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Tue Sep 18 Intro 1: Computing, statistics, Perl, MathematicaTue Sep 25 Intro 2: Biology, comparative genomics, models & evidence, applications Tue Oct 02 DNA 1: Polymorphisms, populations, statistics, pharmacogenomics, databasesTue Oct 09 DNA 2: Dynamic programming, Blast, multi-alignment, HiddenMarkovModelsTue Oct 16 RNA 1: 3D-structure, microarrays, library sequencing & quantitation concepts Tue Oct 23 RNA 2: Clustering by gene or condition, DNA/RNA motifs.Tue Oct 30 Protein 1: 3D structural genomics, homology, dynamics, function & drug designTue Nov 06 Protein 2: Mass spectrometry, modifications, quantitation of interactionsTue Nov 13 Network 1: Metabolic kinetic & flux balance optimization methodsTue Nov 20 Network 2: Molecular computing, self-assembly, genetic algorithms, neural-netsTue Nov 27 Network 3: Cellular, developmental, social, ecological & commercial modelsTue Dec 04 Project presentationsTue Dec 11 Project PresentationsTue Jan 08 Project PresentationsTue Jan 15 Project Presentations,Bio 101: Genomics & Computational Biology,Protein2: Last weeks take home lessons,Separation of proteins & peptidesProtein localization & complexes Peptide identification (MS/MS)Database searching & sequencing.Protein quantitationAbsolute & relativeProtein modifications & crosslinkingProtein - metabolite quantitation,Net1: Todays story & goals,Macroscopic continuous concentration ratesCooperativity & Hill coefficientsBistability Mesoscopic discrete molecular numbersApproximate & exact stochasticChromosome Copy Number ControlFlux balance optimizationUniversal stoichiometric matrix Genomic sequence comparisons,Networks Why model?,Red blood cell metabolism Enzyme kinetics (Pro2)Cell division cycle Checkpoints (RNA2)Plasmid Copy No. Control Single molecules Phage l switch Stochastic bistabilityComparative metabolism Genomic connectionsCircadian rhythm Long time delaysE. coli chemotaxis Adaptive, spatial effectsalso, all have large genetic & kinetic datasets.,Types of interaction models,Quantum ElectrodynamicssubatomicQuantum mechanicselectron cloudsMolecular mechanicsspherical atoms (101Pro1)Master equationsstochastic single molecules (Net1),Phenomenological rates ODEConcentration & time (C,t)Flux Balance dCik/dt optima steady state (Net1)Thermodynamic modelsdCik/dt = 0 k reversible reactions Steady StateSdCik/dt = 0 (sum k reactions) Metabolic Control Analysisd(dCik/dt)/dCj (i = chem.species) Spatially inhomogenous models dCi/dx,Increasing scope, decreasing resolution,In vivo & (classical) in vitro,1) Most measurements in enzyme kinetics are based on initial rate measurements, where only the substrate is present enzymes in cells operate in the presence of their products Fell p.54 (Pub) 2) Enzymes 244:269-78. (Pub),Human Red Blood CellODE model,GLCe,GLCi,G6P,F6P,FDP,GA3P,DHAP,1,3 DPG,2,3 DPG,3PG,2PG,PEP,PYR,LACi,LACe,GL6P,GO6P,RU5P,R5P,X5P,GA3P,S7P,F6P,E4P,GA3P,F6P,NADP,NADPH,NADP,NADPH,ADP,ATP,ADP,ATP,ADP,ATP,NADH,NAD,ADP,ATP,NADH,NAD,K+,Na+,ADP,ATP,ADP,ATP,2 GSH,GSSG,NADPH,NADP,ADO,INO,AMP,IMP,ADOe,INOe,ADE,ADEe,HYPX,PRPP,PRPP,R1P,R5P,ATP,AMP,ATP,ADP,Cl-,pH,HCO3-,ODE modelJamshidi et al.2000 (Pub),Factors Constraining Metabolic Function,Physicochemical factorsMass, energy, and redox balance: Systemic stoichiometryosmotic pressure, electroneutrality, solvent capacity, molecular diffusion, thermodynamicsNon-adjustable constraintsSystem specific factors Capacity: Maximum fluxesRates: Enzyme kineticsGene RegulationAdjustable constraints,Dynamic mass balances on each metabolite,Time derivatives of metabolite concentrations are linear combination of the reaction rates. The reaction rates are non-linear functions of the metabolite concentrations (typically from in vitro kinetics). vj is the jth reaction rate, b is the transport rate vector,Sij is the “Stoichiometric matrix” = moles of metabolite i produced in reaction j,Vsyn,Vdeg,Vtrans,Vuse,RBC model integration,Reference Glyc- PPP ANM Na+/K+ Osmot. Trans- Hb-5 Gpx Shape olysis Pump port ligands Hb Ca Rapoport 74-6 + - - - - - - - - -Heinrich 77 + - - - - - - - - -Ataullakhanov81 + + - - - - - - - -Schauer 81 + - + - - - - - - -Brumen 84 + - - + + - - - - -Werner 85 + - - + + + - - - -Joshi 90 + + + + + + - - - -Yoshida 90 - - - - - - + - - -Lee 92 + + + + + + (+) - - -Gimsa 98 - - - - - - - - - +Destro-Bisol 99 - - - - - - - (-) - -Jamshidi 00 + + + + + + - - - -,Scopes & Assumptions,Mechanism of ATP utilization other than nucleotide metabolism and the Na+/K+ pump (75%) is not specifically definedCa2+ transport not includedGuanine nucleotide metabolism neglectedlittle information, minor importanceCl-, HCO3-, LAC, etc. are in “pseudo” equilibriumNo intracellular concentration gradientsRate constants represent a “typical cell”Surface area of the membrane is constantEnvironment is treated as a sink,Glycolysis Dynamic Mass Balances,Enzyme Kinetic Expressions,Phosphofructokinase,Kinetic Expressions,All rate expressions are similar to the previously shown rate expression for phosphofructokinase.Model has 44 rate expressions with 5 constants each 200 parametersWhat are the assumptions associated with using these expressions?,Kinetic parameter assumptions,in vitro values represent the in vivo parametersprotein concentration in vitro much lower than in vivoenzyme interactions (enzymes, cytoskeleton, membrane, )samples used to measure kinetics may contain unknown conc. of effectors (i.e. fructose 2,6-bisphosphate)enzyme catalyzed enzyme modificationsall possible concentrations of interacting molecules been considered (interpolating)e.g. glutamine synthase (unusually large # of known effectors)3 substrates, 3 products, 9 significant effectors415 (109) measurements: 4 different conc. of 15 molecules (Savageau, 1976)in vivo probably even more complex, but approximations are effective.have all interacting molecules been discovered?and so on ,Additional constraints:Physicochemical constrains,Osmotic Pressure Equilibrium (interior & exterior, m chem. species),Electroneutrality (z = charge, Concentration),RBC steady-state in vivo vs calculated,|obs-calc| = Y sd(obs),X= metabolites (ordered by Y),Phase plane diagrams: concentration of metabolite A vs B over a specific time course,1: conservation relationship. 2: a pair of concentrations in equilibrium 3: two dynamically independent metabolites 4: a closed loop trace,1 23 4,Red 0 hoursGreen 0.1Blue 1.0Yellow 10End 300,1 hours,300 hours,ATP load,Redox load,ATP & Redox loads,0 to 300hourdynamics34 metabolitescalculated,RedoxLoad,ODE model Jamshidi et al. 2000 (Pub),RBC Metabolic “Machinery”,Glucose,Glycolysis,Pyruvate Lactate,ATP,NucleotideMetabolism,PPP,NADH,2,3 DPG,TransmembranePumps,Maintenance& Repair,Oxidants,Hb Met Hb,Cell DivisionCycleG2 arrestto M arrest switch,Hill coefficients,ResponseR = 1 1+(K/S)H,H simple hyperbolic = 1H (R=HbO2, S=O2) sigmoidal = 2.8H (R=Mapk-P, S=Mos) = 3H (R=Mapk-P, S=Progesterone in vivo) = 42,ProgesteroneAA Mos Mos-P Mek Mek-P Mapk Mapk-P,k1 k2 k-1 k-2,“The biochemical basis of an all-or-none cell fate switch in Xenopus oocytes.”,Science 1998;280:895-8 Ferrell & Machleder, (Pub),positive,(a chain of enzyme modifiers close to saturation generate higher sensitivity to signals than one enzyme can),Net1: Todays story & goals,Macroscopic continuous concentration ratesCooperativity & Hill coefficientsBistability Mesoscopic discrete molecular numbersApproximate & exact stochasticChromosome Copy Number ControlFlux balance optimizationUniversal stoichiometric matrix Genomic sequence comparisons,Arkin A, Ross J, McAdams HH Genetics 1998 149(4):1633.,Stochastic kinetic analysis of developmental pathway bifurcation in phage lambda-infected E. coli cells.,Variation in level, time & whole cell effect,Efficient exact stochastic simulation of chemical systems with many species & many channels,the Next Reaction Method, an exact algorithm .time proportional to the logarithm of the number of reactions, not to the number of reactions itself. Gibson J. Physical Chemistry. (Pub),Gillespie J.Phys Chem 81:2340-61. 1977. Exact stochastic simulation of coupled chemical reactions,Utilizing Noise,Hasty, et al. PNAS 2000; 97:2075-2080, Noise-based switches and amplifiers for gene expression (Pub) “Bistability . arises naturally. Additive external noise allows construction of a protein switch. using short noise pulses. In the multiplicative case, . small deviations in the transcription rate can lead to large fluctuations in the production of protein”.Paulsson, et al. PNAS 2000; 97:7148-53. Stochastic focusing: fluctuation-enhanced sensitivity of intracellular regulation. (Pub) (exact master equations),Vc= sd/mean fluorescence intensities of 75 to 150 individual cells. Becskei & Serrano, Nature 405, 590-593 (2000). (Pub),Engineering stability in gene networks byautoregulation,Feedback simulation with linear stability analysis,F(R) = dR/dt = n kpP kIa - kdegR 1+ kpP + krRf(R* + h) = f(R*) + h f(R*) . (Taylor approximation)R* = steady-state level of repressor, i.e. when f(R) = 0P = RNA polymerase concentration, kp and kr = binding constants of polymerase & repressor, kI = promoter isomerization rate to initiate, a = ratio of mRNA and protein concentrations, kdeg = degradation rate of , n = gene copy number.,Net1: Todays story & goals,Macroscopic continuous concentration ratesCooperativity & Hill coefficientsBistability Mesoscopic discrete molecular numbersApproximate & exact stochasticChromosome Copy Number ControlFlux balance optimizationUniversal stoichiometric matrix Genomic sequence comparisons,Copy Number Control Models,Replication of ColE1 & R1 PlasmidsDetermine the factors that govern the plasmid copy numbercellular growth rateOne way to address this question is via the use of a kinetic analysis of the replication process, and relate copy number to overall cellular growth.Why? the copy number can be an important determinant of cloned protein production in recombinant microorganisms,RNA II,RNA I,RNAPolymerase,Rom protein,RNA II,RNA I,RNase H,DNAPolymerase,ColE1 CNC mechanism,Rnase H cleaved RNAII forms a primer for DNA replication,RNA I binding to RNA II prevents RNaseH from cleaving RNA II,Where do we start?Dynamic mass balanceWhat are the important parameters?Plasmid, RNA I, RNA II, Rom, mAll the constantsdegradation, initiation, inhibitionRNaseH rate is very fast instantaneousDNA polymerization is very rapidSimplify assume do not consider RNA II model RNA I inhibitionRNA I and RNA II transcription is independent (neglect convergent transcription)Rom protein effects constantConsider 2 species: RNA I and plasmidMany more assumptions.,Assumptions?,Dynamic Mass Balance: ColE1 RNAIconcentration in moles/liter,Rate of changeof RNA I,Synthesis ofRNA I,Degradationof RNA I,Dilution dueto cell growth,=,-,-,R = RNA Ik1 = rate of RNA I initiationN = plasmidkd = rate of degradationm = growth rate,Keasling, 141, 447-61.,Dynamic Mass Balance: ColE1 Plasmid,Rate of changeof N,PlasmidReplication,Dilution dueto cell growth,=,-,R = RNA Ik2 = rate of RNA II initiationN = plasmidKI = RNA I/RNA II binding constant(an inhibition constant)m = growth rate,Solve for N(t).,Mathematica ODE program,Formulae for steady state start at mu=1 shift to mu=.5and then solve for plasmid concentration N as a function of time.,Stochastic models for CNC,Paulsson 297:179-92. Molecular clocks reduce plasmid loss rates: the R1 case. (Pub) While copy number control for ColE1 efficiently corrects for fluctuations that have already occurred, R1 copy number control prevents their emergence in cells that by chance start their cycle with only one plasmid copy. Regular, clock-like, behaviour of single plasmid copies becomes hidden in experiments probing collective properties of a population of plasmid copies . The model is formulated using master equations, taking a stochastic approach to regulation”,From RBC & CNC to models for whole cell replication?,e.g. E. coli ?What are the difficulties?The number of parametersMeasuring the parametersAre parameters measured in vitro representative to the parameters in vivo,Factors Constraining Metabolic Function,Physicochemical factors: Mass, energy, and redox balance: Systemic stoichiometryosmotic pressure, electroneutrality, solvent capacity, molecular diffusion, thermodynamicsNon-adjustable constraintsSystem specific factors:Capacity: Maximum fluxesRates: Enzyme kineticsGene RegulationAdjustable constraints,Net1: Todays story & goals,Macroscopic continuous concentration ratesCooperativity & Hill coefficientsBistability Mesoscopic discrete molecular numbersApproximate & exact stochasticChromosome Copy Number ControlFlux balance optimizationUniversal stoichiometric matrix Genomic sequence comparisons,Dynamic mass balances on each metabolite,Time derivatives of metabolite concentrations are linear combination of the reaction rates. The reaction rates are non-linear functions of the metabolite concentrations (typically from in vitro kinetics). Where vj is the jth reaction rate, b is the transport rate vector,Sij is the “Stoichiometric matrix” = moles of metabolite i produced in reaction j,Vsyn,Vdeg,Vtrans,Vuse,Flux-Balance Analysis,Make simplifications based on the properties of the system.Time constants for metabolic reactions are very fast (sec - min) compared to cell growth and culture fermentations (hrs)There is not a net accumulation of metabolites in the cell over time.One may thus consider the steady-state approximation.,Removes the metabolite concentrations as a variable in the equation.Time is also not present in the equation.We are left with a simple matrix equation that contains:Stoichiometry: knownUptake rates, secretion rates, and requirements: knownMetabolic fluxes: Can be solved for!In the ODE cases before we already had fluxes (rate equations, but lacked C(t).,Flux-Balance Analysis,Additional Constraints,Fluxes = 0 (reversible = forward - reverse)The flux level through certain reactions is knownSpecific measurement typically for uptake rxnsmaximal values uptake limitations due to diffusion constraintsmaximal internal flux,Flux Balance Example,A,2C,B,RC,RB,RA,x1,x2,Flux Balances:A: RA x1 x2 = 0B: x1 RB = 0C: 2 x2 RC = 0Constraints:RA = 3RB = 1,Equations:A: x1+x2 = 3B: x1 = 1C: 2 x2 RC = 0,FBA Example,A,2C,B,4,1,3,1,2,FBA,Often, enough measurements of the metabolic fluxes cannot be made so that the remaining metabolic fluxes can be calculated.Now we have an underdetermined systemmore fluxes to determine than mass balance constraints on the systemwhat can we do?,Incomplete Set of Metabolic Constraints,Identify a specific point within the feasible set under any given conditionLinear programming - Determine the optimal utilization of the metabolic network, subject to the physicochemical constraints, to maximize the growth of the cell,FluxA,FluxB,FluxC,Assumption:The cell has found the optimal solution by adjusting the system specific constraints (enzyme kinetics and gene regulation) through evolution and natural selection.Find the optimal solution by linear programming,Under-Determined System,All real metabolic systems fall into this category, so far.Systems are moved into the other categories by measurement of fluxes and additional assumptions.Infinite feasible flux distributions, however, they fall into a solution space defined by the convex polyhedral cone.The actual flux distribution is determined by the cells regulatory mechanisms.It absence of kinetic information, we can estimate the metabolic flux distribution by postulating objective functions(Z) that underlie the cells behavior.Within this framework, one can address questions related to the capabilities of metabolic networks to perform functions while constrained by stoichiometry, limited thermodynamic information (reversibility), and physicochemical constraints (ie. uptake rates),FBA - Linear Program,For growth, define a growth flux where a linear combination of monomer (M) fluxes reflects the known ratios (d) of the monomers in the final cell polymers.A linear programming problem is formulated where one finds a solution to the above equations, while minimizing an objective function (Z). Typically Z= ngrowth (or production of a key compound).Constraints to the LP problem: i reactions,Very simple LP solution,A,B,RA,x1,x2,RB,D,C,Flu

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