dupreez7

v_ACEclear

∅ = ACE

v_ADH

ACE + NADH = NAD

v_ADPclear

∅ = ADP

v_AK

{2.0}ADP = AMP + ATP

v_ALD

F16P = {2.0}TRIO

v_AMPclear

∅ = AMP

v_ATP

ATP = ADP

v_ATPclear

∅ = ATP

v_BPGclear

∅ = BPG

v_ENO

P2G = PEP

v_F16Pclear

∅ = F16P

v_F6Pclear

∅ = F6P

v_G3PA

G3P = ∅

v_G3PDH

NADH + TRIO = G3P + NAD

v_G3Pclear

∅ = G3P

v_G6Pclear

∅ = G6P

v_GAPDH

NAD + TRIO = BPG + NADH

v_GLCiclear

∅ = GLCi

v_GLK

ATP + GLCi = ADP + G6P

v_GLYCO

ATP + G6P = ADP

v_NADHclear

∅ = NADH

v_NADclear

∅ = NAD

v_P2Gclear

∅ = P2G

v_P3Gclear

∅ = P3G

v_PDC

PYR = ACE

v_PEPclear

∅ = PEP

v_PFK

ATP + F6P = ADP + F16P

v_PGI

G6P = F6P

v_PGK

ADP + BPG = ATP + P3G

v_PGM

P3G = P2G

v_PYK

ADP + PEP = ATP + PYR

v_PYRclear

∅ = PYR

v_SUC

{2.0}ACE + {3.0}NAD + {4.0}ATP = {3.0}NADH + {4.0}ADP

v_TRIOclear

∅ = TRIO

v_Treha

ATP + {2.0}G6P = ADP

Global parameters

Note that constraints are not enforced in simulations. It remains the responsibility of the user to verify that simulation results satisfy these constraints.


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From steady-state to synchronized yeast glycolytic oscillations II: model validation.

  • Franco B du Preez
  • David D van Niekerk
  • Jacky L Snoep
FEBS J. 2012; 279 (16): 2823-2836
Abstract
UNLABELLED: In an accompanying paper [du Preez et al., (2012) FEBS J279, 2810-2822], we adapt an existing kinetic model for steady-state yeast glycolysis to simulate limit-cycle oscillations. Here we validate the model by testing its capacity to simulate a wide range of experiments on dynamics of yeast glycolysis. In addition to its description of the oscillations of glycolytic intermediates in intact cells and the rapid synchronization observed when mixing out-of-phase oscillatory cell populations (see accompanying paper), the model was able to predict the Hopf bifurcation diagram with glucose as the bifurcation parameter (and one of the bifurcation points with cyanide as the bifurcation parameter), the glucose- and acetaldehyde-driven forced oscillations, glucose and acetaldehyde quenching, and cell-free extract oscillations (including complex oscillations and mixed-mode oscillations). Thus, the model was compliant, at least qualitatively, with the majority of available experimental data for glycolytic oscillations in yeast. To our knowledge, this is the first time that a model for yeast glycolysis has been tested against such a wide variety of independent data sets.
DATABASE: The mathematical models described here have been submitted to the JWS Online Cellular Systems Modelling Database and can be accessed at http://jjj.biochem.sun.ac.za/database/dupreez/index.html.

No additional notes are available for this model.