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<raweb xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:html="http://www.w3.org/1999/xhtml" xml:lang="en" year="2004" id="id2614750"><identification id="bipop" isproject="false"><shortname id="id2614730">BIPOP</shortname><projectName id="id2614738">Modeling, Simulating, Controlling Non-Regular Dynamical Systems</projectName><theme id="id2588555">NUM</theme><team id="uid1"><participants id="id2614790" category="Head_of_project-team"><person key="bipop-2005-id2245512"><firstname id="id2614798">Bernard</firstname><lastname id="id2614802">Brogliato</lastname><moreinfo id="id2614806">senior research scientist</moreinfo></person></participants><participants id="id2614813" category="Administrative_assistant"><person key="sardes-2005-id2245484"><firstname id="id2614822">Elodie</firstname><lastname id="id2614826">Toihein</lastname><moreinfo id="id2614830">jointly with Popart, Mistis</moreinfo></person></participants><participants id="id2614837" category="Staff_members_Inria"><person key="bipop-2005-id2245453"><firstname id="id2640099">Vincent</firstname><lastname id="id2640103">Acary</lastname><moreinfo id="id2640107">junior research scientist</moreinfo></person><person key="bipop-2005-id2244422"><firstname id="id2640116">Claude</firstname><lastname id="id2640120">Lemaréchal</lastname><moreinfo id="id2640124">senior research scientist</moreinfo></person><person key="bipop-2005-id2245385"><firstname id="id2640133">Pierre-Brice</firstname><lastname id="id2640137">Wieber</lastname><moreinfo id="id2640141">junior research scientist</moreinfo></person></participants><participants id="id2640148" category="Ph._D._students"><person key="bipop-2004-id2244495"><firstname id="id2640157">Jean-Mathieu</firstname><lastname id="id2640161">Bourgeot</lastname><moreinfo id="id2640165">Ministry fellowship, till November 2004</moreinfo></person><person key="bipop-2005-id2244721"><firstname id="id2640173">Sophie</firstname><lastname id="id2640177">Chareyron</lastname><moreinfo id="id2640181">Siconos fellowship</moreinfo></person><person key="bipop-2005-id2244748"><firstname id="id2640190">Mathieu</firstname><lastname id="id2640194">Guilbert</lastname><moreinfo id="id2640198">Cifre fellowship</moreinfo></person><person key="demar-2005-id2244966"><firstname id="id2640207">Rodolphe</firstname><lastname id="id2640211">Heliot</lastname><moreinfo id="id2640215"><span id="id2640218" align="left" class="smallcap">CEA</span> fellowship</moreinfo></person><person key="bipop-2005-id2244530"><firstname id="id2640232">Jérôme</firstname><lastname id="id2640236">Malick</lastname><moreinfo id="id2640241">ENS fellowship</moreinfo></person><person key="bipop-2005-id2244867"><firstname id="id2640249">Doh-Elvis</firstname><lastname id="id2640253">Taha</lastname><moreinfo id="id2640257">as of November 2004;
Inria - Scheider Electric fellowship</moreinfo></person></participants><participants id="id2640266" category="Post-Doc_students"><person key="bipop-2005-id2244886"><firstname id="id2640274">Matthieu</firstname><lastname id="id2640278">Renouf</lastname><moreinfo id="id2640282">Bipop-Siames, as of October 2004; Ministry fellowship</moreinfo></person></participants><participants id="id2640290" category="Training_students"><person key="bipop-2004-id2244680"><firstname id="id2640299">Alexandre</firstname><lastname id="id2640303">Ravoux</lastname><moreinfo id="id2640307">January-June 2004; Siconos fellowship</moreinfo></person><person key="bipop-2005-id2244961"><firstname id="id2640315">Jean-Michel</firstname><lastname id="id2640319">Barbier</lastname><moreinfo id="id2640323">January-September 2004; Siconos fellowship</moreinfo></person><person key="bipop-2004-id2244726"><firstname id="id2640332">Jérémie</firstname><lastname id="id2640337">Blanc-Tranchant</lastname><moreinfo id="id2640340">January-June 2004; Siconos fellowship</moreinfo></person></participants><participants id="id2640349" category="Expert_engineers"><person key="bipop-2005-id2244735"><firstname id="id2640358">Jean-Baptiste</firstname><lastname id="id2640362">Charlety</lastname><moreinfo id="id2640366">as of October 2004; Siconos fellowship</moreinfo></person></participants></team><UR id="id2640375" name="Grenoble"/><moreinfo id="id2640380"><p id="id2640381">This newly created project team gathers researchers from the former
teams Bip and Numopt.</p></moreinfo></identification><presentation id="uid3"><bodyTitle id="id2640394">Overall Objectives</bodyTitle><subsection id="uid4"><bodyTitle id="id2640404">(Sans Titre)</bodyTitle><p id="id2640408">Generally speaking, this project deals with non-regular systems, with
emphasis on</p><simplelist id="id2640414"><li id="uid5"><p id="id2640422">dynamic systems, mostly mechanical systems with unilateral
constraints and Coulomb friction, but also
electrical circuits with ideal diodes, etc;</p></li><li id="uid6"><p id="id2640436">biped robots and their connection with human walking,
a rich and instructive instance of such systems;</p></li><li id="uid7"><p id="id2640448">numerical methods for nonsmooth optimization, and more
generally the connection between continuous and combinatorial optimization.</p></li></simplelist></subsection></presentation><fondements id="uid8"><bodyTitle id="id2640461">Scientific Foundations</bodyTitle><subsection id="uid9"><bodyTitle id="id2640471">Dynamic non-regular systems</bodyTitle><keyword id="id2640474">mechanical systems</keyword><keyword id="id2640477">impacts</keyword><keyword id="id2640480">unilateral constraints</keyword><keyword id="id2640483">complementarity</keyword><keyword id="id2640486">modeling</keyword><keyword id="id2640488">analysis</keyword><keyword id="id2640491">simulation</keyword><keyword id="id2640494">control</keyword><keyword id="id2640497">convex analysis</keyword><p id="id2640501">Dynamical systems (we limit ourselves to finite-dimensional ones) are said to
be <i id="id2640506">non-regular</i> whenever some nonsmoothness of the state arises. This
nonsmoothness may have various roots: for
example some outer impulse, entailing so-called <i id="id2640512">differential equations
with measure</i>. An important class of such systems can be described by the
complementarity system</p><p id="id2640519"><formula type="display" id="uid10"><img align="middle" width="185" height="54" src="math_image_1.png" xylemeAttach="1" border="0" alt="Im1 $\mfenced o={ c=. \mtable{...}$"/></formula></p><p id="id2640771" noindent="true">where <span class="math" align="left"><img width="14" height="13" align="bottom" border="0" src="/images/img_other_bottom.png" alt="$ \bottom$"/></span> denotes orthogonality; <hi rend="italic">u</hi> is a control input. Now
(<ref id="id2640804" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#uid10" location="intern" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/>) can be viewed from different angles.</p><simplelist id="id2640821"><li id="uid11"><p id="id2640830">Hybrid systems: it is in fact natural to consider that
(<ref id="id2640835" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#uid10" location="intern" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/>) corresponds to different models,
depending whether <span class="math" align="left"><hi rend="it">y</hi><sub><hi rend="it">i</hi></sub> = 0</span> or <span class="math" align="left"><hi rend="it">y</hi><sub><hi rend="it">i</hi></sub>&gt;0</span> (<span class="math" align="left"><hi rend="it">y</hi><sub><hi rend="it">i</hi></sub></span> being a component of the vector
<hi rend="italic">y</hi>). In some
cases, passing from one mode to the other implies a jump in the state <hi rend="italic">x</hi>;
then the continuous dynamics in (<ref id="id2640956" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#uid10" location="intern" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/>) may contain distibutions.</p></li><li id="uid12"><p id="id2640980">Differential inclusions: <span class="math" align="left">0<img width="14" height="24" align="middle" border="0" src="/images/img_other_le.png" alt="$ \le$"/><hi rend="it">y</hi><img width="14" height="13" align="bottom" border="0" src="/images/img_other_bottom.png" alt="$ \bottom$"/><img width="11" height="13" align="bottom" border="0" src="/images/img_lambda.png" alt="$ \lambda$"/><img width="14" height="24" align="middle" border="0" src="/images/img_other_ge.png" alt="$ \ge$"/>0</span>
is equivalent to <span class="math" align="left">-<img width="11" height="13" align="bottom" border="0" src="/images/img_lambda.png" alt="$ \lambda$"/><img width="13" height="24" align="middle" border="0" src="/images/img_other_in.png" alt="$ \in$"/> N <sub><hi rend="it">K</hi></sub>(<hi rend="it">y</hi>)</span>, where <hi rend="italic">K</hi> is the nonnegative orthant
and <span class="math" align="left"> N <sub><hi rend="it">K</hi></sub>(<hi rend="it">y</hi>)</span> denotes the normal cone to <hi rend="italic">K</hi> at <hi rend="italic">y</hi>. Then it is not
difficult to reformulate (<ref id="id2590647" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#uid10" location="intern" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/>) as a differential inclusion.</p></li><li id="uid13"><p id="id2590671">Dynamic variational inequalities: such a
formalism reads as <span class="math" align="left"><img align="middle" width="135" height="16" src="math_image_2.png" xylemeAttach="2" border="0" alt="Im2 ${\#9001 \mover x\#729 {(t)}+F(x(t),t),v-x(t)\#9002 \#8805 0}$"/></span>
for all <span class="math" align="left"><hi rend="it">v</hi><img width="13" height="24" align="middle" border="0" src="/images/img_other_in.png" alt="$ \in$"/><hi rend="it">K</hi></span> and <span class="math" align="left"><hi rend="it">x</hi>(<hi rend="it">t</hi>)<img width="13" height="24" align="middle" border="0" src="/images/img_other_in.png" alt="$ \in$"/><hi rend="it">K</hi></span>, where <hi rend="italic">K</hi> is a nonempty closed convex
set. When <hi rend="italic">K</hi> is a polyhedron, then this can also be written as a
complementarity system as in (<ref id="id2590846" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#uid10" location="intern" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/>).</p></li></simplelist><p id="id2590864">Thus, the 2nd and 3rd lines in (<ref id="id2590868" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#uid10" location="intern" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/>) define the modes of the
hybrid systems, as well as the conditions under which transitions occur from
one mode to another. The 4th line
defines how transitions are performed by the state <hi rend="italic">x</hi>. There are
several other formalisms which are quite related to complementarity.
Two tutorial-survey papers have been published <ref id="id2590902" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid9" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/><ref id="id2590918" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid10" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/>,
whose aim is to introduce the dynamics of complementarity systems and
the main available results in the fields of mathematical analysis,
analysis for control (controllability, observability, stability), and
feedback control.
</p></subsection><subsection id="uid14"><bodyTitle id="id2590944">Biped robots</bodyTitle><keyword id="id2590947">control</keyword><keyword id="id2590950">sensor-based control</keyword><keyword id="id2590953">mechanics</keyword><keyword id="id2590955">solid
mechanics</keyword><keyword id="id2590958">modeling</keyword><keyword id="id2590961">robotics</keyword><keyword id="id2590964">mobile robotics</keyword><keyword id="id2590967">simulation of mechanical
systems</keyword><subsection id="uid15"><bodyTitle id="id2590976">Modeling</bodyTitle><p id="id2590980">A biped robot can be modeled <ref id="id2590986" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid11" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/><ref id="id2591002" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid12" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/>
as a tree-like articulated chain of rigid bodies
in <span class="math" align="left"> R <sup>3</sup></span>. Walking is characterized by different phases, mainly (for a given
leg): swing (35% of the cycle), support (65%); there is a double-support
phase (12%), which does not exist when running. A finer decomposition takes
into account the movement of the mass center, and above all of the foot.
These different phases are characterized by different contacts between the
system and the ground.</p><p id="id2591050">As a result, the mechanical model of such a system has three aspects:</p><simplelist id="id2591055"><li id="uid16"><p id="id2591064">the dynamics of a rigid articulated system, free in the space,
representable by Lagrangian equation;</p></li><li id="uid17"><p id="id2591076">a set of equality and inequality constraints, depending on
the phase, which expresses the existence of contacts without penetration nor
sliding; each one of these sets defines an operating mode;</p></li><li id="uid18"><p id="id2591090">the selection of impact laws modeling the transitions (assumed
instantaneous) between these modes.</p></li></simplelist><p id="id2591097">This makes up a sophisticated hybrid system, whose study is still little
explored, see <ref id="id2591103" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid13" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/> for a survey on modeling, stability and
control of biped robots.</p></subsection><subsection id="uid19"><bodyTitle id="id2591127">Controlling</bodyTitle><p id="id2591131">The pace naturally adopted by a human walker
is regular and symmetric, consuming little energy for a reasonable speed.
Some hybrid systems, such as leaping robots or transmissions with slack,
present likewise limit cycles corresponding to dynamic equilibria, possibly
stable in a certain domain. For the simplest walking robot – a compass on a
slope – these cycles correspond to passive periodic trajectories (without
external action), in which the transition between kinematic and potential
energies is entirely balanced by the energy absorbtion during the
impact <ref id="id2591148" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid14" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/>.</p><p id="id2591166">As a result of these considerations, our approach of control aims at
constructing cyclic trajectories, minimizing energy – whatever this means.
Also, it is important to guarantee a global progression while preserving a
particular mechanical stability, which is dynamic. Classical approaches
– for example following accurately nominal articulated trajectories – are
therefore inadequate, except if one is just interested in controlling the
attitude. The field is far from being settled, so we have to explore
diverse control
techniques: nonsmooth optimization, predictive control, adaptive learning,
task function control <ref id="id2591186" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid15" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/>... including sensor-based
control, allowing to use local measures of distance, proximity,
reaction to the ground etc.
</p></subsection></subsection><subsection id="uid20"><bodyTitle id="id2591210">Nonsmooth optimization</bodyTitle><keyword id="id2591212">optimization</keyword><keyword id="id2591215">numerical algorithm</keyword><keyword id="id2591218">convexity</keyword><keyword id="id2591221">Lagrangian relaxation</keyword><keyword id="id2591224">combinatorial optimization</keyword><p id="id2591229">Here we are dealing with the minimization of a function <hi rend="italic">f</hi> (say over
the whole space <span class="math" align="left"> R <sup><hi rend="it">n</hi></sup></span>), whose derivatives are discontinuous. A typical
situation is when <hi rend="italic">f</hi> comes from dualization, if the primal problem is
not strictly convex – for example a large-scale
linear program – or even nonconvex – for example a combinatorial
optimization problem. Also important is the case of spectral functions, where
<span class="math" align="left"><hi rend="it">f</hi>(<hi rend="it">x</hi>) = <hi rend="it">F</hi>(<img width="11" height="13" align="bottom" border="0" src="/images/img_lambda.png" alt="$ \lambda$"/>(<hi rend="it">A</hi>(<hi rend="it">x</hi>)))</span>, <hi rend="italic">A</hi> being a symmetric matrix and <span class="math" align="left"><img width="11" height="13" align="bottom" border="0" src="/images/img_lambda.png" alt="$ \lambda$"/></span> its
spectrum.</p><p id="id2591371">For these types of problems, we are mainly interested in developing efficient
resolution algorithms. Our basic tool is bundling <ref id="id2591377" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid16" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink">Chap. XV</ref>
and we act along two directions:</p><simplelist id="id2591396"><li id="uid21"><p id="id2591404">To explore application areas where nonsmooth optimization
algorithms
can be applied, possibly after some tayloring. A rich field of such
application is combinatorial optimization, with all forms of relaxation
<ref id="id2591412" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid17" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/><ref id="id2591428" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid18" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/>.</p></li><li id="uid22"><p id="id2591452">To explore the possibility of designing more sophisticated
algorithms. This implies an appropriate generalization of second derivatives
when the first derivative does not exist and uses advanced tools of
nonsmooth analysis, for example <ref id="id2591461" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid19" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/>.</p></li></simplelist></subsection></fondements><domaine id="uid23"><bodyTitle id="id2591485">Application Domains</bodyTitle><subsection id="uid24"><bodyTitle id="id2591495">(Sans Titre)</bodyTitle><p id="id2591499">Many systems (either actual or abstract) can be represented by
(<ref id="id2591504" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#uid10" location="intern" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/>). Some typical examples are:</p><simplelist id="id2591523"><li id="uid25"><p id="id2591530">Mechanical systems with unilateral constraints and dry friction (the
biped robot is a typical example), including kinematic chains with slack,
phenomena of liquid slosh, etc.</p></li><li id="uid26"><p id="id2591544">Electrical circuits with ideal diodes and/or transistors MOS.</p></li><li id="uid27"><p id="id2591555">Optimal control with constraints on the state, closed loop of a
system controlled by an MPC algorithm, etc.</p></li></simplelist><p id="id2591562">This class of models is not too large (to allow thorough studies), yet rich
enough to include many applications. This goes in contrast to a study of
general hybrid systems. Note for example that (<ref id="id2591571" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#uid10" location="intern" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/>) is a
``continuous'' hybrid system, in that the continuous variables <hi rend="italic">x</hi> and <hi rend="italic">u</hi>
prevail in the evolution (there is no discrete control to commute from a
mode to the other: only the input <hi rend="italic">u</hi> can be used).</p><p id="id2591623">Walking robots – for example hexapods – possess
definite advantages over the rolling ones whenever the ground is not
plane or free: clearing obstacles is easier, holding on the ground is lighter,
adaptivity is improved. However, if the working environment of the system is
adapted to man, the biped technology must be preferred, to preserve good
displacement abilities without modifying the environment. This explains the
interest displayed by the international community in robotics toward humanoid
systems, whose aim is to back man in some of his activities, professional or
others. For example, a certain form of help at home to disabled persons
could be done by biped robots, as they are able to move without any special
adaptation of the environment.</p><p id="id2591659">In virtual reality and real-time
applications, a major issue is the representation of real phenomena
and the fine control of the model behind it. In particular, the interaction
between objects and therefore the treatment of contact, friction and
impacts is crucial. This treatment is usually decomposed into two tasks:</p><simplelist id="id2591669"><li id="uid28"><p id="id2591679">Geometric detection of the interaction; this is now carried out in a
very efficient way for simple geometric primitives.</p></li><li id="uid29"><p id="id2591691">Numerical treatment, which constitutes the core of
the collaboration between the Siames (Irisa/Rennes) and Bipop
projects. Our main aim is to bridge the gap between the know-how
of Bipop on the nonsmooth mechanics and the know-how of
Siames on virtual reality applications.</p></li></simplelist><p id="id2591701">ptimization exists in virtually all economic sectors. Simulation
tools can be used to optimize the system they simulate. Another domain is
parameter <i id="id2591707">identification</i> (Idopt or Estime teams), where the
deviation between measurements and theoretical predictions must be minimized.
Accordingly, giving an exhaustive list of applications is impossible. Some
domains where Inria has been implied in the past, possibly through the
former Promath and Numopt teams are: production management, geophysics,
finance, molecular modeling, robotics, networks, astrophysics,
crystallography, ...</p></subsection></domaine><logiciels id="uid30"><bodyTitle id="id2591734">Software</bodyTitle><subsection id="uid31"><bodyTitle id="id2591744">(Sans Titre)</bodyTitle><p id="id2591748">Two sorts of software are developed within Bipop.</p><subsection id="uid32"><bodyTitle id="id2591759">Nonsmooth dynamics</bodyTitle><p id="id2591763">In the framework of the European project Siconos, Bipop is the leader of
the Work Package 2 (WP2), dedicated to the numerical methods and the software
design for nonsmooth dynamical systems. The aim
of this work is to provide a common platform for the simulation, modeling,
analysis and control of abstract nonsmooth dynamical systems. Besides usual
quality attributes for scientific computing
software, we want to provide a common framework for various scientific
fields, to be able to rely on the
existing developments (numerical algorithms, description and modeling
software), to support exchanges and
comparisons of methods, to disseminate the know-how to other fields of
research and industry, and to take
into account the diversity of users (end-users, algorithm developers,
framework builders) in building expert
interfaces in Python and end-user front-end through Scilab.</p><p id="id2591784">After the requirements elicitation phase, the Siconos Software project
has been divided into 5 work packages which are identified to software
products:</p><orderedlist id="id2591791"><li id="uid33"><p id="id2591800"><i id="id2591802">Siconos/Numerics</i> This library contains a set of
numerical algorithms, already well identified, to solve non smooth dynamical
systems. This library is written in low-level languages (C,F77) is order to
ensure numerical efficiency and the use of standard libraries (Blas,
Lapack, ...)</p></li><li id="uid34"><p id="id2591825"><i id="id2591826">Siconos/Kernel(Engine<span class="math" align="left">  +  </span>Front-End)</i> The Engine is an
object-oriented structure (C++) for modeling and simulation of abstract
dynamical systems. The Front-End is the driver interface of the Engine
thanks to two types of API's. The first one is an API in C++, interfaced
in Python for scripting uses. The second API, in C, will be interfaced with
Scilab for a more user-friendly platform.</p></li><li id="uid35"><p id="id2591875"><i id="id2591876">Siconos/Analysis</i> This part is devoted to the stability and
bifurcation analysis of nonsmooth dynamical systems.</p></li><li id="uid36"><p id="id2591891"><i id="id2591892">Siconos/Control</i> This part is devoted to the implementation=
of control strategies of non smooth dynamical systems.</p></li><li id="uid37"><p id="id2591906"><i id="id2591907">Siconos/</i><span id="id2591911" align="left" class="smallcap">imse</span><i id="id2591918"/> The final product is an Integrated modeling
and Simulation Environment dedicated to applied nonsmooth problems.</p></li></orderedlist><p id="id2591925">Further informations may be found at
<ref id="id2591931" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="http://siconos.inrialpes.fr/software" location="extern" xyref="401543881006" xmlns:xlink="http://www.w3.org/1999/xlink">http://siconos.inrialpes.fr/software</ref></p></subsection><subsection id="uid38"><bodyTitle id="id2591956">Optimization</bodyTitle><p id="id2591960">Essentially two possibilities exist to distribute our optimization
software: library
programs (say Modulopt codes), communicated either freely or not, depending on
what they are used for, and on the other hand specific software, developed for
a given application.</p><p id="id2591969">The following optimization codes have been developed in the
framework of the former Promath project.</p><subsection id="uid39"><bodyTitle id="id2591980">Code <small id="id2591983"/><small id="id2591984"><b id="id2591986">M1QN3</b></small></bodyTitle><participants id="id2591990" category="None"><person><firstname id="id2591995">Jean-Charles</firstname><lastname id="id2591998">Gilbert</lastname><moreinfo id="id2592000">Estime team – partner</moreinfo></person><person><firstname id="id2592006">Claude</firstname><lastname id="id2592009">Lemaréchal</lastname><moreinfo id="id2592012">partner</moreinfo></person></participants><p id="id2592017">Optimization without constraints for problems with many variables
(<span class="math" align="left"><hi rend="it">n</hi><img width="14" height="24" align="middle" border="0" src="/images/img_other_ge.png" alt="$ \ge$"/>10<sup>3</sup></span>, has been used for <span class="math" align="left"><hi rend="it">n</hi> = 10<sup>6</sup></span>). Technically, uses a limited-memory
<span id="id2592086" align="left" class="smallcap">bfgs</span> algorithm with Wolfe's line-search (see
<ref id="id2592097" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid20" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink">Chap. 4</ref> for the terminology).</p></subsection><subsection id="uid40"><bodyTitle id="id2592122">Code <small id="id2592125"/><small id="id2592126"><b id="id2592128">M2QN1</b></small></bodyTitle><participants id="id2592131" category="None"><person><firstname id="id2592136">Claude</firstname><lastname id="id2592139">Lemaréchal</lastname></person></participants><p id="id2592145">Optimization with simple bound-constraints for (small) problems:
<hi rend="italic">D</hi> is a parallelotope in <span class="math" align="left"> R <sup><hi rend="it">n</hi></sup></span>. Uses <span id="id2592183" align="left" class="smallcap">bfgs</span> with Wolfe's linesearch
and active-set strategy.</p></subsection><subsection id="uid41"><bodyTitle id="id2592200">Code <small id="id2592203"/><small id="id2592204"><b id="id2592206">N1CV2</b></small></bodyTitle><participants id="id2592209" category="None"><person><firstname id="id2592214">Claude</firstname><lastname id="id2592217">Lemaréchal</lastname><moreinfo id="id2592220">partner</moreinfo></person><person><firstname id="id2592226">Claudia</firstname><lastname id="id2592229">Sagastizábal</lastname></person></participants><p id="id2592234">Minimization without constraints of a convex nonsmooth function by a proximal
bundle method (<ref id="id2592240" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid16" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink">Chap.XV</ref>, <ref id="id2592258" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid20" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink">Chap.9</ref>).</p></subsection><subsection id="uid42"><bodyTitle id="id2592283">Modulopt</bodyTitle><participants id="id2592286" category="None"><person><firstname id="id2592292">Jean-Charles</firstname><lastname id="id2592295">Gilbert</lastname><moreinfo id="id2641145">Estime team – partner</moreinfo></person><person><firstname id="id2641150">Claude</firstname><lastname id="id2641153">Lemaréchal</lastname><moreinfo id="id2641156">partner</moreinfo></person></participants><p id="id2641161">In addition to codes such as above, the Modulopt library contains application
problems, synthetic or from the real world. It is a field for experimentation,
functioning both ways: to assess a new algorithm on a set of test-problems, or
to select among several codes one best suited to a given problem.</p></subsection></subsection></subsection></logiciels><resultats id="uid43"><bodyTitle id="id2641176">New Results</bodyTitle><subsection id="uid44"><bodyTitle id="id2641185">Stability and Feedback Control</bodyTitle><subsection id="uid45"><bodyTitle id="id2641195">Stability of evolution variational inequalities</bodyTitle><participants id="id2641199" category="None"><person key="bipop-2005-id2245512"><firstname id="id2641205">Bernard</firstname><lastname id="id2641208">Brogliato</lastname></person></participants><p id="id2641212">We continued our work with D. Goeleven, from the University of la Réunion on
systems of the type <span class="math" align="left"><img align="middle" width="119" height="16" src="math_image_3.png" xylemeAttach="3" border="0" alt="Im3 ${\#9001 \mover x\#729 (t)+Ax{(t)},v-x{(t)}\#9002 \#8805 0}$"/></span>
for all <span class="math" align="left"><hi rend="it">v</hi><img width="13" height="24" align="middle" border="0" src="/images/img_other_in.png" alt="$ \in$"/><hi rend="it">K</hi></span>, <span class="math" align="left"><hi rend="it">x</hi>(<hi rend="it">t</hi>)<img width="13" height="24" align="middle" border="0" src="/images/img_other_in.png" alt="$ \in$"/><hi rend="it">K</hi></span> (<hi rend="italic">K</hi> being a nonempty closed convex set).
Necessary conditions for the asymptotic stability have been obtained in
<ref id="id2641369" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid21" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/>, where the notion of Brouwer degree of a function is used.
The difficulty
here is that the function is nonsmooth. The results are applied to the
asymptotic stabilization of a controlled variational inequality. They
show that in general the controllability of the unconstrained system, is
neither sufficient nor necessary to assure the existence of a constant
feedback which guarantee asymptotic stability.</p><p id="id2641395">The LaSalle invariance principle has also been studied for the case of
evolution variational inequalities, see Sect. <ref id="id2641403" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#uid48" location="intern" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/>.</p></subsection><subsection id="uid46"><bodyTitle id="id2641426">Absolute stability with maximal monotone mappings</bodyTitle><participants id="id2641430" category="None"><person key="bipop-2005-id2245512"><firstname id="id2641436">Bernard</firstname><lastname id="id2641439">Brogliato</lastname></person></participants><p id="id2641444">We recall that the absolute stability problem
consists of studying the stability of a system made
of the negative feedback interconnection of a dissipative system with a
nonlinear characteristic. Last year in <ref id="id2641452" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid6" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/> we extended
absolute stability to a
feedback branch containing a maximal monotone operator. These results have
been used subsequently in <ref id="id2641474" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid22" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/><ref id="id2641489" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid23" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/> to design stable observers
(open-loop <ref id="id2641507" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid23" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/>), and feedback controllers using observed states
(closed-loop <ref id="id2641525" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid22" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/>). There is an additional difficulty in the sense
that we now
consider inclusions which are non-autonomous. All of these works use
well-posedness results for monotone diferential inclusions
<i id="id2641546">à la</i> Brézis.</p></subsection><subsection id="uid47"><bodyTitle id="id2641556">Tracking control of complementarity Lagrangian systems</bodyTitle><participants id="id2641560" category="None"><person key="bipop-2004-id2244495"><firstname id="id2641565">Jean-Matthieu</firstname><lastname id="id2641568">Bourgeot</lastname></person><person key="bipop-2005-id2245512"><firstname id="id2641574">Bernard</firstname><lastname id="id2641577">Brogliato</lastname></person></participants><p id="id2641582">As a sequel to our previous works <ref id="id2641587" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid24" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/><ref id="id2641603" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid25" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/>,
we clarified in <ref id="id2641620" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid3" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/> the design and the role of the
transition phases (stabilisation on the constraint surface or detachment
from this surface) in the closed-loop stability, extending the so-called
passivity-based control design to unilaterally constrained systems.
In <ref id="id2641642" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid4" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/>, the robustness of these family of controllers has been tested
with numerical simulations.</p></subsection><subsection id="uid48"><bodyTitle id="id2641667">Lyapunov stability theory and LaSalle's invariant theorem
for nonsmooth dynamical systems</bodyTitle><participants id="id2641672" category="None"><person key="bipop-2005-id2244721"><firstname id="id2641678">Sophie</firstname><lastname id="id2641680">Chareyron</lastname></person><person key="bipop-2005-id2245385"><firstname id="id2641685">Pierre-Brice</firstname><lastname id="id2641688">Wieber</lastname></person></participants><p id="id2641693">The mathematical analysis of nonsmooth Lagrangian
dynamical systems requires mathematical tools which are
unusual in control theory: velocities with locally bounded variations,
measure accelerations, measure differential inclusions, to name a
few. The control theory for such dynamical systems is just beginning
to appear, and even the basic Lyapunov stability theory still needs to
be stated. In <ref id="id2641707" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid26" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/>, we propose a Lyapunov stability theorem
for dynamical systems with state discontinuities. Based on this theorem, we are
then able to propose a Lagrange-Dirichlet
theorem for nonsmooth Lagrangian dynamical systems that can be
applied through Potential Shaping to the regulation of the position
and force of a robotic manipulator <ref id="id2641730" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid27" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/>.
Note that though we have been able to derive a Lyapunov stability analysis for
nonsmooth dynamical systems very similar to what appear in the smooth case,
the derivation of a theorem equivalent to the LaSalle's invariance theorem is
far from being straighforward. A key condition for the statement of Lasalle's
invariance theorem is
the continuity of the trajectories of the systems with respect to
initial conditions. Nonsmooth Lagrangian dynamical systems generally
do not present such a continuity, but they do in many
specific cases. So we propose in <ref id="id2641758" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid28" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/>
a version of LaSalle's invariance theorem for
time-invariant flows that are countinuous with respect to initial
conditions.</p></subsection><subsection id="uid49"><bodyTitle id="id2641784">The BIP robot, an experimental setup for humanoid walking</bodyTitle><participants id="id2641788" category="None"><person key="bipop-2005-id2245385"><firstname id="id2641794">Pierre-Brice</firstname><lastname id="id2641797">Wieber</lastname></person></participants><p id="id2641802">First experiments of standing with different task function control
laws have been undertaken, but the results in tracking reference
trajectories revealed deficiencies in the velocity observer and the
friction compensation. Then
a breakage of the mechanical structure (left hip) stopped
experimentations for 4 months; as a result, our work on
improvement of the trajectory tracking resumed by the end of the year.</p></subsection><subsection id="uid50"><bodyTitle id="id2641820">Simulation of walking: humanoid robots and
electro-stimulated paraplegic people</bodyTitle><participants id="id2641825" category="None"><person key="bipop-2005-id2245385"><firstname id="id2641830">Pierre-Brice</firstname><lastname id="id2641833">Wieber</lastname></person></participants><p id="id2641839">The modeling and simulation software for humanoid robots and
electro-stimulated paraplegic people, developed the team in
C/C++/Scilab/Maple, is used at Inria Rhône-Alpes, LMS in
Poitiers and LIRM in Montpellier. It is soon to reach its first
official release, with more realistic models of the sensors of the Bip
robot, and a complete dynamical model of the electro-stimulated
muscles of paraplegic people.</p></subsection><subsection id="uid51"><bodyTitle id="id2641863">Trajectory generation for industrial robot</bodyTitle><participants id="id2641867" category="None"><person key="bipop-2005-id2245385"><firstname id="id2641873">Pierre-Brice</firstname><lastname id="id2641876">Wieber</lastname></person><person key="bipop-2005-id2244748"><firstname id="id2641881">Matthieu</firstname><lastname id="id2641884">Guilbert</lastname></person></participants><p id="id2641889">Work done with Stäubli SCA, Faverges (Luc Joly).</p><p id="id2641895">Trajectory generation in industry is usually based on simple laws like
bang-bang profile. Such a profile is not adapted to industrial
problems because it makes it difficult to search the best trajectory for a
given task. Accordingly, we formulate the problem of trajectory
generation as a constrained optimization problem. We model the robot
(geometry, kinematics and dynamics) and the physical constraints (on actuators,
temperature, etc.) in a traditional way. For a numerical resolution, the profile
is discretized by cubic splines and the constrained optimization problem is
solved by a Sequential Quadratic Programming solver. Our
algorithm is robust to the initial conditions, and it can be implemented as
an off-line optimization tool; see <ref id="id2641914" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid29" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/>.
</p></subsection></subsection><subsection id="uid52"><bodyTitle id="id2641936">Controllability</bodyTitle><p id="id2641940">Our controllability studies concern two classes of complementarity
systems: juggling systems and planar evolution variational inequalities.
In the first case, it is shown that studying controllability amounts to
solving a nonlinear system subject to inequality
constraints <ref id="id2641950" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid30" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/>. The second study <ref id="id2641967" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid31" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/> shows that
controllability
depends on the form of the convex set <hi rend="italic">K</hi> in which the system is
constrained to evolve. Interestingly enough, the complementarity
conditions that are activated on the boundary of <hi rend="italic">K</hi> may improve
controllability in some cases.
</p></subsection><subsection id="uid53"><bodyTitle id="id2642015">Modeling</bodyTitle><subsection id="uid54"><bodyTitle id="id2642024">Unified models in nonsmooth mechanics</bodyTitle><participants id="id2642028" category="None"><person key="bipop-2005-id2245453"><firstname id="id2642034">Vincent</firstname><lastname id="id2642036">Acary</lastname></person><person key="bipop-2005-id2245512"><firstname id="id2642042">Bernard</firstname><lastname id="id2642045">Brogliato</lastname></person><person><firstname id="id2642050">Claude</firstname><lastname id="id2642053">Lemaréchal</lastname></person></participants><p id="id2642058">Work done with A. Daniilidis (Autonomous Univ. of Barcelona), a former
post-doctoral fellow at Inria Rhône-Alpes.</p><p id="id2642067">A complementarity model such as (<ref id="id2642073" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#uid10" location="intern" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/>) is actually an instance of
more general differential <i id="id2642091">inclusions</i>, where the speed <span class="math" align="left"><img align="bottom" width="6" height="7" src="math_image_4.png" xylemeAttach="4" border="0" alt="Im4 $\mover x\#729 $"/></span> is
constrained to lie in some set <hi rend="italic">T</hi>. Equivalence of a few such models was
known before under fairly <i id="id2642128">ad hoc</i>
assumptions <ref id="id2642135" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid32" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/>. Using exclusively
tools from standard convex and nonsmooth analysis, we establish in
<ref id="id2642154" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid33" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/> the same
equivalence with several other models, under much simpler assumptions; this
work in particular reveals the importance of the concept of <i id="id2642174">slow</i>
solution <ref id="id2642178" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid34" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/>.</p></subsection><subsection id="uid55"><bodyTitle id="id2642202">Multiple impacts</bodyTitle><participants id="id2642205" category="None"><person key="bipop-2005-id2245453"><firstname id="id2642210">Vincent</firstname><lastname id="id2642213">Acary</lastname></person><person key="bipop-2005-id2245512"><firstname id="id2642219">Bernard</firstname><lastname id="id2642222">Brogliato</lastname></person><person key="bipop-2005-id2244867"><firstname id="id2642227">Doh-Elvis</firstname><lastname id="id2642230">Taha</lastname></person></participants><p id="id2642234">An impact is said to be multiple when several impacts occur at the same time
on the system. The multiple impact mappings which have already been proposed
in the literature are not satisfactory, because they often entail
post-impact velocities that obviously disagree with experiments, and/or
are not tractable from the numerical point of view. Based on previous
works in Bipop <ref id="id2642247" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid35" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/>, <ref id="id2642264" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid36" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/>,
the goal of the PhD thesis D.E. Taha in
collaboration with Schneider Electric is to extend the multiple impact law to
finite-dimensional systems such as circuit breakers and to exhibit the
limit of validity of the approach (assumption of quasi-rigid solids).
</p></subsection></subsection><subsection id="uid56"><bodyTitle id="id2642291">Nonsmooth optimization</bodyTitle><p id="id2642295">Generally speaking, our activity this year has mainly consisted
of <i id="id2642299">synthetic works</i>, revisiting various technical subjects from a
higher convex-analysis perspective.</p><subsection id="uid57"><bodyTitle id="id2642311">Classification of nonsmooth functions</bodyTitle><participants id="id2642315" category="None"><person key="bipop-2005-id2244530"><firstname id="id2642320">Jerôme</firstname><lastname id="id2642323">Malick</lastname></person></participants><p id="id2642328">Work done with A. Daniilidis (Autonomous Univ. of Barcelona), a former
post-doctoral fellow at Inria Rhône-Alpes.</p><p id="id2642337">Important nonsmooth functions are lower-<span class="math" align="left"><hi rend="it">C</hi><sup>1</sup></span> and lower-<span class="math" align="left"><hi rend="it">C</hi><sup>2</sup></span> functions
(a lower-<span class="math" align="left"><hi rend="it">C</hi><sup><hi rend="it">k</hi></sup></span> function is the supremum of <span class="math" align="left"><hi rend="it">C</hi><sup><hi rend="it">k</hi></sup></span> functions). We have defined
and studied in <ref id="id2642432" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid37" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/> a class of intermediate functions,
called lower-<span class="math" align="left"><img align="bottom" width="20" height="8" src="math_image_5.png" xylemeAttach="5" border="0" alt="Im5 $C^{1,\#945 }$"/></span>; they play a role analogous to
Hölder functions in standard analysis.</p></subsection><subsection id="uid58"><bodyTitle id="id2642486">Separation in combinatorial optimization</bodyTitle><participants id="id2642490" category="None"><person><firstname id="id2642496">Claude</firstname><lastname id="id2642499">Lemaréchal</lastname></person></participants><p id="id2642504">Work done in collaboration with
Gérard Cornuéjols (Carnegie Mellon) and funded by the Inria new
investigation grant ODW, extending over 2003-04.</p><p id="id2642514">One of the crucial techniques in combinatorial optimization
is <i id="id2642518">separation</i>: given a closed convex set <hi rend="italic">P</hi>
and a point <span class="math" align="left"><img align="middle" width="26" height="15" src="math_image_6.png" xylemeAttach="6" border="0" alt="Im6 ${\mover x¯\#8713 P}$"/></span>, find a hyperplane separating <span class="math" align="left"><img align="bottom" width="6" height="7" src="math_image_7.png" xylemeAttach="7" border="0" alt="Im7 $\mover x¯$"/></span> from
<hi rend="italic">P</hi> ``best''. Traditional studies of this problem are limited to a polyhedral
<hi rend="italic">P</hi> and rely heavily on LP theory.
In <ref id="id2642612" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid38" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/> (submitted to Mathematical Programming),
we consider this question from the
higher point of view of convex analysis, confirming the importance of
the <i id="id2642631">reverse polar</i><ref id="id2642637" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid39" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/> of a set <hi rend="italic">Q</hi>:</p><p id="id2642663"><formula type="display"><img align="middle" width="165" height="18" src="math_image_8.png" xylemeAttach="8" border="0" alt="Im8 ${Q_-^\#8728 :={d:d^\#8868 x\#8804 -1{~\mtext for~\mtext all~{x\#8712 Q}}}~.}$"/></formula></p><p id="id2642778" noindent="true">It is the set of directions separating <hi rend="italic">Q</hi> from 0 <i id="id2642793">strictly</i>,
and is at the same time a <i id="id2642797">closed</i> set, which considerably eases theory
and computations. We show how this new perspective can be applied to
disjunctive cuts <ref id="id2642807" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid40" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/>.
This synthetic point of view helps understanding
better the issue, suggests an appropriate definition of ``best'' separations,
and opens the way to generalizations (say to SDP relaxations).</p></subsection><subsection id="uid59"><bodyTitle id="id2642834">Unified perspective on partly smooth functions</bodyTitle><participants id="id2642838" category="None"><person key="bipop-2005-id2244530"><firstname id="id2642844">Jerôme</firstname><lastname id="id2642847">Malick</lastname></person></participants><p id="id2642852">Work done with S. Miller (Univ. of Cal. at San Diego), a former
post-doctoral fellow at Inria Rhône-Alpes.</p><p id="id2642860">The concept of smooth restriction of a nonsmooth function <hi rend="italic">f</hi> to a smooth
manifold was exhibited in <ref id="id2642877" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid19" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/>; it is
fundamental to design fast algorithms minimizing <hi rend="italic">f</hi>. Making use of its
formalization <ref id="id2642907" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid41" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/>, we analyze in
<ref id="id2642924" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid42" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/> (submitted to Mathematical Programming)
fruitful links with
Riemannian geometry <ref id="id2642943" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid43" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/>, SQP theory <ref id="id2642960" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid20" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/>,
proximal mapping <ref id="id2642977" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid44" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/>. Our study reveals the
importance of the existence of the so-called U-gradient (essentially: the
gradient of the smooth part of <hi rend="italic">f</hi>), without which developing the smooth part
of <hi rend="italic">f</hi> to second order is hardly conceivable.</p></subsection><subsection id="uid60"><bodyTitle id="id2643026">The spherical constraint in combinatorial optimization</bodyTitle><participants id="id2643030" category="None"><person key="bipop-2005-id2244530"><firstname id="id2643035">Jerôme</firstname><lastname id="id2643038">Malick</lastname></person></participants><p id="id2643043">Recall (see <ref id="id2643048" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid17" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/> for example) that SDP relaxations of
a combinatorial problem replace the variable <span class="math" align="left"><hi rend="it">x</hi><img width="13" height="24" align="middle" border="0" src="/images/img_other_in.png" alt="$ \in$"/>{-1,  + 1}<sup><hi rend="it">n</hi></sup></span> by a
symmetric <span class="math" align="left"><hi rend="it">n</hi>×<hi rend="it">n</hi></span> matrix <hi rend="italic">X</hi> (standing for <span class="math" align="left"><img align="bottom" width="19" height="8" src="math_image_9.png" xylemeAttach="9" border="0" alt="Im9 ${xx^\#8868 }$"/></span>) of rank 1 and whose
diagonal entries are all 1
(then they relax the rank-one constraint to <span class="math" align="left"><img align="middle" width="28" height="15" src="math_image_10.png" xylemeAttach="10" border="0" alt="Im10 ${X\#10928 0}$"/></span>).</p><p id="id2643196">In <ref id="id2643200" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid45" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/> we note that
the set of such matrices can also be described by the constraits
<span class="math" align="left"><img align="middle" width="28" height="15" src="math_image_10.png" xylemeAttach="10" border="0" alt="Im10 ${X\#10928 0}$"/></span> and <span class="math" align="left"><img align="middle" width="59" height="17" src="math_image_11.png" xylemeAttach="11" border="0" alt="Im11 ${\#8721 _{ij}X_{ij}=n^2}$"/></span>.
Then we propose to dualize this latter <i id="id2643292">single</i> quadratic constraint,
say with a multiplier <span class="math" align="left"><img width="12" height="12" align="bottom" border="0" src="/images/img_alpha.png" alt="$ \alpha$"/></span>. For
<span class="math" align="left"><img width="12" height="12" align="bottom" border="0" src="/images/img_alpha.png" alt="$ \alpha$"/> = 0</span>, the optimal value of the Lagrangian is the SDP bound, while the
duality gap is closed when <span class="math" align="left"><img width="12" height="12" align="bottom" border="0" src="/images/img_alpha.png" alt="$ \alpha$"/><img width="17" height="12" align="bottom" border="0" src="/images/img_other_rightarrow.png" alt="$ \rightarrow$"/>-<img width="17" height="12" align="bottom" border="0" src="/images/img_infty.png" alt="$ \infty$"/></span>. On the other hand,
the Lagrangian problem for <span class="math" align="left"><img width="12" height="12" align="bottom" border="0" src="/images/img_alpha.png" alt="$ \alpha$"/>&gt;0</span> is a so-called SDLS problem, which
is substantially easier than a standard linear SDP: <ref id="id2643388" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid46" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/>.
This opens the way to potentially more efficient relaxations than SDP.
Besides, an interesting class of nonconvex problems with no duality gap is
thus revealed.</p></subsection><subsection id="uid61"><bodyTitle id="id2643414">Convex optimization and column generation</bodyTitle><participants id="id2643417" category="None"><person><firstname id="id2643422">Claude</firstname><lastname id="id2643425">Lemaréchal</lastname></person></participants><p id="id2643430">Work done in collaboration with F. Vanderbeck (Univ. Bordeaux 1) and
K.C. Kiwiel (Systems Research Institute, Warsaw) and funded by the Inria new
investigation grant ODW, extending over 2003-04; see Numopt
Activity Report 2003, §6.2).</p><p id="id2643444">For technical reasons the team from Geneva had to withdraw from this project.
Our continued collaboration with the team from Bordeaux
confirmed last year's results: compared with the traditional Dantzig-Wolfe
algorithm, the bundle approach is always competitive and sometimes
drastiscally faster. This, however, holds in terms of numbers of calls to the
oracle. On the other hand, we observed strange behaviours:
an NP oracle may take considerably more CPU time when called by bundle.
It is therefore crucial for bundle to accept inaccurate oracles, thereby
reducing computing times (see Numopt Activity Report 2003, §6.3).
Accordingly, we implemented with K.C. Kiwiel his version of bundle with
noise <ref id="id2643476" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid47" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/>.</p><p id="id2643494">This work was also the occasion to revisit <i id="id2643496">stabilization</i> of
Dantzig-Wolfe (see <ref id="id2643502" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid48" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/><ref id="id2643518" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid49" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/><ref id="id2643534" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid50" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/> among others), relating it with the
Moreau-Yosida regularization in the dual space. These results are published in
<ref id="id2643554" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="#bid51" location="biblio" xyref="3693816422022" xmlns:xlink="http://www.w3.org/1999/xlink"/>, submitted to Mathematical Programming.
</p></subsection></subsection><subsection id="uid62"><bodyTitle id="id2643576">Software development</bodyTitle><participants id="id2643580" category="None"><person key="bipop-2005-id2245453"><firstname id="id2643585">Vincent</firstname><lastname id="id2643588">Acary</lastname></person><person key="bipop-2005-id2244735"><firstname id="id2643594">Jean-Baptiste</firstname><lastname id="id2643596">Charlety</lastname></person><person key="bipop-2004-id2244726"><firstname id="id2643602">Jérémie</firstname><lastname id="id2643605">Blanc-Tranchant</lastname></person><person key="bipop-2005-id2244961"><firstname id="id2643611">Jean-Michel</firstname><lastname id="id2643613">Barbier</lastname></person><person key="bipop-2004-id2244680"><firstname id="id2643619">Alexandre</firstname><lastname id="id2643622">Ravoux</lastname></person></participants><p id="id2643627">The deliverable D2.2 has been successfully delivered in March 2004. It
reports on the work carried out at Inria (CO1) and <span id="id2643633" align="left" class="smallcap">Lmgc</span> (AC2) on the
architectural design of the Siconos Platform. The contents of this
deliverable follow the work performed between September 2003 and March 2004:</p><orderedlist id="id2643646"><li id="uid63"><p id="id2643654">The Quality Plan (QP v1.0). Following the recommendations of the
first review meeting, a project management plan has been defined with the
definition of a work breakdown structure and a set of milestones for the
development process.</p></li><li id="uid64"><p id="id2643669">The Software Requirements Document (SRD v1.0) summarizes the work
done with the end-users on the elicitation of functional requirements. It
contains also the requirements concerning the performance, interface,
resources, portability and quality. All of the specifications are
classified in order to facilitate the definition of Milestones.</p></li><li id="uid65"><p id="id2643686">The External Specification Document (ESD v1.0) specifies the using
context and the user interfaces.</p></li><li id="uid66"><p id="id2643698">The Architectural Design Document (ADD) describes the major features
of the general architecture of the platform. This work is based on the
SA/SD method and the UML tools.</p></li><li id="uid67"><p id="id2643712">The contents of the Theory Manual (TM). This document contains a
first attempt at collecting some theoretical material in order to use
the platform. It will be finished with the first version of the Software
User Manual (SUM).</p></li><li id="uid68"><p id="id2643727">A first Template on the numerical simulation of Lagrangian
systems associated with ``Guidelines for authors'' for a template.</p></li></orderedlist><p id="id2643734">The four first documents are based on the ESA (European Space Agency)
standards for software engineering. Most of these documents are still in
progress. A stable version in June 2004 has been tagged as version 1.0,
available on the private area of the Siconos WP2 website.</p><p id="id2643742">The major achievement performed by the Bipop Project between April 2004
and September 2004 is the detailed design and the first implementation of
the Siconos/Engine, the kernel of the Siconos platform. The general
implementation in C++ of the complete skeleton of the architecture has been
carried out as it has been defined in the ADD document. The development
provides the first version of the <span id="id2643754" align="left" class="smallcap">api</span> C++ as an expert interface to
the platform. The detailed implementation of the data input and output in XML
format has been completed. This module is based on the API DOM and SAX,
norms of the W3C, implemented in the Libxml2 library. Specific XML formats
have been defined with the help of the XML scheme. This data file serves
as expert users data files and as internal data base for the platform.
The platform is now able to read an XML data file, check its validity with
respect to the scheme, and save it. Dynamic instantiation of new object in
the platform through the user interface is also taken into account.
Finally, the detailed implementation of the formalization of various
nonsmooth dynamical system has been performed together with validations and
benchmarks.
</p></subsection></resultats><international id="uid69"><bodyTitle id="id2643784">Other Grants and Activities</bodyTitle><subsection id="uid70"><bodyTitle id="id2643794">European Actions</bodyTitle><p id="id2643798">The Bipop project coordinates the European project Siconos (modeling,
SImulation and COntrol of NOnsmooth dynamical Systems, IST 2001-37172),
which is an FP5 project starting September 2002 and ending September
2006. See <ref id="id2643808" xlink:actuate="onRequest" xlink:show="replace" xlink:type="simple" xlink:href="http://siconos.inrialpes.fr" location="extern" xyref="1011774959017" xmlns:xlink="http://www.w3.org/1999/xlink">http://siconos.inrialpes.fr</ref>.
</p></subsection><subsection id="uid71"><bodyTitle id="id2643832">Invitations of specialists</bodyTitle><p id="id2643836" noindent="true">– G. Cornuéjols (Carnegie Mellon) 2 weeks;</p><p id="id2643845" noindent="true">– K. Goeleven (Univ. la Réunion) 1 week;</p><p id="id2643853" noindent="true">– K.C. Kiwiel (Systems Research Institute, Warsaw) 2 weeks;</p><p id="id2643862" noindent="true">– F. Potra (Univ. Maryland, Baltimore) 1 week.
</p></subsection><subsection id="uid72"><bodyTitle id="id2643875">Teaching</bodyTitle><p id="id2643880" noindent="true">– Univ. Joseph Fourier, Grenoble
(V. Acary: tutoring ``Mathematical models for physics'' 48h;
S. Chareyron: tutoring discrete time control, 21h;
J. Malick: various, 70h);</p><p id="id2643892" noindent="true">– Polytech'Grenoble (J.-M. Bourgeot: tutoring automatic control, 21h;
S. Chareyron: tutoring identification and control, 21h);</p><p id="id2643904" noindent="true">– Ensimag, Grenoble (C. Lemaréchal, J. Malick: Numerical
Optimization, 21h);</p><p id="id2643915" noindent="true">– École de Physique, Chimie, Électronique de Lyon
(C. Lemaréchal: Numerical Optimization, 16h);</p><p id="id2643925" noindent="true">– Artelys Lectures, Paris (C. Lemaréchal: Nonlinear Programming,
Combinatorics 2, 10h);</p><p id="id2643937" noindent="true">– RTE, Versailles (C. Lemaréchal: Nonlinear Programming and
Lagrangian relaxation, 10h);</p></subsection><subsection id="uid73"><bodyTitle id="id2643954">Participation to conferences, seminars, invitations</bodyTitle><p id="id2643960" noindent="true">– 8th Workshop on Combinatorial Optimization; Aussois, Jan. 2003;</p><p id="id2643969" noindent="true">– Journées du Groupe Mode; le Havre, March 2004 (1 presentation);</p><p id="id2643978" noindent="true">– Siconos General Meetings; Grenoble, March 2004; Univ. of Bristol,
Sept. 2004 (3-5 participants, 2-3 presentations each time).</p><p id="id2643990" noindent="true">– Meetings for the Robea Project ``Commande pour la marche et la
course d'un robot bipède''; Paris, March 2004; Metz, Oct. 2004 (1 participant,
2 presentations each time);</p><p id="id2644000" noindent="true">– Meeting for the Robea Project ``Contrôle du mouvement du member
inférieur humain paralysé sous stimulation électrique'' Montpellier,
June and Nov. 2004 (1 participant, 1 presentation each time);</p><p id="id2644016" noindent="true">– Journées SFDS (French Assoc. Statistics); Montpellier, May 2004
(1 presentation);</p><p id="id2644026" noindent="true">– School on Constrained Control and Estimation; Grenoble, Sept. 2004
(2 participants);</p><p id="id2644036" noindent="true">– Piecewise Smooth Dynamical Systems: Analysis, Numerics and
Applications, Sept. 2004 ( participants, 2 presentations);</p><p id="id2644048" noindent="true">– HLR'04 workshop on humanoid and legged robots; Metz, Oct. 2004 (2
presentations).</p></subsection></international><diffusion id="uid74"><bodyTitle id="id2644063">Dissemination</bodyTitle><subsection id="uid75"><bodyTitle id="id2644073">Dissemination of software</bodyTitle><p id="id2644077">N1cv2 is used at Univ. Polit. Catalunya (E.C. Sancho, bilevel programming)
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