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  PUBLIC "-//NLM//DTD JATS (Z39.96) Journal Publishing DTD v1.0 20120330//EN" "http://jats.nlm.nih.gov/publishing/1.0/JATS-journalpublishing1.dtd">
<article article-type="research-article" dtd-version="1.0" specific-use="sps-1.6" xml:lang="en" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">
	<front>
		<journal-meta>
			<journal-id journal-id-type="publisher-id">dyna</journal-id>
			<journal-title-group>
				<journal-title>DYNA</journal-title>
				<abbrev-journal-title abbrev-type="publisher">Dyna rev.fac.nac.minas</abbrev-journal-title>
			</journal-title-group>
			<issn pub-type="ppub">0012-7353</issn>
			<publisher>
				<publisher-name>Universidad Nacional de Colombia</publisher-name>
			</publisher>
		</journal-meta>
		<article-meta>
			<article-id pub-id-type="doi">10.15446/dyna.v84n200.52429</article-id>
			<article-categories>
				<subj-group subj-group-type="heading">
					<subject>Articles</subject>
				</subj-group>
			</article-categories>
			<title-group>
				<article-title>Power converter circuits: A hybrid dynamical case</article-title>
				<trans-title-group xml:lang="es">
					<trans-title>Convertidores de potencia: Un caso dinámico híbrido</trans-title>
				</trans-title-group>
			</title-group>
			<contrib-group>
				<contrib contrib-type="author">
					<name>
						<surname>Flórez-Vargas</surname>
						<given-names>Julio Andelfo</given-names>
					</name>
					<xref ref-type="aff" rid="aff1"><sup>a</sup></xref>
				</contrib>
				<contrib contrib-type="author">
					<name>
						<surname>Alzate-Castaño</surname>
						<given-names>Ricardo</given-names>
					</name>
					<xref ref-type="aff" rid="aff1"><sup>a</sup></xref>
				</contrib>
				<aff id="aff1">
					<label>a</label>
					<institution content-type="original"> Escuela de Ingenierías Eléctrica, Electrónica y de Telecomunicaciones, Universidad Industrial de Santander, Bucaramanga, Colombia. julio.florez@correo.uis.edu.co, ralzatec@uis.edu.co</institution>
					<institution content-type="normalized">Universidad Industrial de Santander</institution>
					<institution content-type="orgname">Universidad Industrial de Santander</institution>
					<addr-line>
						<named-content content-type="city">Bucaramanga</named-content>
					</addr-line>
					<country country="CO">Colombia</country>
					<email>julio.florez@correo.uis.edu.co</email>
					<email>ralzatec@uis.edu.co</email>
				</aff>
			</contrib-group>
			<pub-date pub-type="epub-ppub">
				<season>Jan-Mar</season>
				<year>2017</year>
			</pub-date>
			<volume>84</volume>
			<issue>200</issue>
			<fpage>143</fpage>
			<lpage>150</lpage>
			<history>
				<date date-type="received">
					<day>10</day>
					<month>08</month>
					<year>2015</year>
				</date>
				<date date-type="rev-recd">
					<day>10</day>
					<month>07</month>
					<year>2016</year>
				</date>
				<date date-type="accepted">
					<day>05</day>
					<month>11</month>
					<year>2016</year>
				</date>
			</history>
			<permissions>
				<license license-type="open-access" xlink:href="http://creativecommons.org/licenses/by-nc-nd/4.0/" xml:lang="en">
					<license-p>This is an open-access article distributed under the terms of the Creative Commons Attribution License</license-p>
				</license>
			</permissions>
			<abstract>
				<title>Abstract</title>
				<p>The hybrid paradigm (often referred to as Cyber-Physical-Systems) can be employed to understand (by modelling) or to manipulate (by control design) the dynamical behavior of systems. In this paper, a system of wide use in applications (<italic>Buck</italic>-type power converter) with a simple type of controller (On-Off) is addressed from a perspective of hybrid modelling, developed upon a set-based formulation scheme. This approach is novel in the sense that it allows the formulation of generic formal rules as sets for the transition between continuous and discrete modes of a hybrid model, which can be further implemented as software routines for simulation purposes. Indeed, it is shown how the controlled system can be understood as the union between the system and controller sets. Numerical results obtained with a commercial circuit simulator were replicated by evaluating the set-based formulations, constituting a valuable tool in the path to understand the behavior of complex discontinuous systems.</p>
			</abstract>
			<trans-abstract xml:lang="es">
				<title>Resumen</title>
				<p>El paradigma híbrido (o de Sistemas Ciber-físicos) puede ser empleado para entender (modelar) o manipular (controlar) el comportamiento dinámico de sistemas. Este artículo aborda el modelado desde una perspectiva híbrida para describir la dinámica de un circuito convertidor de potencia bajo la acción de un controlador encendido-apagado, a través de una formulación basada en conjuntos. Este enfoque es novedoso en cuanto permite formular reglas genéricas pero formales, a partir de transiciones entre modos de operación del sistema, lo cual facilita su posterior implementación computacional en entornos de simulación. De hecho, se muestra como el sistema controlado puede explicarse en términos de la unión de los conjuntos que describen el circuito y su control. Resultados generados en un simulador comercial de circuitos replican las predicciones obtenidas tras evaluar las reglas de conjuntos propuestas, representando un paso importante en el camino hacia la comprensión del comportamiento dinámico de sistemas discontinuos más complejos.</p>
			</trans-abstract>
			<kwd-group xml:lang="en">
				<title><bold>
 <italic>Keywords</italic>
</bold>: </title>
				<kwd>buck-type power converter</kwd>
				<kwd>hybrid dynamical system</kwd>
				<kwd>modeling</kwd>
				<kwd>on-off controller</kwd>
			</kwd-group>
			<kwd-group xml:lang="es">
				<title><bold>
 <italic>Palabras clave</italic>
</bold>: </title>
				<kwd>controlador encendido-apagado</kwd>
				<kwd>convertidor de potencia reductor</kwd>
				<kwd>modelamiento</kwd>
				<kwd>sistema dinámico híbrido</kwd>
			</kwd-group>
			<counts>
				<fig-count count="15"/>
				<table-count count="1"/>
				<equation-count count="31"/>
				<ref-count count="20"/>
				<page-count count="8"/>
			</counts>
		</article-meta>
	</front>
	<body>
		<sec sec-type="intro">
			<title>1. Introduction</title>
			<p>Dynamical systems when thought as operating under realistic conditions are usually constrained to evolve inside delimited zones of the state-space, as a natural consequence of physical limitations appearing by implementations, such as the saturation of actuation components and the boundaries of motion trajectories. Moreover, different operational modes of the system define particular regions in the solution space and therefore, a conditioned representation of the dynamics. Such interaction of continuous behavior and discrete transition-rules between operation modes is defined in terms of the so-called Hybrid Dynamical Systems (HDS).</p>
			<p>An HDS can be stated as one with solution trajectories composed of continuous paths linked by discontinuous transitions obeying a discrete rule [<xref ref-type="bibr" rid="B1">1</xref>]. Hybrid models can be employed as simplified representations of complex systems [<xref ref-type="bibr" rid="B2">2</xref>-<xref ref-type="bibr" rid="B4">4</xref>] by taking advantage of the information reduction provided by discrete domains (e.g. the bouncing-ball system). Then, an HDS is the best way to describe the coupling between the continuous nature of physical systems and the discrete fashion of computations; i.e. a Cyber-Physical System (CPS), as topic of current research interest for development of intelligent computational systems interacting with nature [<xref ref-type="bibr" rid="B5">5</xref>,<xref ref-type="bibr" rid="B6">6</xref>]. On the other hand, it is necessary to design more efficient engineering systems in terms of energy consumption, as consequence of an increasing power demand under limited resources [<xref ref-type="bibr" rid="B2">2</xref>,<xref ref-type="bibr" rid="B7">7</xref>,<xref ref-type="bibr" rid="B8">8</xref>]. In particular, for the case of electrical systems it is well known the role of a power converter circuit for delivering to the load, in an efficient manner, the energy stored in a power supply (i.e. with a minimum loss) [<xref ref-type="bibr" rid="B9">9</xref>,<xref ref-type="bibr" rid="B10">10</xref>]. The operation of a power converter circuit is determined by the commutation pattern of the switching devices in the corresponding circuit topology. Pulse-width modulated signals (PWM) are often employed to accomplish this task. In a PWM-generation block the input is a continuous signal corresponding to the duty cycle, and the output is a discrete signal with only two possible values: ON or OFF [<xref ref-type="bibr" rid="B11">11</xref>,<xref ref-type="bibr" rid="B12">12</xref>]. Such a feature imposes a discrete change over the continuous nature of an electric circuit, allowing to model the power converter as a hybrid system [<xref ref-type="bibr" rid="B1">1</xref>,<xref ref-type="bibr" rid="B12">12</xref>]. To model a power converter is, in general, a complicated task given the discontinuities induced by switching devices [<xref ref-type="bibr" rid="B13">13</xref>,<xref ref-type="bibr" rid="B14">14</xref>]. Nevertheless, there are several works in the literature proposing isolated models for the converter and the control laws [<xref ref-type="bibr" rid="B15">15</xref>-<xref ref-type="bibr" rid="B18">18</xref>]. This paper shows a general definition for the hybrid system in terms of a set of continuous and discrete components, being applied to link the power converter and a simple control law, in an attempt to model and to explain the behavior of the controlled circuit, as an HDS. The contents of the paper are organized as follows: Section 2 introduces the hybrid dynamical systems and a set-based formulation for modelling its dynamics; Section 3 uses the proposed approach to model a power converter circuit; in Section 4 the hybrid modelling is extended to an On-Off controller being, furthermore, linked to the converter circuit; finally, Section 5 presents numerical validation of the models and discussion of results, with general conclusions given in section 6.</p>
		</sec>
		<sec>
			<title>2. Hybrid Dynamical Systems HDS</title>
			<p>Hybrid Dynamical Systems (HDS) have been a subject of increasing interest from the earlier developments in the Eastern literature till nowadays. In particular, new methodologies and techniques for analysis and control tasks appeared in an attempt to deal with the impossibility to apply the well-developed classical theory of smooth-dynamical systems. Interested readers are referred to [<xref ref-type="bibr" rid="B19">19</xref>] for a deeper review on some developments concerning piecewise-smooth dynamical systems (including hybrid systems) and applications.</p>
			<p>As a representative example, let us consider the dynamical system described by:</p>
			<p>
				<disp-formula id="e1">
					<graphic xlink:href="0012-7353-dyna-84-200-00143-e1.png"/>
					<label>(1)</label>
				</disp-formula>
			</p>
			<p>with <sub>
 <sup>
 <italic>F1</italic>
</sup> 
</sub> and <sub>
 <sup>
 <italic>F2</italic>
</sup> 
</sub> representing two different modes of operation across the discontinuity boundary <italic>Σ</italic> in <xref ref-type="fig" rid="f1">Fig. 1</xref> (where the solution space S has been partitioned into S<sub>1</sub> and S<sub>2</sub>), generating respectively the flow paths <sub>
 <sup>
 <italic>(1</italic>
</sup> 
</sub> and <sub>
 <sup>
 <italic>(2</italic>
</sup> 
</sub> .</p>
			<p>Then in order to solve (1) for an arbitrary time <italic>t &gt; 0</italic>, we must be able to detect accurately the crossing instants of the system flow through the boundary <italic>Σ</italic> for an appropriate commutation of the vector fields <italic>F</italic>. In general, it is not straightforward to find closed-form analytical solutions for these kinds of trajectory, moreover, when the boundary conditions may include discontinuities in the resulting flow. As a valid resource, numerical approximations of the trajectories are considered by appropriate formulations of automata resembling conditionals and transitions between discrete and continuous states. Synthesis and conditioning of numerical methods are then of remarkable importance in the analysis of hybrid dynamics. See [<xref ref-type="bibr" rid="B20">20</xref>] and references therein for a detailed description of event-driven simulators applied to systems with discontinuous flows.</p>
			<sec>
				<title><italic>2.1. A set-based formulation for the hybrid automaton</italic></title>
				<p>In general, a dynamical system given by:</p>
				<p>
					<disp-formula id="e2">
						<graphic xlink:href="0012-7353-dyna-84-200-00143-e2.png"/>
						<label>(2)</label>
					</disp-formula>
				</p>
				<p>where <bold>
 <italic>x</italic>
</bold> is the state-vector of <italic>n</italic> state-variables, ƒ (.) is a continuous function (non-necessarily linear) of the states, <bold>u</bold> is a vector of allowed inputs and <italic>x</italic>
 <sub>0</sub> is a set of initial conditions; can be solved as a trajectory in the state space <bold>Φ</bold>(t) <bold>
 <italic>= x(t).</italic>
</bold> </p>
				<p>In an HDS such flow path Φ(<italic>t</italic>) can be described in terms of a combination of continuous sets of points, linked to discrete conditions between them; i.e. by considering the ordered pair<inline-graphic xlink:href="0012-7353-dyna-84-200-00143-i003.png"/>, each point of the state-space for the solution path Φ(<italic>t</italic>) belongs exclusively to any of both, a continuous set <italic>C</italic> defined by: </p>
				<p>
					<disp-formula id="e3">
						<graphic xlink:href="0012-7353-dyna-84-200-00143-e3.png"/>
						<label>(3)</label>
					</disp-formula>
				</p>
				<p>where <inline-graphic xlink:href="0012-7353-dyna-84-200-00143-i005.png"/> represents the <sub>
 <sup>
 <italic>ith</italic>
</sup> 
</sub> interval of the domain where <italic>x</italic>(<italic>t</italic>) is smooth for <italic>l</italic> continuous trajectories; or the discrete set <italic>D</italic>:</p>
				<p>
					<disp-formula id="e4">
						<graphic xlink:href="0012-7353-dyna-84-200-00143-e4.png"/>,<label>(4)</label>
					</disp-formula>
				</p>
				<p>where <inline-graphic xlink:href="0012-7353-dyna-84-200-00143-i007.png"/> and <inline-graphic xlink:href="0012-7353-dyna-84-200-00143-i008.png"/> stand respectively for the infinitesimals of time just after and before the discrete transition at <sub>
 <sup>
 <italic>ti</italic>
</sup> 
</sub> .</p>
				<p>Hence, the total hybrid trajectory can be stated as:</p>
				<p>
					<disp-formula id="e5">
						<graphic xlink:href="0012-7353-dyna-84-200-00143-e5.png"/>. <label>(5)</label>
					</disp-formula>
				</p>
				<p>Such a result is illustrated in <xref ref-type="fig" rid="f2">Fig. 2</xref> for <italic>n = 2</italic>. Notice that it graphically explains, by an automaton, the situation depicted previously in <xref ref-type="fig" rid="f1">Fig. 1</xref>. Then, the system jumps from the descriptions of the vector fields <inline-graphic xlink:href="0012-7353-dyna-84-200-00143-i010.jpg"/> and <inline-graphic xlink:href="0012-7353-dyna-84-200-00143-i011.jpg"/> depending on the event occurring at; <inline-graphic xlink:href="0012-7353-dyna-84-200-00143-i012.jpg"/>. <inline-graphic xlink:href="0012-7353-dyna-84-200-00143-i013.jpg"/>
				</p>
				<p>
					<fig id="f1">
						<label>Figure 1</label>
						<caption>
							<title>Graphical representation of a hybrid dynamical system.</title>
						</caption>
						<graphic xlink:href="0012-7353-dyna-84-200-00143-gf1.jpg"/>
						<attrib>Source: Authors</attrib>
					</fig>
				</p>
				<p>
					<fig id="f2">
						<label>Figure 2</label>
						<caption>
							<title>Hybrid dynamical system as automaton.</title>
						</caption>
						<graphic xlink:href="0012-7353-dyna-84-200-00143-gf2.jpg"/>
						<attrib>Source: Authors</attrib>
					</fig>
				</p>
				<p>
					<fig id="f3">
						<label>Figure 3</label>
						<caption>
							<title><italic>Buck</italic> type DC-DC power converter circuit.</title>
						</caption>
						<graphic xlink:href="0012-7353-dyna-84-200-00143-gf3.png"/>
						<attrib>Source: Authors</attrib>
					</fig>
				</p>
				<p>The mathematical representation of HDS introduced here, will be employed in the following to describe the dynamic behavior of a power converter circuit.</p>
			</sec>
		</sec>
		<sec>
			<title><bold>3. A</bold> 
 <bold>
 <italic>Buck</italic>
</bold> 
 <bold>type power converter circuit</bold></title>
			<p>
				<xref ref-type="fig" rid="f3">Fig. 3</xref>, shows the general circuit describing a buck DC-DC power converter. The operation of the system can be split in two modes depending on the conduction state of the MOSFET transistor which operates as a switch. Let us first consider the operational mode of conduction (<italic>u</italic> = 1).</p>
			<p>The equivalent circuit is depicted in <xref ref-type="fig" rid="f4">Fig. 4</xref>. As it can be seen, the source applies the power input to the load. <xref ref-type="disp-formula" rid="e6">Equations (6)</xref> and (<xref ref-type="disp-formula" rid="e7">7</xref>) describe respectively, the Kirchhoff's Voltage (KVL) and Current (KCL) laws applied to the circuit, where <italic>V</italic>
 <sub>0</sub> represents the output voltage in the load and<sub>
 <sup>
 <italic>VL</italic>
</sup> 
</sub> , <sub>
 <sup>
 <italic>VC</italic>
</sup> 
</sub> the corresponding to inductor and capacitor devices.</p>
			<p>
				<disp-formula id="e6">
					<graphic xlink:href="0012-7353-dyna-84-200-00143-e6.png"/>
					<label>(6)</label>
				</disp-formula>
			</p>
			<p>
				<disp-formula id="e7">
					<graphic xlink:href="0012-7353-dyna-84-200-00143-e7.png"/>
					<label>(7)</label>
				</disp-formula>
			</p>
			<p>In the second mode, the switch is open (<italic>u</italic> =0) and then the energy stored in the capacitor and the inductor should supply the load temporarily until the next conduction mode occurs. Nevertheless, it is necessary to take into account the influence of the diode into the circuit. Hence, <xref ref-type="fig" rid="f5">Fig. 5</xref> shows the equivalent circuit when the diode is forward-biased (<sub>
 <sup>
 <italic>iL</italic>
</sup> 
</sub> &gt;0), with <xref ref-type="disp-formula" rid="e8">eq. (8)</xref>-(<xref ref-type="disp-formula" rid="e9">9</xref>) representing its KVL and KCL equations.</p>
			<p>
				<fig id="f4">
					<label>Figure 4</label>
					<caption>
						<title>Conduction mode of the <italic>Buck</italic> circuit.</title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-84-200-00143-gf4.png"/>
					<attrib>Source: Authors</attrib>
				</fig>
			</p>
			<p>
				<fig id="f5">
					<label>Figure 5</label>
					<caption>
						<title>Non-conduction mode of the <italic>Buck</italic> circuit, diode forward-biased.</title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-84-200-00143-gf5.png"/>
					<attrib>Source: Authors</attrib>
				</fig>
			</p>
			<p>
				<disp-formula id="e8">
					<graphic xlink:href="0012-7353-dyna-84-200-00143-e8.png"/>
					<label>(8)</label>
				</disp-formula>
			</p>
			<p>
				<disp-formula id="e9">
					<graphic xlink:href="0012-7353-dyna-84-200-00143-e9.png"/>
					<label>(9)</label>
				</disp-formula>
			</p>
			<p>On the other hand, <xref ref-type="fig" rid="f6">Fig. 6</xref> shows the non-conduction mode when the diode is reverse-biased. <xref ref-type="disp-formula" rid="e10">eq. (10)</xref>-(<xref ref-type="disp-formula" rid="e11">11</xref>) represent the KVL and KCL equations for the corresponding circuit.</p>
			<p>
				<disp-formula id="e10">
					<graphic xlink:href="0012-7353-dyna-84-200-00143-e10.png"/>
					<label>(10)</label>
				</disp-formula>
			</p>
			<p>
				<disp-formula id="e11">
					<graphic xlink:href="0012-7353-dyna-84-200-00143-e11.png"/>
					<label>(11)</label>
				</disp-formula>
			</p>
			<p>
				<fig id="f6">
					<label>Figure 6</label>
					<caption>
						<title>Non-conduction mode of the Buck circuit, diode reverse-biased.</title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-84-200-00143-gf6.png"/>
					<attrib>Source: Authors</attrib>
				</fig>
			</p>
			<p>Then, after defining as state variables the current of the coil<inline-graphic xlink:href="0012-7353-dyna-84-200-00143-i026.png"/> and the voltage of the load <inline-graphic xlink:href="0012-7353-dyna-84-200-00143-i027.png"/>, it is possible to formulate a state-space representation of the circuit according to (2) by combining expressions (6)-(11) in the following matrix representation:</p>
			<p>
				<disp-formula id="e12">
					<graphic xlink:href="0012-7353-dyna-84-200-00143-e12.png"/>
					<label>(12)</label>
				</disp-formula>
			</p>
			<p>where <inline-graphic xlink:href="0012-7353-dyna-84-200-00143-i029.png"/>is the set of initial conditions.</p>
			<p>Notice that the signum function sgn(.) includes the discontinuity to the system flow and, therefore, an HDS representation of the model can be achieved easily, shown as follows.</p>
			<sec>
				<title>3.1. A set-based formulation for the Buck circuit</title>
				<p>The dynamics of the Buck-type power converter circuit depend on the pattern of the PWM signal, given that it provides the time instants where the command input u changes among its binary values.</p>
				<p>In a more precise manner, each period T of the PWM signal is composed of an activation interval tON (for u = 1) followed by a gap of inactivity tOOF (for u = 0) i.e.</p>
				<p>
					<disp-formula id="e13">
						<graphic xlink:href="0012-7353-dyna-84-200-00143-e13.png"/>
						<label>(13)</label>
					</disp-formula>
				</p>
				<p>Hence, by starting from t =t0, the ith conduction instant can be defined as:</p>
				<p>
					<disp-formula id="e14">
						<graphic xlink:href="0012-7353-dyna-84-200-00143-e14.png"/>
						<label>(14)</label>
					</disp-formula>
				</p>
				<p>Also, the jth inactivity event can be stated by:</p>
				<p>
					<disp-formula id="e15">
						<graphic xlink:href="0012-7353-dyna-84-200-00143-e15.png"/>
						<label>(15)</label>
					</disp-formula>
				</p>
				<p>In accordance, the continuous set C describing the solution trajectory can be formulated as:</p>
				<p>
					<disp-formula id="e16">
						<graphic xlink:href="0012-7353-dyna-84-200-00143-e16.png"/>
						<label>(16)</label>
					</disp-formula>
				</p>
				<p>and equivalently, the discrete events are defined by:</p>
				<p>
					<disp-formula id="e17">
						<graphic xlink:href="0012-7353-dyna-84-200-00143-e17.png"/>. <label>(17)</label>
					</disp-formula>
				</p>
				<p>In this way, it is possible to express the system flow, or solution trajectory, for the Buck-type converter circuit in <xref ref-type="disp-formula" rid="e12">eq. (12)</xref> by:</p>
				<p>
					<disp-formula id="e18">
						<graphic xlink:href="0012-7353-dyna-84-200-00143-e18.png"/>
						<label>(18)</label>
					</disp-formula>
				</p>
			</sec>
		</sec>
		<sec>
			<title>4. On-Off controller as a hybrid system</title>
			<p>It is well known, that a proportional control action, defined by:</p>
			<p>
				<disp-formula id="e19">
					<graphic xlink:href="0012-7353-dyna-84-200-00143-e19.png"/>
					<label>(19)</label>
				</disp-formula>
			</p>
			<p>where e (t) represents the output error and KP constitutes the loop gain, is the most basic governing law that can be stated in a feedback control system. Moreover, if KP = 1 we have a unit gain negative feedback created naturally after closing the loop.</p>
			<p>If KP is increased, the disturbance effects start to vanish and steady-state errors become diminished. In practice, however, the maximum value for this loop gain is constrained by saturation boundaries (<inline-graphic xlink:href="0012-7353-dyna-84-200-00143-i037.jpg"/> and <inline-graphic xlink:href="0012-7353-dyna-84-200-00143-i038.jpg"/>) of signal levels as depicted in <xref ref-type="fig" rid="f7">Fig. 7</xref>.</p>
			<p>In spite of this, for higher values of the loop gain KP, the controller responses are strong enough to annihilate the error, with a limiting theoretical value of <inline-graphic xlink:href="0012-7353-dyna-84-200-00143-i039.png"/>. The latter is the special case usually termed On-Off controller, a situation illustrated in <xref ref-type="fig" rid="f8">Fig. 8</xref> and described mathematically by:</p>
			<p>
				<disp-formula id="e20">
					<graphic xlink:href="0012-7353-dyna-84-200-00143-e20.png"/>
					<label>(20)</label>
				</disp-formula>
			</p>
			<p>An On-Off controller delivers as control action, the maximum energy in a minimum time. There are several examples of practical applications for this kind of controller, including heat and cooling systems, level control and end-position control, among others.</p>
			<p>As can be seen from (20), the controller has a discontinuous fashion that can be modelled as an HDS.</p>
			<p>
				<fig id="f7">
					<label>Figure 7</label>
					<caption>
						<title>Proportional control action limited by saturation boundaries. </title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-84-200-00143-gf7.png"/>
					<attrib>Source: Authors</attrib>
				</fig>
			</p>
			<p>
				<fig id="f8">
					<label>Figure 8</label>
					<caption>
						<title>On-Off control action as infinite loop gain of a proportional controller.</title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-84-200-00143-gf8.png"/>
					<attrib>Source: Authors</attrib>
				</fig>
			</p>
			<sec>
				<title>4.1. A set-based formulation for the On-Off controller</title>
				<p>In accordance with (2), the dynamical representation of an On-Off controller of the form (20) can be stated as:</p>
				<p>
					<disp-formula id="e21">
						<graphic xlink:href="0012-7353-dyna-84-200-00143-e21.png"/>
						<label>(21)</label>
					</disp-formula>
				</p>
				<p>for <inline-graphic xlink:href="0012-7353-dyna-84-200-00143-i044.png"/> representing the rate of the control signal <inline-graphic xlink:href="0012-7353-dyna-84-200-00143-i045.png"/> in terms of variations in <inline-graphic xlink:href="0012-7353-dyna-84-200-00143-i046.png"/>i.e.</p>
				<p>
					<disp-formula id="e22">
						<graphic xlink:href="0012-7353-dyna-84-200-00143-e22.png"/>
						<label>(22)</label>
					</disp-formula>
				</p>
				<p>Then, by considering that a sgn(.) function can be expressed as the following sum of step functions µ(.): </p>
				<p>
					<disp-formula id="e23">
						<graphic xlink:href="0012-7353-dyna-84-200-00143-e23.png"/>
						<label>(23)</label>
					</disp-formula>
				</p>
				<p>
					<xref ref-type="disp-formula" rid="e20">equations (20)</xref>, (<xref ref-type="disp-formula" rid="e22">22</xref>) and (<xref ref-type="disp-formula" rid="e23">23</xref>) can be combined to give:</p>
				<p>
					<disp-formula id="e24">
						<graphic xlink:href="0012-7353-dyna-84-200-00143-e24.png"/>
						<label>(24)</label>
					</disp-formula>
				</p>
				<p>by using the fact that the derivative of a step function µ(.) is a Dirac delta function δ(.).</p>
				<p>Then, if dynamics of the On-Off controller (21) can be solved in terms of the ordered pair:</p>
				<p>
					<disp-formula id="e25">
						<graphic xlink:href="0012-7353-dyna-84-200-00143-e25.png"/>
						<label>(25)</label>
					</disp-formula>
				</p>
				<p>the continuous set C describing the flow path of the system is: </p>
				<p>
					<disp-formula id="e26">
						<graphic xlink:href="0012-7353-dyna-84-200-00143-e26.png"/>
						<label>(26)</label>
					</disp-formula>
				</p>
				<p>and the corresponding discrete events D are given by:</p>
				<p>
					<disp-formula id="e27">
						<graphic xlink:href="0012-7353-dyna-84-200-00143-e27.png"/>
						<label>(27)</label>
					</disp-formula>
				</p>
				<p>Therefore, the solution trajectory describing the On-Off control action can be stated as:</p>
				<p>
					<disp-formula id="e28">
						<graphic xlink:href="0012-7353-dyna-84-200-00143-e28.png"/>
						<label>(28)</label>
					</disp-formula>
				</p>
			</sec>
			<sec>
				<title>4.2. Hybrid formulation of the Buck circuit On-Off controlled</title>
				<p>The sets proposed in section 2.1 for the continuous paths and discrete events composing the solution trajectory of hybrid systems, further applied in sections 3.1 and 4.1 to describe dynamics of a Buck-type power converter circuit and an On-Off controller, can be merged here to define the hybrid controlled circuit.</p>
				<p>In essence, the two models can be coupled by considering that the time instants governing the commutation changes in the circuit, coincide with the zero crossing of the error signal, i.e. by combining <xref ref-type="disp-formula" rid="e16">equations (16)</xref> and (<xref ref-type="disp-formula" rid="e26">26</xref>), the continuous set C describing the flow path of the controlled circuit is: </p>
				<p>
					<disp-formula id="e29">
						<graphic xlink:href="0012-7353-dyna-84-200-00143-e29.png"/>
						<label>(29)</label>
					</disp-formula>
				</p>
				<p>and equivalently, by combining (17) and (26) the discrete events are defined by:</p>
				<p>
					<disp-formula id="e30">
						<graphic xlink:href="0012-7353-dyna-84-200-00143-e30.png"/>
						<label>(30)</label>
					</disp-formula>
				</p>
				<p>Finally, the flow-path of the controlled system can be stated by:</p>
				<p>
					<disp-formula id="e31">
						<graphic xlink:href="0012-7353-dyna-84-200-00143-e31.png"/>
						<label>(31)</label>
					</disp-formula>
				</p>
			</sec>
		</sec>
		<sec sec-type="discussion">
			<title>5. Numerical verification of the hybrid models and discussion</title>
			<p>The analytic results shown in previous sections have been tested by comparing numerical evaluation of the proposed sets, with results of the commercial circuit simulation package OrCAD-Cadence®.</p>
			<p>
				<xref ref-type="fig" rid="f9">Figs. 9</xref>, <xref ref-type="fig" rid="f11">11</xref> show the numerical evaluation in MATLAB® of the data sets given by <xref ref-type="disp-formula" rid="e18">eq. (18)</xref>, as solution trajectories of the Buck-type converter circuit, for the parameter values listed in <xref ref-type="table" rid="t1">Table 1</xref>. </p>
			<p>
				<table-wrap id="t1">
					<label>Table 1</label>
					<caption>
						<title>Circuit parameters used in simulations.</title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-84-200-00143-gt1.png"/>
					<table-wrap-foot>
						<fn id="TFN1">
							<p>Source: Authors</p>
						</fn>
					</table-wrap-foot>
				</table-wrap>
			</p>
			<p>
				<fig id="f9">
					<label>Figure 9</label>
					<caption>
						<title>Output voltage of a Buck-type power converter reproduced by numerical evaluation in MATLAB® of the hybrid model.</title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-84-200-00143-gf9.jpg"/>
					<attrib>Source: Authors</attrib>
				</fig>
			</p>
			<p>
				<fig id="f10">
					<label>Figure 10</label>
					<caption>
						<title>Output voltage of a Buck-type power converter reproduced by numerical simulation in OrCAD-Cadence®. </title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-84-200-00143-gf10.jpg"/>
					<attrib>Source: Authors</attrib>
				</fig>
			</p>
			<p>In comparison, <xref ref-type="fig" rid="f10">Figs. 10</xref>, <xref ref-type="fig" rid="f12">12</xref> reproduce equivalent results by employing OrCAD-Cadence®.</p>
			<p>As can be noticed, the qualitative behavior of the voltage and current signals is replicated in both simulation environments. In particular, a smooth shape for the capacitor voltage is achieved with a peak time around 0.5[s] and a falling slope reaching a steady state regime close to the expected value of 12 [V] near to 3 [ms].</p>
			<p>In contrast, the behavior of the inductor current is characterized by a discontinuous shape with an initial lobe followed by a stable average of around 2 [A] starting close to 0.5 [s].</p>
			<p>However, there are also qualitative disagreements in the results that can be explained by special features added to the commercial circuit simulator (e.g. temperature dependence, non-idealization of circuit elements), not considered in our simple approach. Nevertheless, the agreement achieved is good enough to validate the correctness of the proposed scheme to model the dynamic behavior of the <italic>Buck</italic>-type power converter circuit as an HDS. </p>
			<p>Now, in order to verify the hybrid model of the On-Off controller, <xref ref-type="fig" rid="f13">Fig. 13</xref> shows the synthesis in MATLAB® of a control signal <italic>u(t) = u(e)</italic>, obtained by applying a predefined error waveform <italic>e(t)</italic> to the system.</p>
			<p>
				<fig id="f11">
					<label>Figure 11</label>
					<caption>
						<title>Inductor current of a Buck-type power converter reproduced by numerical evaluation in MATLAB® of the hybrid model.</title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-84-200-00143-gf11.jpg"/>
					<attrib>Source: Authors</attrib>
				</fig>
			</p>
			<p>
				<fig id="f12">
					<label>Figure 12</label>
					<caption>
						<title>Inductor current of a Buck-type power converter reproduced by numerical simulation in OrCAD-Cadence®.</title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-84-200-00143-gf12.jpg"/>
					<attrib>Source: Authors</attrib>
				</fig>
			</p>
			<p>The same principle is employed in <xref ref-type="fig" rid="f14">Fig. 14</xref> to reproduce artificially in MATLAB® the output voltage signal of <xref ref-type="fig" rid="f9">Fig. 9</xref>, by numerical evaluation of the data sets given by <xref ref-type="disp-formula" rid="e31">eq. (31)</xref>, as solution trajectories of the Buck-type converter circuit when controlled by the hybrid On-Off action. </p>
			<p>In such a case, the error signal applied to the controller as input, has a constant frequency and duty cycle values in accordance to the nominal values illustrated in <xref ref-type="table" rid="t1">Table 1</xref>. A detail of the waveform generated is illustrated in <xref ref-type="fig" rid="f15">Fig. 15</xref>.</p>
		</sec>
		<sec sec-type="conclusions">
			<title>6. Conclusions</title>
			<p>An HDS can be represented in terms of a trajectory composed of continuous paths linked by discrete events. Those continuous and discrete intervals have been defined by sets including all the possible points in the state-space which, belonging to the system-flow solutions, can be classified as part of one of the hybrid components.</p>
			<p>
				<fig id="f13">
					<label>Figure 13</label>
					<caption>
						<title>Input-output relationship of On-Off hybrid controller reproduced numerically in MATLAB®. </title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-84-200-00143-gf13.jpg"/>
					<attrib>Source: Authors</attrib>
				</fig>
			</p>
			<p>
				<fig id="f14">
					<label>Figure 14</label>
					<caption>
						<title>Output voltage of Buck-type converter synthetized by numerical evaluation in MATLAB® of the hybrid model proposed for the controlled circuit.</title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-84-200-00143-gf14.jpg"/>
					<attrib>Source: Authors</attrib>
				</fig>
			</p>
			<p>
				<fig id="f15">
					<label>Figure 15</label>
					<caption>
						<title>Detail for the output voltage of Buck-type converter synthetized in MATLAB® for the hybrid model proposed. </title>
					</caption>
					<graphic xlink:href="0012-7353-dyna-84-200-00143-gf15.jpg"/>
					<attrib>Source: Authors</attrib>
				</fig>
			</p>
			<p>A <italic>Buck</italic>-type power converter circuit has been shown as an example of HDS in terms of the proposed set-based formulation. Numerical evaluation of the hybrid scheme allowed to verify the agreement for capturing the main dynamical features of the system responses compared with a reference framework given by a commercial circuit simulator package.</p>
			<p>The proposed set-based approach has been further employed to define an On-Off controller as HDS. In such a case, the dynamics of the control signal at the output of the system was described in terms of variations on the error signal.</p>
			<p>An approximation for the On-Off controlled <italic>Buck</italic>-type power converter circuit was then performed by merging the individual representations. As a result, the time instants corresponding to the events where the continuous flow of the circuit solution jumps discontinuously to the next continuous interval, correspond with the zero crossings of the error signal applied as input of the controller.</p>
			<p>The numerical results obtained with the commercial circuit simulator were replicated by evaluating the set-based formulation of the controlled circuit, constituting a valuable tool in the path to understand the dynamical behavior of discontinuous systems.</p>
			<p>It is interesting to notice the way it was possible to express the behavior of the controlled system, as the union of sets describing individually the circuit and the controller dynamics. This can be understood as a new framework that complements existing approaches, such as finite state machines, Petri nets and Markovian models, by defining formal rules scalable onto more complex systems. The potential of the proposed approach can be exploited by exploring the wide possibilities offered by sets theory in order to describe and to formalize continuous and discrete formulations and interactions in between.</p>
			<p>A natural evolution for the application case considered is the study of more complex topologies of power conversion systems, including more than a simple converter with more than a simple controller. This is part of the current ongoing work on which the proposed approach is being applied as a way to model hybrid dynamic behavior.</p>
		</sec>
	</body>
	<back>
		<ack>
			<title>Acknowledgements</title>
			<p>The authors acknowledge Universidad Industrial de Santander (UIS) in Colombia for supporting this research under the project VIE-UIS 5568. We also thank Dr. Elder Jesús Villamizar, School of Mathematics-UIS, for his helpful suggestions.</p>
		</ack>
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