3 Pages

A07

Course: ICSB 07, Fall 2009
School: Caltech
Rating:
 
 
 
 
 

Word Count: 762

Document Preview

Control Optimal Formulation of Constrained Least-Square Estimation for Biochemical Pathway Estimation Cranos Williams 1, , Winser Alexander 1 , William Edmonson 1 1. Department of Electrical and Computer Engineering, North Carolina State University, Raleigh, NC, USA E-mail: cmwilli5@ncsu.edu Introduction In our work, we present an optimal control formulation of a constrained-least squares estimation problem...

Register Now

Unformatted Document Excerpt

Coursehero >> California >> Caltech >> ICSB 07

Course Hero has millions of student submitted documents similar to the one
below including study guides, practice problems, reference materials, practice exams, textbook help and tutor support.

Course Hero has millions of student submitted documents similar to the one below including study guides, practice problems, reference materials, practice exams, textbook help and tutor support.
Control Optimal Formulation of Constrained Least-Square Estimation for Biochemical Pathway Estimation Cranos Williams 1, , Winser Alexander 1 , William Edmonson 1 1. Department of Electrical and Computer Engineering, North Carolina State University, Raleigh, NC, USA E-mail: cmwilli5@ncsu.edu Introduction In our work, we present an optimal control formulation of a constrained-least squares estimation problem that addresses several issues inherent to biochemical pathway modeling which include limited sparse measurements, nonlinear system characteristics, and biological constraints of pathway components. We verify the functionality of this algorithm on a single-step signal transduction pathway, which serves as a chemical reaction template for larger more complex biochemical pathways. Our results suggests that efforts spents towards further development of these approaches may lead to more successful applications of pathway modeling to problems like drug design, cancer treatment, and biofuel synthesis. Methodology Single-Step Signal Transduction Pathway Kutalik et al. present a description of a single-step signal transduction pathway in [3]. S + E ES E + P p 1 p2 p3 (1) The series of reactions in (1) are comprised of four components, the substrate (S), the enzyme (E), the enzyme-substrate complex (ES), and the product (P). The system of difference equations that describe the dynamics of this pathway can be written in discrete state space form xk+1 = f(xk , p) (2) where x R41 represents the state vector, p R31 represents the kinetic parameter vector, and f() : R41 R41 is a nonlinear vector function. This system has no external inputs, thus the dynamics of the system are completely described by the initial concentrations of the system components and the values of the kinetic rate parameters. Theory Define the following least-squares approach to estimating the initial component concentrations x0 and the kinetic parameters p of the pathway: x0 , p min J0 (x0 , p) = 1 2 (h(xi ) - yi )T (h(xi ) - yi ) iI (3) subject to xk+1 = f(xk , p), k = 0, . . . , N - 1 xk 0, k = 0, . . . , N - 1 (4) where I is the set of time points where measurements are observed, h() models our ability to measure the system, and yi are the observed measurements. We formulate an optimal control approach to solving this minimization problem, utilizing Lagrange multipliers, the Hamiltonian of the system, and a technique used to handle explicit constraints on the states [4] [5]. This results in a two-point boundary value problem represented by a system of coupled difference equations. These coupled difference equations, along with the associated boundary conditions, were used to implement a conjugate gradient based to approach estimating the initial concentrations and kinetic parameters of the pathway. Analysis and Results Our analysis poses a problem where estimates of x0 and p are acquired using simulated discrete-time measurements of the substrate and the product. The system was simulated using an initial concentration vector x = [12, 12, 0, 0]T and a kinetic parameter vector 0 p = [0.18, 0.02, 0.23]T . The simulated discrete-time measurements were obtained at 6 uniformly spaced intervals corresponding to 0 min, 2 min, 4 min, 6 min, 8 min, and 10 min. We tested the consistency of the algorithm by executing 50 independent runs at 50 different initial guess where all initial guess were within valid biological ranges. Table 1 summarizes the average and variance of the estimates over 50 runs. The initial concentrations for x1 and x4 are observed and assumed known and constant. The largest absolute error between true value and average estimates are on order O(10-6). We see a maximum variation of order O(10-11) over the 50 independent runs. These results highlight the algorithm's ability to consistently provide accurate estimates. Figure 1 shows both the true and estimated state trajectories, illustrating very little difference between the two. The maximum average relative error over all states was on order O(10-6) with the maximum relative error on order O(10-5). Our results suggests that efforts spent towards further improvement of these estimation approaches may lead to more successful applications of pathway modeling to practical biological and environmental problems. References [1] H. Kitano, "Systems Biology: A Brief Ov...

Find millions of documents on Course Hero - Study Guides, Lecture Notes, Reference Materials, Practice Exams and more. Course Hero has millions of course specific materials providing students with the best way to expand their education.

Below is a small sample set of documents:

Caltech - ICSB - 07
Invasive Behaviors of Growing Solid TumorsFang Jin 1 , Yao-Li Chuang 1, , Steven Wise 2 , Xiaoming Zheng 3 , John Lowengrub 1,4,5 , Hermann Frieboes 6,1 , Vittorio Cristini 6,7 1. Mathematics Department, University of California, Irvine, Irvine, CA,
Caltech - ICSB - 07
Integrating system for segmenting and tracking fluorescent objects on the image data of growing cell colonies.Tigran Bacarian1,*, Eric Mjolsness1 1. Institute for Genomics and Bioinformatics, UC Irvine, Irvine, USA *email: tbacaria@uci.eduThe probl
Caltech - ICSB - 07
Application of genome-scale stoichiometric model of Vibrio vulnificus CMCP6 for in silico drug targetingHyun Uk Kim1, Tae Yong Kim1, Kwangjoon Jeong3, Soo Young Kim3, Joon Haeng Rhee3, Sang Yup Lee 1,2* 1. Department of Chemical and Biomolecular Eng
Caltech - ICSB - 07
Gene regulation of metabolic pathways: a continuous model for Escherichia coli carbon sources uptakeP. Moreno 1, , A. Maass 2 , B. Andrews 3 , J. Asenjo 31. Bioinformatics and Mathematics of Genome Laboratory, Centre for Mathematical Modeling, U.Ch
Caltech - ICSB - 07
Transcriptional program of the cell cycle: high-resolution timingMaga Rowicka1, Andrzej Kudlicki1, Benjamin P. Tu1, Zbyszek Otwinowski11University of Texas Southwestern Medical Center, Dallas, TX 75390.The eukaryotic cell division cycle is depe
Caltech - ICSB - 07
Proximate Parameter Tuning: a novel strategy for system identification1Stephen J. Wilkinson, 2Neil Benson & 1,*Douglas B. Kell 1 School of Chemistry and MCISB, Manchester Interdiscplinary Biocentre, University of Manchester, Manchester M1 7DN, UK.
Caltech - ICSB - 07
HGT and innovation of Genome Systems Complexity: Where do the selective pressures originate from?Torbjrn Karfunkel 1, , Devdatt Dubhashi 1 , Malte Hermansson 2 o 1. Department of Computing Science, Chalmers University of Technology, Gothenburg, Swed
Caltech - ICSB - 07
Surface phase separation and morphological transition of a multicomponent vesicleShuwang Li and J.S. Lowengrub,Introduction Vesicle membranes usually have bilayer structures composed by lipid molecules with hydrophilic heads and hydrophobic tails
Caltech - ICSB - 07
Constructal View of Formation of Dissimilar Patterns inside Similar Living SystemsAntonio F. Miguel 1,2,* 1. Department of Physics, University of Evora, Evora, Portugal 2. Geophysics Centre of Evora, Evora, Portugal *email: afm@uevora.pt Abstract Th
Caltech - PH - 127
Physics 127b: Statistical Mechanics Renormalization Group: General CaseThe steps in the renormalization group are 1. Eliminate degrees of freedom by a scale factor b so that N = N , bd (1)whilst preserving the free energy. This might be done by "b
Caltech - PH - 127
Physics 127b: Statistical Mechanics Lecture 2: Dense Gas and the Liquid StateMayer Cluster ExpansionThis is a method to calculate the higher order terms in the virial expansion. It introduces some general features of perturbation theory in many bod
Caltech - PH - 127
Physics 127b: Statistical Mechanics Brownian MotionBrownian motion is the motion of a particle due to the buffeting by the molecules in a gas or liquid. The particle must be small enough that the effects of the discrete nature of matter are apparent
Caltech - PH - 127
Physics 127c: Statistical Mechanics Bose Condensation in Trapped Alkali GasesFigure 1: Observation of Bose-Einstein condensation of Rubidium atoms by Anderson et al. Science 269, 198 (1995). The plots show the momentum distribution (measured by tur
Caltech - PH - 127
Physics 127a: Class NotesLecture 15: Statistical Mechanics of SuperuidityElementary excitations/quasiparticles In general, it is hard to list the energy eigenstates, needed to calculate the statistical mechanics of an interacting system. Indeed for
Caltech - G - 010132
Investigating Higher Order Statistics and GaussianitySteve Penn, Syracuse UniversityLIGO-G010132-00-ZSynopsisGIntroduction to Higher Order Statistics 1D: Correlation, Coherence, Power Spectra 2D: Bicorrelation, Bicoherence, Bispectrum 3D
Caltech - M - 030260
LIGO-M030260-00-MLSC Six-Month Progress ReportOrganization Carleton College Relativity Group (CCRG) Report Date August 15, 2003 LIGO I / Attachment A We have been extremely busy with LIGO related research. Carleton College is an active member of t
Caltech - M - 040034
LIGO-M040034-00-MLSC Six-Month Progress ReportOrganization Carleton College Relativity Group (CCRG) Report Date February 15, 2004 Attachment A / LIGO I We have been extremely busy with LIGO related research. Carleton College is an active member of
Caltech - G - 070084
Studies of Thermal Loading in Pre-Modecleaners for Advanced LIGOAmber Bullington Stanford University LSC/Virgo March 2007 Meeting Optics Working GroupG070084-00-ZOutlineThermal Loading Experiment Ring cavity known as pre-modecleaner (PMC) Sam
Caltech - G - 070145
Recent Parametric Instability ModelingBill Kells Caltech LIGOG070145-00-Z13/21/2007PI R calculation from entire cavity fieldPrevious: model arm cavity field as discreet SHOsEach acoustic {m}Stokes a-StokesBraginsky, VyatchaninCavity sp
Caltech - G - 060331
Thermal noise and high order Laguerre-Gauss modesJ-Y. Vinet, B. Mours, E. TournefierGWADW meeting, Isola d'Elba May 27th Jun 2nd , 20061LIGO-G060331-00-ZIntroduction Mirror thermal noise will limit the interferometers sensitivities around
Caltech - ECLIPSE - 02
Caltech - ECLIPSE - 02
Caltech - ECLIPSE - 02
Caltech - ECLIPSE - 02
Caltech - ECLIPSE - 02
Caltech - ECLIPSE - 02
Caltech - ECLIPSE - 02
Frames DSC_2736 through DSC_2776 were exposed in Messina, South Africa on Wednesday, Dec 4 2002 at the local times indicated. (GMT +2). The imaging system was a TeleVue 70mm 520mm f/7.4 refractor and a Nikon D-100 digital SLR. Exposure times are list
Caltech - MS - 250
Caltech - MS - 250
Caltech - MS - 250
Caltech - GE - 11
1Ge 11d Notes #3 for Mon 1/12/09 The Big Picture Earth exhibits large scale circulation of the mantle, which expresses itself as plate tectonics. This shows the fluid nature of the solid part of Earth. The circulation is expressed as plate tectonic
Caltech - GE - 11
Ge 11d Notes #5 for Fri 1/16/09 Example Calculation We found from Gauss' law that g= 2Gh. Consider a layer of thickness 3 km and density 3000kg/m3. Then g~ 4 x1 0-3 m/s2. Now there is a standard unit used in gravity, called the milligal (one thousand
Caltech - GE - 11
Ge 11d Notes #4 for Wed 1/14/09 Postglacial rebound implies a viscous mantle. The origin of this viscosity is crystal imperfections. But since the energy scale for these is electron volts (large compared to thermal energy) it follows that the viscosi
Caltech - GE - 11
Ge 11d 2009 Homework # 1 Made available, Friday, Jan 9 Due Friday, Jan 16, 5pm to TA Lingsen Meng . Guidelines: Some questions in Ge 11d are routine applications of numbers to equations in the book or in lectures (e.g., first question below) but ofte
Caltech - GE - 11
Ge 11d Notes #2 for Fri 1/09/09 But What does Hydrostatic Equilibrium have to do with the Real Earth? In addition to the bulk modulus K already introduced above, we have the shear modulus which is an elastic constant that describes the response of a
Minnesota - DOCS - 0
Minnesota - DOCS - 0
ENSEMBLE AVERAGED AND MIXTURE THEORY EQUATIONS FOR INCOMPRESSIBLE FLUID-PARTICLE SUSPENSIONSBy Daniel D. Joseph and Thomas S. Lundgren with an appendix by R. Jackson and D. A. SavilleIMA Preprint Series #515 April 1989ENSEMBLE AVERAGED AND MIXTU
Minnesota - DOCS - 0
Minnesota - DOCS - 0
Minnesota - DOCS - 0
Minnesota - DOCS - 0
Minnesota - DOCS - 0
Minnesota - DOCS - 0
Minnesota - DOCS - 0
Minnesota - DOCS - 0
Minnesota - DOCS - 0
Minnesota - DOCS - 0
Minnesota - DOCS - 0
Minnesota - DOCS - 0
Minnesota - DOCS - 0
Minnesota - ME - 3331
IrreversibilityIncrease of Entropy PrincipleHeat, Work and Energy. A First Course in Thermodynamics 2009, F. A. Kulacki Module 30 Slide 1 Irreversibility and the Increase of Entropy PrincipleOverview Irreversibility Increase of entropy princi
Minnesota - IE - 5080
Introduction Examples and Tricks Chvatal-Gomory ProcedureValid InequalitiesBharath RangarajanJan 29, 2009B. RangarajanValid Inequalities01/29/091 / 14From P to PIntroduction Examples and Tricks Chvatal-Gomory ProcedureFor X = {x
Minnesota - IE - 5531
Section 4.6 in textMinimize x1max6x 2- x1, 4x 2, -5x1 , 9 Constraints on x 1, x2. Minimize x1t Constraints on x 1, x2 max 6x2 -x 1, 4x 2,-5x 1 , 9t.t does not interfere with original constraints value for t is determined only by the min/max obje
Minnesota - BERRI - 016
University Technology Training CenterMoodle 1.8:GradesUNIVERSITY TECHNOLOGY TRAINING CENTERMoodle 1.8:Grades 2007 Regents of the University of Minnesota University Technology Training Center All Rights Reserved uttc.umn.eduThe University
Caltech - WIN - 03
What do the complex workings of a cell have in common with the relentless unrest of the New York Stock Exchange? Are these dynamic storehouses of information obeying similar laws in terms of the ebb and flow of information, and can they be modeled, a
Caltech - WIN - 03
Markets and Other Noisy Human ArtifactsCan Computation Bring Them Out of the Bronze Age? A Conversation with Yaser S. Abu-Mostafa, K. Mani Chandy, and John O. LedyardSocial systems such as financial markets, political processes, and organizations ag
Caltech - WIN - 03
progressreportsUnderstanding Material Deformation: Insights into the Inner Workings of Complex Materialsby Ersan stndagIn most engineering calculations, the mechanical performance of structures or components is esti
Caltech - WIN - 03
Soft Circuitry and Liquid Algorithms- A New Bioengineering Frontier Takes Form A Conversation with Niles Pierce, Paul Sternberg, Erik Winfree, and Barbara WoldBiology computes, that is, living structures store, process, and communicate information i
Caltech - WIN - 03
newfacultyInflux of Talent: Division Grows by NineSix new professors have joined the Division and Caltech over the past several months, bringing fresh insights and new research directions our way. Also new to the Division are thr
Caltech - WIN - 03
alumniprofilesIvett Leyva: An Experimentalist with International FlairAeronautics, PhD 99With this issue we are beginning our practice of offering two alumni profilesone of a neophyte (an alum who has recently graduated)
Caltech - WIN - 03
i n f o r m a t i o ns c i e n c ea n dt e c h n o l o g yCenter for the Mathematics of Information: Information Theory Revisited:Mathematicians and Friends Tackle the Whole Enchilada A Conversation with Emmanuel Candes, Michelle Effros, and