Stability analysis of two predator-one stage-structured prey model incorporating a prey refuge

Size: px
Start display at page:

Download "Stability analysis of two predator-one stage-structured prey model incorporating a prey refuge"

Transcription

1 IOSR Jornal of Mathematics (IOSR-JM) e-issn: p-issn: X. Volme Isse 3 Ver. II (Ma - Jn. 5) PP -5 Stabilit analsis of two predator-one stage-strctred pre model incorporating a pre refge Zahraa Jawad Kadhim Azhar Abbas Majeed and Raid Kamel Naji Department of Mathematics College of Science Universit of Baghdad Baghdad Iraq. Abstract: In this paper a food web model consisting of two predator-one stage strctred pre involving Lotka-Voltera tpe of fnctional response and a pre refge is proposed and analzed. It is assmed that the pre growth logisticall in the absence of predator. The role of pre refges in predator-pre model is investigated. The existence niqeness and bondedness of the soltion are stdied. The existence and the stabilit analsis of all possible eqilibrim points are stdied. Sitable Lapnov fnctions are sed to std the global dnamics of the proposed model. Nmerical simlation for different sets of parameter vale and for different sets of initial conditions are carried ot to investigate the inflence of parameters on the dnamical behavior of the model and to spport the obtained analtical reslts of the model. Kewords: food web Lapnov fnction refge stabilit analsis stage-strctre. I. Introdction The dnamic relationship between predators and their pre has long been and will contine to be one of the dominant themes in both ecolog and mathematical ecolog de to its niversal existence and importance. Over the past decades Mathematics has made a considerable impact as a tool to model and nderstand biological phenomena. In retrn biologists have confronted the mathematics with variet of challenging problems which have simlated developments in the theor of nonlinear differential eqations. Sch differential eqations have long plaed important role in the field of theoretical poplation dnamics and the will no dobt contine to serve as indispensable tools in ftre investigations. Differential eqation models for interactions between species are one of the classical applications of mathematics to biolog. The development and se of analtical techniqes and the growth of compter power have progressivel improved or nderstanding of these tpes of models. Althogh the predator-pre theor has been mch progress man long standing mathematical and ecological problems remain open. Food chains and food webs depict the network of feeding relationship within ecological commnities. Dring the last few decades a large nmber of food-chain and food-web sstems have been proposed to describe the food transition patterns and processes.living organisms enter into a variet of relationships sch as Pre-Predator Competition Mtalism Commensalism and so on among themselves according to the needs of individals as well as those of species grops. Food webs are one example of interactions that go beond feeding relationships. Recentl nmber of researchers have been proposed and stdied the dnamics of food webs involving some tpes of these relationships for example see 5 8 and the references their in.the std of the conseqences of hiding behavior of pre on the dnamics of predator pre interactions can be recognized as a major isse in applied mathematics and theoretical ecolog 9. Some of the empirical and theoretical work have investigated the effect of pre refges and drawn a conclsion that the refges sed b pre have a stabilizing effect on the considered interactions and pre extinction can be prevented b the addition of refges.in fact the effect of pre refges on the poplation dnamics are ver complex in natre bt for modeling prposes it can be considered as constitted b two components the first effects which affect positivel the growth of pre and negativel that of predators. Comprise the redction of pre mortalit de to decrease in predation sccess. The second one ma be the trad-offs and b-prodcts of the hiding behavior of pre which cold be advantageos or detrimental for all the interacting poplations. A classic secondar effect is the redction in the birth rate of pre poplation becase refges are safe bt rarel offer feeding or mating opportnities 3.Z. Ma and et.al 5 derived a predator-pre model with Lotka-Voltera fnctional response incorporating pre refges the refges are considered as two tpes: a constant proportion of pre and a fixed nmber of pre sing refges. The evalate the effect with regard to the stabilit of the interior eqilibrim. The reslts show that the refges sed b pre can increase the eqilibrim densit of the pre poplation while decrease that of predator.on the other hand it is well known that the age factor is importance for the dnamics and evoltion of man mammals. The rate of srvival growth and reprodction almost depend on age or development stage and it has been noticed that the life histor of man species is composed of at least two stages immatre and matre and the species in the first stage ma often neither interact with other species nor reprodce being raised b their matre parents. Most of classical pre-predator models of two species in the literatre assmed that all predators are able to attack their pre and reprodce ignoring the fact that the life ccle of most animals consists of at least DOI:.979/ Page

2 Stabilit analsis of two predator-one stage-strctred pre model incorporating a pre refge two stages ( immatre and matre ). Recentl several of the pre-predator models with stage-strctre of species with or withot time delas are proposed and analzed 6 9. In this paper the food web prepredator model involving pre s refges is proposed and analzed so that the pre growing logisticall in the absence of predators. The effect of pre s refges and pre stage-strctre on the dnamical behavior of the food web model is investigated theoreticall as well as nmericall. II. The mathematical model Consider the food web model consisting of two predators-stage strctre pre in which the pre species growth logisticall in the absence of predation while the predators deca exponentiall in the absence of pre species. It is assmed that the pre poplation divides into two compartments: immatre pre poplation N (t) that represents the poplation size at time t and matre pre poplation N (t) which denotes to poplation size at time t. Frthermore the poplation size of the first predator at time t is denoted b N 3 (t) while N (t) represents the poplation size of second predator at time t. Now in order to formlate the dnamics of sch sstem the following assmptions are considered :. The immatre pre depends completel in its feeding on the matre pre that growth logisticall with intrinsic growth rate α > and carring capacit k >. The immatre pre individals grown p and becomes matre pre individals with grown p rate β >. However the matre pre facing death with natral death rate d >.. There is tpe of protection of the pre species from facing predation b first and second predators with refge rate constant m ). 3. The first and second predators consmed the matre pre individals onl according to the Lotka-Voltera tpe of fnctional response with predation rates c > and c > respectivel and contribte a portion of sch food with conversion rates < e < and < e < respectivel. Moreover there is an enter specific competition between these two predators with competition force rate c 3 > and c > respectivel. Finall in the absence of food the first and second predators facing death with natral death rate d > and d 3 >. Therefore the dnamics of this model can be represented b the set of first order nonlinear differential eqations: dn = α N N K β N dn = β N d N c m N N 3 c m N N dn 3 = d N 3 + e c m N N 3 c 3 N 3 N dn = d 3 N + e c m N N c N 3 N with initial conditions N i (). Note that the above proposed model has thirteen parameters in all which make the analsis difficlt. So in order to simplif the sstem the nmber of parameters is redced b sing the following dimensionless variables and parameters : t = α T = β α = d α 3 = d α = e c K α 5 = c 3 c 6 = d 3 α 7 = e c K α 8 = c c x = N = N z = c N 3 w = c N. K K α α Then the non-dimensional form of sstem can be written as : dx = x x = x f x z w d = x m z m w = f x z w dz = z 3 + m 5 w = z f 3 x z w dw = w m 8 z = w f x z w with x z and w. It is observed that the nmber of parameters have been redced from thirteen in the sstem to eight in the sstem.obviosl the interaction fnctions of the sstem are continos and have continos partial derivatives on the following positive for dimensional space. R + = x z w R x z w. Therefore these fnctions are DOI:.979/ Page

3 Stabilit analsis of two predator-one stage-strctred pre model incorporating a pre refge lipschitzian on R + and hence the soltion of the sstem exists and is niqe. Frther all the soltions of sstem with non-negative initial conditions are niforml bonded as shown in the following theorem. Theorem : All the soltions of sstem which initiate in R + are niforml bonded. Proof: Let x t t z t w t be an soltion of the sstem with non-negative initial condition x z w R +. Now according to the first eqation of sstem we have : dx = x. So b sing the comparison theorem on the above differential ineqalit with the initial point x = x we get : x t + x e t. Ths lim t x t and hence sp x t t > >. Now define the fnction : M t = x t + t + z t + w t and 7 then taken the time derivative of M t along the soltion of the sstem. we get : dm + x s M where s = min dm 3 6. Then + s M H where H = +. Again b solving this differential ineqalit for the initial vale M = M we get : M t H + M s H e st. Then lim s t M t H.So M t H s s of sstem are niforml bonded and the proof is complete. t >.Hence all the soltions III. The existence of eqilibrim points In this section the existence of all possible eqilibrim points of sstem is discssed. It is observed that sstem has at most five eqilibrim points which are mentioned in the following : The eqilibrim point E = which known as the vanishing point is alwas exists. The first eqilibrim point E = x where = and x = exists niqel in Int. R + (Interior of R + ) of x plane nder the following necessar and sfficient condition : < 3 The first three species eqilibrim point E = x z where x = 3 m m 3 m = 3 and z = m 3 3 exists niqel in Int. R m m + of xz spacender the following necessar and sfficient condition : 3 < min m m The second three species eqilibrim point E 3 = x w where x = = 6 7 m 6 7 m 7 m 6 7 m and w = 7 m 6 7 m exists niqel in Int.R + 3 of xw space nder the following necessar and sfficient condition : 6 < min 7 m 7 m 5 Finall the positive eqilibrim point E = x z w where x = DOI:.979/ Page = m + 3 m m + m z = 7 m 6 and w = m 3 exists in Int.R nder the 5 5 following necessar and sfficient conditions : + 7 m + m > m + 3 m 6 a m + 6 m + 3 m > m + m 6 b m + 6 m + 3 m > m + m 6 c IV. Local stabilit analsis In this section the local stabilit analsis of sstem arond each of the above eqilibrim points are discssed throgh compting the Jacobian matrix J x z w of sstem at each of them which given b : J = a ij where a = a = a 3 = a = a = a = m z m w a 3 = m a = m a 3 = a 3 = m z a 33 = 3 + m 5 w a 3 = 5 z a = a = 7 m w a 3 = 8 w a = m 8 z. The Local stabilit analsis at E The Jacobian matrix of sstem at E can be written as : J E = 3 6 Then the characteristic eqation of J E is given b : λ + A λ + A 3 λ 6 λ =

4 Stabilit analsis of two predator-one stage-strctred pre model incorporating a pre refge where A = + A =. So either 3 λ 6 λ = 7 a which gives two of the eigenvales of J E b : λ z = 3 < and λ w = 6 < Or λ + A λ + A = 7 b which gives the other two eigenvales of J E b : λ x = A + A A and λ = A A A Therefore if the following condition holds : > 7 c E is locall asmptoticall stable in the R +. However it is a saddle point otherwise. The Local stabilit analsis at E The Jacobian matrix of sstem at E can be written as : J E = m m 3 + m m Then the characteristic eqation of J E is given b : λ + A λ + A 3 + m λ m λ = where A = + and A = + So either 3 + m λ m λ = 8 a which gives two of the eigenvales of J E b : λ z = 3 + m and λ w = m Or λ + A λ + A = 8 b which gives the other two eigenvales of J E b : λ x = A holds : + A A and λ = A < < min 3 m 6 7 m A A.Therefore if the following condition Under condition 3. E is locall asmptoticall stable in the R +. However it is a saddle point otherwise. The Local stabilit analsis at E The Jacobian matrix of sstem at E can be written as : J E = b ij where : b = < b = b 3 = b = b = > b = m z < b 3 = m < b = m < b 3 = b 3 = m > b 33 = 3 + m b 3 = 5 z < b = b = b 3 = b = m 8 z. Then the characteristic eqation of J E is given b : λ 3 + A λ + A λ + A m 8 z λ = where 3 A = + m A = m + 3 m m 3 m A 3 = 3 m 3. m So either m 8 z λ = 9 a Or λ 3 + A λ + A λ + A 3 = 9 b Hence from eqation.9 a we obtain that : λ w = m 8 z which is negative provided that : 7 m < z 9 c On the other hand b sing Roth-Hawirtiz criterion eqation 9 b has roots ( eigenvales ) with negative real parts if and onl if : A > A 3 > and = A A A 3 >. Now direct comptation gives that : = 3 m m + 3 m 3 + m m So > nder the following condition : m m + 3 > 3 + m Now it is eas to verif that A > and A 3 > nder condition.then all the eigenvales λ x λ and λ z of eqation 9 b have negative real parts. So E is locall asmptoticall stable if and onl if conditions 9 c and are hold. However it is a saddle point otherwise. The Local stabilit analsis at E 3 The Jacobian matrix of sstem at E 3 can be written as : J E 3 = c ij where c = < c = c 3 = c = c = > c = m w > c 3 = m > c = m < c 3 = c 3 = c 33 = 3 + m 5 w DOI:.979/ Page 8 c

5 Stabilit analsis of two predator-one stage-strctred pre model incorporating a pre refge c 3 = c = c = 7 m w > c 3 = 8 w < c = m. Then the characteristic eqation of J E 3 is given b : λ 3 + B λ + B λ + B m 5 w λ = where 6 B = + 7 m B = 7 m + 7 m m 6 7 m B 3 = 6 7 m m 6. 7 m 7 m while Δ = B B B 3 = 6 7 m m 7 m m 7 m So either 3 + m 5 w λ = a Or λ 3 + B λ + B λ + B 3 = b From eqation a we obtain that : λ 3z = 3 + m 5 w which is negative provided that: m < w On the other hand it is eas to verif that B > and B 3 > nder condition 5 while > nder the following condition : 7 m m > m 3 Then all the eigenvales λ 3x λ 3 and λ 3w of eqation b have negative real parts. So E 3 is locall asmptoticall stable if and onl if conditions and 3 are hold. However it is a saddle point otherwise. Theorem : Assme that the positive eqilibrim point E = x z w of sstem exists in IntR +. Then it is locall asmptoticall stable provided that the following conditions hold : P < 3 P P a P 3 < 3 P P 33 b P < 3 P P P 33 P < P 3 Proof : It is eas to verif that the linearized sstem of sstem can be written as : dx = dr = J E R here X = x z w and R = r r r 3 r t where r = x x r = x x r 3 = x 3 x 3 and r = x x. Moreover J E = d ij where d = d = d 3 = d = d = d = m m w d 3 = m d = m d 3 = d 3 = m d 33 = 3 + m 5 w d 3 = 5 z d = d = 7 m w d 3 = 8 w d = m 8 z. Now consider the following positive definite fnction : V = r + r + r 3 + r. It is clearl that V R + R and is a C positive definite fnction. Now b differentiating V with respect to time t and doing some algebraic maniplation gives that : dv = P r + P r r P r + P 3 r r 3 + P r r P 33 r 3 + P 3 r 3 r P r where P = P = + P = + m z + m w P 3 = m z P = m 7 w P 33 = 3 m + 5 w P 3 = 5 z 8 w P = 6 7 m + 8 z. Now it is eas to verif that the above set of conditions garantee the qadratic terms give below : dv P r P 3 r P 3 r P 33 r 3 P 3 r P r P 33 r 3 + P r So dv is negative definite and hence V is a Lapnov fnction.ths E is locall asmptoticall stable and the proof is complete. V. Global stabilit analsis In this section the global stabilit analsis for the eqilibrim points which are locall asmptoticall stable of sstem is stdied analticall with the help of Lapnov method as shown in the following theorems. c d DOI:.979/ Page

6 Stabilit analsis of two predator-one stage-strctred pre model incorporating a pre refge Theorem 3 : Assme that the eqilibrim point E = of sstem is locall asmptoticall stable in the R +. Then the eqilibrim point E of sstem is globall asmptoticall stable. Proof: Consider the following fnction : V x z w = c x + c + c 3 z + c w where c c c 3 and c are positive constants to be determine.clearl V : R + R is a C positive definite fnction. Now b differentiating V with respect to time t and doing some algebraic maniplation gives that : dv = c + c c x c + c 3 c m z c + c 7 c m w c 3 3 z c 6 w c c 8 w z. B choosing c = c = c 3 = c = dv we get : dv 7. Then we obtain that is negative definite and hence V is a Lapnov fnction. Ths E is globall asmptoticall stable and the proof is complete. Theorem Assme that the eqilibrim point E = x of sstem is locall asmptoticall stable in the Int R + Then E is globall asmptoticall stable on an region Ω Int R + that satisfies the following conditions : + + x + m m x < x + m x x < x x Proof: Consider the following fnction : x m V x z w = c x x x ln x + c x ln + c 3 z + c w where c c c 3 and c are positive constants to be determine.clearl V : R + R is a C positive definite fnction. Now b differentiating V with respect to time t and doing some algebraic maniplation gives that : dv = c x x + c x c + + c x x c x x x c x +c x x c m z c m w c 3 3 z +c 3 m c 6 w + c 7 m w c c 8 w z. B choosing c = c = c m 3 = c = we get : 3 6 dv x x 6 7 m 6 x m w So according to condition 8 c we obtain that : dv DOI:.979/ Page + x x xx x x 3 m 3 z 5 a 5 b 5 c x + x x m However conditions 5 a and 5 b garantee the completeness of the qadratic term between x and. So if condition 5 c holds then we obtain that is negative definite on the region Ω and hence V is a Lapnov fnction defined on the region Ω. Ths E is globall asmptoticall stable on the region Ω and the proof is complete. Theorem 5 : Assme that the eqilibrim point E = x z of sstem is locall asmptoticall stable in IntR + 3. Then E is globall asmptoticall stable on an region Ω Int R + 3 that satisfied the following conditions : x + + x + x < x + x x < x x x x dv 6 a 6 b 6 c.

7 Stabilit analsis of two predator-one stage-strctred pre model incorporating a pre refge In addition that the following condition holds : 5 z + m < 6 7 Proof: Consider the following fnction : V 3 x z w = c x x x ln + c ln + c 3 z z z ln z + c z w where c c c 3 and c are positive constants to be determine.clearl V 3 : R + R is a C positive definite fnction. Now b differentiating V 3 with respect to time t and doing some algebraic maniplation gives that : dv 3 = c x x + c c + + c x x + c x x x x c c m z z c m w + c 3 m z z c 3 5 z z w c 6 w + c 7 m w c 8 w z. B choosing c = c = c 3 = c = we get : 7 dv 3 x x x Now according to condition 6 d we obtain that : + x x 6 7 5z m w DOI:.979/ Page dv 3 x x x + 6 d x x. However conditions 6 a and 6 b garantee the completeness of the qadratic term between x and. So if condition 6 c holds. Therefore dv 3 is negative on the region Ω and hence V 3 is a Lapnov fnction defined on the region Ω. Ths E is globall asmptoticall stable and the proof is complete. Theorem 6 : Assme that the eqilibrim point E 3 = x w of sstem is locall asmptoticall 3 3 stable in Int R +.Then E 3 is globall asmptoticall stable on an region Ω 3 Int R + that satisfies the following conditions : + + x < x + x x < + x x x x In addition that the following condition holds : 8 w + m < 3 7 Proof: Consider the following fnction : V x z w = c x x x ln + c ln + c 3 z + c w w w ln w w where c c c 3 and c are positive constants to be determine.clearl V : R + R is a C positive definite fnction. Now b differentiating V with respect to time t and doing some algebraic maniplation gives that : dv = c x x + c x c + + c x x + c x x x x c c m z c m w w c 3 3 z + c 3 m z c 3 5 w z + c 7 m w w c 8 w w z. B choosing c = c = c 3 = c = we get : 7 dv x x x m Now according to condition 7 d we obtain that : dv 3 m 8 7 w z + 7 a 7 b 7 c 7 d x x x x x + m x x. However conditions 7 a and 7 b garantee the completeness of the qadratic term between x and.so if condition 7 c holds then we obtain that is negative definite on the region Ω 3 and hence V is a Lapnov fnction defined on the region Ω 3. Ths E 3 is globall asmptoticall stable on the region Ω 3 and the proof is complete. dv

8 Stabilit analsis of two predator-one stage-strctred pre model incorporating a pre refge Theorem 7 : Assme that the eqilibrim point E = x z w of sstem is locall asmptoticall stable in the R +. Then E is globall asmptoticall stable on an region Ω Int R + that satisfies the following conditions : + + x + x < x + 8 b x x w z + w z < β where 8 c β = x x Proof: Consider the following fnction : x 8 a V 5 x z w = c x x x ln + c ln + c 3 z z z ln z z + c w w w ln w w where c c c 3 and c are positive constants to be determine.clearl V 5 : R + R is a C positive definite fnction. Now b differentiating V 5 with respect to time t and doing some algebraic maniplation gives that : dv 5 = c x x + c x c + x + c x x c x + c x x c 8 + c 3 w w z z + c 7 c m w w + c 3 c m z z B choosing c = c = c 3 = c = we get : 7 dv 5 x x x + x x w z + w z However conditions 8 a and 8 b garantee the completeness of the qadratic term between x and. So if condition 8 c holds then we obtain that dv 5 is negative definite on the region Ω and hence V 5 is a Lapnov fnction defined on the region Ω. Ths E is globall asmptoticall stable on the region Ω and the proof is complete. VI. Nmerical simlation In this section the dnamical behavior of sstem is stdied nmericall for different sets of parameters and different sets of initial points. The objectives of this std are : first investigate the effect of varing the vale of each parameter on the dnamical behavior of sstem and second confirm or obtained analtical reslts. It is observed that for the following set of hpothetical parameters that satisfies stabilit conditions of the positive eqilibrim point sstem has a globall asmptoticall stable positive eqilibrim point as shown in Fig.. =. =. 3 =. =.8 5 =. 6 =. 7 =.8 8 =. m =.8 9 DOI:.979/ Page

9 Poplation Poplation Stabilit analsis of two predator-one stage-strctred pre model incorporating a pre refge Fig. : Time series of the soltion of sstem that started from for different initial points and.7... for the data given b Eq..9. a trajectories of x as a fnction of time b trajectories of as a fnction of time c trajectories of z as a fnction of time d trajectories of w as a fnction of time. Clearl Fig. shows that sstem has a globall asmptoticall stable as the soltion of sstem approaches asmptoticall to the positive eqilibrim point E = starting from for different initial points and this is confirming or obtained analtical reslts..now in order to discss the effect of the parameters vales of sstem on the dnamical behavior of the sstem the sstem is solved nmericall for the data given in Eq. 9 with varing one parameter at each time. It is observed that for the data as given in Eq. 9 with..9 the soltion of sstem approaches asmptoticall to the positive eqilibrim point as shown in Fig immatre pre matre pre first predator second predator Time Fig. : Time series of the soltion of sstem for the data given b Eq. 9 which approaches to in the interior of R +. B varing the parameter and keeping the rest of parameters vales as in Eq. 9 it is observed that for.. the soltion of sstem approaches asmptoticall to a positive eqilibrim point E while for.5.9 the soltion of sstem approaches asmptoticall to E = x in the interior of the positive qadrant of x plane as shown in Fig immatre pre matre pre first predator second predator Time Fig. 3 : Times series of the soltion of sstem for the data given b Eq. 9 which approaches to.97.8 in the interior of the positive qadrant of x plane. On the other hand varing the parameter 3 keeping the rest of parameters vales as in Eq. 9 it is observed that for. 3.9 sstem approaches asmptoticall to E = x in the interior of the positive qadrant of x plane.moreover varing the parameter and keeping the rest of parameters vales as in Eq. 9 it is observed that for.. the soltion of sstem approaches asmptoticall to E = x in the interior of the positive qadrant of x plane while for.5.9 the soltion of sstem approaches asmptoticall to a positive eqilibrim point E.For the parameter. 5.9 and keeping the rest of parameters vales as in Eq. 9 showed that the soltion of sstem approaches asmptoticall to a positive eqilibrim point E.Moreover for the parameters vales given in Eq. 9 with. 6.9 the soltion of sstem approaches asmptoticall to a positive eqilibrim point E. For the parameters vales given in Eq. 9 with. 7.9 the soltion of sstem approaches asmptoticall to a positive eqilibrim point E. For the parameter. 8.9 and keeping the rest of parameters vales as in Eq. 9 showed that the soltion of sstem approaches DOI:.979/ Page

10 Poplation Poplation Poplation Stabilit analsis of two predator-one stage-strctred pre model incorporating a pre refge asmptoticall to a positive eqilibrim point E.For the parameters vale given in Eq. 9 and varing the parameter m in the rang. m.9 showed that the soltion of sstem approaches asmptoticall to a positive eqilibrim point E.For the parameters vales given in Eq. 9 with =.9 5 =. 7 =. and 8 =.8 the soltion of sstem approaches asmptoticall to E = x z in the interior of the positive qadrant of xz plane as shown in Fig...5 immatre pre matre pre first predator second predator Time Fig. : Time series of the soltion of sstem for the data given b Eq. 9 with =.9 5 =. 7 =. and 8 =.8 which approaches asmptoticall to in the interior of the positive qadrant of xz space. Moreover for the parameters vales given in Eq. 9 with =. 5 =.8 6 =. the soltion of sstem approaches asmptoticall to E 3 = x w in the interior of the positive qadrant of xw space as shown in Fig immatre pre matre pre first predator second predator Time Fig. 5 : Time series of the soltion of sstem for the data given b Eq. 9 with =. 5 =.8 6 =. which approaches asmptoticall to in the interior of the positive qadrant of xw space. Finall the dnamical behavior at the vanishing eqilibrim point E = is investigated b choosing = and keeping other parameters fixed as given in Eq. 9 and then the soltion of sstem is drawn in Fig immatre pre matre pre first predator second predator Time Fig. 6 : Time series of the soltion of sstem for the data given b Eq. 9 with = which approaches to. Obviosl Fig. 6 shows clearl the convergence of the soltion of sstem to the vanishing eqilibrim point E = when the parameters increase p to a specific vales. clearl the sed valed in Fig. 6 satisf the stabilit condition of the vanishing eqilibrim point. VII. Conclsion and discssion In this chapter we have considered a pre-predator sstem incorporating a stage strctre of pre with refge. It is assmed that the predator species pre pon the pre according to Lotka-Voltera tpe of fnctional response. The existence niqeness and bondedness of the soltion of the sstem are discssed. The existence of all possible eqilibrim points is stdied. The local and global dnamical behaviors of the sstem are stdied analticall as well as nmericall. Finall to nderstand the effect of varing each parameter on the global dnamics of sstem has been solved nmericall for a biological feasible set of hpothetical parameters vales and the following reslts are obtained :. For the set of hpothetical parameters vales given in Eq. 9 the sstem approaches asmptoticall to global stable positive eqilibrim point. DOI:.979/ Page

11 Stabilit analsis of two predator-one stage-strctred pre model incorporating a pre refge. It is observed that the sstem has no effect on the dnamical behavior for the data given in Eq. 9 with varing the parameter vale and the sstem still approaches to positive eqilibrim point. 3. As the natral death rate of matre pre increasing in the range. < <. and keeping other parameters fixed as in Eq. 9 then again the soltion of sstem approaches asmptoticall to the positive eqilibrim point.however increasing in the range.5 < <.9 will case extinction in the predators and the soltion of sstem approaches asmptoticall to E = x.. As the first predator natral death rate 3 increasing keeping the rest of parameters as in Eq. 9 then again the soltion of sstem approaches asmptoticall to E = x. It is observed that the natral death rate 6 of the second predator has the same effect as. 5. As the predation rate increasing in the range..7 cases extinction in the predators and the soltion of sstem approaches asmptoticall to E = x. However increasing in the range.5.9 then again the soltion of sstem approaches asmptoticall to the positive eqilibrim point. 6. As the competition rate 5 increasing keeping the rest of parameters as in Eq. 9 then again the soltion of sstem approaches asmptoticall to the positive eqilibrim point. It is observed that the competition rate 8 and the nmber of pres inside refge m have the same effect as. 7. As the predation rate 7 increasing in the range. 7.9 and keeping the rest of parameters as in Eq. 9 then again the soltion of sstem approaches asmptoticall to the positive eqilibrim point. References []. T. K. Kar and Ashim Batabal Persistence and stabilit of a two pre one predator International Jornal of Engineering Science and Technolog Vol. No. pp.7-9. []. Weiming Wang Hailing Wan and Zhenqing Li Chaotic behavior of a three-species beddington-tpe sstem with implsive pertrbations Chaos Soltion and Fractals [3]. Snita Gakkar Brahampal Singh and Raid Kamel Naji Dnamical behavior of two predators competing over a single pre BioSstems []. Jawdat Alebraheem and YahYa Ab-Hasan Presistence of predators in a two predators-one pre model with non-preiodic soltion App.Math.Scie.Vol.6 No [5]. Madhsdanan V. Vijaa S. and Gnasekaran M Impact of harvesting in three species food web model with two distinct fnctional response International Jornal of Innovative Research in Science Engineering and TechnologVol.3 Isse p [6]. R. K. Naji and I.H. Kasim The dnamics of food web model with defensive switching propert Nonlinear Analsis: Modelling and Control Vol.3 No [7]. B-Dbe and R.K. Upadha Persistence and extinction of one-pre and two-predators sstem Nonlinear Analsis: Modeling and Control Vol.9 No. ew [8]. Sze-Bi Hs Shigi Ran and Ting-Hi Yang Analsis of three species Lotka-Voltera food web models with omnivor J. Math. Anal. Applic [9].. Manard Smith Models in ecolog Cambridge Universit Cambridge 97. []. M. P. Hassell The dnamics of arthropod predator-pre sstems Princeton Universit Princeton NJ 978. []. T. K. Kar Stabilit analsis of a per-predator model incorporating a pre refge Commnications Nonlinear Science and Nmerical Simlation []. Vlastimil Krivan On the Gase predator-pre model with a refge: A fresh look at the histor Jornal of Theoretical Biolog [3]. R. J. Talor Predation Chapman and Hall NewYork 98. []. Xiao lei Y and Fqin Sn Global dnamics of a predator-pre model incorporating a constant pre refge Electronic Jornal of differential eqations Vol.3 No. 3 pp.-8. [5]. Zhihi Ma Wenlong Li Y. ZhaoWenting Wang Hi Zhang and Zizhen Li Effects of pre refges on a predator-pre model with a class of fnctional responses: The role of refges Mathematical BioSciences [6]. Kai Hong and Peixam Weng Stabilit and traveling waves of diffsive predator-pre model with age-strctre and nonlocal effect Jornal of Applied Analsis and Comptation Vol. No. p [7]. Ri X Global stabilit and Hopf bifrcation of a predator-pre model with stage strctre and delaed predator response Nonlinear Dnamics Vol.67 Isse pp [8]. O. P. Misra Poonam Sinha and Chhatrapal Singh Stabilit and bifrcation analsis of a pre-predator model with age based predation Applied Mathematical Modelling [9]. Ye Kaili and Song XinY Predator-pre sstem with stage strctre and dela Appl. Math. J. Chinese Univ. Ser. B 8() []. Pal-Georgesc and Ying-Hen Hsieh Global dnamics of a predator-pre model with stage strctre for the predator SIAMJ.App.Math.Vol.67 No.5 7 pp DOI:.979/ Page

Research Article Permanence of a Discrete Predator-Prey Systems with Beddington-DeAngelis Functional Response and Feedback Controls

Research Article Permanence of a Discrete Predator-Prey Systems with Beddington-DeAngelis Functional Response and Feedback Controls Hindawi Pblishing Corporation Discrete Dynamics in Natre and Society Volme 2008 Article ID 149267 8 pages doi:101155/2008/149267 Research Article Permanence of a Discrete Predator-Prey Systems with Beddington-DeAngelis

More information

Dynamics of a Holling-Tanner Model

Dynamics of a Holling-Tanner Model American Jornal of Engineering Research (AJER) 07 American Jornal of Engineering Research (AJER) e-issn: 30-0847 p-issn : 30-0936 Volme-6 Isse-4 pp-3-40 wwwajerorg Research Paper Open Access Dynamics of

More information

A Decomposition Method for Volume Flux. and Average Velocity of Thin Film Flow. of a Third Grade Fluid Down an Inclined Plane

A Decomposition Method for Volume Flux. and Average Velocity of Thin Film Flow. of a Third Grade Fluid Down an Inclined Plane Adv. Theor. Appl. Mech., Vol. 1, 8, no. 1, 9 A Decomposition Method for Volme Flx and Average Velocit of Thin Film Flow of a Third Grade Flid Down an Inclined Plane A. Sadighi, D.D. Ganji,. Sabzehmeidani

More information

Conditions for Approaching the Origin without Intersecting the x-axis in the Liénard Plane

Conditions for Approaching the Origin without Intersecting the x-axis in the Liénard Plane Filomat 3:2 (27), 376 377 https://doi.org/.2298/fil7276a Pblished by Faclty of Sciences and Mathematics, University of Niš, Serbia Available at: http://www.pmf.ni.ac.rs/filomat Conditions for Approaching

More information

Homotopy Perturbation Method for Solving Linear Boundary Value Problems

Homotopy Perturbation Method for Solving Linear Boundary Value Problems International Jornal of Crrent Engineering and Technolog E-ISSN 2277 4106, P-ISSN 2347 5161 2016 INPRESSCO, All Rights Reserved Available at http://inpressco.com/categor/ijcet Research Article Homotop

More information

ON PREDATOR-PREY POPULATION DYNAMICS UNDER STOCHASTIC SWITCHED LIVING CONDITIONS

ON PREDATOR-PREY POPULATION DYNAMICS UNDER STOCHASTIC SWITCHED LIVING CONDITIONS ON PREDATOR-PREY POPULATION DYNAMICS UNDER STOCHASTIC SWITCHED LIVING CONDITIONS Aleksandrs Gehsbargs, Vitalijs Krjacko Riga Technical University agehsbarg@gmail.com Abstract. The dynamical system theory

More information

A Single Species in One Spatial Dimension

A Single Species in One Spatial Dimension Lectre 6 A Single Species in One Spatial Dimension Reading: Material similar to that in this section of the corse appears in Sections 1. and 13.5 of James D. Mrray (), Mathematical Biology I: An introction,

More information

Nonlocal Symmetries and Interaction Solutions for Potential Kadomtsev Petviashvili Equation

Nonlocal Symmetries and Interaction Solutions for Potential Kadomtsev Petviashvili Equation Commn. Theor. Phs. 65 (16) 31 36 Vol. 65, No. 3, March 1, 16 Nonlocal Smmetries and Interaction Soltions for Potential Kadomtsev Petviashvili Eqation Bo Ren ( ), Jn Y ( ), and Xi-Zhong Li ( ) Institte

More information

Mathematical Analysis of Nipah Virus Infections Using Optimal Control Theory

Mathematical Analysis of Nipah Virus Infections Using Optimal Control Theory Jornal of Applied Mathematics and Physics, 06, 4, 099- Pblished Online Jne 06 in SciRes. http://www.scirp.org/jornal/jamp http://dx.doi.org/0.436/jamp.06.464 Mathematical Analysis of Nipah Virs nfections

More information

1. State-Space Linear Systems 2. Block Diagrams 3. Exercises

1. State-Space Linear Systems 2. Block Diagrams 3. Exercises LECTURE 1 State-Space Linear Sstems This lectre introdces state-space linear sstems, which are the main focs of this book. Contents 1. State-Space Linear Sstems 2. Block Diagrams 3. Exercises 1.1 State-Space

More information

1 Introduction. r + _

1 Introduction. r + _ A method and an algorithm for obtaining the Stable Oscillator Regimes Parameters of the Nonlinear Sstems, with two time constants and Rela with Dela and Hsteresis NUŢU VASILE, MOLDOVEANU CRISTIAN-EMIL,

More information

2 Faculty of Mechanics and Mathematics, Moscow State University.

2 Faculty of Mechanics and Mathematics, Moscow State University. th World IMACS / MODSIM Congress, Cairns, Astralia 3-7 Jl 9 http://mssanz.org.a/modsim9 Nmerical eamination of competitie and predator behaior for the Lotka-Volterra eqations with diffsion based on the

More information

B-469 Simplified Copositive and Lagrangian Relaxations for Linearly Constrained Quadratic Optimization Problems in Continuous and Binary Variables

B-469 Simplified Copositive and Lagrangian Relaxations for Linearly Constrained Quadratic Optimization Problems in Continuous and Binary Variables B-469 Simplified Copositive and Lagrangian Relaxations for Linearly Constrained Qadratic Optimization Problems in Continos and Binary Variables Naohiko Arima, Snyong Kim and Masakaz Kojima October 2012,

More information

Study on the impulsive pressure of tank oscillating by force towards multiple degrees of freedom

Study on the impulsive pressure of tank oscillating by force towards multiple degrees of freedom EPJ Web of Conferences 80, 0034 (08) EFM 07 Stdy on the implsive pressre of tank oscillating by force towards mltiple degrees of freedom Shigeyki Hibi,* The ational Defense Academy, Department of Mechanical

More information

Finite Element Analysis of Heat and Mass Transfer of a MHD / Micropolar fluid over a Vertical Channel

Finite Element Analysis of Heat and Mass Transfer of a MHD / Micropolar fluid over a Vertical Channel International Jornal of Scientific and Innovative Mathematical Research (IJSIMR) Volme 2, Isse 5, Ma 214, PP 515-52 ISSN 2347-37X (Print) & ISSN 2347-3142 (Online) www.arcjornals.org Finite Element Analsis

More information

Subcritical bifurcation to innitely many rotating waves. Arnd Scheel. Freie Universitat Berlin. Arnimallee Berlin, Germany

Subcritical bifurcation to innitely many rotating waves. Arnd Scheel. Freie Universitat Berlin. Arnimallee Berlin, Germany Sbcritical bifrcation to innitely many rotating waves Arnd Scheel Institt fr Mathematik I Freie Universitat Berlin Arnimallee 2-6 14195 Berlin, Germany 1 Abstract We consider the eqation 00 + 1 r 0 k2

More information

FREQUENCY DOMAIN FLUTTER SOLUTION TECHNIQUE USING COMPLEX MU-ANALYSIS

FREQUENCY DOMAIN FLUTTER SOLUTION TECHNIQUE USING COMPLEX MU-ANALYSIS 7 TH INTERNATIONAL CONGRESS O THE AERONAUTICAL SCIENCES REQUENCY DOMAIN LUTTER SOLUTION TECHNIQUE USING COMPLEX MU-ANALYSIS Yingsong G, Zhichn Yang Northwestern Polytechnical University, Xi an, P. R. China,

More information

Control Using Logic & Switching: Part III Supervisory Control

Control Using Logic & Switching: Part III Supervisory Control Control Using Logic & Switching: Part III Spervisor Control Ttorial for the 40th CDC João P. Hespanha Universit of Sothern California Universit of California at Santa Barbara Otline Spervisor control overview

More information

1 Differential Equations for Solid Mechanics

1 Differential Equations for Solid Mechanics 1 Differential Eqations for Solid Mechanics Simple problems involving homogeneos stress states have been considered so far, wherein the stress is the same throghot the component nder std. An eception to

More information

Incompressible Viscoelastic Flow of a Generalised Oldroyed-B Fluid through Porous Medium between Two Infinite Parallel Plates in a Rotating System

Incompressible Viscoelastic Flow of a Generalised Oldroyed-B Fluid through Porous Medium between Two Infinite Parallel Plates in a Rotating System International Jornal of Compter Applications (97 8887) Volme 79 No., October Incompressible Viscoelastic Flow of a Generalised Oldroed-B Flid throgh Poros Medim between Two Infinite Parallel Plates in

More information

A Radial Basis Function Method for Solving PDE Constrained Optimization Problems

A Radial Basis Function Method for Solving PDE Constrained Optimization Problems Report no. /6 A Radial Basis Fnction Method for Solving PDE Constrained Optimization Problems John W. Pearson In this article, we appl the theor of meshfree methods to the problem of PDE constrained optimization.

More information

QUANTILE ESTIMATION IN SUCCESSIVE SAMPLING

QUANTILE ESTIMATION IN SUCCESSIVE SAMPLING Jornal of the Korean Statistical Society 2007, 36: 4, pp 543 556 QUANTILE ESTIMATION IN SUCCESSIVE SAMPLING Hosila P. Singh 1, Ritesh Tailor 2, Sarjinder Singh 3 and Jong-Min Kim 4 Abstract In sccessive

More information

Boundary Layer Flow and Heat Transfer over a. Continuous Surface in the Presence of. Hydromagnetic Field

Boundary Layer Flow and Heat Transfer over a. Continuous Surface in the Presence of. Hydromagnetic Field International Jornal of Mathematical Analsis Vol. 8, 4, no. 38, 859-87 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/.988/ijma.4.4789 Bondar Laer Flow and Heat Transfer over a Continos Srface in the Presence

More information

Study of the diffusion operator by the SPH method

Study of the diffusion operator by the SPH method IOSR Jornal of Mechanical and Civil Engineering (IOSR-JMCE) e-issn: 2278-684,p-ISSN: 2320-334X, Volme, Isse 5 Ver. I (Sep- Oct. 204), PP 96-0 Stdy of the diffsion operator by the SPH method Abdelabbar.Nait

More information

The spreading residue harmonic balance method for nonlinear vibration of an electrostatically actuated microbeam

The spreading residue harmonic balance method for nonlinear vibration of an electrostatically actuated microbeam J.L. Pan W.Y. Zh Nonlinear Sci. Lett. Vol.8 No. pp.- September The spreading reside harmonic balance method for nonlinear vibration of an electrostatically actated microbeam J. L. Pan W. Y. Zh * College

More information

Pankaj Charan Jena 1, Dayal R. Parhi 2, G. Pohit 3. Pankaj Charan Jena et al. / International Journal of Engineering and Technology (IJET)

Pankaj Charan Jena 1, Dayal R. Parhi 2, G. Pohit 3. Pankaj Charan Jena et al. / International Journal of Engineering and Technology (IJET) Theoretical, Nmerical (FEM) and Experimental Analsis of composite cracked beams of different bondar conditions sing vibration mode shape crvatres Pankaj Charan Jena, Daal R. Parhi, G. Pohit 3 Department

More information

BIFURCATIONS OF TRAVELING WAVE SOLUTIONS FOR A GENERALIZED CAMASSA-HOLM EQUATION

BIFURCATIONS OF TRAVELING WAVE SOLUTIONS FOR A GENERALIZED CAMASSA-HOLM EQUATION Jornal of Alied Analsis and Comtation Volme 8, Nmber 6, December 8, 85 86 Website:htt://jaac.ijornal.cn DOI:.98/8.85 BIFURCATIONS OF TRAVELING WAVE SOLUTIONS FOR A GENERALIZED CAMASSA-HOLM EQUATION Minzhi

More information

Nonlinear predictive control of dynamic systems represented by Wiener Hammerstein models

Nonlinear predictive control of dynamic systems represented by Wiener Hammerstein models Nonlinear Dn (26) 86:93 24 DOI.7/s7-6-2957- ORIGINAL PAPER Nonlinear predictive control of dnamic sstems represented b Wiener Hammerstein models Maciej Ławrńcz Received: 7 December 25 / Accepted: 2 Jl

More information

Math 263 Assignment #3 Solutions. 1. A function z = f(x, y) is called harmonic if it satisfies Laplace s equation:

Math 263 Assignment #3 Solutions. 1. A function z = f(x, y) is called harmonic if it satisfies Laplace s equation: Math 263 Assignment #3 Soltions 1. A fnction z f(x, ) is called harmonic if it satisfies Laplace s eqation: 2 + 2 z 2 0 Determine whether or not the following are harmonic. (a) z x 2 + 2. We se the one-variable

More information

Chapter 3. Preferences and Utility

Chapter 3. Preferences and Utility Chapter 3 Preferences and Utilit Microeconomics stdies how individals make choices; different individals make different choices n important factor in making choices is individal s tastes or preferences

More information

Robust Tracking and Regulation Control of Uncertain Piecewise Linear Hybrid Systems

Robust Tracking and Regulation Control of Uncertain Piecewise Linear Hybrid Systems ISIS Tech. Rept. - 2003-005 Robst Tracking and Reglation Control of Uncertain Piecewise Linear Hybrid Systems Hai Lin Panos J. Antsaklis Department of Electrical Engineering, University of Notre Dame,

More information

Complex Variables. For ECON 397 Macroeconometrics Steve Cunningham

Complex Variables. For ECON 397 Macroeconometrics Steve Cunningham Comple Variables For ECON 397 Macroeconometrics Steve Cnningham Open Disks or Neighborhoods Deinition. The set o all points which satis the ineqalit

More information

Approximate Solution of Convection- Diffusion Equation by the Homotopy Perturbation Method

Approximate Solution of Convection- Diffusion Equation by the Homotopy Perturbation Method Gen. Math. Notes, Vol. 1, No., December 1, pp. 18-114 ISSN 19-7184; Copyright ICSRS Pblication, 1 www.i-csrs.org Available free online at http://www.geman.in Approximate Soltion of Convection- Diffsion

More information

A Model-Free Adaptive Control of Pulsed GTAW

A Model-Free Adaptive Control of Pulsed GTAW A Model-Free Adaptive Control of Plsed GTAW F.L. Lv 1, S.B. Chen 1, and S.W. Dai 1 Institte of Welding Technology, Shanghai Jiao Tong University, Shanghai 00030, P.R. China Department of Atomatic Control,

More information

Classify by number of ports and examine the possible structures that result. Using only one-port elements, no more than two elements can be assembled.

Classify by number of ports and examine the possible structures that result. Using only one-port elements, no more than two elements can be assembled. Jnction elements in network models. Classify by nmber of ports and examine the possible strctres that reslt. Using only one-port elements, no more than two elements can be assembled. Combining two two-ports

More information

Chapter 2 Difficulties associated with corners

Chapter 2 Difficulties associated with corners Chapter Difficlties associated with corners This chapter is aimed at resolving the problems revealed in Chapter, which are cased b corners and/or discontinos bondar conditions. The first section introdces

More information

FOUNTAIN codes [3], [4] provide an efficient solution

FOUNTAIN codes [3], [4] provide an efficient solution Inactivation Decoding of LT and Raptor Codes: Analysis and Code Design Francisco Lázaro, Stdent Member, IEEE, Gianligi Liva, Senior Member, IEEE, Gerhard Bach, Fellow, IEEE arxiv:176.5814v1 [cs.it 19 Jn

More information

Chaotic and Hyperchaotic Complex Jerk Equations

Chaotic and Hyperchaotic Complex Jerk Equations International Jornal of Modern Nonlinear Theory and Application 0 6-3 http://dxdoiorg/0436/ijmnta000 Pblished Online March 0 (http://wwwscirporg/jornal/ijmnta) Chaotic and Hyperchaotic Complex Jerk Eqations

More information

Modelling the Optimal Control of Transmission Dynamics of

Modelling the Optimal Control of Transmission Dynamics of Open Jornal of Epidemiology, 5, 5, 9-4 Pblished Online November 5 in SciRes http://wwwscirporg/jornal/ojepi http://dxdoiorg/46/ojepi5547 Modelling the Optimal Control of Transmission Dynamics of Mycobacterim

More information

Chapter 3 MATHEMATICAL MODELING OF DYNAMIC SYSTEMS

Chapter 3 MATHEMATICAL MODELING OF DYNAMIC SYSTEMS Chapter 3 MATHEMATICAL MODELING OF DYNAMIC SYSTEMS 3. System Modeling Mathematical Modeling In designing control systems we mst be able to model engineered system dynamics. The model of a dynamic system

More information

Wall treatment in Large Eddy Simulation

Wall treatment in Large Eddy Simulation Wall treatment in arge Edd Simlation David Monfort Sofiane Benhamadoche (ED R&D) Pierre Sagat (Université Pierre et Marie Crie) 9 novembre 007 Code_Satrne User Meeting Wall treatment in arge Edd Simlation

More information

Sources of Non Stationarity in the Semivariogram

Sources of Non Stationarity in the Semivariogram Sorces of Non Stationarity in the Semivariogram Migel A. Cba and Oy Leangthong Traditional ncertainty characterization techniqes sch as Simple Kriging or Seqential Gassian Simlation rely on stationary

More information

IT is well known that searching for travelling wave solutions

IT is well known that searching for travelling wave solutions IAENG International Jornal of Applied Mathematics 44: IJAM_44 2 A Modification of Fan Sb-Eqation Method for Nonlinear Partial Differential Eqations Sheng Zhang Ao-Xe Peng Abstract In this paper a modification

More information

Lotka Volterra Model with Time Delay

Lotka Volterra Model with Time Delay International Journal of Mathematics Research. ISSN 976-584 Volume 6, Number (4), pp. 5- International Research Publication House http://www.irphouse.com Lotka Volterra Model with Time Dela Tapas Kumar

More information

Safe Manual Control of the Furuta Pendulum

Safe Manual Control of the Furuta Pendulum Safe Manal Control of the Frta Pendlm Johan Åkesson, Karl Johan Åström Department of Atomatic Control, Lnd Institte of Technology (LTH) Box 8, Lnd, Sweden PSfrag {jakesson,kja}@control.lth.se replacements

More information

International Journal of Modern Engineering Research (IJMER) Vol. 3, Issue. 4, Jul - Aug pp ISSN:

International Journal of Modern Engineering Research (IJMER)   Vol. 3, Issue. 4, Jul - Aug pp ISSN: Vol. 3, sse. 4, Jl - Ag. 3 pp-89-97 SSN: 49-6645 Effect of Chemical Reaction and Radiation Absorption on Unstead Convective Heat and Mass Transfer Flow in a Vertical Channel with Oscillator Wall Temperatre

More information

Elastico-Viscous MHD Free Convective Flow Past an Inclined Permeable Plate with Dufour Effects in Presence of Chemical Reaction

Elastico-Viscous MHD Free Convective Flow Past an Inclined Permeable Plate with Dufour Effects in Presence of Chemical Reaction International Jornal of Engineering and Technical Research (IJETR) ISSN: 2321-0869 (O) 2454-4698 (P), Volme-3, Isse-8, Agst 2015 Elastico-Viscos MHD Free Convective Flow Past an Inclined Permeable Plate

More information

Lecture Notes On THEORY OF COMPUTATION MODULE - 2 UNIT - 2

Lecture Notes On THEORY OF COMPUTATION MODULE - 2 UNIT - 2 BIJU PATNAIK UNIVERSITY OF TECHNOLOGY, ODISHA Lectre Notes On THEORY OF COMPUTATION MODULE - 2 UNIT - 2 Prepared by, Dr. Sbhend Kmar Rath, BPUT, Odisha. Tring Machine- Miscellany UNIT 2 TURING MACHINE

More information

Approximate Solution for the System of Non-linear Volterra Integral Equations of the Second Kind by using Block-by-block Method

Approximate Solution for the System of Non-linear Volterra Integral Equations of the Second Kind by using Block-by-block Method Astralian Jornal of Basic and Applied Sciences, (1): 114-14, 008 ISSN 1991-8178 Approximate Soltion for the System of Non-linear Volterra Integral Eqations of the Second Kind by sing Block-by-block Method

More information

Home Range Formation in Wolves Due to Scent Marking

Home Range Formation in Wolves Due to Scent Marking Blletin of Mathematical Biology () 64, 61 84 doi:1.16/blm.1.73 Available online at http://www.idealibrary.com on Home Range Formation in Wolves De to Scent Marking BRIAN K. BRISCOE, MARK A. LEWIS AND STEPHEN

More information

Optimal Control of a Heterogeneous Two Server System with Consideration for Power and Performance

Optimal Control of a Heterogeneous Two Server System with Consideration for Power and Performance Optimal Control of a Heterogeneos Two Server System with Consideration for Power and Performance by Jiazheng Li A thesis presented to the University of Waterloo in flfilment of the thesis reqirement for

More information

Similarity Solution for MHD Flow of Non-Newtonian Fluids

Similarity Solution for MHD Flow of Non-Newtonian Fluids P P P P IJISET - International Jornal of Innovative Science, Engineering & Technology, Vol. Isse 6, Jne 06 ISSN (Online) 48 7968 Impact Factor (05) - 4. Similarity Soltion for MHD Flow of Non-Newtonian

More information

Gravitational Instability of a Nonrotating Galaxy *

Gravitational Instability of a Nonrotating Galaxy * SLAC-PUB-536 October 25 Gravitational Instability of a Nonrotating Galaxy * Alexander W. Chao ;) Stanford Linear Accelerator Center Abstract Gravitational instability of the distribtion of stars in a galaxy

More information

Applied Mathematics Letters

Applied Mathematics Letters Applied Mathematics Letters 23 (21 49 416 Contents lists available at ScienceDirect Applied Mathematics Letters jornal homepage: www.elsevier.com/locate/aml Exponential trichotomy and homoclinic bifrcation

More information

A Theory of Markovian Time Inconsistent Stochastic Control in Discrete Time

A Theory of Markovian Time Inconsistent Stochastic Control in Discrete Time A Theory of Markovian Time Inconsistent Stochastic Control in Discrete Time Tomas Björk Department of Finance, Stockholm School of Economics tomas.bjork@hhs.se Agatha Mrgoci Department of Economics Aarhs

More information

BLOOM S TAXONOMY. Following Bloom s Taxonomy to Assess Students

BLOOM S TAXONOMY. Following Bloom s Taxonomy to Assess Students BLOOM S TAXONOMY Topic Following Bloom s Taonomy to Assess Stdents Smmary A handot for stdents to eplain Bloom s taonomy that is sed for item writing and test constrction to test stdents to see if they

More information

Reducing Conservatism in Flutterometer Predictions Using Volterra Modeling with Modal Parameter Estimation

Reducing Conservatism in Flutterometer Predictions Using Volterra Modeling with Modal Parameter Estimation JOURNAL OF AIRCRAFT Vol. 42, No. 4, Jly Agst 2005 Redcing Conservatism in Fltterometer Predictions Using Volterra Modeling with Modal Parameter Estimation Rick Lind and Joao Pedro Mortaga University of

More information

Entropy ISSN

Entropy ISSN Entrop 3, 5, 56-518 56 Entrop ISSN 199-43 www.mdpi.org/entrop/ Entrop Generation Dring Flid Flow Between wo Parallel Plates With Moving Bottom Plate Latife Berrin Erba 1, Mehmet Ş. Ercan, Birsen Sülüş

More information

AMS subject classifications. 47N70, 47A48, 47A20, 47A56, 47A62, 93B28, 93C55, 93D15

AMS subject classifications. 47N70, 47A48, 47A20, 47A56, 47A62, 93B28, 93C55, 93D15 OPTIMAL INPUT-OUTPUT STABILIZATION OF INFINITE-DIMENSIONAL DISCRETE TIME-INVARIANT LINEAR SYSTEMS BY OUTPUT INJECTION MARK R. OPMEER AND OLOF J. STAFFANS Abstract. We std the optimal inpt-otpt stabilization

More information

Bäcklund transformation, multiple wave solutions and lump solutions to a (3 + 1)-dimensional nonlinear evolution equation

Bäcklund transformation, multiple wave solutions and lump solutions to a (3 + 1)-dimensional nonlinear evolution equation Nonlinear Dyn 7 89:33 4 DOI.7/s7-7-38-3 ORIGINAL PAPER Bäcklnd transformation, mltiple wave soltions and lmp soltions to a 3 + -dimensional nonlinear evoltion eqation Li-Na Gao Yao-Yao Zi Y-Hang Yin Wen-Xi

More information

arxiv: v3 [gr-qc] 29 Jun 2015

arxiv: v3 [gr-qc] 29 Jun 2015 QUANTITATIVE DECAY RATES FOR DISPERSIVE SOLUTIONS TO THE EINSTEIN-SCALAR FIELD SYSTEM IN SPHERICAL SYMMETRY JONATHAN LUK AND SUNG-JIN OH arxiv:402.2984v3 [gr-qc] 29 Jn 205 Abstract. In this paper, we stdy

More information

Gradient Projection Anti-windup Scheme on Constrained Planar LTI Systems. Justin Teo and Jonathan P. How

Gradient Projection Anti-windup Scheme on Constrained Planar LTI Systems. Justin Teo and Jonathan P. How 1 Gradient Projection Anti-windp Scheme on Constrained Planar LTI Systems Jstin Teo and Jonathan P. How Technical Report ACL1 1 Aerospace Controls Laboratory Department of Aeronatics and Astronatics Massachsetts

More information

Introdction In the three papers [NS97], [SG96], [SGN97], the combined setp or both eedback and alt detection lter design problem has been considered.

Introdction In the three papers [NS97], [SG96], [SGN97], the combined setp or both eedback and alt detection lter design problem has been considered. Robst Falt Detection in Open Loop s. losed Loop Henrik Niemann Jakob Stostrp z Version: Robst_FDI4.tex { Printed 5h 47m, Febrar 9, 998 Abstract The robstness aspects o alt detection and isolation (FDI)

More information

Partial Differential Equations with Applications

Partial Differential Equations with Applications Universit of Leeds MATH 33 Partial Differential Eqations with Applications Eamples to spplement Chapter on First Order PDEs Eample (Simple linear eqation, k + = 0, (, 0) = ϕ(), k a constant.) The characteristic

More information

Modelling by Differential Equations from Properties of Phenomenon to its Investigation

Modelling by Differential Equations from Properties of Phenomenon to its Investigation Modelling by Differential Eqations from Properties of Phenomenon to its Investigation V. Kleiza and O. Prvinis Kanas University of Technology, Lithania Abstract The Panevezys camps of Kanas University

More information

ARTICLE IN PRESS. Nonlinear Analysis: Real World Applications. Contents lists available at ScienceDirect

ARTICLE IN PRESS. Nonlinear Analysis: Real World Applications. Contents lists available at ScienceDirect Nonlinear Analsis: Real World Applications ( Contents lists available at ScienceDirect Nonlinear Analsis: Real World Applications journal homepage: www.elsevier.com/locate/nonrwa Qualitative analsis of

More information

A Characterization of Interventional Distributions in Semi-Markovian Causal Models

A Characterization of Interventional Distributions in Semi-Markovian Causal Models A Characterization of Interventional Distribtions in Semi-Markovian Casal Models Jin Tian and Changsng Kang Department of Compter Science Iowa State University Ames, IA 50011 {jtian, cskang}@cs.iastate.ed

More information

3 2D Elastostatic Problems in Cartesian Coordinates

3 2D Elastostatic Problems in Cartesian Coordinates D lastostatic Problems in Cartesian Coordinates Two dimensional elastostatic problems are discssed in this Chapter, that is, static problems of either plane stress or plane strain. Cartesian coordinates

More information

The Oscillatory Stable Regime of Nonlinear Systems, with two time constants

The Oscillatory Stable Regime of Nonlinear Systems, with two time constants 6th WSES International Conference on CIRCUITS SYSTEMS ELECTRONICSCONTROL & SIGNL PROCESSING Cairo Egpt Dec 9-3 7 5 The Oscillator Stable Regime of Nonlinear Sstems with two time constants NUŢU VSILE *

More information

The Linear Quadratic Regulator

The Linear Quadratic Regulator 10 The Linear Qadratic Reglator 10.1 Problem formlation This chapter concerns optimal control of dynamical systems. Most of this development concerns linear models with a particlarly simple notion of optimality.

More information

BIOSTATISTICAL METHODS

BIOSTATISTICAL METHODS BIOSTATISTICAL METHOS FOR TRANSLATIONAL & CLINICAL RESEARCH ROC Crve: IAGNOSTIC MEICINE iagnostic tests have been presented as alwas having dichotomos otcomes. In some cases, the reslt of the test ma be

More information

Decision Oriented Bayesian Design of Experiments

Decision Oriented Bayesian Design of Experiments Decision Oriented Bayesian Design of Experiments Farminder S. Anand*, Jay H. Lee**, Matthew J. Realff*** *School of Chemical & Biomoleclar Engineering Georgia Institte of echnology, Atlanta, GA 3332 USA

More information

DIGITAL LINEAR QUADRATIC SMITH PREDICTOR

DIGITAL LINEAR QUADRATIC SMITH PREDICTOR DIGITAL LINEAR QUADRATIC SMITH PREDICTOR Vladimír Bobál,, Marek Kbalčík, Petr Dostál, and Stanislav Talaš Tomas Bata Universit in Zlín Centre of Polmer Sstems, Universit Institte Department of Process

More information

A State Space Based Implicit Integration Algorithm. for Differential Algebraic Equations of Multibody. Dynamics

A State Space Based Implicit Integration Algorithm. for Differential Algebraic Equations of Multibody. Dynamics A State Space Based Implicit Integration Algorithm for Differential Algebraic Eqations of Mltibody Dynamics E. J. Hag, D. Negrt, M. Ianc Janary 28, 1997 To Appear Mechanics of Strctres and Machines Abstract.

More information

Move Blocking Strategies in Receding Horizon Control

Move Blocking Strategies in Receding Horizon Control Move Blocking Strategies in Receding Horizon Control Raphael Cagienard, Pascal Grieder, Eric C. Kerrigan and Manfred Morari Abstract In order to deal with the comptational brden of optimal control, it

More information

We automate the bivariate change-of-variables technique for bivariate continuous random variables with

We automate the bivariate change-of-variables technique for bivariate continuous random variables with INFORMS Jornal on Compting Vol. 4, No., Winter 0, pp. 9 ISSN 09-9856 (print) ISSN 56-558 (online) http://dx.doi.org/0.87/ijoc.046 0 INFORMS Atomating Biariate Transformations Jeff X. Yang, John H. Drew,

More information

THE EFFECTS OF RADIATION ON UNSTEADY MHD CONVECTIVE HEAT TRANSFER PAST A SEMI-INFINITE VERTICAL POROUS MOVING SURFACE WITH VARIABLE SUCTION

THE EFFECTS OF RADIATION ON UNSTEADY MHD CONVECTIVE HEAT TRANSFER PAST A SEMI-INFINITE VERTICAL POROUS MOVING SURFACE WITH VARIABLE SUCTION Latin merican pplied Research 8:7-4 (8 THE EFFECTS OF RDITION ON UNSTEDY MHD CONVECTIVE HET TRNSFER PST SEMI-INFINITE VERTICL POROUS MOVING SURFCE WITH VRIBLE SUCTION. MHDY Math. Department Science, Soth

More information

Robust H 2 Synthesis for Dual-stage Multi-sensing Track-following Servo Systems in HDDs

Robust H 2 Synthesis for Dual-stage Multi-sensing Track-following Servo Systems in HDDs Proceedings of the 6 American Control Conference Minneapolis Minnesota USA Jne 14-16 6 WeB18.1 Robst H Snthesis for al-stage Mlti-sensing Track-following Servo Sstems in Hs Rozo Nagamne Xinghi Hang and

More information

ON THE SHAPES OF BILATERAL GAMMA DENSITIES

ON THE SHAPES OF BILATERAL GAMMA DENSITIES ON THE SHAPES OF BILATERAL GAMMA DENSITIES UWE KÜCHLER, STEFAN TAPPE Abstract. We investigate the for parameter family of bilateral Gamma distribtions. The goal of this paper is to provide a thorogh treatment

More information

REINFORCEMENT LEARNING AND OPTIMAL ADAPTIVE CONTROL

REINFORCEMENT LEARNING AND OPTIMAL ADAPTIVE CONTROL Lewis c11.tex V1-10/19/2011 4:10pm Page 461 11 REINFORCEMENT LEARNING AND OPTIMAL ADAPTIVE CONTROL In this book we have presented a variety of methods for the analysis and design of optimal control systems.

More information

1 Undiscounted Problem (Deterministic)

1 Undiscounted Problem (Deterministic) Lectre 9: Linear Qadratic Control Problems 1 Undisconted Problem (Deterministic) Choose ( t ) 0 to Minimize (x trx t + tq t ) t=0 sbject to x t+1 = Ax t + B t, x 0 given. x t is an n-vector state, t a

More information

On Multiobjective Duality For Variational Problems

On Multiobjective Duality For Variational Problems The Open Operational Research Jornal, 202, 6, -8 On Mltiobjective Dality For Variational Problems. Hsain *,, Bilal Ahmad 2 and Z. Jabeen 3 Open Access Department of Mathematics, Jaypee University of Engineering

More information

DEFINITION OF A NEW UO 2 F 2 DENSITY LAW FOR LOW- MODERATED SOLUTIONS (H/U < 20) AND CONSEQUENCES ON CRITICALITY SAFETY

DEFINITION OF A NEW UO 2 F 2 DENSITY LAW FOR LOW- MODERATED SOLUTIONS (H/U < 20) AND CONSEQUENCES ON CRITICALITY SAFETY DEFINITION OF A NEW UO 2 F 2 DENSITY LAW FOR LOW- MODERATED SOLUTIONS ( < 20) AND CONSEQUENCES ON CRITICALITY SAFETY N. Leclaire, S. Evo, I.R.S.N., France Introdction In criticality stdies, the blk density

More information

Optimal Control, Statistics and Path Planning

Optimal Control, Statistics and Path Planning PERGAMON Mathematical and Compter Modelling 33 (21) 237 253 www.elsevier.nl/locate/mcm Optimal Control, Statistics and Path Planning C. F. Martin and Shan Sn Department of Mathematics and Statistics Texas

More information

Queueing analysis of service deferrals for load management in power systems

Queueing analysis of service deferrals for load management in power systems Qeeing analysis of service deferrals for load management in power systems Andrés Ferragt and Fernando Paganini Universidad ORT Urgay Abstract With the advent of renewable sorces and Smart- Grid deployments,

More information

DISPLACEMENT ANALYSIS OF SUBMARINE SLOPES USING ENHANCED NEWMARK METHOD

DISPLACEMENT ANALYSIS OF SUBMARINE SLOPES USING ENHANCED NEWMARK METHOD DISPLACEMENT ANALYSIS OF SUBMARINE SLOPES USING ENHANCED NEWMARK METHOD N. ZANGENEH and R. POPESCU Faclt of Engineering & Applied Science, Memorial Universit, St. John s, Newfondland, Canada A1B 3X5 Abstract

More information

Linear Strain Triangle and other types of 2D elements. By S. Ziaei Rad

Linear Strain Triangle and other types of 2D elements. By S. Ziaei Rad Linear Strain Triangle and other tpes o D elements B S. Ziaei Rad Linear Strain Triangle (LST or T6 This element is also called qadratic trianglar element. Qadratic Trianglar Element Linear Strain Triangle

More information

Nonlinear parametric optimization using cylindrical algebraic decomposition

Nonlinear parametric optimization using cylindrical algebraic decomposition Proceedings of the 44th IEEE Conference on Decision and Control, and the Eropean Control Conference 2005 Seville, Spain, December 12-15, 2005 TC08.5 Nonlinear parametric optimization sing cylindrical algebraic

More information

Chem 4501 Introduction to Thermodynamics, 3 Credits Kinetics, and Statistical Mechanics. Fall Semester Homework Problem Set Number 10 Solutions

Chem 4501 Introduction to Thermodynamics, 3 Credits Kinetics, and Statistical Mechanics. Fall Semester Homework Problem Set Number 10 Solutions Chem 4501 Introdction to Thermodynamics, 3 Credits Kinetics, and Statistical Mechanics Fall Semester 2017 Homework Problem Set Nmber 10 Soltions 1. McQarrie and Simon, 10-4. Paraphrase: Apply Eler s theorem

More information

NEURAL CONTROLLERS FOR NONLINEAR SYSTEMS IN MATLAB

NEURAL CONTROLLERS FOR NONLINEAR SYSTEMS IN MATLAB NEURAL CONTROLLERS FOR NONLINEAR SYSTEMS IN MATLAB S.Kajan Institte of Control and Indstrial Informatics, Faclt of Electrical Engineering and Information Technolog, Slovak Universit of Technolog in Bratislava,

More information

TRANSONIC EVAPORATION WAVES IN A SPHERICALLY SYMMETRIC NOZZLE

TRANSONIC EVAPORATION WAVES IN A SPHERICALLY SYMMETRIC NOZZLE TRANSONIC EVAPORATION WAVES IN A SPHERICALLY SYMMETRIC NOZZLE XIAOBIAO LIN AND MARTIN WECHSELBERGER Abstract. This paper stdies the liqid to vapor phase transition in a cone shaped nozzle. Using the geometric

More information

Hybrid modelling and model reduction for control & optimisation

Hybrid modelling and model reduction for control & optimisation Hybrid modelling and model redction for control & optimisation based on research done by RWTH-Aachen and TU Delft presented by Johan Grievink Models for control and optimiation market and environmental

More information

Konyalioglu, Serpil. Konyalioglu, A.Cihan. Ipek, A.Sabri. Isik, Ahmet

Konyalioglu, Serpil. Konyalioglu, A.Cihan. Ipek, A.Sabri. Isik, Ahmet The Role of Visalization Approach on Stdent s Conceptal Learning Konyaliogl, Serpil Department of Secondary Science and Mathematics Edcation, K.K. Edcation Faclty, Atatürk University, 25240- Erzrm-Trkey;

More information

Time-adaptive non-linear finite-element analysis of contact problems

Time-adaptive non-linear finite-element analysis of contact problems Proceedings of the 7th GACM Colloqim on Comptational Mechanics for Yong Scientists from Academia and Indstr October -, 7 in Stttgart, German Time-adaptive non-linear finite-element analsis of contact problems

More information

UNCERTAINTY FOCUSED STRENGTH ANALYSIS MODEL

UNCERTAINTY FOCUSED STRENGTH ANALYSIS MODEL 8th International DAAAM Baltic Conference "INDUSTRIAL ENGINEERING - 19-1 April 01, Tallinn, Estonia UNCERTAINTY FOCUSED STRENGTH ANALYSIS MODEL Põdra, P. & Laaneots, R. Abstract: Strength analysis is a

More information

AN ISOGEOMETRIC SOLID-SHELL FORMULATION OF THE KOITER METHOD FOR BUCKLING AND INITIAL POST-BUCKLING ANALYSIS OF COMPOSITE SHELLS

AN ISOGEOMETRIC SOLID-SHELL FORMULATION OF THE KOITER METHOD FOR BUCKLING AND INITIAL POST-BUCKLING ANALYSIS OF COMPOSITE SHELLS th Eropean Conference on Comptational Mechanics (ECCM ) 7th Eropean Conference on Comptational Flid Dynamics (ECFD 7) 5 Jne 28, Glasgow, UK AN ISOGEOMETRIC SOLID-SHELL FORMULATION OF THE KOITER METHOD

More information

Direct linearization method for nonlinear PDE s and the related kernel RBFs

Direct linearization method for nonlinear PDE s and the related kernel RBFs Direct linearization method for nonlinear PDE s and the related kernel BFs W. Chen Department of Informatics, Uniersity of Oslo, P.O.Box 1080, Blindern, 0316 Oslo, Norway Email: wenc@ifi.io.no Abstract

More information

The Dual of the Maximum Likelihood Method

The Dual of the Maximum Likelihood Method Department of Agricltral and Resorce Economics University of California, Davis The Dal of the Maximm Likelihood Method by Qirino Paris Working Paper No. 12-002 2012 Copyright @ 2012 by Qirino Paris All

More information

Solving the Lienard equation by differential transform method

Solving the Lienard equation by differential transform method ISSN 1 746-7233, England, U World Jornal of Modelling and Simlation Vol. 8 (2012) No. 2, pp. 142-146 Solving the Lienard eqation by differential transform method Mashallah Matinfar, Saber Rakhshan Bahar,

More information

Discussion of The Forward Search: Theory and Data Analysis by Anthony C. Atkinson, Marco Riani, and Andrea Ceroli

Discussion of The Forward Search: Theory and Data Analysis by Anthony C. Atkinson, Marco Riani, and Andrea Ceroli 1 Introdction Discssion of The Forward Search: Theory and Data Analysis by Anthony C. Atkinson, Marco Riani, and Andrea Ceroli Søren Johansen Department of Economics, University of Copenhagen and CREATES,

More information