Modelling the Dynamical State of the Projected Primary and Secondary Intra-Solution-Particle

International Journal of Modern Nonlinear Theory and pplication 0-7 http://www.scirp.org/journal/ijmnta ISSN Online: 7-987 ISSN Print: 7-979 Modelling the Dynamical State of the Projected Primary and Secondary Intra-Solution-Particle Movement System of Efavirenz In-Vivo Tafireyi Nemaura Department of Clinical Pharmacology University of Zimbabwe Harare Zimbabwe Department of pplied Mathematics National University of Science and Technology Bulawayo Zimbabwe How to cite this paper: Nemaura T. (0 Modelling the Dynamical State of the Projected Primary and Secondary Intra-Solution-Particle Movement System of Efavirenz In-Vivo. International Journal of Modern Nonlinear Theory and pplication - 7. http://d.doi.org/0./ijmnta.0.0 Received: October 8 0 ccepted: December 0 Published: December 0 Copyright 0 by author and Scientific Research Publishing Inc. This work is licensed under the Creative Commons ttribution International License (CC BY.0. http://creativecommons.org/licenses/by/.0/ Open ccess bstract This work seeks to describe intra-solution particle movement system. It makes use of data obtained from simulations of patients on efavirenz. system of ordinary differential equations is used to model movement state at some particular concentration. The movement states description is found for the primary and secondary level. The primary system is found to be predominantly an unstable system while the secondary system is stable. This is derived from the state of dynamic eigenvalues associated with the system. The saturated solution-particle is projected to be stable both for the primary potential and secondary state. volume conserving linear system has been suggested to describe the dynamical state of movement of a solution particle. Keywords Ordinary Differential Equations Stability Nonautonomous Linear System Concentration-Varying Eigenvalues Solution Particle. Introduction The intra-solution-particle movement system is described in this work. system which consists of the primary and secondary movement states that is proposed in Nemaura (0 is investigated. Differential Equations are used to describe dynamical systems. Most systems are described relative to time [] [] []. In this work they are used to describe a dynamical system of the state of a solution particle relative to concentration. Multiple compartmental modelling finds its use in fields such as Physiologically Based Pharmacokinetics Engineering and Mathematical Biology [] [] []. Other researchers work with constant parameters that are obtained for autonomous linear systems. In this DOI: 0./ijmnta.0.0 December 0

work a simple system (nonautonomous linear system whose parameters vary according to concentration is considered [] []. The miing problems have been widely studied by the use of ordinary differential equations [] [7] [8]. dditionally some researchers consider probable systems that arise from these miing problems [7] [8]. This work proposes a system of linear ordinary differential equations that potentially govern the state of solution particle and shares a relation to the miing problems. In addition there is consideration of a volume conserving state of a solution particle. The dynamic eigenvalues from the corresponding matri and stability of the concentration varying linear systems are proposed. The dynamic eigenvalues have found applications for linear time-varying systems []. This work highlights possible intra-particle movement potential/states inferred to be present in the solution particle at primary and secondary level and attempts to give mathematical form as in Nemaura (0 [9]. It proposes multiple-compartmental models one for the primary level and the other for the secondary level. The resultant form gives a general representation of movement within a solution particle.. Methods The primary and secondary movement system of projected simulated data from patients who had been on efavirenz is used [9]. The software used were R and Mathematica... The Primary System The primary system is a sub-system of the secondary and describes potential. It is projected to consist of four main movement entities that is convection saturation passive and advection. The form entity being the advective component [9]... The Primary System of Solution Particle solution particle with concentration ( is made up of four movement components (variables at primary level C-convective -advective P-Passive and S-Saturation at primary level satisfying C( = S( + ( P( ( = S( + ( + P( ( where P = P. We analyse the following system of differential equations in order to infer on the overall process occuring in describing state of movement in a solution particle (See Figure. ds Å = ( ( S+ ( = h( S ( d d = ( S ( ( + ( + ( + ( P= q( S P d Å ( Subject to dp = ( ( P= w( S P ( d

Figure. compartmental representation of the model for solution particle movement state dynamics at primary level driven by the advective component. It is noted that this representation is not necessarily unique for all forms of advective component. nd ( ( ( Å + + = 0 ( ( + = 0 P Å With P and are the variable parameters. These two conditions allows no net change in the volumetric consituencies of the four movement components where single phase third generation solution sub-particle at primary level form inducing movement interaction with four main movement entities single phase second generation solution sub-particle at primary level with four main movement entities and altering phase(s first generation solution sub-particle at primary level with three main movement entities. Solving the primary system above ( - in terms of advective components dc Å ( = d Å Å ds ( ( ( d = S + ds Å Å ( ( S ( d = S + dp d + P ( = = ( and. P.. Stability nalysis of the Primary System The equlibrium steady state points are constant solutions S( ( and P( 7

which satisfy the nonlinear system of equations d S 0 d dp = = 0 and 0. d d d = These points govern the behaviour of physical models. Thus we obtain ( = (form po- P = (negative bind- tential S ( = (space accesory potential and ( ing-orientation potential. It is important to note that the convective potential at equilibrium (primary level is negative (nullifying/compensating accesory potential. Furthermore it has the value of. Local nalysis near Steady-State Points ( S P Local analysis is studied near each steady state point ( S P. We begin by the following where ν ( ζ ( and ( ( ( ν ( S = S + ( ( ζ ( = ( + (7 ( ( ψ ( P = P + (8 ψ are small. dν ( ( ( ( ( h h h = h S + ν + ζ P ( + ψ ( ν + ζ + ψ d S P dζ ( ( ( ( ( q q q = q S + ν + ζ P ( + ψ ( ν + ζ + ψ d S P d ( ( ( ( ( w w w = w S + ν + ζ P ( + ψ ( ν + ζ + ψ. d S P S P. The sta- The partial derivatives are evaluated at the equilibrium point ( bility of the steady state point ( (9 (0 ( S P is investigated by studying the eigenvalues of the Jacobian matri ( matri of the partial derivatives. The Jacobian matri for the primary system is given by h h h S P 0 q q q Å J( S P = = ( + + P S P ( w w w 0 P S P ( S P (IUndisturbed potential ( = 0 ( = = 0 = P where =. The characteristic equation of J is given by λ λ + = 0 Eigenvalues of this system are given by ( 0 i i. The equilibrium point has neutral stability. Thus the primary unique space interacting potential has a neutral equilibrium before disturbances. > ( Å = P The dynamic eigenvalues follows from the characteristic equation of J given by (II Disturbed (dissolving potential ( 0 8

( ( λ λ + + + = 0 which is similar + ( + ( λ λ = 0. Å Å Thus the eigenvalues for this system are nd M N λ = + N zm z N λ = N z M zn λ = N Å where z i z i M ( = + = = + and Å ( Å Å 7 + 79 + 08 + N = Å : ( = 0 ( ( (III Saturated potential ( s 0 s = s = = = 0. The characteristic equation is given by ( ( s P s s λ =.. The Secondary System of Solution Particle 0. 0 The product of advective primary interaction potential with its unique space (the relative uptake results in a secondary advective movement system [9]. solution particle with concentration ( is made up of three movement components (variables at secondary level C convective advective and S Saturation at secondary level satisfying ( ( (. C = S + ( This is represented by the following constituent system (See Figure Subject to ds d d d ( Å ( ( = S + = f S ( ( ( ( ( S S ( ( ( ( Å ( S ( S ( S ( g S = + = ( ( Å ( ( ( + S ( ( 0 + S = ( Å ( ( With S S (variable parameters. The condition allows no net change in the volumetric consituents of the movement components. Where single phase third generation solution sub-particle at secondary level form 9

Figure. compartmental representation of the model for solution particle movement state dynamics at secondary level driven by the advective component. inducing movement interaction with four main movement entities single phase second generation solution sub-particle at secondary level with four main movement entities. Solving the secondary system above ( - ( ( S ( dc ( Å ( = d ( ( ( ( = S + ds d Å Å ds ( Å ( Å ( ( S ( and ( d. S = S +.. Stability nalysis of the Secondary System The equlibrium steady state points are constant solutions S ( and ( which satisfy the nonlinear system of equations d S 0 d = and d 0 d =. It is shown that this system is orbitally stable which signifies that the solutions remain near the equilibrium point. Local nalysis near Steady-State Points ( S Considering ds 0 d = d 0. d = Thus we obtain ( = (form state and S ( ( Å ( ( + ( S = = ( S ( 0

(space accessory state. It is important to note that the convective movement at secondary level is a stable state which is 0 (nullifying/stabilising accessory state. We study local analysis near each steady state point ( S for Equations ( & (. We begin by the following where ( and ( (9. ( ( ( ( ( η ( S = S + ( = + (7 η are small. Net we substitute Equations ( & (7 into (8 & d ( ( ( f f = f S + ( + η( + η (8 d S dη ( ( ( g g = g S + ( η( η. d + + S (9 The Jacobian matri for the secondary system is given by f f ( ( S S S J ( S = =. ( ( Å ( g g S ( S (0 + S ( S ( Å ( The eigenvalues λ and λ for this system are given by i S and ( Å ( i respectively. The secondary system gives a form of neutral stability. S. Results.. Numerical Projections of Sub-Particle and Particle of Solution for the Primary System The graphical representation of the advective components (sub-systems are shown (see Figure. The solution is developed from the primary system equation in Nemaura (0 and the system ( -. The primary system and sub-system equations and estimated parameters are given (See Equations ( - (7 and Table. Primary system equation S( ( ( = + + + e. ( + C( P( Primary sub-particle equation given by e e. Primary Å = + + + ( ( sub-particle equation given by ( = ( e + + e. + ( (

Figure. (a The intra-advective movement potential of the primary sub-system from to P against concentration. Note the intra-advective movement potential of the primary sub- system from P to against concentration is equivalent to. (b The intra-advective movement potential of the primary sub-system from to S against concentration. (c The intra-advective movement potential of the primary sub-system from S to against concentration. (d The intra-advective movement potential of the primary sub-system against concentration. Table. Parameter estimates in modelling movement rates associated with the primary system. dvective Parameters Estimate Std Error t value Pr ( > t Å 0.00 0.8808 0.0 7. 0.0089 0.098 0.07.8 0.0 0.(Fi 0.008 0. 0.8 0.9 0. 0. 0.007 0.0 0.000 0.087 0.007 0.9 0.000 0.00 0.0 0.79 0.07 0.000 0.00 0.007 0.0 0.00 0.0 0.000 0.0007.00 0.07 9.7 0.77.89 9.90...07.09 9.0 9.7 8.9 9.8 7.9 7.7 7.. 0.7 0 0.8 0 0 7.9 0 < 0 < 0 0.00 7.0 0 0.009 0.000.8 0 < 0 < 0 < 0 < 0 < 0 < 0

Continued 0.80 0.9 0.9 0.(Fi 0.00 0.0 0.007 0.070 0.008 0.000 0.00 8.89 0.89 8.0 9.9 7. < 0 < 0 < 0. 0 < 0 α ( α ( α ( α.9.0.80 0.00 0.00 0.09 7. 99. 0.0 < 0 < 0 < 0 β ( β ( β. 0 9.77 0. 0. 0 8.7 0 < 0 0 < 0 γ ( γ ( γ. 0 8.9 0.07 0 7 8.8 0 7.9.9 0 00.8. 0 Primary Primary where Primary Primary sub-particle equation given by e e. + ( = ( + + sub-particle ( α equation given by = n ( α ( α ( α ( α ( α = + e 0 < n ( d n : = 0. d sub-particle ( β equation given by ( β ( β ( β ( β m = + e. n < m sub-particle ( γ equation given by ( γ ( γ ( γ ( γ m = e >. m where m = 9.888 is the point when the system is projected to show considerable loss of homogeneity-potential. Furthermore =. P.. Numerical Projections of Sub-Particle and Particle of Solution Movement for the Secondary System The graphical representation of the advective components (sub-systems are shown (see Figure. The solution is developed from the secondary system equation in Nemaura (0 and the system ( -. ( ( (7

Figure. (a The advective intra-secondary sub-system modelling the movement from to S against concentration. (b The advective intra-secondary sub-system modelling the movement from S to against concentration. (c The advective intra-secondary sub-system which initiates the process against concentration. The secondary system and sub-system equations and estimated parameters are given (See Equations (8 - ( and Table. Secondary system equation is given by ( ( = + + S ( C ( e. (8 Secondary sub-particle equation given by ( Å 7 = e + + e. + ( ( (9 Secondary Secondary sub-particle equation given by S S ( S S ( e. S = + + + + sub-particle equation given by S S S S ( S S S ( e. = + + + S + (0 (.. Stability Numerical nalysis for Secondary System ( Å ( Let π = ˆ ˆ S and the plot of π against is given (See Figure. The results show that π 0 for almost all values of concentration (. The following is proposed ( Å ( ( ( = π ( + φ( where φ ( is the error term in estimating

Table. Parameter estimates in modelling movement rates associated with the secondary system. dvective Parameters Estimate Std Error t value Pr ( > t ( Å 7 0.88.9 0. 0.0 0. 0.0 0.77 0. 9.99(Fi 0.000 0.070 0.009 0. 0.0007 0.000 0.008 0.0 0.0 0.008 0.000 0.000.7.87 8..9.89 8.9.7.89 9.7 8. < 0 < 0 < 0 < 0 < 0 < 0 < 0 < 0 < 0 < 0 ( S S S S S S S 0. 0.7 0. 9.990 0.00 0.0 0.00 0.008 0.00 0.9 0.000 0.000 8.7 8.7 8.7.9 87. < 0 < 0 < 0 < 0 < 0 < 0 ( S S S S S S S 0.0.99 0.0 9.99(Fi 0.00 0.00 0.00 0.000 0.00 0.000 0.0009 8.0 9.90 8..9. < 0 < 0 < 0 < 0 < 0 Figure. The value π of the characteristic equation against concentration.

( Å (. The system is inferred to be stable. (. Discussion ( nonautonomous linear system is developed that enables characterisation of the projected movement in a solution-particle [] []. There are four main movement potential components at primary level with respect to advection. They are held together by the sub-system also a potential which is inferred to have five distinct systems (that is the two s and two s. While the secondary system consists of two s and. The variable parameters in the system of ordinary differential equations are inferred to describe (advective form components of movement. The movement description gives the state of solution particle and there is suggestion of the constituent entities. The primary system is generally projected to be an unstable system relative to concentration. The saturated system is inferred to have stable potential. The reaction allowing state (non-saturated concentration has unstable equilibrium potential at primary level. However the secondary system is stable. This work has managed to describe the possible state of kinetics of a solution-particle of efavirenz. It has shown that a saturated state can be equated to a stable state both at primary and secondary level. The constcted matri in this case is traceless that is it has zero trace. The volume conserving systems have been considered in modelling of the physical systems and the theoretical framework is also developed in Lie Theory [0] []. cknowledgements The author would like to thank the following; C. Nhachi C. Masimirembwa and G. Kadzirange IBST and The College of Health Sciences University of Zimbabwe. References [] Ette E.I. and Williams P.J. (007 Pharmacometrics. The Science of Quantitative Pharmacology. Hoboken Wiley. [] van der Kloet P. and Neerhoff F.L. (00 Dynamic Eigenvalues for Scalar Linear Time- Varying Systems. Proceedings of th International Symposium on Mathematical Theory of Net. and Sys. MTNS Notre Dame. [] Murray J.D. (00 Mathematical Biology. rd Edition Springer Berlin. [] Kreyszig E. (00 dvanced Engineering Mathematics. 9th Edition Wiley. [] Sideris T.C. (0 Ordinary Differential Equations and Dynamical Systems. Springer tlantis Press. https://doi.org/0.99/978-9-9-0-8 [] Hirsch M.W. Smale S. and Devaney R.L. (0 Differential Equations Dynamical Systems and an Introduction to Chaos. cademic Press. [7] Slavík. (0 Miing Problems with Many Tanks. merican Mathematical Monthly 0 80-8. https://doi.org/0.9/amer.math.monthly.0.09.80 [8] Edwards C.H. and Penney D.E. (00 Elementary Differential Equations. th Edition Pearson Upper Saddle River. [9] Nemaura T. (0 Modeling Transportation of Efavirenz: Inference on Possibility of Mied

Modes of Transportation and Kinetic Solubility. Frontiers in Pharmacology. https://doi.org/0.89/fphar.0.00 [0] Kirillov Jr.. (008 n Introduction to Lie Groups and Lie lgebras. Cambridge Studies in dvanced Mathematics Vol. Cambridge University Press Cambridge. https://doi.org/0.07/cbo97807 [] van den Ban E.P. (00 Lie Groups. Lecture Notes Spring. Submit or recommend net manuscript to SCIRP and we will provide best service for you: ccepting pre-submission inquiries through Email Facebook LinkedIn Twitter etc. wide selection of journals (inclusive of 9 subjects more than 00 journals Providing -hour high-quality service User-friendly online submission system Fair and swift peer-review system Efficient typesetting and proofreading procedure Display of the result of downloads and visits as well as the number of cited articles Maimum dissemination of your research work Submit your manuscript at: http://papersubmission.scirp.org/ Or contact ijmnta@scirp.org 7