF RESIDUAL ERRORS IN FREQUENCY DOMAIN SYSTEM IDENTIFICATION
IAC Symposium on System Identification, SYSID 006 Marc 9-3 006, Newcastle, Australia CORRELATION TEST O RESIDUAL ERRORS IN REQUENCY DOMAIN SYSTEM IDENTIICATION István Kollár *, Ri Pintelon **, Joan Scouens
More informationContinuity and Differentiability Worksheet
Continuity and Differentiability Workseet (Be sure tat you can also do te grapical eercises from te tet- Tese were not included below! Typical problems are like problems -3, p. 6; -3, p. 7; 33-34, p. 7;
More informationNew Fourth Order Quartic Spline Method for Solving Second Order Boundary Value Problems
MATEMATIKA, 2015, Volume 31, Number 2, 149 157 c UTM Centre for Industrial Applied Matematics New Fourt Order Quartic Spline Metod for Solving Second Order Boundary Value Problems 1 Osama Ala yed, 2 Te
More informationQuantum Numbers and Rules
OpenStax-CNX module: m42614 1 Quantum Numbers and Rules OpenStax College Tis work is produced by OpenStax-CNX and licensed under te Creative Commons Attribution License 3.0 Abstract Dene quantum number.
More informationDerivatives. By: OpenStaxCollege
By: OpenStaxCollege Te average teen in te United States opens a refrigerator door an estimated 25 times per day. Supposedly, tis average is up from 10 years ago wen te average teenager opened a refrigerator
More informationMODIFIED DIFFERENTIAL EQUATIONS. Dedicated to Prof. Michel Crouzeix
ESAIM: PROCEEDINGS, September 2007, Vol.21, 16-20 Gabriel Caloz & Monique Dauge, Editors MODIFIED DIFFERENTIAL EQUATIONS Pilippe Cartier 1, Ernst Hairer 2 and Gilles Vilmart 1,2 Dedicated to Prof. Micel
More informationCopyright IEEE, 13th Stat. Signal Proc. Workshop (SSP), July 2005, Bordeaux (F)
Copyrigt IEEE, 13t Stat. Signal Proc. Worksop SSP), 17-0 July 005, Bordeaux F) ROBUSTNESS ANALYSIS OF A GRADIENT IDENTIFICATION METHOD FOR A NONLINEAR WIENER SYSTEM Ernst Ascbacer, Markus Rupp Institute
More informationTeaching Differentiation: A Rare Case for the Problem of the Slope of the Tangent Line
Teacing Differentiation: A Rare Case for te Problem of te Slope of te Tangent Line arxiv:1805.00343v1 [mat.ho] 29 Apr 2018 Roman Kvasov Department of Matematics University of Puerto Rico at Aguadilla Aguadilla,
More informationReflection Symmetries of q-bernoulli Polynomials
Journal of Nonlinear Matematical Pysics Volume 1, Supplement 1 005, 41 4 Birtday Issue Reflection Symmetries of q-bernoulli Polynomials Boris A KUPERSHMIDT Te University of Tennessee Space Institute Tullaoma,
More informationSolution to Sylvester equation associated to linear descriptor systems
Solution to Sylvester equation associated to linear descriptor systems Mohamed Darouach To cite this version: Mohamed Darouach. Solution to Sylvester equation associated to linear descriptor systems. Systems
More informationLast lecture (#4): J vortex. J tr
Last lecture (#4): We completed te discussion of te B-T pase diagram of type- and type- superconductors. n contrast to type-, te type- state as finite resistance unless vortices are pinned by defects.
More informationA non-commutative algorithm for multiplying (7 7) matrices using 250 multiplications
A non-commutative algorithm for multiplying (7 7) matrices using 250 multiplications Alexandre Sedoglavic To cite this version: Alexandre Sedoglavic. A non-commutative algorithm for multiplying (7 7) matrices
More information