<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">JAMP</journal-id><journal-title-group><journal-title>Journal of Applied Mathematics and Physics</journal-title></journal-title-group><issn pub-type="epub">2327-4352</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jamp.2015.39139</article-id><article-id pub-id-type="publisher-id">JAMP-59547</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Time Optimal Control in Time Series Movement
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>gnjen</surname><given-names>Vukovic</given-names></name><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><author-notes><corresp id="cor1">* E-mail:<email>ognjen.vukovic@uni.li, oggyvukovich@gmail.com</email>;<email>Department for Finance, University of Liechtenstein, Vaduz, Liechtenstein</email>;</corresp></author-notes><pub-date pub-type="epub"><day>04</day><month>09</month><year>2015</year></pub-date><volume>03</volume><issue>09</issue><fpage>1122</fpage><lpage>1125</lpage><history><date date-type="received"><day>14</day>	<month>August</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>8</month>	<year>September</year>	</date><date date-type="accepted"><day>11</day>	<month>September</month>	<year>2015</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  The paper analyses time series that exhibit equilibrium states. It analyses the formation of equilibrium and how the system can return to the aforementioned equilibrium. The tool that is used in the aforementioned analysis is time optimal control in the phase plane. It is proved that equilibrium state is sustainable if initial state is not too far from the equilibrium as well as control vector is large enough. On the other hand, if initial state is one standard deviation away from equilibrium state, it is proved that equilibrium cannot be reached. It is the same case with control vector. If it is unbounded, time optimal control cannot be applied. The approach that is introduced represents unconventional method of analysing equilibrium in time series.
 
</p></abstract><kwd-group><kwd>Time-Series</kwd><kwd> Equilibrium State</kwd><kwd> Time Optimal Control</kwd><kwd> Analysis</kwd><kwd> Control Vector</kwd><kwd> Financial Disruption</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Some physical systems exhibit equilibrium movement without intervention. Other physical systems exhibit disequilibrium movement but due to external factors, the equilibrium state is reached [<xref ref-type="bibr" rid="scirp.59547-ref1">1</xref>] . In mathematics, especially in differential equations, an equilibrium points is an optimal solution to a differential equation. Time optimal control is a method of mathematical optimisation for deriving control policies [<xref ref-type="bibr" rid="scirp.59547-ref1">1</xref>] .</p><p>Firstly, we will introduce the system of ordinary differential equations [<xref ref-type="bibr" rid="scirp.59547-ref2">2</xref>] :</p><disp-formula id="scirp.59547-formula858"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1720356x5.png"  xlink:type="simple"/></disp-formula><p>The Equation (1) introduces the system of ordinary differential equations with an initial state. The <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x6.png" xlink:type="simple"/></inline-formula> is considered to be the state vector. The components <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x7.png" xlink:type="simple"/></inline-formula> are state variables while u is the control vector with control variables presented as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x8.png" xlink:type="simple"/></inline-formula>. Firstly, u is merely integrable while f is continuously differentiable with respect to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x9.png" xlink:type="simple"/></inline-formula> so that we can allow for discontinuous changes in its components, the control variables.</p></sec><sec id="s2"><title>2. Theoretical Results and Findings</title><p>A control problem that we pose is the following: if we take initial state as <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x10.png" xlink:type="simple"/></inline-formula> when t = 0 what control vector <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x11.png" xlink:type="simple"/></inline-formula> can we choose that will take us to the target state<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x12.png" xlink:type="simple"/></inline-formula>, at time<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x13.png" xlink:type="simple"/></inline-formula>. How can this system be controlled [<xref ref-type="bibr" rid="scirp.59547-ref2">2</xref>] ?</p><p>If the cost function is introduced</p><disp-formula id="scirp.59547-formula859"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1720356x14.png"  xlink:type="simple"/></disp-formula><p>and it is related to control problem, its minimisation by seeking controls u results with an optimal control problem. But we want to have time-optimal control problem. In order to obtain time-optimal control problem, we put <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x15.png" xlink:type="simple"/></inline-formula> and hence <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x16.png" xlink:type="simple"/></inline-formula> so that we seek to minimize the time taken to reach the state<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x17.png" xlink:type="simple"/></inline-formula>. We will study this problem for the relatively simple first order differential linear, constant, coefficient equations:</p><disp-formula id="scirp.59547-formula860"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1720356x18.png"  xlink:type="simple"/></disp-formula><p>We are going to study a time series graph, one line that is dependent of time and some other variable [<xref ref-type="bibr" rid="scirp.59547-ref3">3</xref>] . We assume that time series graph has an equilibrium position [<xref ref-type="bibr" rid="scirp.59547-ref3">3</xref>] , it is unstable and it can be moving in infinitely small time up and down. However, irrespectively of the other factors, we assume that time series graph has attained its equilibrium value. We want to find out what kind of external factor can affect it and make it move it out of equilibrium, as it is possible, that the time series graph tends to stay in equilibrium. In order to analyse the following problem, we use the following differential equation:</p><disp-formula id="scirp.59547-formula861"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1720356x19.png"  xlink:type="simple"/></disp-formula><p>where x represents the deviation from the equilibrium value, it could be called vertical deviation from the equilibrium as the 2D time series can move only up and down. As we assume that time series is in equilibrium, u represents external attempts that make the time series graph stays in equilibrium. If we assume that at<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x20.png" xlink:type="simple"/></inline-formula>, the deviation is existent and is presented like<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x21.png" xlink:type="simple"/></inline-formula>. Can this deviation be controlled and if it can be controlled, how quickly can it be controlled?</p><p>First case that we will analyse is that there is no attempt to control the deviation with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x22.png" xlink:type="simple"/></inline-formula>, then the solution of equation is the following:</p><disp-formula id="scirp.59547-formula862"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1720356x23.png"  xlink:type="simple"/></disp-formula><p>With no external factor affecting the time series graph, it is almost certain that the graph will move out of its equilibrium.</p><p>The equilibrium with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x24.png" xlink:type="simple"/></inline-formula> is an unstable equilibrium point. In order to apply general control<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x25.png" xlink:type="simple"/></inline-formula>, we can solve (4) by using the integrating factor<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x26.png" xlink:type="simple"/></inline-formula>, so we have the following [<xref ref-type="bibr" rid="scirp.59547-ref4">4</xref>] :</p><disp-formula id="scirp.59547-formula863"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1720356x27.png"  xlink:type="simple"/></disp-formula><p>And hence we have:</p><disp-formula id="scirp.59547-formula864"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1720356x28.png"  xlink:type="simple"/></disp-formula><p>Since we want to have to analyse the system in equilibrium, we must have <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x29.png" xlink:type="simple"/></inline-formula> when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x30.png" xlink:type="simple"/></inline-formula>, so we must have:</p><disp-formula id="scirp.59547-formula865"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1720356x31.png"  xlink:type="simple"/></disp-formula><p>As<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x32.png" xlink:type="simple"/></inline-formula>, u must be negative for at least some period from<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x33.png" xlink:type="simple"/></inline-formula>. If <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x34.png" xlink:type="simple"/></inline-formula> is not bounded below, it is easy to choose u to satisfy, for example with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x35.png" xlink:type="simple"/></inline-formula>, but however as we can only react in short time as stock price movement follows random walk and exchange rate is changing in infinitely small time intervals, we can control the system in an arbitrarily short time <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x36.png" xlink:type="simple"/></inline-formula> by making <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x37.png" xlink:type="simple"/></inline-formula> sufficiently large. At the same time, there are the systems in economy which control is unbounded, but then time-optimal problem is meaningless. We will take external factors to be in the range of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x38.png" xlink:type="simple"/></inline-formula>.</p><p>In order to push x back towards the equilibrium as quickly as possible, we need to push as hard as possible by taking<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x39.png" xlink:type="simple"/></inline-formula>, so we get:</p><disp-formula id="scirp.59547-formula866"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1720356x40.png"  xlink:type="simple"/></disp-formula><p>The solution is then</p><disp-formula id="scirp.59547-formula867"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1720356x41.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59547-formula868"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1720356x42.png"  xlink:type="simple"/></disp-formula><p>Equation (10) shows that as <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x43.png" xlink:type="simple"/></inline-formula> as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x44.png" xlink:type="simple"/></inline-formula>. If <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x45.png" xlink:type="simple"/></inline-formula> then the system cannot be controlled back to equilibrium.</p><p><xref ref-type="fig" rid="fig1">Figure 1</xref> demonstrates that the equilibrium can only be achieved when deviation is less than one, then equilibrium can be reached. For the values that are higher than <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x46.png" xlink:type="simple"/></inline-formula> the equilibrium solution cannot be reached.</p><p>What is important to notice is that if x is above or below 1, the system is out of equilibrium, and as the time passes it diverges more from the equilibrium. We will introduce the controllable set which represents the set of initial states that can be controlled to the origin or equilibrium in some time. This is the union of all the controllable sets at time<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x47.png" xlink:type="simple"/></inline-formula>.</p><p>The controllable set is given as following [<xref ref-type="bibr" rid="scirp.59547-ref5">5</xref>] :</p><disp-formula id="scirp.59547-formula869"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1720356x48.png"  xlink:type="simple"/></disp-formula><p>If C is the whole real line, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x49.png" xlink:type="simple"/></inline-formula>, we say that the system is completely controllable. Since our system is not the whole real line, it means it is not completely controllable. Now, we must define the reachable set. It is the set where control exists.</p><p>From Equation (7), we have:</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Some time optimal solutions of the problem [<xref ref-type="bibr" rid="scirp.59547-ref2">2</xref>] </title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-1720356x50.png"/></fig><disp-formula id="scirp.59547-formula870"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1720356x51.png"  xlink:type="simple"/></disp-formula><p>and since<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x52.png" xlink:type="simple"/></inline-formula>, we obtain:</p><disp-formula id="scirp.59547-formula871"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1720356x53.png"  xlink:type="simple"/></disp-formula><p>so that we have:</p><disp-formula id="scirp.59547-formula872"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1720356x54.png"  xlink:type="simple"/></disp-formula><p>defines the points in the reachable set<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x55.png" xlink:type="simple"/></inline-formula>. For<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x56.png" xlink:type="simple"/></inline-formula>, the reachable set doesn’t contain the origin and cannot reach the equilibrium. On the other side for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x57.png" xlink:type="simple"/></inline-formula>, the origin or equilibrium is reachable for</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x58.png" xlink:type="simple"/></inline-formula>.</p><p>In order to make the final assumption and summarise the analysis the following will be stated.</p><p>If time series graphs exhibit equilibrium state and tend to diverge from the aforementioned equilibrium state, external influence must be exerted via some of the external factors in order to attain equilibrium. This exertion of external influence can only be conducted in infinitely small time interval and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1720356x59.png" xlink:type="simple"/></inline-formula> must be sufficiently large. If the external influence or factor is unbounded, then optimal time control is not effective and this is what causes big financial disruptions or disruptions in any sense. It is also proved if equilibrium state of time series exhibit maximally one standard deviation, it can be returned to equilibrium state. Deviations larger than one standard deviation cause series to diverge from equilibrium level and to attain new equilibrium. At the same time, even if new financial equilibrium is established, there is still risk of financial disruption and crisis. Unfortunately, when we move away from time optimal control problem, we have to develop a new theory. At the same time, next step concerning the proposed theory is its testing and calibration.</p></sec><sec id="s3"><title>3. Conclusion</title><p>This paper tries to introduce an innovative approach in time series analysis pertaining in that sense to time series that are characterized by equilibrium value. It introduces time optimal control problem and proves that the aforementioned time series can keep their equilibrium in case when the deviation is less than one standard deviation and under the condition that external influence is large enough. In case that external influence is too large, easily financial disruption can be caused. If the deviation from equilibrium is bigger than one s.d, it is possible that new equilibrium state is sought or the system doesn’t know how to behave and that there is a possibility of financial disruption until the state is stabilised again.</p></sec><sec id="s4"><title>Acknowledgements</title><p>My sister Anna thanks a lot.</p></sec><sec id="s5"><title>Cite this paper</title><p>OgnjenVukovic, (2015) Time Optimal Control in Time Series Movement. Journal of Applied Mathematics and Physics,03,1122-1125. doi: 10.4236/jamp.2015.39139</p></sec></body><back><ref-list><title>References</title><ref id="scirp.59547-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Lions, J.L. (1971) Optimal Control of Systems Governed by Partial Differential Equations. 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