27 research outputs found

    Π€ΡƒΠ½ΠΊΡ†ΠΈΠΎΠ½Π°Π»ΡŒΠ½Ρ‹ΠΉ ΠΌΠ΅Ρ‚ΠΎΠ΄ Π»ΠΎΠΊΠ°Π»ΠΈΠ·Π°Ρ†ΠΈΠΈ ΠΈ ΠΏΡ€ΠΈΠ½Ρ†ΠΈΠΏ инвариантности Π›Π°-Балля

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    A functional method of localization has proved to be good in solving the qualitative analysis problems of dynamic systems. Proposed in the 90s, it was intensively used when studying a number of well-known systems of differential equations, both of autonomous and of non-autonomous discrete systems, including systems that involve control and / or disturbances.The method essence is to construct a set containing all invariant compact sets in the phase space of a dynamical system. A concept of the invariant compact set includes equilibrium positions, limit cycles, attractors, repellers, and other structures in the phase space of a system that play an important role in describing the behavior of a dynamical system. The constructed set is called localizing and represents an external assessment of the appropriate structures in the phase space.Relatively recently, it was found that the functional localization method allows one to analyze a behavior of the dynamical system trajectories. In particular, the localization method can be used to check the stability of the equilibrium positions.Here naturally emerges an issue of the relationship between the functional localization method and the well-known La Salle invariance principle, which can be regarded as a further development of the method of Lyapunov functions for establishing stability. The article discusses this issue.Π’ Π·Π°Π΄Π°Ρ‡Π°Ρ… качСствСнного Π°Π½Π°Π»ΠΈΠ·Π° динамичСских систСм Ρ…ΠΎΡ€ΠΎΡˆΠΎ Π·Π°Ρ€Π΅ΠΊΠΎΠΌΠ΅Π½Π΄ΠΎΠ²Π°Π» сСбя Ρ„ΡƒΠ½ΠΊΡ†ΠΈΠΎΠ½Π°Π»ΡŒΠ½Ρ‹ΠΉ ΠΌΠ΅Ρ‚ΠΎΠ΄ Π»ΠΎΠΊΠ°Π»ΠΈΠ·Π°Ρ†ΠΈΠΈ. ΠŸΡ€Π΅Π΄Π»ΠΎΠΆΠ΅Π½Π½Ρ‹ΠΉ Π² 90-Ρ…Ρ… Π³Π³., ΠΎΠ½ Π°ΠΊΡ‚ΠΈΠ²Π½ΠΎ использовался Π² исслСдовании ряда извСстных систСм Π΄ΠΈΡ„Ρ„Π΅Ρ€Π΅Π½Ρ†ΠΈΠ°Π»ΡŒΠ½Ρ‹Ρ… ΡƒΡ€Π°Π²Π½Π΅Π½ΠΈΠΉ, ΠΊΠ°ΠΊ Π°Π²Ρ‚ΠΎΠ½ΠΎΠΌΠ½Ρ‹Ρ…, Ρ‚Π°ΠΊ ΠΈ Π½Π΅Π°Π²Ρ‚ΠΎΠ½ΠΎΠΌΠ½Ρ‹Ρ…, дискрСтных систСм, Π² Ρ‚ΠΎΠΌ числС систСм Π²ΠΊΠ»ΡŽΡ‡Π°ΡŽΡ‰ΠΈΡ… ΡƒΠΏΡ€Π°Π²Π»Π΅Π½ΠΈΠ΅ ΠΈ/ΠΈΠ»ΠΈ возмущСния.Π‘ΡƒΡ‚ΡŒ ΠΌΠ΅Ρ‚ΠΎΠ΄Π° состоит Π² построСнии Ρ‚Π°ΠΊΠΎΠ³ΠΎ мноТСства Π² Ρ„Π°Π·ΠΎΠ²ΠΎΠΌ пространствС динамичСской систСмы, ΠΊΠΎΡ‚ΠΎΡ€ΠΎΠ΅ содСрТит всС ΠΈΠ½Π²Π°Ρ€ΠΈΠ°Π½Ρ‚Π½Ρ‹Π΅ ΠΊΠΎΠΌΠΏΠ°ΠΊΡ‚Π½Ρ‹Π΅ мноТСства. ΠŸΠΎΠ½ΡΡ‚ΠΈΠ΅ ΠΈΠ½Π²Π°Ρ€ΠΈΠ°Π½Ρ‚Π½ΠΎΠ³ΠΎ ΠΊΠΎΠΌΠΏΠ°ΠΊΡ‚Π½ΠΎΠ³ΠΎ мноТСства Π²ΠΊΠ»ΡŽΡ‡Π°Π΅Ρ‚ полоТСния равновСсия, ΠΏΡ€Π΅Π΄Π΅Π»ΡŒΠ½Ρ‹Π΅ Ρ†ΠΈΠΊΠ»Ρ‹, Π°Ρ‚Ρ‚Ρ€Π°ΠΊΡ‚ΠΎΡ€Ρ‹, Ρ€Π΅ΠΏΠ΅Π»Π»Π΅Ρ€Ρ‹ ΠΈ Π΄Ρ€ΡƒΠ³ΠΈΠ΅ структуры Π² Ρ„Π°Π·ΠΎΠ²ΠΎΠΌ пространствС систСмы, ΠΈΠ³Ρ€Π°ΡŽΡ‰ΠΈΠ΅ Π²Π°ΠΆΠ½ΡƒΡŽ Ρ€ΠΎΠ»ΡŒ Π² описании повСдСния динамичСской систСмы. ΠŸΠΎΡΡ‚Ρ€ΠΎΠ΅Π½Π½ΠΎΠ΅ мноТСство Π½Π°Π·Ρ‹Π²Π°ΡŽΡ‚ Π»ΠΎΠΊΠ°Π»ΠΈΠ·ΠΈΡ€ΡƒΡŽΡ‰ΠΈΠΌ. Оно слуТит внСшнСй ΠΎΡ†Π΅Π½ΠΊΠΎΠΉ ΡΠΎΠΎΡ‚Π²Π΅Ρ‚ΡΡ‚Π²ΡƒΡŽΡ‰ΠΈΡ… структур Π² Ρ„Π°Π·ΠΎΠ²ΠΎΠΌ пространствС.ΠžΡ‚Π½ΠΎΡΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎ Π½Π΅Π΄Π°Π²Π½ΠΎ Π±Ρ‹Π»ΠΎ установлСно, Ρ‡Ρ‚ΠΎ Ρ„ΡƒΠ½ΠΊΡ†ΠΈΠΎΠ½Π°Π»ΡŒΠ½Ρ‹ΠΉ ΠΌΠ΅Ρ‚ΠΎΠ΄ Π»ΠΎΠΊΠ°Π»ΠΈΠ·Π°Ρ†ΠΈΠΈ позволяСт Π°Π½Π°Π»ΠΈΠ·ΠΈΡ€ΠΎΠ²Π°Ρ‚ΡŒ ΠΏΠΎΠ²Π΅Π΄Π΅Π½ΠΈΠ΅ Ρ‚Ρ€Π°Π΅ΠΊΡ‚ΠΎΡ€ΠΈΠΉ динамичСской систСмы. Π’ частности, с ΠΏΠΎΠΌΠΎΡ‰ΡŒΡŽ ΠΌΠ΅Ρ‚ΠΎΠ΄Π° Π»ΠΎΠΊΠ°Π»ΠΈΠ·Π°Ρ†ΠΈΠΈ ΠΌΠΎΠΆΠ½ΠΎ ΠΏΡ€ΠΎΠ²Π΅Ρ€ΡΡ‚ΡŒ ΡƒΡΡ‚ΠΎΠΉΡ‡ΠΈΠ²ΠΎΡΡ‚ΡŒ ΠΏΠΎΠ»ΠΎΠΆΠ΅Π½ΠΈΠΉ равновСсия.Π—Π΄Π΅ΡΡŒ СстСствСнным ΠΎΠ±Ρ€Π°Π·ΠΎΠΌ Π²ΠΎΠ·Π½ΠΈΠΊΠ°Π΅Ρ‚ вопрос ΠΎ связи Ρ„ΡƒΠ½ΠΊΡ†ΠΈΠΎΠ½Π°Π»ΡŒΠ½ΠΎΠ³ΠΎ ΠΌΠ΅Ρ‚ΠΎΠ΄Π° Π»ΠΎΠΊΠ°Π»ΠΈΠ·Π°Ρ†ΠΈΠΈ с извСстным ΠΏΡ€ΠΈΠ½Ρ†ΠΈΠΏΠΎΠΌ инвариантности Π›Π°-Балля, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹ΠΉ ΠΌΠΎΠΆΠ½ΠΎ Ρ€Π°ΡΡΠΌΠ°Ρ‚Ρ€ΠΈΠ²Π°Ρ‚ΡŒ ΠΊΠ°ΠΊ дальнСйшСС Ρ€Π°Π·Π²ΠΈΡ‚ΠΈΠ΅ ΠΌΠ΅Ρ‚ΠΎΠ΄Π° Ρ„ΡƒΠ½ΠΊΡ†ΠΈΠΉ Ляпунова для установлСния устойчивости. Настоящая ΡΡ‚Π°Ρ‚ΡŒΡ посвящСна ΠΎΠ±ΡΡƒΠΆΠ΄Π΅Π½ΠΈΡŽ этого вопроса

    ΠΠ°Π±Π»ΡŽΠ΄Π°Ρ‚Π΅Π»ΡŒ состояния для ΠΌΠΎΠ΄Π΅Π»ΠΈ кардиостимулятора Π½Π° основС уравнСния Π’Π°Π½ Π΄Π΅Ρ€ Поля

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    A Dutch physiologist and a founder of electrocardiography V. Einthoven [10] proposed the first known model of the cardiac electrical activity. Β Later, van der Pol and van der Mark [11] developed a model of the heart, where the heartbeat is considered as a relaxation oscillation. From this point of view, to model the operation of pacemakers, the van der Pol equation [14,15,19] can be useful. The paper offers modeling of only one heart node that is the S-A (sinoatrial) node, which is the main heart pacemaker [20].Many control algorithms for dynamic systems are based on feedback, which involves the full state vector of a dynamic system. However, in practice, the full state vector is not always known. So, in the case of cardiac electrical activity, the potentials of the nodes rather than their changing rates are measured. To restore the full state vector from existing measurements, state observers are often used.In this paper, we solve the task of constructing an observer with linear error dynamics [22.25]. A necessary condition for the existence of such an observer is the system observability. The sufficient conditions can be formulated in the framework of the differential-geometric approach [25] using the ideas of duplicity [25,26]. Within this approach, an algorithm for observer construction can be developed. In the paper, a general problem to construct an observer for two-dimensional systems is solved and the results obtained are applied to the pacemaker model based on the Van der Pol oscillator. The numerical simulation enables us to illustrate operation of the observer developed.ΠŸΠ΅Ρ€Π²Π°Ρ извСстная модСль элСктричСской активности сСрдца Π±Ρ‹Π»Π° ΠΏΡ€Π΅Π΄Π»ΠΎΠΆΠ΅Π½Π° нидСрландским Ρ„ΠΈΠ·ΠΈΠΎΠ»ΠΎΠ³ΠΎΠΌ ΠΈ основополоТником элСктрокардиографии Π’.Β Π­ΠΉΠ½Ρ‚Ρ…ΠΎΠ²Π΅Π½ΠΎΠΌ [10]. ПозТС Π’Π°Π½ Π΄Π΅Ρ€ Поль ΠΈ Π’Π°Π½ Π΄Π΅Ρ€ ΠœΠ°Ρ€ΠΊ [11] построили модСль сСрдца, Π³Π΄Π΅ сСрдцСбиСниС рассматриваСтся ΠΊΠ°ΠΊ рСлаксационноС ΠΊΠΎΠ»Π΅Π±Π°Π½ΠΈΠ΅. Π‘ этой Ρ‚ΠΎΡ‡ΠΊΠΈ зрСния для модСлирования Ρ€Π°Π±ΠΎΡ‚Ρ‹ кардиостимуляторов ΠΌΠΎΠΆΠ½ΠΎ ΠΈΡΠΏΠΎΠ»ΡŒΠ·ΠΎΠ²Π°Ρ‚ΡŒ ΡƒΡ€Π°Π²Π½Π΅Π½ΠΈΠ΅ Π’Π°Π½ Π΄Π΅Ρ€ Поля [14,15,19]. Π’ Π΄Π°Π½Π½ΠΎΠΉ Ρ€Π°Π±ΠΎΡ‚Π΅ модСлируСтся Ρ€Π°Π±ΠΎΡ‚Π° Ρ‚ΠΎΠ»ΡŒΠΊΠΎ ΠΎΠ΄Π½ΠΎΠ³ΠΎ ΡƒΠ·Π»Π° сСрдца — сино-Π°Ρ‚Ρ€ΠΈΠ°Π»ΡŒΠ½ΠΎΠ³ΠΎ ΡƒΠ·Π»Π° (БАУ), ΡΠ²Π»ΡΡŽΡ‰Π΅Π³ΠΎΡΡ основным кардиостимулятором сСрдца [20].МногиС Π°Π»Π³ΠΎΡ€ΠΈΡ‚ΠΌΡ‹ управлСния динамичСскими систСмами Π±Π°Π·ΠΈΡ€ΡƒΡŽΡ‚ΡΡ Π½Π° ΠΎΠ±Ρ€Π°Ρ‚Π½ΠΎΠΉ связи, Π² ΠΊΠΎΡ‚ΠΎΡ€ΠΎΠΉ задСйствуСтся ΠΏΠΎΠ»Π½Ρ‹ΠΉ Π²Π΅ΠΊΡ‚ΠΎΡ€ состояния динамичСской систСмы. Однако Π½Π° ΠΏΡ€Π°ΠΊΡ‚ΠΈΠΊΠ΅ ΠΏΠΎΠ»Π½Ρ‹ΠΉ Π²Π΅ΠΊΡ‚ΠΎΡ€ состояния извСстСн Π½Π΅ всСгда. Π’Π°ΠΊ, Π² случаС элСктричСской активности сСрдца ΠΈΠ·ΠΌΠ΅Ρ€ΡΡŽΡ‚ ΠΏΠΎΡ‚Π΅Π½Ρ†ΠΈΠ°Π»Ρ‹ ΡƒΠ·Π»ΠΎΠ², Π° скорости ΠΈΡ… измСнСния Π½Π΅ ΠΈΠ·ΠΌΠ΅Ρ€ΡΡŽΡ‚ΡΡ. Для восстановлСния ΠΏΠΎΠ»Π½ΠΎΠ³ΠΎ Π²Π΅ΠΊΡ‚ΠΎΡ€Π° состояния ΠΏΠΎ ΠΈΠΌΠ΅ΡŽΡ‰ΠΈΠΌΡΡ измСрСниям часто ΠΏΡ€ΠΈΠΌΠ΅Π½ΡΡŽΡ‚ Π½Π°Π±Π»ΡŽΠ΄Π°Ρ‚Π΅Π»ΠΈ состояния.Π’ Π΄Π°Π½Π½ΠΎΠΉ Ρ€Π°Π±ΠΎΡ‚Π΅ Ρ€Π΅ΡˆΠ°Π΅Ρ‚ΡΡ Π·Π°Π΄Π°Ρ‡Π° построСния Π½Π°Π±Π»ΡŽΠ΄Π°Ρ‚Π΅Π»Ρ с Π»ΠΈΠ½Π΅ΠΉΠ½ΠΎΠΉ Π΄ΠΈΠ½Π°ΠΌΠΈΠΊΠΎΠΉ ошибки [22,25]. НСобходимым условиСм сущСствования Ρ‚Π°ΠΊΠΎΠ³ΠΎ Π½Π°Π±Π»ΡŽΠ΄Π°Ρ‚Π΅Π»Ρ являСтся Π½Π°Π±Π»ΡŽΠ΄Π°Π΅ΠΌΠΎΡΡ‚ΡŒ систСмы. ДостаточныС условия ΠΌΠΎΠΆΠ½ΠΎ ΡΡ„ΠΎΡ€ΠΌΡƒΠ»ΠΈΡ€ΠΎΠ²Π°Ρ‚ΡŒ Π² Ρ€Π°ΠΌΠΊΠ°Ρ… Π΄ΠΈΡ„Ρ„Π΅Ρ€Π΅Π½Ρ†ΠΈΠ°Π»ΡŒΠ½ΠΎ-гСомСтричСского ΠΏΠΎΠ΄Ρ…ΠΎΠ΄Π° [25] с использованиСм ΠΈΠ΄Π΅ΠΉ двойствСнности [25,26]. Π’ Ρ€Π°ΠΌΠΊΠ°Ρ… этого ΠΏΠΎΠ΄Ρ…ΠΎΠ΄Π° ΠΌΠΎΠΆΠ½ΠΎ Ρ€Π°Π·Ρ€Π°Π±ΠΎΡ‚Π°Ρ‚ΡŒ Π°Π»Π³ΠΎΡ€ΠΈΡ‚ΠΌ построСния Π½Π°Π±Π»ΡŽΠ΄Π°Ρ‚Π΅Π»Ρ. Π’ Ρ€Π°Π±ΠΎΡ‚Π΅ для Π΄Π²ΡƒΠΌΠ΅Ρ€Π½Ρ‹Ρ… систСм Ρ€Π΅ΡˆΠ°Π΅Ρ‚ΡΡ общая Π·Π°Π΄Π°Ρ‡Π° построСния Π½Π°Π±Π»ΡŽΠ΄Π°Ρ‚Π΅Π»Ρ, Π·Π°Ρ‚Π΅ΠΌ ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Π½Ρ‹Π΅ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ ΠΏΡ€ΠΈΠΌΠ΅Π½ΡΡŽΡ‚ΡΡ ΠΊ ΠΌΠΎΠ΄Π΅Π»ΠΈ кардиостимулятора Π½Π° основС осциллятора Π’Π°Π½ Π΄Π΅Ρ€ Поля. Π Π°Π±ΠΎΡ‚Π° построСнного Π½Π°Π±Π»ΡŽΠ΄Π°Ρ‚Π΅Π»Ρ ΠΈΠ»Π»ΡŽΡΡ‚Ρ€ΠΈΡ€ΡƒΠ΅Ρ‚ΡΡ ΠΏΡƒΡ‚Π΅ΠΌ числСнного модСлирования

    The Dini Derivative and Generalization of the Direct Lyapunov Method

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    The contemporary theory of stability for systems of differential equations is based on the concept of Lyapunov stability, A.M.Β Lyapunov’s results and their certain generalizations. Analysis of the first approximation of a system is used as a main method to study a stability of the equilibrium points. In publications this method is known as the first Lyapunov method. But this method does not allow drawing conclusions in the critical case, and then the second Luapunov method can be used, which is also known as a direct Lyapunov method.The direct Lyapunov method is based on existing function with certain properties. The function has to be positive definite. If in the certain vicinity of the equilibrium point a function derivative by virtue of the system is not positive, then it is called Lyapunov function. The existence of Lyapunov function means that the equilibrium point is stable.A role of the Lyapunov function is not only to establish the fact of the equilibrium point stability (or stronger property of asymptotic or exponential stability). It gives a lower bound of the region of attraction of an equilibrium point, which can be important in the control theory. So, to construct the Lyapunov function is a problem of importance, even if the fact of equilibrium stability has been already established.Herewith there are no universal methods to construct the Lyapunov function for the autonomous system of differential equations. To solve the problem are used various numerical methods in which it is difficult to provide the important conditionΒ β€”differentiability of function under construction. At the same time, in the Lyapunov method the differentiability condition is non-essential and is related only to the mathematical technique. Therefore, generalizations of the Lyapunov method, which are directed to the abandonment of strong conditions of function smoothness, are important. One of such generalizations is the use of the Dini derivative. The use of the Dini derivative allows us to construct, for example, the piecewise linear Lyapunov functions.The results connected with the Dini derivative are rarely included in standard monographs, and an objective of the present article is to make these results more accessible

    Realization of the Iteration Procedure in Localization Problems of Autonomous Systems

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    In the last 15 years one way for a qualitative analysis of dynamical systems was formed i.e. the localization of invariant compact sets of a dynamical system. Here the localization means creating a system of such sets, which contain all invariant compact sets of a dynamic system [1], in the phase space.Invariant compact sets are closely connected with bounded trajectories of the system, the structure of which in the phase space play key role in many applications of dynamical system theory. The problems of invariant compact sets localization abut upon other important problems, for instance, the problems of estimation of attractor basins, control problems, etc.Back investigations of localization problems was oriented both to development of solving methods [28] and to investigation of particular dynamical systems encountered in applications (see, for example, [9 { 16]).One of quite efficient methods of localization problem solving is based on smooth functions defined in the phase space. It is so called functional method [1 { 3]. Effectiveness of the method is enhanced when we use several functions. Thus, using the next function gives the restriction of the already constructed localizing set. An iteration procedure for sequential narrowing of the localizing set [1 { 2] arises.The paper presents analysis of the iteration procedure, which naturally occur in the autonomous systems of special type where the right side of each differential equation is resolvable relative to the corresponding phase variable. Such systems are encountered in applications [17].</p

    The Qualitative Analysis of a Lorenz-Type System

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    In modern natural sciences, the term of a dynamic system plays an important role and is a common type of mathematical models. Dynamical systems are rarely come to simple functional dependencies. Therefore, qualitative analysis methods of dynamical systems are crucial. In the paper, we consider the simplest type of dynamic systems | continuous dynamical systems described by the systems of ordinary differential equations.Qualitative analysis of differential equations systems usually starts with a search for equilibrium points and a study of the behaviour of a dynamic system in the neighborhood of each equilibrium points. The main attention is paid to the stability of equilibrium, as well as their behaviour type classification. Effective qualitative analysis of differential equations systems is best approached through the bifurcation theory which explains modification of quality in the behaviour of a dynamic system if its parameters are changed.In the behavior of dynamic systems, in addition to the equilibrium points, other bounded trajectories (for example, boundary cycles or separatrix) and their certain conglomerates (such as attractors, invariant tori) play an important role. Investigation of bounded trajectories, in particular, attractors is a difficult task and a lot of scientific articles deal with this problem.In this paper, we study a continuous Lorenz-type system. For this system, all of the equilibrium points are defined and the analysis of equilibrium points types are performed in accordance with the system parameters. The analysis of some bifurcations of equilibrium points are carried out. In particular, the Andronov | Hopf bifurcation is determined and it is shown that it leads to a bifurcation of boundary cycles.DOI: 10.7463/mathm.0315.078949

    The plane motion control of the quadrocopter

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    Among a large number of modern flying vehicles, the quadrocopter relates to unmanned aerial vehicles (UAV) which are relatively cheap and easy to design. Quadrocopters are able to fly in bad weather, hang in the air for quite a long time, observe the objects and perform many other tasks. They have been applied in rescue operations, in agriculture, in the military and many other fields.For quadrocopters, the problems of path planning and control are relevant. These problems have many variants in which limited resources of modern UAV, possible obstacles, for instance, for flying in a cross-country terrain or in a city environment and weather conditions (particularly, wind conditions) are taken into account. Many research studies are concerned with these problems and reflected in series of publications (note the interesting survey [1] and references therein). Various methods were used for the control synthesis for these vehicles: linear approximations [2], sliding mode control [3], the covering method [4] and so on.In the paper, a quadrocopter is considered as a rigid body. The kinematic and dynamic equations of the motion are analyzed. Two cases of motion are emphasized: a motion in a vertical plane and in a horizontal plane. The control is based on transferring of the affine system to the canonical form [5] and the nonlinear stabilization method [6].DOI: 10.7463/mathm.0215.078947

    The Behavior of a Two-Component Population System in Vicinity of the Zero Equilibrium Point

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    A clinical behaviour of the cell-based therapy in recent decades has encouraged a great interest in the culture of cell populations in vitro. One of the directions of cell therapy is transplantation of stem cells. The cell material for transplantation is obtained by culturing the patient’s cells. However, there are often problems because of the genetic mutations of cells in the process of culture, namely, the degeneration of a portion of mutated cells into "immortal" (cancerous) cells, which makes the transplantation of such material unsafe for a patient. To study development dynamics of the cell populations in vitro is quite costly. Such studies are, usually, conducted at the beginning of culture, in the middle of the process, and when completing the process of culture. It is difficult to judge t the cell population development in detail by such data. Here mathematical modelling is of importance.The papers [8-11] propose a cell population system consisting of two types of cells, namely normal (healthy) and abnormal (aneuploid) cells. Interest in such a population system is due to the fact that, although the aneuploid cells have a life time less than the normal ones, a small portion of the aneuploid cells can degenerate into practically "immortal" cancer cells, whose population may, eventually, become dominant.In the qualitative analysis of the nonlinear dynamic systems, a standard component is information on the number of rest points, their nature and location. Earlier, [16] a detailed study of the rest points and their possible nature was performed depending on the biological parameters, such as the proportion of dead cells, the average time of the cell cycle, the proportions of normal cells becoming the population of abnormal ones, etc. However, there is no exhaustive answer, yet, concerning this issueThe paper continues to study the two-component population model considered earlier [9-11, 16]. The study focuses on the zero equilibrium point. The conditions of stability are specified taking into account the fact that the dynamic system, by virtue of its biological content, must be considered in the first quadrant of the plane. In addition, a study of the zero equilibrium point has been conducted in critical cases in which the method to investigate linear approximation stability the does not work
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