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Models for Physiological Systems 2 J. M. Lemos-INESC-ID/IST T. Mendonça-FC UP Summary ! A basic principle for writing state equations: The law of mass action. ! HIV 1 infection: State space, equilibrium points and linearised dynamics. ! Modelling anaesthesia: Compartmental models and Wiener models. ! Models at a glance. Models for Physiological Systems 3 J. M. Lemos-INESC-ID/IST T. Mendonça-FC UP Can we build mathematical models for physiological systems? Physiological systems are very complex. They are made of cells and tissues that interact in complex ways to perform the functions required by living beings. Yet, the basic mechanisms are relatively simple, relying in many cases in basic principles from Chemistry and Physics (e. g. Electricity). Thus, it is possible to build tractable mathematical models in the form of differential or difference equations. A key issue is variability: The parameters entering the mathematical model vary from individual to individual and, very often, in the same individual as time passes. Models for Physiological Systems 4 J. M. Lemos-INESC-ID/IST T. Mendonça-FC UP Objective The objective of this lecture is to illustrate how the use basic principles may be used in a few examples to yield models of physiological systems (sometimes called mechanistic models) that are useful for modelling or control design. The treatment of the subject is by no means exhaustive. People interested are invited to pursue the subjects of their interest in the literature, e. g. the references quoted in the end of this lecture.
2012
Although mathematical modeling has a long and very rich tradition in physiology, the recent explosion of biological, biomedical, and clinical data from the cellular level all the way to the organismic level promises to require a renewed emphasis on computational physiology, to enable integration and analysis of vast amounts of life-science data. In this introductory chapter, we touch upon four modeling-related themes that are central to a computational approach to physiology, namely simulation, exploration of hypotheses, parameter estimation, and modelorder reduction. In illustrating these themes, we will make reference to the work of others contained in this volume, but will also give examples from our own work on cardiovascular modeling at the systems-physiology level.
Rossiĭskii fiziologicheskiĭ zhurnal imeni I.M. Sechenova / Rossiĭskaia akademiia nauk
The article illustrates the method of mathematical modelling in physiology as a unique tool to study physiological processes. A number of demonstrated examples appear as a result of long-term experience in mathematical modelling of electrical and mechanical phenomena in the heart muscle. These examples are presented here to show that the modelling provides insight into mechanisms underlying these phenomena and is capable to predict new ones that were previously unknown. While potentialities of the mathematical modelling are analyzed with regard to the myocardium, they are quite universal to deal with any physiological processes.
2004
The purpose of this book is to study mathematical models of human physiology. The book is a result of work by Math-Tech (in Copenhagen, Denmark) and the BioMath group at the Department of Mathematics and Physics at Roskilde University (in Roskilde, Denmark) on mathematical models related to anesthesia simulation. The work presented in this book has been carried out as part of a larger project SIMA (SIMulation in Anesthesia) 1 , which has resulted in the production of a commercially available anesthesia simulator and several scientific research publications contributing to the understanding of human physiology. This book contains the scientific contributions and does not discuss the details of the models implemented in the SIMA project.
Signals and Systems in Biomedical Engineering: Physiological Systems Modeling and Signal Processing, 2019
Model-Based Analysis of Physiological Systems Sometimes a computing machine does do something rather weird that we hadn't expected. In principle one could have predicted it, but in practice it's usually too much trouble.-Alan Turing Physiological modeling involves the development of mathematical, electrical, chemical, or other analogs whose behavior closely approximates the behavior of a particular physiological system. Such models allow us to extend intuitive knowledge gained in one area to another less familiar area. The earliest models of physiological system were physical analogies. Even now many students in high school are introduced to the ideas of respiration and blood flow using physical models involving air flow and water in tubes, respectively. Mathematical descriptions of physiological systems use differential equations and the analysis of these systems requires solving differential equations. Such solutions of differential equations can in principle be done analytically (i.e., on paper), physically (i.e., by building a physical analog), or numerically (i.e., on a digital computer). With modern personal computers, the last of these options is very attractive. Since models rely on experimental data to provide the basic relationship between parameters, the accuracy of the model rests on the accuracy of the experimental measurement. The majority of contemporary models are computer based, using computational solutions of equations and graphical presentations to analyze and simulate the system under study. 7.1 Biophysical and Black Box Models There are two main approaches to modeling physiological systems and the choice of either approach depends on the end purpose and the ease of implementation. The first approach is to obtain a set of mathematical equations that will mimic
Bioengineering
Mathematical models can improve the understanding of physiological systems behaviour, which is a fundamental topic in the bioengineering field. Having a reliable model enables researchers to carry out in silico experiments, which require less time and resources compared to their in vivo and in vitro counterparts. This work’s objective is to capture the characteristics that a nonlinear dynamical mathematical model should exhibit, in order to describe physiological control systems at different scales. The similarities among various negative feedback physiological systems have been investigated and a unique general framework to describe them has been proposed. Within such a framework, both the existence and stability of equilibrium points are investigated. The model here introduced is based on a closed-loop topology, on which the homeostatic process is based. Finally, to validate the model, three paradigmatic examples of physiological control systems are illustrated and discussed: the ...
Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences, 2006
Computational modelling of biological processes and systems has witnessed a remarkable development in recent years. The search-term ( modelling OR modeling ) yields over 58 000 entries in PubMed, with more than 34 000 since the year 2000: thus, almost two-thirds of papers appeared in the last 5–6 years, compared to only about one-third in the preceding 5–6 decades. The development is fuelled both by the continuously improving tools and techniques available for bio-mathematical modelling and by the increasing demand in quantitative assessment of element inter-relations in complex biological systems. This has given rise to a worldwide public domain effort to build a computational framework that provides a comprehensive theoretical representation of integrated biological function—the Physiome. The current and next issues of this journal are devoted to a small sub-set of this initiative and address biocomputation and modelling in physiology, illustrating the breadth and depth of experim...
2007
Although recent enthousiasm has emerged for Systems Biology, it is of major importance to identify the roots it has with computational (mathematical) modeling. In fact, major contributions have been made for decades with the aim to quantitatively analyze and model the function of living systems in order, ultimately, to better understand the underlying constituents and collective behaviors and use them for diagnosis and therapeutic purposes. However, the impressive evolution of technological resources and methods allows today to revisit these early attempts and to bring to light new concepts, targets, and expectations. This chapter, after a tentative definition of the generic elements behind Systems Biology and Physiology, will provide a review of current efforts devoted to multimodal, multilevel, multiresolution approaches, all being addressed from the joint observational, modeling and information processing points of view. The several theoretical frames at our disposal will also be addressed, in particular the capability to handle multiple modeling formalisms. Examples from the literature and the research conducted by the authors will exemplify these multidisciplinary developments and results. The forthcoming challenges to be faced will then be outlined.
2015
The paper gives a summary of 2014 year results in the topic of physiological modeling and control achieved by the Physiological Controls Group of the Obuda University. The presentation is integrated in the tradition established years ago at IEEE INES conferences and 2014's IEEE SACI conference summarizing the latest results obtained by the group. Four topics are presented, highlighting collaboration with our partner research institutes as well: modern robust control of diabetes, antiangiogenic model-based tumor control, biostatistical modeling methods of diabetes, control of peristaltic pumps in hemodialyisis problem. I.
2018
Biological systems such as cell cycle are complex systems consisting of an enormous number of elements. These elements interact in ways that produce nonlinear and complex systems behaviour such as oscillations. A number of modelling approaches have been used to explain these kinds of systems; they are classified into four classes (continuous, discrete, stochastic and hybrid). Ordinary Differential Equations (ODEs) are used to mimic the continuous dynamic behaviour of system components, while discrete models can simulate the biological elements as straightforward binary variables providing a qualitative view of system behaviour. Stochastic models are used to model the effect of noise in biological systems. Combined methods together introduce hybrid models to cover the limitations of individual models and take advantage of their strengths. This study introduces a series of advanced models with increasing resolution from discrete to continuous in a systematic way to model the mammalian...
1998
Finite-difference numerical methods are developed for the solution of some systems in the biomedical sciences; namely, a predator-prey model and the SEIR (Susceptible/Exposed/ Infectious/Recovered) measles model. First-order methods are developed to solve the predator-prey model and one second-order method is developed to solve the SEIR measles model. The predator-prey model is extended to one-space dimension to incorporate diffusion. The SEIR measles model is extended to one-space dimension to incorporate (i) diffusion, (ii) convection and (iii) diffusion-convection. The SEIR measles model is extended further to model diffusion in two-space dimensions. The reaction terms in these systems of partial differntial equations contain nonlinear expressions. Nevetheless, it is seen that the numerical solutions are obtained by solving a linear algebraic system at each time step, as opposed to solving a nonlinear algebraic systems, which is often required when integrating non-linear partial differential equations. The development of each numerical method is made in the light of experience gained in solving the system of ordinary differential equations for each system.
2007
2 3.1. Structured population modeling 3.1.1. Structured modeling in demography and epidemiology 3.1.2. Invasion processes in fragile isolated environments 3.1.3. Indirectly transmitted diseases 3.1.4. Direct movement of population 3.2. Optimal control problems in biomathematics 3.2.1. Disease control 3.2.2. Controlling the size of a population 3.2.3. Public prevention of epidemics in an optimal economic growth model 3.2.4. Age structured population dynamics as a problem of control 3.3. Developping mathematical methods of optimal control, inverse problems and dynamical systems; software tools 3.3.1. Inverse problems : application to parameter identification and data assimilation in biomathematics 3.3.2. Dynamic programming and factorization of boundary value problems 3.3.3. Applications of the factorization method to devise new numerical methods 3.3.4. Differential equations with delay modeling cellular replication 3.3.5. Tools for modeling and control in biomathematics 3.4. Application fields and collaborations with biologists 3.4.1. Epidemiology 3.4.1.1. Brucellosis 3.4.1.2. HIV-1 Infection in tissue culture 3.4.1.3. Contamination of a trophic chain by radionuclides 3.4.2. Blood cells 3.4.2.1. Generating process for blood cells (Hematopoiesis) 3.4.2.2. Malignant proliferation of hematopoietic stem cells 3.4.2.3. Socio-biological activities of the Immune-System cells 3.4.3. Modeling in viticulture; collaboration with INRA 3.4.3.1. Integrated Pest Management in viticulture. 3.4.3.2. Spreading of a fungal disease over a vineyard 3.4.4. Modeling in neurobiology 3.4.4.1. The biological model of aplysia 3.4.4.2. MEG-EEG inverse problem 3.4.4.3. Inverse problem for Aplysia's ganglion model 3.4.4.4. Modeling of the treatment of Parkinson's disease by deep brain stimulation
Biosystems Engineering: Biofactories for Food Production in the Century XXI, 2014
Mathematics is an important tool for system modeling allows us to describe the behavior of a phenomenon or system in the real world, in particular biological systems. This chapter gives an overview of mathematical models, their construction, types of models, and examples of possible applications in biosystems models. Essential for building a model is determining its scope. In addition, the mechanistic and phenomenological mathematical models are described. Applications on fish biomass estimation, quality of fruits and crops are presented.
Texts in Applied Mathematics, 2002
Annals of Biomedical Engineering, 2000
Effective modeling of nonlinear dynamic systems can be achieved by employing Laguerre expansions and feedforward artificial neural networks in the form of the Laguerre-Volterra network ͑LVN͒. This paper presents a different formulation of the LVN that can be employed to model nonlinear systems displaying complex dynamics effectively. This is achieved by using two different filter banks, instead of one as in the original definition of the LVN, in the input stage and selecting their structural parameters in an appropriate way. Results from simulated systems show that this method can yield accurate nonlinear models of Volterra systems, even when considerable noise is present, separating at the same time the fast from the slow components of these systems effectively.
Since its "foundation," computational intelligence has been creating novel-high perspectives on modeling, on the other hand, the "old-fashioned" mathematics offers powerful methods that should not be forgotten or underestimated. On this paper, it is discussed a novel methodology proposed by the authors on the mathematical modeling, with emphasis in biomedical and biological modeling. The methodology comprises of an attempt to use simultaneously mathematics and computational intelligence in a single picture, using the concept of blindness of a model. The methodology proposed can be summarized into the name of "the middle-way-out principle." Besides the theory is presented and discussed, no real problem is treated, it is left to future works, due to the choice of the authors and current incipient state of the theory. The paper is concluded with some conclusions and final remarks, the main references used all over the work are presented in the end.
Proc. Second Symp. Biomed. Infor. Manag. Systems, 1987
Physiological research on many mechanisms has reached the subcellular and molecular level. While molecules have been identified for some processes, it is not yet possible to describe physiological function directly in terms of molecular structure. The state diagram, as used in chemical kinetics, is an ideal language for expressing hypotheses of physiological mechanism at the subcellular and molecular level. No only does a state diagram express a hypothesis in specific, quantitative terms, it also facilitates the inclusion of physical constraints such as conservation laws and chemical data. Approximations and graphical methods frequently used to simplify the solution of state diagrams are shown to be inaccurate and should now be replaced by direct computer solutions of the kinetic equations.
Journal of General Physiology, 2011
Readers of the current issue will find something unfamiliar, perhaps tantalizing, perhaps unsettling. I am referring to the articles by Cha et al. (see "Ionic mechanisms and Ca 2+ dynamics..." and "Time-dependent changes in membrane excitability..."). The first of these articles is less exotic; it presents computer simulations of a model for bursting electrical activity in pancreatic cells. The second uses bifurcation diagrams to analyze the behavior of the model. I will argue that this is relevant far beyond cells-the leading edge of a wedge driving the methods of dynamical systems theory into the heart of biology. Mathematical modeling of cell electrical activity has a long history in physiology, going back to the work of Hodgkin and Huxley (Hodgkin and Huxley, 1952; Chay and Keizer, 1983) for action potential generation and propagation in squid giant axon. The model of Cha et al. (2011a,b) is based on the Hodgkin and Huxley formalism, but augmented with mechanisms for maintaining ionic balance (pumps and exchangers for Ca 2+ , Na + , and K + , and the endoplasmic reticulum). In addition, a nod is given in the direction of metabolism, as cells are first and foremost metabolic sensors and use ATP-dependent K + (K(ATP)) channels, to transduce the rate of glucose metabolism into intensity of electrical activity. Cha et al. (2011a,b) follow the path blazed by Chay and Keizer (1983). Their model was based on the simple idea, first proposed by Atwater et al. (1980), that bursting results from slow modulation of spiking by calcium. That is, during the active spiking phase of the burst, calcium builds up and turns on calcium-activated K + (K(Ca)) channels until membrane potential falls below the threshold level and spiking terminates. During the ensuing silent phase, calcium would be pumped out of the cell, lowering the spike threshold and allowing the next active phase to begin. Rinzel (1985) formalized this mathematically, recognizing that the key element of Chay-Keizer was a fast spiking system modulated by slow negative feedback. This led to a profusion of models, different biophysically but essentially equivalent mathematically, with alternate proposals for the source of the negative feedback. These included inactivation of the L-type Ca 2+ channel (Chay, 1990), indirect activation of K(ATP) channels by Ca 2+ via its effects on ATP consumption or production (Keizer and Magnus, 1989
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