Adaptive neuro-fuzzy inference system-based controllers for smart material actuator modelling

Size: px
Start display at page:

Download "Adaptive neuro-fuzzy inference system-based controllers for smart material actuator modelling"

Transcription

1 Adaptive neuro-fuzzy inferene system-based ontrollers for smart material atuator modelling T L Grigorie and R M Botez Éole de Tehnologie Supérieure, Montréal, Quebe, Canada The manusript was reeived on 6 February 009 and was aepted after revision for publiation on 15 May 009. DOI: / JAERO5 655 Abstrat: An intelligent approah for smart material atuator modelling of the atuation lines in a morphing wing system is presented, based on adaptive neuro-fuzzy inferene systems. Four independent neuro-fuzzy ontrollers are reated from the experimental data using a hybrid method a ombination of bak propagation and least-mean-square methods to train the fuzzy inferene systems. The ontrollers objetive is to orrelate eah set of fores and eletrial urrents applied on the smart material atuator to the atuator s elongation. The atuator experimental testing is performed for five fore ases, using a variable eletrial urrent. An integrated ontroller is reated from four neuro-fuzzy ontrollers, developed with Matlab/Simulink software for eletrial urrent inreases, onstant eletrial urrent, eletrial urrent dereases, and for null eletrial urrent in the ooling phase of the atuator, and is then validated by omparison with the experimentally obtained data. Keywords: smart material atuator, neuro-fuzzy ontroller, simulation, modelling, testing 1 INTRODUCTION The aim of this artile is to obtain a reliable, easyto-implement model for smart material atuators (SMAs), with diret appliations in the morphing wing projet. Based on adaptive neuro-fuzzy inferene systems, an integrated ontroller is built to model the SMAs used in the atuation lines of a wing. This model uses the numerial values from the SMAs experimental testing and it takes advantage of the outstanding properties of fuzzy logi, whih allow the signal s empirial proessing without the use of mathematial analytial models. Fuzzy logi systems an emulate human deision-making more losely than many other lassifiers through the proessing of expert system knowledge, formulated linguistially in fuzzy rules in an IFTHEN form. Fuzzy logi is reommended for very omplex proesses, when no simple mathematial model exists, for highly non-linear proesses and for multi-dimensional systems. Corresponding author: Laboratory of Researh in Ative Controls, Avionis and AeroServoElastiity LARCASE, Éole de Tehnologie Supérieure, 1100, rue Notre-Dame Ouest, Montréal, Québe H3C 1K3, Canada. ruxandra.botez@etsmtl.a JAERO5 The input variables in a fuzzy ontrol system are usually mapped into plae by sets of membership funtions (mf) known as fuzzy sets ; the mapping proess is alled fuzzifiation. The ontrol system s deisions are made on the basis of a fuzzy rules set, and are invoked using the membership funtions and the truth values obtained from the inputs; a proess alled inferene. These deisions are mapped into a membership funtion and truth value that ontrols the output variable. The results are ombined to give a speifi answer in a proedure alled defuzzifiation. Elaboration of the model thus requires a fuzzy rules set and the mf assoiated with eah of the inputs [1, ]. The ability and the experiene of a designer in evaluating the rules and the membership funtions of all of the inputs are deisive in obtaining a good fuzzy model. However, a relatively new design method allows a ompetitive model to be built using a ombination of fuzzy logi and neural-network tehniques. Moreover, this method allows the possibility to generate and optimize the fuzzy rules set and the parameters of the membership funtions by means of fuzzy inferene systems (FISs) training. To this end, a hybrid method a ombination of bak propagation and least-mean-square (LMS) methods is used, in whih experimentally obtained data are onsidered. Already Pro. IMehE Vol. 3 Part G: J. Aerospae Engineering

2 656 T L Grigorie andrmbotez implemented in Matlab [1, 3], the method is easy to use, and gives exellent results in a very short time. ACTUATOR EXPERIMENTAL TESTING The SMA testing was performed using the benh test in Fig. 1 at T amb = 4 C, for five load ases with fores of 10, 140, 150, 180, and 190 N. The eletrial urrents following the inreasing-onstantdereasingzero values evolution were applied on the SMA in eah of the five ases onsidered for load fores. In eah of the ases to be analysed, the following parameters were reorded: time, the eletrial urrent applied to the SMA, the load fore, the material temperature, and the atuator elongation (measured using a linear variable differential transformer (LVDT)). To model the SMA, the present authors built an integrated ontroller based on adaptive neuro-fiss. The experimental elongation-urrent urves obtained in the five load ases are shown in Fig.. One an observe that all five of the obtained urves have four distint zones: eletrial urrent inrease, onstant eletrial urrent, eletrial urrent derease, and null eletrial urrent in the ooling phase of the SMA. Four FISs are used to obtain four neuro-fuzzy ontrollers: one for the urrent inrease, one for the onstant urrent, one for the urrent derease, and one ontroller for the null urrent (after its derease). For the first and the third ontrollers, inputs suh as the fore and the urrent are used, whereas for the seond and the fourth, inputs suh as the fore and the time values refleting the SMA s thermal inertia are used (the time values required for the SMA to reover its initial temperature value ( 4 C) are used for the four ontroller). Finally, the four obtained ontrollers must be integrated into a single ontroller. The reasoning behind the design of the first and the third ontrollers is that, from the available experimental data, two elongations for the same values of fores and urrents are used (see Fig. ). Due to the experimental data values, these data annot be represented as algebrai funtions; therefore, it is impossible to use the same FIS representation. Matlab produes an interpolation between the two elongation values obtained for the same values of fores and urrents, whih annot be valid for our appliation. The onstant values, namely the null values of the urrent before and after the urrent derease phase should not be onsidered as inputs in the seond and fourth ontrollers beause they are not suggestive for the haraterization of the SMA elongation. The values of the atuator temperatures may appear to be very suggestive in these phases, but the temperature must be a model output. For these phases the time values are very suggestive, as they represent a measure of the atuator thermal inertia. Time is the seond input of the third ontroller, and so time is also the seond input of the seond and the fourth ontrollers sine fore was onsidered as the first input (the time values must be onsidered when the urrent beomes onstant or null). Fig. 1 The SMA benh test 3 THE PROPOSED METHOD Fig. Elongation versus the urrent values for different fore values for four ases Fuzzy ontrollers are very simple oneptually and are based on FISs. Three steps are onsidered in an FIS design: an input, the proessing, and then an output step. In the input step, the ontroller inputs are mapped into the appropriate mf. Next, a olletion of IFTHEN logi rules is reated; the IF part is alled the anteedent and the THEN part is alled the onsequent. In this step, eah appropriate rule is invoked and a result is generated. The results of all of the rules are then ombined. In the last step, the ombined result is onverted into a speifi ontrol output value. Considering the numerial values resulting from the SMA experimental testing, an empirial model an be developed, whih is based on a neuro-fuzzy network. The model an learn the proess behaviour based on Pro. IMehE Vol. 3 Part G: J. Aerospae Engineering JAERO5

3 Adaptive neuro-fuzzy inferene system-based ontrollers 657 the inputoutput proess data by using an FIS, whih should model the experimental data. Using methods already implemented in ommerial software, an FIS an be generated simply with the Matlab genfis1 or genfis funtions. The genfis1 funtion generates a single-output Sugeno-type FIS using a grid partition on the data (no lustering). This FIS is used to provide initial onditions for ANFIS training. The genfis1 funtion uses generalized Bell-type membership funtions for eah input. Eah rule generated by the genfis1 funtion has one output membership funtion, whih is, by default, of a linear type. It is also possible to reate an FIS using the Matlab genfis funtion. This funtion generates an initial Sugeno-type FIS by deomposing the operation domain into different regions using the fuzzy subtrative lustering method. For eah region, a loworder linear model an desribe the loal proess parameters. Thus, the non-linear proess is loally linearized around a funtioning point by using the LSM. The obtained model is then onsidered valid in the entire region around this point. The limitation of the operating regions implies the existene of overlapping among these different regions; their definition is given in a fuzzy manner. Thus, for eah model input, several fuzzy sets are assoiated with their membership funtions orresponding definitions. By ombining these fuzzy inputs, the input spae is divided into fuzzy regions. A loal linear model is used for eah of these regions, whereas the global model is obtained by defuzzifiation with the gravity entre method (Sugeno), whih performs the interpolation of the loal models outputs [1, 3]. Based on the goal of finding regions with a high density of data points in the featured spae, the subtrative lustering method is used to divide the spae into a number of lusters. All of the points with the highest number of neighbours are seleted as entres of lusters. The lusters are identified one by one, as the data points within a pre-speified fuzzy radius are removed (subtrated) for eah luster. Following the identifiation of eah luster, the algorithm loates a new luster until all of the data points have been heked. If a olletion of M data points, speified by l-dimensional vetors u k, k = 1,,..., M, is onsidered, a density measure at data point u k an be defined as follows ρ k = M j=1 ( exp u ) k u j (r m /) (1) where r m is a positive onstant that defines the radius within the fuzzy neighbourhood and ontributes to the density measure. The point with the highest density is seleted as the first luster entre. Let u 1 be the seleted point and ρ 1 its density measure. Next, the density measure for eah data point u k is revised by JAERO5 the formula ρ k = ρ k ρ 1 exp ( u ) k u 1 (r n /) () where r n is a positive onstant, greater than r m, that defines a neighbourhood where density measures will be redued in order to prevent losely spaed luster entres. In this way, the data points near the first luster entre u 1 will have signifiantly redued density measures, and therefore annot be seleted as subsequent luster entres. After the density measures for eah point have been revised, then the next luster entre u is seleted and all the density measures are again revised. The proess is repeated until all the data points have been heked and a suffiient number of luster entres generated. When the subtrative lustering method is applied to an inputoutput data set, eah of the luster entres are used as the entres for the premise sets in a singleton type of rule base [4]. The Matlab genfis1 funtion generates membership funtions of the generalized Bell type, defined as follows [, 5] A i q (x) = x 1 i q + a b 1 where q i is the luster entre defining the position of the membership funtion, a and b are two parameters that define the membership funtion shape, and Aq i (i = 1, N) are the assoiated individual anteedent fuzzy sets of eah input variable (N = number of rules). Matlab s genfis funtion generates Gaussian-type membership funtions, defined with the following expression [, 5] A i q (3) ( ) x i q (x) = exp 0.5 (4) σq i where q i is the luster entre and σ q i is the dispersion of the luster. The Sugeno fuzzy model was proposed by Takagi, Sugeno, and Kang to generate fuzzy rules from a given inputoutput data set [6]. In our system, for eah of the four FISs (two inputs and one output), a first-order model is onsidered, whih for N rules is given by [5, 6] Rule 1 : If x 1 is A 1 1 and x is A 1, then y1 (x 1, x ) = b a1 1 x 1 + a 1 x. Rule i :Ifx 1 is A i 1 and x is A i, then yi (x 1, x ) = b i 0 + ai 1 x 1 + a i x. Pro. IMehE Vol. 3 Part G: J. Aerospae Engineering

4 658 T L Grigorie andrmbotez Rule N :Ifx 1 is A N 1 and x is A N, then yn (x 1, x ) = b N 0 + an 1 x 1 + a N x (5) where x q (q = 1, ) are the individual input variables and y i (i = 1, N) is the first-order polynomial funtion in the onsequent. a i k (k = 1,, i = 1, N) are parameters of the linear funtion and b0 i (i = 1, N) denotes a salar offset. The parameters a i, k bi 0 (k = 1,, i = 1, N) are optimized by the LSM. For any input vetor, x =[x 1, x ] T, if the singleton fuzzifier, the produt fuzzy inferene, and the entre average defuzzifier are applied, then the output of the fuzzy model y is inferred as follows (weighted average) ( N ) i=1 wi (x)y i y = ( N ) (6) i=1 wi (x) where w i (x) = A i 1 (x 1) A i (x ) (7) w i (x) represents the degree of fulfilment of the anteedent, i.e. the level of firing of the ith rule. The adaptive neuro-fis alulates the Sugeno-type FIS parameters using neural networks. A very simple way to train these FISs is to use Matlab s ANFIS funtion, whih uses a learning algorithm to identify the membership funtion parameters of a Sugeno-type FIS with two outputs and one input. As a starting point, the inputoutput data and the FIS models generated with the genfis1 or genfis funtions are onsidered. ANFIS optimizes the membership funtions parameters for a number of training epohs, determined by the user. With this optimization, the neuro-fuzzy model an produe a better proess approximation by means of a quality parameter in the training algorithm [3]. After this training, the models may be used to generate the elongation values orresponding to the input parameters. To train the fuzzy systems, ANFIS employs a bakpropagation algorithm for the parameters assoiated with the input membership funtions, and LMS estimations for the parameters assoiated with the output membership funtions. For the FISs generated using the genfis1 or genfis funtions, the membership funtions are generalized Bell type or Gaussian type, respetively. Aording to equations (3) and (4), in these types of membership funtions, a, b, and, respetively, σ and, are onsidered variables and must be adjusted. The bak-propagation algorithm may, therefore, be used to train these parameters. The goal is to minimize a ost funtion of the following form ε = 1 (y des y) (8) Pro. IMehE Vol. 3 Part G: J. Aerospae Engineering where y des is the desired output. The output of eah rule y i (x 1, x ) is defined by y i (t + 1) = y i ε (t) k y (9) y i where k y is the step size. Starting from the Sugeno-system s output (equation (6)), modifying with equation (9) results in ε = ε y (10) y i y y i with ε y = y des y, y w i (x) = y i N i=1 wi (x) (11) Therefore, the output of eah rule is obtained with the equation y i (t + 1) = y i (y des y)w i (x) (t) k y N (1) i=1 wi (x) If a generalized Bell-type membership funtion is used, the parameters for the jth membership funtion of the ith fuzzy rule are determined with the following equations a i j (t + 1) = ai j (t) k ε a a i j b i j (t + 1) = bi j (t) k ε b b i j i j (t + 1) = i j (t) k ε i j (13) For a Gaussian-type membership funtion, the parameters of the jth membership funtion of the ith fuzzy rule are alulated with σ i i j (t + 1) = σj (t) k ε σ σj i i j (t + 1) = i j (t) k ε i j (14) After the four ontrollers (Controller 1 for inreasing urrent, Controller for onstant urrent, Controller 3 for dereasing urrent, and Controller 4 for null urrent) have been obtained, they must be integrated, resulting in the logial sheme in Fig. 3. The deision to use one of the four ontrollers depends on the urrent vetor types (inreasing, dereasing, onstant, or zero) and on the k variable value. Depending on the value of k, it an be deided if a onstant urrent value is part of an inreasing vetor or part of a dereasing vetor. The initial k value is equal to 1 when Controller 1 is used, and is equal to 0 when Controllers, 3, or 4 are used. JAERO5

5 Adaptive neuro-fuzzy inferene system-based ontrollers 659 Fig. 3 The logial sheme for the four ontroller s integration 4 THE INTEGRATED CONTROLLER DESIGN AND EVALUATION In the first phase, the genfis Matlab funtion [3] was used to generate and train the FISs assoiated with the four ontrollers in Fig. 3: ElongationFis (for the urrent inrease phase), ElongationFis (for the onstant phase of the urrent), delongationfis (for the derease phase of the urrent), and d0elongationfis (for the null values of the urrent obtained after the derease phase). The FISs are trained for different epohs ( for the first FIS, epohs for the seond and the last FISs, and epohs for the third) using the ANFIS Matlab funtion. Figure 4 displays the deviation between the neuro-fuzzy models and the experimentally obtained data for different training epohs, defining the quality parameter from the training algorithm. A rapid derease in the deviation between the experimental data and the neurofuzzy model is apparent for all four FISs in terms of the quality parameter within the training algorithm over the first 10 3 training epohs. Evaluating eah of the four FISs for the experimental data using the evalfis ommand, the harateristis shown in Fig. 5 were obtained. The means of the relative absolute values of the errors for all four FISs are , , , and per ent for ElongationFis, ElongationFis, delongationfis, and d0elongationfis, respetively. The error obtained for the third FIS ( delongationfis ) is very good, and so this FIS will be onsidered for implementation in the Simulink integrated ontroller. The first, seond, and fourth FISs have large error values and so the generating method must be hanged. During the seond phase, the genfis1 Matlab funtion [3] an be used to build and train the Fig. 4 Training errors for the FISs generated and trained in the first phase JAERO5 Pro. IMehE Vol. 3 Part G: J. Aerospae Engineering

6 660 T L Grigorie andrmbotez Fig. 5 FISs evaluation as a funtion of the number of experimental data points in the first phase remaining three FIS: ElongationFis, ElongationFis, and d0elongationfis. The number of membership funtions onsidered for eah of these is 6 for the first input and 1 for the seond input. The number of training epohs onsidered for the three FISs are for the first and seond FISs, and 1000 for d0elongationfis. Following the evaluation of these three trained FISs for experimental data, the harateristis depited in Fig. 6 were obtained. The evolution of the training errors is represented in Fig. 7. Evaluation of these three FISs gives the following values of the mean of the relative absolute errors: , , and per ent for ElongationFis, ElongationFis, and d0elongationfis, respetively. The errors obtained in the seond phase for the first and the seond FISs are very good, and so these FISs an be implemented in the Simulink-integrated ontroller. For the last FIS ( d0elongationfis ), the error values are still too large, and so the number of membership funtions used to generate it must be adjusted. Therefore, a third phase of FISs building and training is reserved to obtain a better solution for the d0elongationfis FIS. In this phase, two ases were onsidered for the number of membership funtions: ase 1 the mf numbers are 1 for the first input and 1 for the seond input; ase the mf number is 1 for the first input, and 14 for the seond. A number of 4000 training epohs were onsidered in the first ase and 1000 in the seond. The training errors for both ases, after training with the ANFIS funtion, are presented in Fig. 8, and the evaluation as a funtion of the number of experimental data points is shown in Fig. 9. The means of the relative absolute error values for the two ases are and per ent, respetively. Sine the errors in the seond ase are lower, that is the onfiguration that was hosen to be implemented in a Simulink-integrated ontroller. The final values of the relative absolute errors for the four generated and trained FISs are per ent for ElongationFis, per ent for Elongation- Fis, per ent for delongationfis, and per ent for d0elongationfis. Representing the elongations (those obtained experimentally and by using the four FIS models) as funtions of eletrial urrent for the first and third FISs, and as a funtion of time for the other two FISs, produes the graphis in Fig. 10. The urves are represented for all five ases of the SMA load. One an easily observe that, through training, the FISs model the experimental data very well, and the SMA has different thermal onstants, depending on the fore value. A good overlapping of the FIS models elongations with the elongation experimental data is learly visible in Fig. 10. This superposition is dependent on the number of training epohs, and improves as the number of training epohs is higher. Beause the training errors of all of the trained FISs ultimately take onstant values, an improved approximation of the real model Pro. IMehE Vol. 3 Part G: J. Aerospae Engineering JAERO5

7 Adaptive neuro-fuzzy inferene system-based ontrollers 661 Fig. 6 FISs evaluation as a funtion of the number of experimental data points in the seond phase Fig. 7 Training errors for the three FISs generated and trained in the seond phase JAERO5 Pro. IMehE Vol. 3 Part G: J. Aerospae Engineering

8 66 T L Grigorie andrmbotez Fig. 8 Training errors for the d0elongationfis generated and trained in the third phase Fig. 9 FIS s evaluation as a funtion of the number of experimental data points for the third phase Fig. 10 FIS evaluations as funtions of urrent or time Pro. IMehE Vol. 3 Part G: J. Aerospae Engineering JAERO5

9 Adaptive neuro-fuzzy inferene system-based ontrollers an be ahieved with the neuro-fuzzy methods only when a higher quantity of experimental data is used. To visualize the FIS s features, the Matlab anfisedit ommand [3] is used, followed by the FIS s importation on the interfae level. The resulting surfaes for all four 663 final, trained FISs are presented in Fig. 11. The parameters of the input s membership funtions for eah of the four FISs before and after training are shown in Tables 1 and, respetively. For the generalized Bell-type membership funtions, produed with the Fig. 11 The surfaes produed for all four of the final trained FISs Table 1 Parameters of the FIS input s membership funtions before training ElongationFis Fore (N ) mf1 mf mf3 mf4 mf5 mf6 mf7 mf8 mf9 mf10 mf11 mf1 mf13 mf14 ElongationFis Current (A) Fore (N) delongationfis Time (s) Fore (N) Current (A) a b a b a b a b σ / σ / JAERO5 d0elongationfis Fore (N) Time (s) a b a b Pro. IMehE Vol. 3 Part G: J. Aerospae Engineering

10 664 T L Grigorie andrmbotez Table Parameters of the FIS input s membership funtion after training ElongationFis ElongationFis delongationfis d0elongationfis Fore (N) Current (A) Fore (N) Time (s) Fore (N) Current (A) Fore (N) Time (s) a b a b a b a b σ / σ / a b a b mf mf mf mf e mf e mf mf mf mf mf mf mf mf mf genfis1 funtion, the parameters are the membership funtion entre () defining their position, and a, b that define their shape. For the Gaussian-type membership funtions, generated with the genfis funtion, the parameters are one-half of the dispersion (σ /) and the entre of the membership funtion (). For our system, a set of 7 rules for ElongationFis and another 7 for ElongationFis, 6 rules for delongationfis and 168 rules for d0elongationfis are generated. Comparison of the FISs harateristis and membership funtions parameters before and after training, from Tables 1 and, indiates a redistribution of the membership funtions in the working domain and a hange in their shapes, by modifiation of the a, b, and σ parameters. Aording to the parameter values from Table 1, generating FISs with the genfis1 and genfis funtions primarily results in the same values for the a, b, and σ / parameters for all of the membership funtions that haraterize an input. A seondary result is the separation of the working spae for the respetive input using a grid partition on the data (no lustering) if the genfis1 funtion is used, or using the fuzzy subtrative lustering method if generating with the genfis funtion. For the delongationfis FIS (initially generated by using the genfis funtion) the rules are of the type: if (in1 is in1luster k ) and (in is inluster k ) then (out1 is out1luster k ). For both of the inputs of this FIS, six Gaussian-type mf were generated; within the set of rules they are noted by in j luster k ; j is the input number (1/), and k is the number of the membership funtion (1/6). The delongationfis FIS has the struture shown in Fig. 1, whereas the orresponding ontroller (Controller 3) has the struture presented in Fig. 13. For the other three FISs (initially generated by using the genfis1 funtion) the rules are of the type: if (in1 is in1mf k ) and (in is inmf p ) then (out1 is out1mf r ). The number of output mf is k p (r = 1/(k p)) and is equal to the number of rules. For these three FISs, generalized Bell-type membership funtions were generated; within the sets of rules they are noted by in j mf n ; j is the input number (1/) and n is the number of the membership funtions. For ElongationFis and ElongationFis, six membership funtions for the first input (k = 6) and 1 membership funtions for the seond input (p = 1 r = 7) are produed. The d0elongationfis results in 1 membership funtions for the first input (k = 1) and 14 for the seond input (p = 14 r = 168). For example, the ElongationFis FIS has the struture shown in Fig. 14, whereas the orresponding ontroller (Controller 1) has the same struture as Controller 3 (see Fig. 13). Eah of the four FISs is imported at the fuzzy ontroller level, resulting in four ontrollers: Controller 1 ( ElongationFis ), Controller ( ElongationFis ), Controller 3 ( delongationfis ), and Controller 4 Pro. IMehE Vol. 3 Part G: J. Aerospae Engineering JAERO5

11 Adaptive neuro-fuzzy inferene system-based ontrollers 665 Fig. 1 Struture of the delongationfis FIS Fig. 13 The struture of Controller 3 ( d0elongationfis ). These four ontrollers are integrated using the logial sheme given in Fig. 3; the Matlab/Simulink model in Fig. 15 is the result. In the Matlab/Simulink model shown in Fig. 15, the seond input of Controller and that of Controller 4 (time) are generated by using integrators, starting from the moment that these inputs are used in Controller or Controller 4 (the input of the Gain blok is 0 if the shema deides not to work with one of the Controllers or 4). It is possible that the simulation sample time may be different from the sample time used in the experimental data aquisition proess, and therefore the Gain blok that gives their ratio is used; Te is the sample time in the experimental data and T is the simulation sample time. In the shema, the onstant C represents the maximum time onsidered for the atuator to reover its initial temperature ( 4 C) when the urrent beomes 0 A. Evaluating the integrated ontroller model (see Fig. 15) for all five experimental data ases produes the results shown in Figs 16 and 17. These graphis show the elongations versus the number of experimental data points and versus the applied eletrial urrent, respetively, using the experimental data and the integrated neuro-fuzzy ontroller model for the SMA. A good overlapping of the outputs of the integrated neuro-fuzzy ontroller with the experimental data an be easily observed. Fig. 14 Struture of the ElongationFis FIS JAERO5 Pro. IMehE Vol. 3 Part G: J. Aerospae Engineering

12 666 T L Grigorie andrmbotez Fig. 15 The integration model shema in Matlab/Simulink Fig. 16 Elongations versus the number of experimental data points Pro. IMehE Vol. 3 Part G: J. Aerospae Engineering JAERO5

13 Adaptive neuro-fuzzy inferene system-based ontrollers 667 Fig. 17 Elongations versus the applied eletrial urrent Fig. 18 Three-dimensional evaluation of the integrated neuro-fuzzy ontroller The same observation an be made from the threedimensional harateristis of the experimental data and the neuro-fuzzy modelled data in terms of temperature, elongation, and fore, depited in Fig. 18(a), and in terms of urrent, elongation, and fore, depited in Fig. 18(b). The mean values of the relative absolute errors of the integrated ontroller for the five load ases of the SMA, based on adaptive neuro-fiss, are per ent for 10 N, per ent for 140 N, per ent for 150 N, per ent for 180 N, and per ent for 190 N. The mean value of the relative absolute error between the experimental data and the outputs of the integrated ontroller is 0.54 per ent. 5 CONCLUSIONS In this artile, an integrated ontroller based on adaptive neuro-fiss for modelling smart material atuators was obtained. The diret appliation of this ontroller is in a morphing wing system. The general aim of the smart material atuators desired model is to alulate the elongation of the atuator under the appliation of a thermo-eletro-mehanial load for a ertain time. Therefore, the smart material atuators were experimentally tested in onditions lose to those in whih they will be used. Testing was performed for five load ases, with fores of 10, 140, 150, 180, and 190 N. Using the experimental data, JAERO5 Pro. IMehE Vol. 3 Part G: J. Aerospae Engineering

14 668 T L Grigorie andrmbotez four FISs were generated and trained to obtain four neuro-fuzzy ontrollers: one ontroller for the urrent inrease ( ElongationFis ), one for a onstant urrent ( ElongationFis ), one for the urrent derease ( delongationfis ), and one ontroller for the null urrent, after its derease ( d0elongationfis ). The genfis1 and genfis Matlab funtions were used to generate the initial FISs, and the adaptive neuro-ifs tehnique was then used to train them.the final values of the relative absolute errors for the four generated and trained FISs were per ent for ElongationFis, per ent for ElongationFis, per ent for delongationfis, and per ent for d0elongationfis. Eah of the four obtained and trained FISs were imported at the fuzzy ontroller level, resulting in four ontrollers. Finally, these four ontrollers were integrated by using the logial sheme given in Fig. 3; resulting in the Matlab/Simulink model for the integrated ontroller shown in Fig. 15. The integrated ontroller performanes were evaluated for all five load ases; the values obtained for the mean relative absolute errors were per ent for 10 N, per ent for 140 N, per ent for 150 N, per ent for 180 N, and per ent for 190 N. Thus, the mean value of the relative absolute error between the experimental data and the outputs of the integrated ontroller was 0.54 per ent. A partiular advantage of this new model is its rapid generation, thanks to the genfis1, genfis, and ANFIS funtions already implemented in Matlab. The user need only assume the four FIS s training performanes using the anfisedit interfae generated with Matlab. Authors 009 REFERENCES 1 Sivanandam, S. N., Sumathi, S., and Deepa, S. N. Introdution to fuzzy logi using MATLAB, 007 (Springer, Berlin, Heidelberg). Kosko, B. Neural networks and fuzzy systems a dynamial systems approah to mahine intelligene, 199 (Prentie Hall, New Jersey, NJ). 3 Matlab fuzzy logi and neural network toolboxes, available from Neural_Network_and_Fuzzy_Logi/. 4 Khezri, M. and Jahed, M. Real-time intelligent pattern reognition algorithm for surfae EMG signals. BioMed. Eng. OnLine, 007, 6, 45. DOI: / X Kung, C. C. and Su, J.Y. Affine TakagiSugeno fuzzy modelling algorithm by fuzzy -regression models lustering with a novel luster validity riterion. IET Control Theory Appl., 007, 1(5), Mahfouf, M., Linkens, D. A., and Kandiah, S. Fuzzy TakagiSugeno Kang model preditive ontrol for proess engineering, 1999, p. 4 (IEE, Savoy plae, London WCPR OBL, UK). APPENDIX Notation a, b parameters of the generalized bell membership funtion a i k parameters of the linear funtion (k = 1,, i = 1, N) Aq i assoiated individual anteedent fuzzy sets of eah input variable (i = 1, N) b0 i salar offset (i = 1, N) luster entre q i luster entre (q = 1, ) C p pressure oeffiient F fore i eletrial urrent k variable for neuro-fuzzy ontroller seletion k y step size l dimension of the data vetors M number of data points N number of rules r m radius within the fuzzy neighbourhood, ontributes to the density measure Re Reynolds number t time T temperature of the smart material atuator T amb ambient temperature u j entre of the jth luster u k data vetors V speed w i degree of fulfilment of the anteedent, i.e. the level of firing of the ith rule x input vetor x q individual input variables (q = 1, ) y output of the fuzzy model y i first-order polynomial funtion in the onsequent (i = 1, N) α δ t ε ρ σ σ i q angle of attak atuator elongation time variation ost funtion density measure dispersion luster dispersion Pro. IMehE Vol. 3 Part G: J. Aerospae Engineering JAERO5

Neuro-Fuzzy Modeling of Heat Recovery Steam Generator

Neuro-Fuzzy Modeling of Heat Recovery Steam Generator International Journal of Mahine Learning and Computing, Vol. 2, No. 5, Otober 202 Neuro-Fuzzy Modeling of Heat Reovery Steam Generator A. Ghaffari, A. Chaibakhsh, and S. Shahhoseini represented in a network

More information

Control Theory association of mathematics and engineering

Control Theory association of mathematics and engineering Control Theory assoiation of mathematis and engineering Wojieh Mitkowski Krzysztof Oprzedkiewiz Department of Automatis AGH Univ. of Siene & Tehnology, Craow, Poland, Abstrat In this paper a methodology

More information

Developing Excel Macros for Solving Heat Diffusion Problems

Developing Excel Macros for Solving Heat Diffusion Problems Session 50 Developing Exel Maros for Solving Heat Diffusion Problems N. N. Sarker and M. A. Ketkar Department of Engineering Tehnology Prairie View A&M University Prairie View, TX 77446 Abstrat This paper

More information

Variation Based Online Travel Time Prediction Using Clustered Neural Networks

Variation Based Online Travel Time Prediction Using Clustered Neural Networks Variation Based Online Travel Time Predition Using lustered Neural Networks Jie Yu, Gang-Len hang, H.W. Ho and Yue Liu Abstrat-This paper proposes a variation-based online travel time predition approah

More information

Millennium Relativity Acceleration Composition. The Relativistic Relationship between Acceleration and Uniform Motion

Millennium Relativity Acceleration Composition. The Relativistic Relationship between Acceleration and Uniform Motion Millennium Relativity Aeleration Composition he Relativisti Relationship between Aeleration and niform Motion Copyright 003 Joseph A. Rybzyk Abstrat he relativisti priniples developed throughout the six

More information

Neuro-Fuzzy Control of Chemical Reactor with Disturbances

Neuro-Fuzzy Control of Chemical Reactor with Disturbances Neuro-Fuzzy Control of Chemial Reator with Disturbanes LENK BLHOÁ, JÁN DORN Department of Information Engineering and Proess Control, Institute of Information Engineering, utomation and Mathematis Faulty

More information

Complexity of Regularization RBF Networks

Complexity of Regularization RBF Networks Complexity of Regularization RBF Networks Mark A Kon Department of Mathematis and Statistis Boston University Boston, MA 02215 mkon@buedu Leszek Plaskota Institute of Applied Mathematis University of Warsaw

More information

Measuring & Inducing Neural Activity Using Extracellular Fields I: Inverse systems approach

Measuring & Inducing Neural Activity Using Extracellular Fields I: Inverse systems approach Measuring & Induing Neural Ativity Using Extraellular Fields I: Inverse systems approah Keith Dillon Department of Eletrial and Computer Engineering University of California San Diego 9500 Gilman Dr. La

More information

Robust Flight Control Design for a Turn Coordination System with Parameter Uncertainties

Robust Flight Control Design for a Turn Coordination System with Parameter Uncertainties Amerian Journal of Applied Sienes 4 (7): 496-501, 007 ISSN 1546-939 007 Siene Publiations Robust Flight ontrol Design for a urn oordination System with Parameter Unertainties 1 Ari Legowo and Hiroshi Okubo

More information

Model-based mixture discriminant analysis an experimental study

Model-based mixture discriminant analysis an experimental study Model-based mixture disriminant analysis an experimental study Zohar Halbe and Mayer Aladjem Department of Eletrial and Computer Engineering, Ben-Gurion University of the Negev P.O.Box 653, Beer-Sheva,

More information

A Queueing Model for Call Blending in Call Centers

A Queueing Model for Call Blending in Call Centers A Queueing Model for Call Blending in Call Centers Sandjai Bhulai and Ger Koole Vrije Universiteit Amsterdam Faulty of Sienes De Boelelaan 1081a 1081 HV Amsterdam The Netherlands E-mail: {sbhulai, koole}@s.vu.nl

More information

Supplementary Materials

Supplementary Materials Supplementary Materials Neural population partitioning and a onurrent brain-mahine interfae for sequential motor funtion Maryam M. Shanehi, Rollin C. Hu, Marissa Powers, Gregory W. Wornell, Emery N. Brown

More information

Aircraft CAS Design with Input Saturation Using Dynamic Model Inversion

Aircraft CAS Design with Input Saturation Using Dynamic Model Inversion International Journal of Control, Automation, and Systems Vol., No. 3, September 003 35 Airraft CAS Design with Input Saturation sing Dynami Model Inversion Sangsoo Lim and Byoung Soo Kim Abstrat: This

More information

An Integrated Architecture of Adaptive Neural Network Control for Dynamic Systems

An Integrated Architecture of Adaptive Neural Network Control for Dynamic Systems An Integrated Arhiteture of Adaptive Neural Network Control for Dynami Systems Robert L. Tokar 2 Brian D.MVey2 'Center for Nonlinear Studies, 2Applied Theoretial Physis Division Los Alamos National Laboratory,

More information

Modelling and Simulation. Study Support. Zora Jančíková

Modelling and Simulation. Study Support. Zora Jančíková VYSOKÁ ŠKOLA BÁŇSKÁ TECHNICKÁ UNIVERZITA OSTRAVA FAKULTA METALURGIE A MATERIÁLOVÉHO INŽENÝRSTVÍ Modelling and Simulation Study Support Zora Jančíková Ostrava 5 Title: Modelling and Simulation Code: 638-3/

More information

SURFACE WAVES OF NON-RAYLEIGH TYPE

SURFACE WAVES OF NON-RAYLEIGH TYPE SURFACE WAVES OF NON-RAYLEIGH TYPE by SERGEY V. KUZNETSOV Institute for Problems in Mehanis Prosp. Vernadskogo, 0, Mosow, 75 Russia e-mail: sv@kuznetsov.msk.ru Abstrat. Existene of surfae waves of non-rayleigh

More information

UTC. Engineering 329. Proportional Controller Design. Speed System. John Beverly. Green Team. John Beverly Keith Skiles John Barker.

UTC. Engineering 329. Proportional Controller Design. Speed System. John Beverly. Green Team. John Beverly Keith Skiles John Barker. UTC Engineering 329 Proportional Controller Design for Speed System By John Beverly Green Team John Beverly Keith Skiles John Barker 24 Mar 2006 Introdution This experiment is intended test the variable

More information

DIGITAL DISTANCE RELAYING SCHEME FOR PARALLEL TRANSMISSION LINES DURING INTER-CIRCUIT FAULTS

DIGITAL DISTANCE RELAYING SCHEME FOR PARALLEL TRANSMISSION LINES DURING INTER-CIRCUIT FAULTS CHAPTER 4 DIGITAL DISTANCE RELAYING SCHEME FOR PARALLEL TRANSMISSION LINES DURING INTER-CIRCUIT FAULTS 4.1 INTRODUCTION Around the world, environmental and ost onsiousness are foring utilities to install

More information

Design and Development of Three Stages Mixed Sampling Plans for Variable Attribute Variable Quality Characteristics

Design and Development of Three Stages Mixed Sampling Plans for Variable Attribute Variable Quality Characteristics International Journal of Statistis and Systems ISSN 0973-2675 Volume 12, Number 4 (2017), pp. 763-772 Researh India Publiations http://www.ripubliation.om Design and Development of Three Stages Mixed Sampling

More information

Optimization of Statistical Decisions for Age Replacement Problems via a New Pivotal Quantity Averaging Approach

Optimization of Statistical Decisions for Age Replacement Problems via a New Pivotal Quantity Averaging Approach Amerian Journal of heoretial and Applied tatistis 6; 5(-): -8 Published online January 7, 6 (http://www.sienepublishinggroup.om/j/ajtas) doi:.648/j.ajtas.s.65.4 IN: 36-8999 (Print); IN: 36-96 (Online)

More information

Normative and descriptive approaches to multiattribute decision making

Normative and descriptive approaches to multiattribute decision making De. 009, Volume 8, No. (Serial No.78) China-USA Business Review, ISSN 57-54, USA Normative and desriptive approahes to multiattribute deision making Milan Terek (Department of Statistis, University of

More information

Modeling of Threading Dislocation Density Reduction in Heteroepitaxial Layers

Modeling of Threading Dislocation Density Reduction in Heteroepitaxial Layers A. E. Romanov et al.: Threading Disloation Density Redution in Layers (II) 33 phys. stat. sol. (b) 99, 33 (997) Subjet lassifiation: 6.72.C; 68.55.Ln; S5.; S5.2; S7.; S7.2 Modeling of Threading Disloation

More information

An Adaptive Optimization Approach to Active Cancellation of Repeated Transient Vibration Disturbances

An Adaptive Optimization Approach to Active Cancellation of Repeated Transient Vibration Disturbances An aptive Optimization Approah to Ative Canellation of Repeated Transient Vibration Disturbanes David L. Bowen RH Lyon Corp / Aenteh, 33 Moulton St., Cambridge, MA 138, U.S.A., owen@lyonorp.om J. Gregory

More information

The gravitational phenomena without the curved spacetime

The gravitational phenomena without the curved spacetime The gravitational phenomena without the urved spaetime Mirosław J. Kubiak Abstrat: In this paper was presented a desription of the gravitational phenomena in the new medium, different than the urved spaetime,

More information

The simulation analysis of the bridge rectifier continuous operation in AC circuit

The simulation analysis of the bridge rectifier continuous operation in AC circuit Computer Appliations in Eletrial Engineering Vol. 4 6 DOI 8/j.8-448.6. The simulation analysis of the bridge retifier ontinuous operation in AC iruit Mirosław Wiślik, Paweł Strząbała Kiele University of

More information

The Effectiveness of the Linear Hull Effect

The Effectiveness of the Linear Hull Effect The Effetiveness of the Linear Hull Effet S. Murphy Tehnial Report RHUL MA 009 9 6 Otober 009 Department of Mathematis Royal Holloway, University of London Egham, Surrey TW0 0EX, England http://www.rhul.a.uk/mathematis/tehreports

More information

Optimal control of solar energy systems

Optimal control of solar energy systems Optimal ontrol of solar energy systems Viorel Badesu Candida Oanea Institute Polytehni University of Buharest Contents. Optimal operation - systems with water storage tanks 2. Sizing solar olletors 3.

More information

A NONLILEAR CONTROLLER FOR SHIP AUTOPILOTS

A NONLILEAR CONTROLLER FOR SHIP AUTOPILOTS Vietnam Journal of Mehanis, VAST, Vol. 4, No. (), pp. A NONLILEAR CONTROLLER FOR SHIP AUTOPILOTS Le Thanh Tung Hanoi University of Siene and Tehnology, Vietnam Abstrat. Conventional ship autopilots are

More information

Nonreversibility of Multiple Unicast Networks

Nonreversibility of Multiple Unicast Networks Nonreversibility of Multiple Uniast Networks Randall Dougherty and Kenneth Zeger September 27, 2005 Abstrat We prove that for any finite direted ayli network, there exists a orresponding multiple uniast

More information

INTERNATIONAL JOURNAL OF CIVIL AND STRUCTURAL ENGINEERING Volume 2, No 4, 2012

INTERNATIONAL JOURNAL OF CIVIL AND STRUCTURAL ENGINEERING Volume 2, No 4, 2012 INTERNATIONAL JOURNAL OF CIVIL AND STRUCTURAL ENGINEERING Volume, No 4, 01 Copyright 010 All rights reserved Integrated Publishing servies Researh artile ISSN 0976 4399 Strutural Modelling of Stability

More information

Development of Fuzzy Extreme Value Theory. Populations

Development of Fuzzy Extreme Value Theory. Populations Applied Mathematial Sienes, Vol. 6, 0, no. 7, 58 5834 Development of Fuzzy Extreme Value Theory Control Charts Using α -uts for Sewed Populations Rungsarit Intaramo Department of Mathematis, Faulty of

More information

Advanced Computational Fluid Dynamics AA215A Lecture 4

Advanced Computational Fluid Dynamics AA215A Lecture 4 Advaned Computational Fluid Dynamis AA5A Leture 4 Antony Jameson Winter Quarter,, Stanford, CA Abstrat Leture 4 overs analysis of the equations of gas dynamis Contents Analysis of the equations of gas

More information

COMBINED PROBE FOR MACH NUMBER, TEMPERATURE AND INCIDENCE INDICATION

COMBINED PROBE FOR MACH NUMBER, TEMPERATURE AND INCIDENCE INDICATION 4 TH INTERNATIONAL CONGRESS OF THE AERONAUTICAL SCIENCES COMBINED PROBE FOR MACH NUMBER, TEMPERATURE AND INCIDENCE INDICATION Jiri Nozika*, Josef Adame*, Daniel Hanus** *Department of Fluid Dynamis and

More information

Evaluation of effect of blade internal modes on sensitivity of Advanced LIGO

Evaluation of effect of blade internal modes on sensitivity of Advanced LIGO Evaluation of effet of blade internal modes on sensitivity of Advaned LIGO T0074-00-R Norna A Robertson 5 th Otober 00. Introdution The urrent model used to estimate the isolation ahieved by the quadruple

More information

Likelihood-confidence intervals for quantiles in Extreme Value Distributions

Likelihood-confidence intervals for quantiles in Extreme Value Distributions Likelihood-onfidene intervals for quantiles in Extreme Value Distributions A. Bolívar, E. Díaz-Franés, J. Ortega, and E. Vilhis. Centro de Investigaión en Matemátias; A.P. 42, Guanajuato, Gto. 36; Méxio

More information

JAST 2015 M.U.C. Women s College, Burdwan ISSN a peer reviewed multidisciplinary research journal Vol.-01, Issue- 01

JAST 2015 M.U.C. Women s College, Burdwan ISSN a peer reviewed multidisciplinary research journal Vol.-01, Issue- 01 JAST 05 M.U.C. Women s College, Burdwan ISSN 395-353 -a peer reviewed multidisiplinary researh journal Vol.-0, Issue- 0 On Type II Fuzzy Parameterized Soft Sets Pinaki Majumdar Department of Mathematis,

More information

RELAXED STABILIZATION CONDITIONS FOR SWITCHING T-S FUZZY SYSTEMS WITH PRACTICAL CONSTRAINTS. Received January 2011; revised July 2011

RELAXED STABILIZATION CONDITIONS FOR SWITCHING T-S FUZZY SYSTEMS WITH PRACTICAL CONSTRAINTS. Received January 2011; revised July 2011 International Journal of Innovative Computing, Information and Control ICIC International 2012 ISSN 139-198 Volume 8, Number 6, June 2012 pp. 133 15 RELAXED STABILIZATION CONDITIONS FOR SWITCHING T-S FUZZY

More information

IMPEDANCE EFFECTS OF LEFT TURNERS FROM THE MAJOR STREET AT A TWSC INTERSECTION

IMPEDANCE EFFECTS OF LEFT TURNERS FROM THE MAJOR STREET AT A TWSC INTERSECTION 09-1289 Citation: Brilon, W. (2009): Impedane Effets of Left Turners from the Major Street at A TWSC Intersetion. Transportation Researh Reord Nr. 2130, pp. 2-8 IMPEDANCE EFFECTS OF LEFT TURNERS FROM THE

More information

Remark 4.1 Unlike Lyapunov theorems, LaSalle s theorem does not require the function V ( x ) to be positive definite.

Remark 4.1 Unlike Lyapunov theorems, LaSalle s theorem does not require the function V ( x ) to be positive definite. Leture Remark 4.1 Unlike Lyapunov theorems, LaSalle s theorem does not require the funtion V ( x ) to be positive definite. ost often, our interest will be to show that x( t) as t. For that we will need

More information

Hankel Optimal Model Order Reduction 1

Hankel Optimal Model Order Reduction 1 Massahusetts Institute of Tehnology Department of Eletrial Engineering and Computer Siene 6.245: MULTIVARIABLE CONTROL SYSTEMS by A. Megretski Hankel Optimal Model Order Redution 1 This leture overs both

More information

Speed-feedback Direct-drive Control of a Low-speed Transverse Flux-type Motor with Large Number of Poles for Ship Propulsion

Speed-feedback Direct-drive Control of a Low-speed Transverse Flux-type Motor with Large Number of Poles for Ship Propulsion Speed-feedbak Diret-drive Control of a Low-speed Transverse Flux-type Motor with Large Number of Poles for Ship Propulsion Y. Yamamoto, T. Nakamura 2, Y. Takada, T. Koseki, Y. Aoyama 3, and Y. Iwaji 3

More information

ONLINE APPENDICES for Cost-Effective Quality Assurance in Crowd Labeling

ONLINE APPENDICES for Cost-Effective Quality Assurance in Crowd Labeling ONLINE APPENDICES for Cost-Effetive Quality Assurane in Crowd Labeling Jing Wang Shool of Business and Management Hong Kong University of Siene and Tehnology Clear Water Bay Kowloon Hong Kong jwang@usthk

More information

Singular Event Detection

Singular Event Detection Singular Event Detetion Rafael S. Garía Eletrial Engineering University of Puerto Rio at Mayagüez Rafael.Garia@ee.uprm.edu Faulty Mentor: S. Shankar Sastry Researh Supervisor: Jonathan Sprinkle Graduate

More information

After the completion of this section the student should recall

After the completion of this section the student should recall Chapter I MTH FUNDMENTLS I. Sets, Numbers, Coordinates, Funtions ugust 30, 08 3 I. SETS, NUMERS, COORDINTES, FUNCTIONS Objetives: fter the ompletion of this setion the student should reall - the definition

More information

Danielle Maddix AA238 Final Project December 9, 2016

Danielle Maddix AA238 Final Project December 9, 2016 Struture and Parameter Learning in Bayesian Networks with Appliations to Prediting Breast Caner Tumor Malignany in a Lower Dimension Feature Spae Danielle Maddix AA238 Final Projet Deember 9, 2016 Abstrat

More information

AC : A GRAPHICAL USER INTERFACE (GUI) FOR A UNIFIED APPROACH FOR CONTINUOUS-TIME COMPENSATOR DESIGN

AC : A GRAPHICAL USER INTERFACE (GUI) FOR A UNIFIED APPROACH FOR CONTINUOUS-TIME COMPENSATOR DESIGN AC 28-1986: A GRAPHICAL USER INTERFACE (GUI) FOR A UNIFIED APPROACH FOR CONTINUOUS-TIME COMPENSATOR DESIGN Minh Cao, Wihita State University Minh Cao ompleted his Bahelor s of Siene degree at Wihita State

More information

A NETWORK SIMPLEX ALGORITHM FOR THE MINIMUM COST-BENEFIT NETWORK FLOW PROBLEM

A NETWORK SIMPLEX ALGORITHM FOR THE MINIMUM COST-BENEFIT NETWORK FLOW PROBLEM NETWORK SIMPLEX LGORITHM FOR THE MINIMUM COST-BENEFIT NETWORK FLOW PROBLEM Cen Çalışan, Utah Valley University, 800 W. University Parway, Orem, UT 84058, 801-863-6487, en.alisan@uvu.edu BSTRCT The minimum

More information

MultiPhysics Analysis of Trapped Field in Multi-Layer YBCO Plates

MultiPhysics Analysis of Trapped Field in Multi-Layer YBCO Plates Exerpt from the Proeedings of the COMSOL Conferene 9 Boston MultiPhysis Analysis of Trapped Field in Multi-Layer YBCO Plates Philippe. Masson Advaned Magnet Lab *7 Main Street, Bldg. #4, Palm Bay, Fl-95,

More information

QCLAS Sensor for Purity Monitoring in Medical Gas Supply Lines

QCLAS Sensor for Purity Monitoring in Medical Gas Supply Lines DOI.56/sensoren6/P3. QLAS Sensor for Purity Monitoring in Medial Gas Supply Lines Henrik Zimmermann, Mathias Wiese, Alessandro Ragnoni neoplas ontrol GmbH, Walther-Rathenau-Str. 49a, 7489 Greifswald, Germany

More information

Determination of the Aerodynamic Characteristics of Flying Vehicles Using Method Large Eddy Simulation with Software ANSYS

Determination of the Aerodynamic Characteristics of Flying Vehicles Using Method Large Eddy Simulation with Software ANSYS Automation, Control and Intelligent Systems 15; 3(6): 118-13 Published online Deember, 15 (http://www.sienepublishinggroup.om//ais) doi: 1.11648/.ais.1536.14 ISSN: 38-5583 (Print); ISSN: 38-5591 (Online)

More information

10.5 Unsupervised Bayesian Learning

10.5 Unsupervised Bayesian Learning The Bayes Classifier Maximum-likelihood methods: Li Yu Hongda Mao Joan Wang parameter vetor is a fixed but unknown value Bayes methods: parameter vetor is a random variable with known prior distribution

More information

A Novel Process for the Study of Breakage Energy versus Particle Size

A Novel Process for the Study of Breakage Energy versus Particle Size Geomaterials, 2013, 3, 102-110 http://dx.doi.org/10.4236/gm.2013.33013 Published Online July 2013 (http://www.sirp.org/journal/gm) A Novel Proess for the Study of Breakage Energy versus Partile Size Elias

More information

EFFECTS OF COUPLE STRESSES ON PURE SQUEEZE EHL MOTION OF CIRCULAR CONTACTS

EFFECTS OF COUPLE STRESSES ON PURE SQUEEZE EHL MOTION OF CIRCULAR CONTACTS -Tehnial Note- EFFECTS OF COUPLE STRESSES ON PURE SQUEEZE EHL MOTION OF CIRCULAR CONTACTS H.-M. Chu * W.-L. Li ** Department of Mehanial Engineering Yung-Ta Institute of Tehnology & Commere Ping-Tung,

More information

A simple expression for radial distribution functions of pure fluids and mixtures

A simple expression for radial distribution functions of pure fluids and mixtures A simple expression for radial distribution funtions of pure fluids and mixtures Enrio Matteoli a) Istituto di Chimia Quantistia ed Energetia Moleolare, CNR, Via Risorgimento, 35, 56126 Pisa, Italy G.

More information

Natural Convection Experiment Measurements from a Vertical Surface

Natural Convection Experiment Measurements from a Vertical Surface OBJECTIVE Natural Convetion Experiment Measurements from a Vertial Surfae 1. To demonstrate te basi priniples of natural onvetion eat transfer inluding determination of te onvetive eat transfer oeffiient.

More information

Subject: Introduction to Component Matching and Off-Design Operation % % ( (1) R T % (

Subject: Introduction to Component Matching and Off-Design Operation % % ( (1) R T % ( 16.50 Leture 0 Subjet: Introdution to Component Mathing and Off-Design Operation At this point it is well to reflet on whih of the many parameters we have introdued (like M, τ, τ t, ϑ t, f, et.) are free

More information

Design of an Adaptive Neural Network Controller for Effective Position Control of Linear Pneumatic Actuators

Design of an Adaptive Neural Network Controller for Effective Position Control of Linear Pneumatic Actuators Researh Artile International Journal of Current Engineering and Tehnology E-ISSN 77 406, P-ISSN 347-56 04 INPRESSCO, All Rights Reserved Available at http://inpresso.om/ategory/ijet Design of an Adaptive

More information

Planning with Uncertainty in Position: an Optimal Planner

Planning with Uncertainty in Position: an Optimal Planner Planning with Unertainty in Position: an Optimal Planner Juan Pablo Gonzalez Anthony (Tony) Stentz CMU-RI -TR-04-63 The Robotis Institute Carnegie Mellon University Pittsburgh, Pennsylvania 15213 Otober

More information

MODELLING THE POSTPEAK STRESS DISPLACEMENT RELATIONSHIP OF CONCRETE IN UNIAXIAL COMPRESSION

MODELLING THE POSTPEAK STRESS DISPLACEMENT RELATIONSHIP OF CONCRETE IN UNIAXIAL COMPRESSION VIII International Conferene on Frature Mehanis of Conrete and Conrete Strutures FraMCoS-8 J.G.M. Van Mier, G. Ruiz, C. Andrade, R.C. Yu and X.X. Zhang Eds) MODELLING THE POSTPEAK STRESS DISPLACEMENT RELATIONSHIP

More information

Document Version Publisher s PDF, also known as Version of Record (includes final page, issue and volume numbers)

Document Version Publisher s PDF, also known as Version of Record (includes final page, issue and volume numbers) A omparison between ylindrial and ross-shaped magneti vibration isolators : ideal and pratial van Casteren, D.T.E.H.; Paulides, J.J.H.; Lomonova, E. Published in: Arhives of Eletrial Engineering DOI: 10.1515/aee-2015-0044

More information

Array Design for Superresolution Direction-Finding Algorithms

Array Design for Superresolution Direction-Finding Algorithms Array Design for Superresolution Diretion-Finding Algorithms Naushad Hussein Dowlut BEng, ACGI, AMIEE Athanassios Manikas PhD, DIC, AMIEE, MIEEE Department of Eletrial Eletroni Engineering Imperial College

More information

The universal model of error of active power measuring channel

The universal model of error of active power measuring channel 7 th Symposium EKO TC 4 3 rd Symposium EKO TC 9 and 5 th WADC Workshop nstrumentation for the CT Era Sept. 8-2 Kosie Slovakia The universal model of error of ative power measuring hannel Boris Stogny Evgeny

More information

Calculation of Desorption Parameters for Mg/Si(111) System

Calculation of Desorption Parameters for Mg/Si(111) System e-journal of Surfae Siene and Nanotehnology 29 August 2009 e-j. Surf. Si. Nanoteh. Vol. 7 (2009) 816-820 Conferene - JSSS-8 - Calulation of Desorption Parameters for Mg/Si(111) System S. A. Dotsenko, N.

More information

Controller Design Based on Transient Response Criteria. Chapter 12 1

Controller Design Based on Transient Response Criteria. Chapter 12 1 Controller Design Based on Transient Response Criteria Chapter 12 1 Desirable Controller Features 0. Stable 1. Quik responding 2. Adequate disturbane rejetion 3. Insensitive to model, measurement errors

More information

Multicomponent analysis on polluted waters by means of an electronic tongue

Multicomponent analysis on polluted waters by means of an electronic tongue Sensors and Atuators B 44 (1997) 423 428 Multiomponent analysis on polluted waters by means of an eletroni tongue C. Di Natale a, *, A. Maagnano a, F. Davide a, A. D Amio a, A. Legin b, Y. Vlasov b, A.

More information

Bilinear Formulated Multiple Kernel Learning for Multi-class Classification Problem

Bilinear Formulated Multiple Kernel Learning for Multi-class Classification Problem Bilinear Formulated Multiple Kernel Learning for Multi-lass Classifiation Problem Takumi Kobayashi and Nobuyuki Otsu National Institute of Advaned Industrial Siene and Tehnology, -- Umezono, Tsukuba, Japan

More information

Physical Laws, Absolutes, Relative Absolutes and Relativistic Time Phenomena

Physical Laws, Absolutes, Relative Absolutes and Relativistic Time Phenomena Page 1 of 10 Physial Laws, Absolutes, Relative Absolutes and Relativisti Time Phenomena Antonio Ruggeri modexp@iafria.om Sine in the field of knowledge we deal with absolutes, there are absolute laws that

More information

A model for measurement of the states in a coupled-dot qubit

A model for measurement of the states in a coupled-dot qubit A model for measurement of the states in a oupled-dot qubit H B Sun and H M Wiseman Centre for Quantum Computer Tehnology Centre for Quantum Dynamis Griffith University Brisbane 4 QLD Australia E-mail:

More information

A Spatiotemporal Approach to Passive Sound Source Localization

A Spatiotemporal Approach to Passive Sound Source Localization A Spatiotemporal Approah Passive Sound Soure Loalization Pasi Pertilä, Mikko Parviainen, Teemu Korhonen and Ari Visa Institute of Signal Proessing Tampere University of Tehnology, P.O.Box 553, FIN-330,

More information

LATTICE BOLTZMANN METHOD FOR MICRO CHANNEL AND MICRO ORIFICE FLOWS TAIHO YEOM. Bachelor of Science in Mechanical Engineering.

LATTICE BOLTZMANN METHOD FOR MICRO CHANNEL AND MICRO ORIFICE FLOWS TAIHO YEOM. Bachelor of Science in Mechanical Engineering. LATTICE BOLTZMANN METHOD FOR MICRO CHANNEL AND MICRO ORIFICE FLOWS By TAIHO YEOM Bahelor of Siene in Mehanial Engineering Ajou University Suwon, South Korea 2005 Submitted to the Faulty of the Graduate

More information

Finite-time stabilization of chaotic gyros based on a homogeneous supertwisting-like algorithm

Finite-time stabilization of chaotic gyros based on a homogeneous supertwisting-like algorithm OP Conferene Series: Materials Siene Engineering PAPER OPEN ACCESS Finite-time stabilization of haoti gyros based on a homogeneous supertwisting-like algorithm To ite this artile: Pitha Khamsuwan et al

More information

SINCE Zadeh s compositional rule of fuzzy inference

SINCE Zadeh s compositional rule of fuzzy inference IEEE TRANSACTIONS ON FUZZY SYSTEMS, VOL. 14, NO. 6, DECEMBER 2006 709 Error Estimation of Perturbations Under CRI Guosheng Cheng Yuxi Fu Abstrat The analysis of stability robustness of fuzzy reasoning

More information

Speed Regulation of a Small BLDC Motor using Genetic-Based Proportional Control

Speed Regulation of a Small BLDC Motor using Genetic-Based Proportional Control World Aademy of Siene, Engineering and Tehnology 47 8 Speed Regulation of a Small BLDC Motor using Geneti-Based Proportional Control S. Poonsawat, and T. Kulworawanihpong Abstrat This paper presents the

More information

max min z i i=1 x j k s.t. j=1 x j j:i T j

max min z i i=1 x j k s.t. j=1 x j j:i T j AM 221: Advaned Optimization Spring 2016 Prof. Yaron Singer Leture 22 April 18th 1 Overview In this leture, we will study the pipage rounding tehnique whih is a deterministi rounding proedure that an be

More information

Maximum Entropy and Exponential Families

Maximum Entropy and Exponential Families Maximum Entropy and Exponential Families April 9, 209 Abstrat The goal of this note is to derive the exponential form of probability distribution from more basi onsiderations, in partiular Entropy. It

More information

UPPER-TRUNCATED POWER LAW DISTRIBUTIONS

UPPER-TRUNCATED POWER LAW DISTRIBUTIONS Fratals, Vol. 9, No. (00) 09 World Sientifi Publishing Company UPPER-TRUNCATED POWER LAW DISTRIBUTIONS STEPHEN M. BURROUGHS and SARAH F. TEBBENS College of Marine Siene, University of South Florida, St.

More information

Improvements in the Modeling of the Self-ignition of Tetrafluoroethylene

Improvements in the Modeling of the Self-ignition of Tetrafluoroethylene Exerpt from the Proeedings of the OMSOL onferene 010 Paris Improvements in the Modeling of the Self-ignition of Tetrafluoroethylene M. Bekmann-Kluge 1 *,. errero 1, V. Shröder 1, A. Aikalin and J. Steinbah

More information

The transition between quasi-static and fully dynamic for interfaces

The transition between quasi-static and fully dynamic for interfaces Physia D 198 (24) 136 147 The transition between quasi-stati and fully dynami for interfaes G. Caginalp, H. Merdan Department of Mathematis, University of Pittsburgh, Pittsburgh, PA 1526, USA Reeived 6

More information

MATHEMATICAL AND NUMERICAL BASIS OF BINARY ALLOY SOLIDIFICATION MODELS WITH SUBSTITUTE THERMAL CAPACITY. PART II

MATHEMATICAL AND NUMERICAL BASIS OF BINARY ALLOY SOLIDIFICATION MODELS WITH SUBSTITUTE THERMAL CAPACITY. PART II Journal of Applied Mathematis and Computational Mehanis 2014, 13(2), 141-147 MATHEMATICA AND NUMERICA BAI OF BINARY AOY OIDIFICATION MODE WITH UBTITUTE THERMA CAPACITY. PART II Ewa Węgrzyn-krzypzak 1,

More information

Intuitionistic Fuzzy Set and Its Application in Selecting Specialization: A Case Study for Engineering Students

Intuitionistic Fuzzy Set and Its Application in Selecting Specialization: A Case Study for Engineering Students International Journal of Mathematial nalysis and ppliations 2015; 2(6): 74-78 Published online Deember 17, 2015 (http://www.aasit.org/journal/ijmaa) ISSN: 2375-3927 Intuitionisti Fuzzy Set and Its ppliation

More information

State Diagrams. Margaret M. Fleck. 14 November 2011

State Diagrams. Margaret M. Fleck. 14 November 2011 State Diagrams Margaret M. Flek 14 November 2011 These notes over state diagrams. 1 Introdution State diagrams are a type of direted graph, in whih the graph nodes represent states and labels on the graph

More information

The Corpuscular Structure of Matter, the Interaction of Material Particles, and Quantum Phenomena as a Consequence of Selfvariations.

The Corpuscular Structure of Matter, the Interaction of Material Particles, and Quantum Phenomena as a Consequence of Selfvariations. The Corpusular Struture of Matter, the Interation of Material Partiles, and Quantum Phenomena as a Consequene of Selfvariations. Emmanuil Manousos APM Institute for the Advanement of Physis and Mathematis,

More information

Development of a user element in ABAQUS for modelling of cohesive laws in composite structures

Development of a user element in ABAQUS for modelling of cohesive laws in composite structures Downloaded from orbit.dtu.dk on: Jan 19, 2019 Development of a user element in ABAQUS for modelling of ohesive laws in omposite strutures Feih, Stefanie Publiation date: 2006 Doument Version Publisher's

More information

3 Tidal systems modelling: ASMITA model

3 Tidal systems modelling: ASMITA model 3 Tidal systems modelling: ASMITA model 3.1 Introdution For many pratial appliations, simulation and predition of oastal behaviour (morphologial development of shorefae, beahes and dunes) at a ertain level

More information

On the Licensing of Innovations under Strategic Delegation

On the Licensing of Innovations under Strategic Delegation On the Liensing of Innovations under Strategi Delegation Judy Hsu Institute of Finanial Management Nanhua University Taiwan and X. Henry Wang Department of Eonomis University of Missouri USA Abstrat This

More information

Transient wave propagation analysis of a pantograph- catenary system

Transient wave propagation analysis of a pantograph- catenary system Journal of Physis: Conferene Series PAPER OPEN ACCESS Transient wave propagation analysis of a pantograph- atenary system To ite this artile: Kyohei Nagao and Arata Masuda 216 J. Phys.: Conf. Ser. 744

More information

LOGISTIC REGRESSION IN DEPRESSION CLASSIFICATION

LOGISTIC REGRESSION IN DEPRESSION CLASSIFICATION LOGISIC REGRESSIO I DEPRESSIO CLASSIFICAIO J. Kual,. V. ran, M. Bareš KSE, FJFI, CVU v Praze PCP, CS, 3LF UK v Praze Abstrat Well nown logisti regression and the other binary response models an be used

More information

Stress triaxiality to evaluate the effective distance in the volumetric approach in fracture mechanics

Stress triaxiality to evaluate the effective distance in the volumetric approach in fracture mechanics IOSR Journal of ehanial and Civil Engineering (IOSR-JCE) e-issn: 78-1684,p-ISSN: 30-334X, Volume 11, Issue 6 Ver. IV (Nov- De. 014), PP 1-6 Stress triaxiality to evaluate the effetive distane in the volumetri

More information

Dynamic Behavior of Double Layer Cylindrical Space Truss Roofs

Dynamic Behavior of Double Layer Cylindrical Space Truss Roofs Australian Journal of Basi and Applied Sienes, 5(8): 68-75, 011 ISSN 1991-8178 Dynami Behavior of Double Layer Cylindrial Spae Truss Roofs 1, M. Jamshidi, T.A. Majid and 1 A. Darvishi 1 Faulty of Engineering,

More information

Vibration Control of Smart Structure Using Sliding Mode Control with Observer

Vibration Control of Smart Structure Using Sliding Mode Control with Observer JOURNAL OF COMPUERS, VOL. 7, NO., FEBRUARY Vibration Control of Smart Struture Using Sliding Mode Control with Observer Junfeng Hu Shool of Mehanial & Eletrial Engineering, Jiangxi University of Siene

More information

THE METHOD OF SECTIONING WITH APPLICATION TO SIMULATION, by Danie 1 Brent ~~uffman'i

THE METHOD OF SECTIONING WITH APPLICATION TO SIMULATION, by Danie 1 Brent ~~uffman'i THE METHOD OF SECTIONING '\ WITH APPLICATION TO SIMULATION, I by Danie 1 Brent ~~uffman'i Thesis submitted to the Graduate Faulty of the Virginia Polytehni Institute and State University in partial fulfillment

More information

A NORMALIZED EQUATION OF AXIALLY LOADED PILES IN ELASTO-PLASTIC SOIL

A NORMALIZED EQUATION OF AXIALLY LOADED PILES IN ELASTO-PLASTIC SOIL Journal of Geongineering, Vol. Yi-Chuan 4, No. 1, Chou pp. 1-7, and April Yun-Mei 009 Hsiung: A Normalized quation of Axially Loaded Piles in lasto-plasti Soil 1 A NORMALIZD QUATION OF AXIALLY LOADD PILS

More information

Simplified Buckling Analysis of Skeletal Structures

Simplified Buckling Analysis of Skeletal Structures Simplified Bukling Analysis of Skeletal Strutures B.A. Izzuddin 1 ABSRAC A simplified approah is proposed for bukling analysis of skeletal strutures, whih employs a rotational spring analogy for the formulation

More information

Four-dimensional equation of motion for viscous compressible substance with regard to the acceleration field, pressure field and dissipation field

Four-dimensional equation of motion for viscous compressible substance with regard to the acceleration field, pressure field and dissipation field Four-dimensional equation of motion for visous ompressible substane with regard to the aeleration field, pressure field and dissipation field Sergey G. Fedosin PO box 6488, Sviazeva str. -79, Perm, Russia

More information

Conformal Mapping among Orthogonal, Symmetric, and Skew-Symmetric Matrices

Conformal Mapping among Orthogonal, Symmetric, and Skew-Symmetric Matrices AAS 03-190 Conformal Mapping among Orthogonal, Symmetri, and Skew-Symmetri Matries Daniele Mortari Department of Aerospae Engineering, Texas A&M University, College Station, TX 77843-3141 Abstrat This

More information

9 Geophysics and Radio-Astronomy: VLBI VeryLongBaseInterferometry

9 Geophysics and Radio-Astronomy: VLBI VeryLongBaseInterferometry 9 Geophysis and Radio-Astronomy: VLBI VeryLongBaseInterferometry VLBI is an interferometry tehnique used in radio astronomy, in whih two or more signals, oming from the same astronomial objet, are reeived

More information

THEORETICAL PROBLEM No. 3 WHY ARE STARS SO LARGE?

THEORETICAL PROBLEM No. 3 WHY ARE STARS SO LARGE? THEORETICAL PROBLEM No. 3 WHY ARE STARS SO LARGE? The stars are spheres of hot gas. Most of them shine beause they are fusing hydrogen into helium in their entral parts. In this problem we use onepts of

More information

Where as discussed previously we interpret solutions to this partial differential equation in the weak sense: b

Where as discussed previously we interpret solutions to this partial differential equation in the weak sense: b Consider the pure initial value problem for a homogeneous system of onservation laws with no soure terms in one spae dimension: Where as disussed previously we interpret solutions to this partial differential

More information

University of Groningen

University of Groningen University of Groningen Port Hamiltonian Formulation of Infinite Dimensional Systems II. Boundary Control by Interonnetion Mahelli, Alessandro; van der Shaft, Abraham; Melhiorri, Claudio Published in:

More information

Optimal Control of Air Pollution

Optimal Control of Air Pollution Punjab University Journal of Mathematis (ISSN 1016-2526) Vol. 49(1)(2017) pp. 139-148 Optimal Control of Air Pollution Y. O. Aderinto and O. M. Bamigbola Mathematis Department, University of Ilorin, Ilorin,

More information