Physiological and Engineering control system look similar to each other. A physiological control system explores some control problem related to biological environment and provides solution to the control researchers. The involvement of control theory makes the biomedical application more efficient and natural. The control mechanism in the biomedical application that comprises components that are necessary for maintenance of homeostasis at all levels of living systems is discussed in this chapter. The positive and negative feedback control mechanisms for maintaining homeostasis are also discussed.
The collection of trillions of cells composes the human body functions in a pattern that is essential for continuation of life process. In physiological control system the human body is considered as a system and the internal environment of the human body refers to each and everything present within the body where the cells live and work together. A specific optimum condition should be maintained within the body for proper functioning of cells which in turn makes the tissues, organs and the total system work properly. It is also necessary that the composition and fluid temperature around the cells must be constant for the cells to survive and function properly.
Homeostasis is the property of a system that helps in maintaining the consistency of the internal environment of the system. In addition, homeostasis can be defined as the property in which the variables of the system are regulated for maintaining a stable and relatively constant environment in the internal environment of the system despite the changes in the external environment. At the optimal temperature, when the internal environment of a system has optimal concentration of gases, nutrients, ions and water, the system is in homeostasis condition. The relationship between the human body and homeostasis is shown in Fig. 12.1. The human body will be operated in such a way that the homeostasis is maintained and it is essential for the survival.
Fig. 12.1 ∣ Relationship between human body and homeostasis
The properties of physiological control systems are:
The characteristic curve of a physiological control system that depicts the properties of the system is shown in Fig. 12.2.
Fig. 12.2 ∣ Characteristic curve of a control system
The special properties of a physiological control system are:
The different systems in the human body—digestive system, circulatory system, respiratory system, excretory system, nervous system, endocrine system, immune system, musculoskeletal system and integumentary system—help in their own way for maintaining the homeostasis in the internal environment. Therefore, the following points are the collective target of the human body or homeostasis:
All the organs present within a body act together through a combination of hormonal and nervous mechanisms for maintaining the homeostasis in the internal environment of the body. In day-to-day activities, the functions such as regulation of respiratory gases, protection against disease agents (pathogens), fluid and salt balance maintenance, regulation of energy and nutrient supply and maintenance of constant body temperature are regulated by the human body. In addition, when the human body gets injured, it must have the capability to repair itself. The following reasons cause an imbalance in the homeostasis:
Some examples of homeostatic imbalances are high core temperature, increase in concentration of salt in the blood or decrease in concentration of oxygen which generate sensations such as warmth, thirst or breathlessness.
The control mechanism used for maintaining the consistency of the internal environment is called homeostasis control mechanism. The homeostasis control mechanism is designed to re-establish homeostasis when there is an imbalance in the internal environment due to improper functioning of cells or due to external environment disturbances. The behaviour such as removal of sweater, drinking of water or slowing down the biological process will result in restoration of homeostatic imbalances that are listed in the previous section.
The homeostatic control mechanism should have at least three parts for restoring the homeostasis imbalances. The simple homeostatic control mechanism is shown in Fig. 12.3.
Fig. 12.3 ∣ Homeostatic control mechanism
The three major parts that are available in the control mechanism as shown in Fig. 12.3 alongwith the functions are listed below:
The homeostatic control mechanism can be clearly understood with the help of an example. If the human body (system) senses hyperglycaemia, i.e., high blood sugar level, it is a homeostasis imbalance and the control mechanism must take necessary actions to balance the blood sugar level. The three major parts required for correcting this imbalance are listed below alongwith their functions.
For the above example, sensor and control centre are the same. Hence, only two parts exist in the control mechanism for maintaining the blood sugar level, i.e., homeostasis imbalance.
The block diagram representing a typical physiological control system is shown in Fig. 12.4.
Fig. 12.4 ∣ Block diagram of physiological control system
The set point is the pre-defined and pre-set value and the optimum value of a parameter. The sensor continuously monitors the value of the parameter and sends the real-time value to the control centre. The control centre compares the real time and pre-defined value of the parameter and generates an error signal and in turn generates a response signal, i.e., stimulus. Finally, the effector takes the signal generated from the control centre and makes the parameter value to be maintained at a pre-defined value. The example discussed in Section 12.3.3 can be represented in the form of a block diagram as shown in Fig. 12.5.
Fig. 12.5 ∣ Physiological control system for maintaining blood sugar level
Any physical system has the natural tendency towards disorderliness and the control mechanism should work in such a way that the orderliness is maintained. Although the physiological control system performs to maintain the constancy of the homeostasis, the main objective is to achieve the steady-state value. The three methods by which the steady state can be achieved are feedback, hierarchical communication and adaptation.
If the external disturbances exist in the physiological control system, then it is called extrinsic; otherwise, it is called intrinsic. If the homeostatic control mechanism fails to restore the homeostasis imbalance in the internal environment when the external disturbance is high, then the living organism will engage in a behaviour such that the homeostasis imbalance is rectified.
The control mechanism can be classified into different types based on the feedback mechanism. The two different types of feedback mechanism are positive feedback mechanism and negative feedback mechanism. The detailed description of these two types of mechanism alongwith their advantages and disadvantages is discussed here. In a positive feedback control mechanism, the set point and output values are added. In a negative feedback control mechanism, the set point and output values are subtracted.
The positive feedback control mechanism is used by a very few organs in the system. Mostly, this is used for intensifying a change instead of correcting it. In positive feedback mechanism, the system acts in such a way that the imbalance or the perturbation increases. In addition, the positive feedback mechanism leads to a vicious cycle, i.e., when A produces more of B, B produces more of A. Further, the positive feedback mechanism acts in such a way that the stimulus gets intensified. In some cases, it is necessary to increase the stimulus. The general block diagram of positive feedback control mechanism is shown in Fig. 12.6.
Fig. 12.6 ∣ Positive feedback control system
The example of positive feedback mechanism is shown in Fig. 12.7, which regulates the child birth.
Fig. 12.7 ∣ Positive feedback mechanism
Also, examples for the positive feedback mechanism that leads to harmful effects are shown below:
The negative feedback mechanism is used in the system for reducing the homeostatic imbalance. Mostly, this is used for making the system self-regulatory so that the stability of the system can be achieved by reducing the effect of fluctuations. In negative feedback mechanism, right amount of corrective measure is applied in the most timely manner, which can make the system very stable, accurate and responsive. The general block diagram of negative feedback control mechanism is shown in Fig. 12.8.
Fig. 12.8 ∣ Negative feedback control system
The simplest and most fundamental of the physiological control system is the muscle stretch reflex. The knee jerk reflex, an example of muscle stretch reflex is used as a routine medical examination in assessing the state of the nervous system. When a sharp tap is given to the patellar tendon in the knee, it leads to an abrupt stretching of the thigh muscle to which patellar tendon is attached. The muscle spindles called stretch receptors get activated due to the stretch in the thigh muscle. The information about the magnitude of the stretch gets encoded by the neural impulses and is sent to the spinal cord of the system through the afferent nerve fibers. The different motor neurons connected to different afferent nerves get activated. This sends the efferent neural impulses back to the same thigh muscle that produces a contraction of the muscle and hence results in extension of knee joint. This concept of reflex is shown in Fig. 12.9.
Fig. 12.9 ∣ Concept of reflex
The block diagram representing this type of reflex is shown in Fig. 12.10. In this example, the thigh muscle corresponds to the plant or controlled system. The initial stretch produced by taping the knee is known as disturbance . The input of the feedback sensor will be the amount of stretch , which is produced in proportion to the . The feedback sensor, i.e., muscle spindle, translates into an increase in afferent neural signal sent to the reflex centre or the controller. The reflex centre in this system will be the spinal cord. The output of the controller will increase the efferent neural signal , which is directed back to the thigh muscle. This is an example of negative feedback system, since the initial tap-induced disturbance leads to a controller action that reduces the effect of the disturbance.
Fig. 12.10 ∣ Block diagram representation of the muscle stretch reflex
Some more examples of negative feedback mechanism are:
Advantages
The advantages of negative feedback mechanism are:
The differences between engineering and physiological control systems are given in Table 12.1.
Table 12.1 ∣ Comparison of engineering control system with physiological control system
The different system elements are resistance capacitance and inductance. The definitions of these elements are obtained with the help of electrical circuits and then analogous to different systems are discussed.
The Ohm's law used for determining the electrical resistance R is given by
(12.1)
where V is the voltage or driving potential across the resistor and I represents the current flowing through it. In physiological control system, V is taken as the “through” variable, called a measure of “effort” and denoted by and I is taken as the “through” variable, called a measure of “flow” and denoted by .
Therefore, in physiological control system, resistance is obtained as:
(12.2)
In electrical system, the generalized system property for storage is taken in the form of capacitance, which is defined as the amount of electrical charge (q) stored in the capacitor per unit voltage (V). Here, the relation between voltage and current is given by
(12.3)
Thus, in physiological control system, we obtain
(12.4)
The final property of electrical system that stores kinetic energy is inductance. The relation between the voltage and current relating the inductance is given by
(12.5)
Thus, in physiological control system, we obtain
(12.6)
The analogous of physiological system with other systems such as electrical, mechanical, fluid, thermal and chemical are shown in Table 12.2.
Table 12.2 ∣ Analogy of variables in physiological system with other systems
The Kirchoff's voltage law and current law govern the electrical system. Therefore, by applying Kirchoff's voltage law for physiological system shown in Fig. 12.11, we obtain
() + () + () = 0(12.8)
Similarly, applying Kirchoff's current law for physiological system shown in Fig. 12.11, we obtain
(12.9)
Fig. 12.11 ∣ Generalized system elements network model
The elements connected in series: The resultant or equivalent value of the elements connected in series is calculated similar to the calculation used in electrical system.
Resistors in series: When the resistors are connected in series as shown in Fig. 12.12(a), the equivalent resistance is the summation of individual resistance values, i.e.,
Capacitors in series: When the capacitors are connected in series as shown in Fig. 12.12(b), the equivalent capacitance is calculated as:
The elements connected in parallel: The equivalent value of the elements connected in parallel are calculated similar to the calculation used in electrical system.
Resistors in parallel: When the resistors are connected in parallel as shown in Fig. 12.12(c), the equivalent resistance is calculated as:
Capacitors in parallel: When the capacitors are connected in parallel as shown in Fig. 12.12(d), the equivalent capacitance is determined as the summation of individual capacitance values, i.e.,
Fig. 12.12 ∣ Model properties of system elements in physiological system: (a) resistors connected in series, (b) capacitors connected in series, (c) resistors connected in parallel and (d) capacitors connected in parallel
The mathematical models are derived in this section, which characterize the input–output properties of two simple physiological models: lung mechanism and skeletal muscle.
The working of lung mechanism should be studied before deriving the mathematical model of the system. The process of modelling the lung mechanism is explained below.
Airways are divided into two categories: the larger or central airways and the smaller or peripheral airways. The fluid mechanical resistances of the two categories of airways are and respectively. The chest wall cavity gets expanded by the volume of air entering the alveoli. The chest wall gets expanded by the same amount of air entering the lungs. This relation is given by the series connection of lung and chest wall compliances represented by and respectively. However, due to the presence of compliance of central airways and gas compressibility, a small fraction of volume of air is shunted away from the alveoli represented by shunt compliance, . In normal circumstances, this shunted volume is very small and if is increased or if or is decreased, it may lead to disease. This effect is taken into consideration by placing in parallel with and . The lung model developed with the help of these variables is shown in Fig. 12.13.
Let the pressures developed at different points of lung model shown in Fig. 12.13 be at the airway opening, at the central airways, in the alveoli and in the pleural space. The reference pressure or the ambient pressure is taken as which can be set to zero. If the flow rate of air entering the respiratory system is Q, the flow delivered to alveoli is , then the flow shunted away from alveoli be and also a mathematical relationship between and Q can be derived by as follows:
Using Kirchhoff's law to the circuit shown in Fig. 12.13,
(12.10)
and
(12.11)
Fig. 12.13 ∣ Linear model of respiratory mechanics
Differentiating Eqn. (12.10) with respect to , we obtain
Rearranging the above equation, we obtain
Substituting in the above equation, we obtain
(12.12)
Differentiating Eqn. (12.11) with respect to , we obtain
(12.13)
Differentiating Eqn. (12.13) with respect to , we obtain
(12.14)
Using Eqn. (12.12), we get
(12.15)
Substituting Eqn. (12.15) in Eqn. (12.14), we obtain
(12.16)
Using Eqn. (12.13), we obtain
(12.17)
Substituting Eqn. (12.17) in Eqn. (12.16), we obtain
Solving the above equation, we obtain
(12.18)
where
The model of the lung mechanism is represented by Eqn. (12.18).
The linearized physiological model of skeletal muscle in the human body is shown in Fig. 12.14.
Fig. 12.14 ∣ Model of a skeletal muscle
Let and represent the force developed by the active contractile element of the muscle and actual force developed due to mechanical properties of muscle respectively. The viscous damping inherent in the tissue is represented by and the elastic storage properties of sarcolemma and muscle tendons are represented as and respectively. The different mechanical constraints that exist in the system shown in Fig. 12.14 are:
Thus, by assuming the above constraints, if is stretched to a length , the extension in the parallel combination of and will be . The velocity with which the dashpot extended is given by . Also, the force transmitted through the element and through the parallel combination of and will be equal. Using this principle, we obtain
(12.19)
As the summation of total force from both limbs of the parallel combination must be equal to F, we have
(12.20)
Differentiating Eqn. (12.20), we obtain
(12.21)
Using Eqn. (12.19), we obtain
(12.22)
Substituting Eqn. (12.22) in Eqn. (12.21), we obtain
Simplifying the above equation, we obtain
(12.23)
Using Eqn. (12.20), we obtain
(12.24)
Substituting Eqn. (12.24) in Eqn. (12.23), we obtain
(12.25)
Simplifying the above equation, we obtain
(12.26)
The above equation represents the mathematical model of the skeletal muscle.
In order to simplify the mathematical characterization of linear systems, models that provide adequate representations of realistic dynamical behaviour are too complicated to deal with analytically. In such complex situations, the logical approach is to translate the system block representation into a computer model and to solve the corresponding problem numerically. A variety of software tools are available that further simplify the task of model simulation and analysis. SIMULINK is currently used by a large segment of the scientific and engineering community. SIMULINK provides a graphical environment allowing the user to easily convert a block diagram into a network of blocks of mathematical functions. It runs within the interactive, command-based environment called MATLAB, wherein MATLAB and SIMULINK are products of The MathWorks, Inc.
To find out how much tidal volume is delivered to a patient in the intensive care unit when the peak pressure of a ventilator is set at a prescribed level, knowledge of the patient's lung mechanics is needed. Assuming the patient to have a normal mechanics, the values of the various pulmonary parameters are (refer to Fig. 12.13) as follows:
, ,
, and
The first method to solve this problem is to derive the transfer function for the overall system and use it as a single “block” in the SIMULINK program. The differential equation relating total airflow Q to the applied pressure at the airway opening has been derived using Kirchhoff's laws and presented in Eqn. (12.12). Substituting the above parameter values into this differential equation and taking Laplace transform and rearranging, we obtain
(12.27)
To implement the above mode, run SIMULINK from within the MATLAB command window (i.e., type simulink at the MATLAB prompt). The SIMULINK main block library will be displayed in a new window.
Steps to follow:
Fig. 12.15 ∣ SIMULINK model of lung mechanics
Figure 12.16 shows sample simulation results produced by the model implementations. The ventilator generates a sinusoidal waveform of amplitude 2.5 cmH2O.
Fig. 12.16 ∣ Simulation results from SIMULINK implementation of lung mechanics model: (a) Predicted dynamics of airflow Q and volume at 15 breaths per min and (b) predicted dynamics of airflow Q and volume at 60 breaths per min.
The ventilator frequency is initially set at 15 breaths per min (Fig. 12.16(a)), which is approximately the normal frequency of breathing at rest. At this relatively low frequency, the volume waveform is more in phase with The airflow shows a substantial phase lead relative to . This demonstrates that lung mechanics are dominated by compliance effects at such low frequencies. The peak-to-peak change in volume (i.e., tidal volume) is approximately 0.5L, while peak . When the ventilator frequency is increased fourfold to 60 breaths per min (Fig. 12.16(b)) with amplitude kept unchanged, peak Q clearly increases (), whereas tidal volume is decreased (). Now, Q has become more in phase with , whereas volume displays a significant lag. Thus, resistive effects have become more dominant at the higher frequency. The changes in peak Q and tidal volume with frequency demonstrate frequency dependence of pulmonary resistance and compliance, i.e., the lungs appear stiffer and less resistive as frequency increases from normal breathing.
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