a kinetic model of the cyclin e ycdk2 developmental timer ... · xenopus embryo undergoes the...

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Biophysical Chemistry 104 (2003) 573–589 0301-4622/03/$ - see front matter 2003 Elsevier Science B.V. All rights reserved. doi:10.1016/S0301-4622Ž03.00060-7 A kinetic model of the cyclin E y Cdk2 developmental timer in Xenopus laevis embryos Andrea Ciliberto, Matthew J. Petrus, John J. Tyson, Jill C. Sible* Biology Department, Virginia Polytechnic Institute and State University, Blacksburg, VA 24061-0406, USA Received 20 December 2002; received in revised form 10 March 2003; accepted 10 March 2003 Abstract Early cell cycles of Xenopus laevis embryos are characterized by rapid oscillations in the activity of two cyclin- dependent kinases. Cdk1 activity peaks at mitosis, driven by periodic degradation of cyclins A and B. In contrast, Cdk2 activity oscillates twice per cell cycle, despite a constant level of its partner, cyclin E. Cyclin E degrades at a fixed time after fertilization, normally corresponding to the midblastula transition. Based on published data and new experiments, we constructed a mathematical model in which: (1) oscillations in Cdk2 activity depend upon changes in phosphorylation, (2) Cdk2 participates in a negative feedback loop with the inhibitory kinase Wee1; (3) cyclin E is cooperatively removed from the oscillatory system; and (4) removed cyclin E is degraded by a pathway activated by cyclin EyCdk2 itself. The model’s predictions about embryos injected with Xic1, a stoichiometric inhibitor of cyclin EyCdk2, were experimentally validated. 2003 Elsevier Science B.V. All rights reserved. Keywords: Cyclin E; Cyclin-dependent kinase 2 (Cdk2); Wee1; Xic1; Midblastula transition; Mathematical model 1. Introduction The chromosome replication–division cycle of cell-free extracts derived from Xenopus laevis eggs has been well characterized by rigorous experi- mentation w1–12x and mathematical modeling w13–16x. In the egg extract system, the chromo- some cycle is driven by oscillations in the activity Abbreviations: Cdk, cyclin-dependent kinase; MPF, M- phase promoting factor; MBT, midblastula transition; ODE, ordinary differential equation; pf, post-fertilization. *Corresponding author. Tel.: q1-540-231-1842; fax: q1- 540-231-9307. E-mail addresses: [email protected] (J.C. Sible), [email protected] (A. Ciliberto), [email protected] (M.J. Petrus), [email protected] (J.J. Tyson). of M-phase promoting factor (MPF), a dimer of a catalytic subunit, Cdk1, and a regulatory subunit, cyclin A1 or B w3x. Oscillations in MPF activity depend upon a negative feedback loop in which active MPF promotes degradation of mitotic cyclins w12,17x. MPF activity is also modulated by inhibitory phosphorylation on threonine 14 and tyrosine 15. These sites are phosphorylated by Wee1 and Myt1 w5,6x, and dephosphorylated by Cdc25 w7,8x. The autocatalytic nature of MPF activation w18–20x depends upon positive feedback loops, whereby MPF activates Cdc25 w11,21x and inhibits Wee1 w5x. Cell cycle controls in intact, developing Xenopus embryos present additional experimental and theo-

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Page 1: A kinetic model of the cyclin E yCdk2 developmental timer ... · Xenopus embryo undergoes the midblastula tran-sition (MBT ), when cells become motile, embry-onic transcription begins

Biophysical Chemistry 104(2003) 573–589

0301-4622/03/$ - see front matter� 2003 Elsevier Science B.V. All rights reserved.doi:10.1016/S0301-4622Ž03.00060-7

A kinetic model of the cyclin EyCdk2 developmental timer inXenopus laevis embryos

Andrea Ciliberto, Matthew J. Petrus, John J. Tyson, Jill C. Sible*

Biology Department, Virginia Polytechnic Institute and State University, Blacksburg, VA 24061-0406, USA

Received 20 December 2002; received in revised form 10 March 2003; accepted 10 March 2003

Abstract

Early cell cycles ofXenopus laevis embryos are characterized by rapid oscillations in the activity of two cyclin-dependent kinases. Cdk1 activity peaks at mitosis, driven by periodic degradation of cyclins A and B. In contrast,Cdk2 activity oscillates twice per cell cycle, despite a constant level of its partner, cyclin E. Cyclin E degrades at afixed time after fertilization, normally corresponding to the midblastula transition. Based on published data and newexperiments, we constructed a mathematical model in which:(1) oscillations in Cdk2 activity depend upon changesin phosphorylation,(2) Cdk2 participates in a negative feedback loop with the inhibitory kinase Wee1;(3) cyclin Eis cooperatively removed from the oscillatory system; and(4) removed cyclin E is degraded by a pathway activatedby cyclin EyCdk2 itself. The model’s predictions about embryos injected with Xic1, a stoichiometric inhibitor ofcyclin EyCdk2, were experimentally validated.� 2003 Elsevier Science B.V. All rights reserved.

Keywords: Cyclin E; Cyclin-dependent kinase 2(Cdk2); Wee1; Xic1; Midblastula transition; Mathematical model

1. Introduction

The chromosome replication–division cycle ofcell-free extracts derived fromXenopus laevis eggshas been well characterized by rigorous experi-mentation w1–12x and mathematical modelingw13–16x. In the egg extract system, the chromo-some cycle is driven by oscillations in the activity

Abbreviations: Cdk, cyclin-dependent kinase; MPF, M-phase promoting factor; MBT, midblastula transition; ODE,ordinary differential equation; pf, post-fertilization.*Corresponding author. Tel.:q1-540-231-1842; fax:q1-

540-231-9307.E-mail addresses: [email protected](J.C. Sible),

[email protected](A. Ciliberto),[email protected](M.J. Petrus), [email protected](J.J. Tyson).

of M-phase promoting factor(MPF), a dimer of acatalytic subunit, Cdk1, and a regulatory subunit,cyclin A1 or B w3x. Oscillations in MPF activitydepend upon a negative feedback loop in whichactive MPF promotes degradation of mitoticcyclins w12,17x. MPF activity is also modulated byinhibitory phosphorylation on threonine 14 andtyrosine 15. These sites are phosphorylated byWee1 and Myt1w5,6x, and dephosphorylated byCdc25 w7,8x. The autocatalytic nature of MPFactivationw18–20x depends upon positive feedbackloops, whereby MPF activates Cdc25w11,21x andinhibits Wee1w5x.Cell cycle controls in intact, developingXenopus

embryos present additional experimental and theo-

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574 A. Ciliberto et al. / Biophysical Chemistry 104 (2003) 573–589

retical challenges. After fertilization, the egg andsperm nuclei undergo DNA replication, nuclearfusion and the first mitotic division. The next 11embryonic cell cycles are rapid, synchronous oscil-lations between DNA replication and mitosis, lack-ing intervening gap phases, cell growth and cellcycle checkpoints. After the 12th division, theXenopus embryo undergoes the midblastula tran-sition (MBT), when cells become motile, embry-onic transcription begins and the cell cycleacquires the gap phases and checkpoints of atypical somatic cellw22,23x.The mechanisms of ‘cell cycle remodeling’w24x

are not fully understood, but recent evidence sug-gests that remodeling depends in part on a maternaldevelopmental timer driven by oscillations in theactivity of cyclin EyCdk2 w25x. During cleavagecycles 2–12 in the frog, the cyclin E level isconstant, while cyclin E-associated kinase activity(cyclin EyCdk2) oscillates twice per cell cyclew25,26x. Cyclin EyCdk2 activity promotes DNAreplicationw27,28x and is essential for centrosomeduplication w29,30x. At the MBT, maternally sup-plied cyclin E is degradedw25,26,31,32x and Cdk2activity declinesw25x, coincident with remodelingof the cell cycle. Maternal cyclin E mRNA dis-appears some hours laterw32x.Injection of embryos withD34Xic1 (a recom-

binant, truncated form of the cyclin-dependentkinase(Cdk) inhibitor, Xic1) specifically inhibitscyclin EyCdk2, causes a 25% increase in interdi-vision time, and delays both the MBT(zygotictranscription) and the degradation of cyclin E untilapproximately the correct nucleocytoplasmic ratiow25x. Although this observation suggests thatcyclin E degradation is causally related to theMBT, the two events can be dissociated. Cyclo-heximide treatment(which inhibits protein synthe-sis) blocks cell division and the MBT, but doesnot prevent cyclin E degradation. Nor doesa-amanitin treatment(which blocks zygotic tran-scription at the MBT) prevent cyclin E degradationw25x. Furthermore, oscillations in cyclin EyCdk2also occur independently of protein synthesis, thenucleocytoplasmic ratio and embryonic transcrip-tion w25x.

We have built a mathematical model of thecyclin EyCdk2 developmental timer that describesboth the oscillations in Cdk2 activity and theabrupt destruction of cyclin E coincident with theMBT. The model was constructed along the samelines as the Novak–Tyson model of MPF oscilla-tions in frog egg extractsw13x, taking into accountthe similarities and differences between cyclin ByCdk1 regulation and cyclin EyCdk2 regulation.For both Cdk1 and Cdk2, there are no abundantCdk inhibitors expressed during this timew33x;hence, oscillations are due to either periodic syn-thesis and degradation of cyclin partners, or peri-odic phosphorylation and dephosphorylation ofkinase subunits(or both). Pre-MBT oscillations ofCdk1 activity are driven by periodic cyclin deg-radation w34x, but pre-MBT oscillations of Cdk2activity are notw25x. Although early reports indi-cated no periodic tyrosine phosphorylation ofeither Cdk1 or Cdk2 until the MBTw26,35x,subsequent studies with a sensitive antibody havedetected periodic tyrosine phosphorylation of aCdk in pre-MBTXenopus embryosw36x. Further-more, Cdk2 activity is regulated in cell-free eggextracts by such phosphorylation eventsw37x.Therefore, if oscillations in Cdk2 activity aregenerated by a negative feedback loop(as forCdk1), the inhibitory phosphorylation state ofCdk2 (rather than cyclin level) is the likely posi-tion of the negative feedback.A second important distinction between the

regulation of Cdk1 and Cdk2 activity is the rapiddestruction of cyclin E at the MBT. Because theonly manipulation known to delay the degradationof cyclin E is to inhibit Cdk2 activity directlyw25x, we propose that degradation of cyclin E isintrinsically dependent on Cdk2 activity.Based on the experimental literature, we devel-

oped a mathematical model to describe the oscil-lations in cyclin EyCdk2 activity and the abruptdegradation of cyclin E at the MBT in the intactXenopus embryo. New experiments were per-formed to help construct the model. The modelshould provide a framework around which todesign future experiments that will specify thedetails of a revised, second-generation model.

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2. Experimental methods

2.1. Maintenance and manipulation of embryos

Eggs from wild-typeXenopus laevis (XenopusExpress) were fertilized in vitro, dejellied in 2%cysteine in 0.1= MMR (0.5 mM HEPES, pH 7.8,10 mM NaCl, 0.2 mM KCl, 0.1 mM MgSO , 0.24

mM CaCl , 0.01 mM EDTA) and maintained in2

0.1= MMR. Embryos were collected at stagesspanning the MBT and staged according toNieuwkoop and Faberw38x. In some experiments,fertilized eggs were injected with indicatedamounts of glutathioneS-transferase(GST)-taggedXic1-C or GST-taggedD34Xic1 protein dissolvedin Xic1 buffer (20 mM HEPES, pH 7.5, 88 mMNaCl, 20 mMb-mercaptoethanol, 7.5 mM MgCl ,2

5% glycerol) at a concentration of 0.08–0.33 mgyml. As described by Su et al.w39x, Xic1-C containsamino acids 97–210 andD34Xic1 contains aminoacids 25–210 of the Xic1 protein. The Xic1proteins were gifts of James Maller(HowardHughes Medical Institute, University of ColoradoHealth Sciences Center). Microinjected embryoswere maintained in 5% Ficoll in 0.1= MMR, andsnap-frozen at the time points indicated. Someembryos were also injected with 50 ng ofa-amanitin dissolved in H O. In some experiments,2

fertilized eggs were injected with buffer or 15 ngof mRNA encoding luciferase or XChk1(tran-scribed in vitro using the mMessage mMachine kitfrom Ambion), as described elsewherew40x.

2.2. Immunoblotting

Embryos were collected at the times indicated,snap-frozen on dry ice and homogenized in EBbuffer (20–30 mM HEPES, pH 7.5, 15 mMMgCl , 20 mM EGTA, 1 mM dithiothreitol, 1 mM2

sodium vanadate, 1 mMmicrocystin, 1mM phenyl-methylsulfonyl fluoride, and 3mgyml each leupep-tin, pepstatin and chymostatin, with or without 80mM b-glycerophosphate and 50 mM sodium flu-oride). Embryo lysates were resolved by sodiumdodecyl sulfate-polyacrylamide gel electrophoresis(SDS-PAGE), transferred to nitrocellulose mem-branes, and hybridized with antibodies, as previ-

ously describedw40,41x. The cyclin E antibodywas purified from serum provided by RebeccaHartley (University of New Mexico Health Sci-ences Center). Xic1 antibodies were generouslyprovided by James Maller(Howard Hughes Med-ical Institute, University of Colorado Health Sci-ences Center). To visualize immunoreactiveproteins, a horseradish peroxidase-conjugated sec-ondary antibody was hybridized, and chemilumi-nescence from the secondary antibody wasdetected with the ECL Plus(Amersham) kit.

2.3. Immunoprecipitation and kinase assays ofcyclinyCdk complexes

Embryos injected at the one-cell stage with 5ng of Xic-C orD34Xic1 were collected at the timeindicated, and antibodies against cyclin B or cyclinE were used to immunoprecipitate cyclin ByCdk1or cyclin EyCdk2 complexes, respectively, asdescribed by Kappas et al.w40x. Cyclin antibodieswere provided by James Maller(Howard HughesInstitute, University of Colorado Health SciencesCenter).

3. Mathematical modeling and computationalsimulation

Mathematical models of hypothetical molecularmechanisms for regulation of cyclin EyCdk2 activ-ity were constructed by translating a mechanisminto a set of ordinary differential equations(ODEs)by standard principles of biochemical kineticsw42x.The ODEs were then provided as input toXPP-AUT, a simulation and analysis softwaresystem, freely downloadable from http:yywww.math.pitt.eduy;bardyxppyxpp.html. XPP

runs on theUNIX operating system. Parametervalues were chosen by trial and error, to fit thebasic phenomenological properties of the controlsystem(rapid fluctuations in cyclin EyCdk2 activ-ity followed by abrupt degradation of cyclin E).

4. Results

4.1. Key assumptions

Based on the experimental evidence summarizedin Section 1, a set of assumptions upon which the

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Fig. 1. Expression of XChk1 delays the degradation of cyclinE in Xenopus embryos. Embryos were injected with buffer or15 ng of mRNA encoding XChk1. Embryos were collected atthe time points indicated and analyzed for cyclin E proteincontent. The migration of molecular weight standards in kDais indicated. In other experiments, control embryos were inject-ed with mRNA encoding luciferase, and the delay in cyclin Edegradation was shown to be a specific effect of XChk1(datanot shown).

Table 1Key assumptions of the cyclin EyCdk2 kinetic model

1 Constant level of cyclin E w25,26,31,32x2 No abundant CKI inhibitor w33,50x3 Regulation of Cdk2 activity by phosphorylation w37,40x4 Negative feedback loop in Cdk2 oscillations To be tested5 Timing of cyclin E degradation linked to Cdk2 activity w25x, Fig. 16 No return of Cdk2 activity in Xic-injected embryos Fig. 27 Degradation of cyclin E independent of transcription w25x, Fig. 3

mathematical model would be based was devel-oped (Table 1). Some assumptions are wellgrounded in the experimental literature(assump-tions 1–3), others remain to be tested(assumption4) and several(assumptions 5–7) were tested byus experimentally, as described below.

4.1.1. Reagents that inhibit Cdk2 delay the deg-radation of cyclin EA fundamental assumption of our working mod-

el is that degradation of cyclin E at the MBTresults from a cooperative transition in cyclin EyCdk2 forms. This assumption is based upon pub-lished studies demonstrating that cyclin E isdegraded at a fixed time post-fertilization, inde-pendent of protein synthesis(hence, independentof Cdk1 activity, which requires continued synthe-sis of mitotic cyclins A and B), cell number, thenucleocytoplasmic ratio and zygotic transcriptionw25,32x. Furthermore, the only manipulationknown to alter the timing of cyclin E degradationis microinjection ofD34Xic1, a recombinant pro-tein that specifically inhibits Cdk2 but not Cdk1activity w25x. BecauseD34Xic1 delays the degra-dation of cyclin E, it seemed likely that the timingmechanism for cyclin E degradation depends uponcyclin EyCdk2 activity itself.If this assumption were correct, then other rea-

gents that interfere with cyclin EyCdk2 activityshould also block or delay the degradation ofcyclin E. Expression of exogenous XChk1 inXenopus embryos inhibits both Cdk1 and Cdk2activity w40x; therefore, expression of XChk1should also block or delay the degradation ofcyclin E. To test this prediction, embryos wereinjected with 15 ng of mRNA encoding FLAG-tagged XChk1. Negative control embryos were

injected with buffer or 15 ng of mRNA encodingFLAG-tagged luciferase. Embryos were collectedat the times indicated and analyzed for cyclin Econtent by immunoblotting(Fig. 1). Analogous toembryos injected withD34Xic1, cyclin E degra-dation was delayed in embryos overexpressingXChk1 compared to both buffer(Fig. 1) andluciferase controls(not shown), supporting thehypothesis that timing of cyclin E degradationdepends directly on Cdk2 activity.

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Fig. 2. Cyclin E degradation inD34Xic1-treated embryos doesnot depend upon transient cyclin EyCdk2 activity. Embryosmicroinjected with 5 ng of Xic1-C orD34Xic1 were collectedat the times indicated, cyclin EyCdk2 was immunoprecipitatedand immunoprecipitates were analyzed for histone H1 kinaseactivity. cpm, counts per minute P incorporated into histone32

H1. Values plotted represent raw cpmybackground cpm on gel(1209 cpm). Cyclin ByCdk1 immunoprecipitates indicated noinhibition of Cdk1 byD34Xic1 (not shown).

Fig. 3. Zygotic transcription is not required for degradation of cyclin E. Embryos were injected at the one-cell stage with H O, 502

ng of a-amanitin, 5 ng ofD34Xic1, or 50 ng ofa-amanitin and 5 ng ofD34Xic1. Embryos were collected at the indicated timespf and analyzed by immunoblotting for steady-state level of cyclin E protein. The migration of molecular weight standards in kDais indicated.

4.1.2. Cyclin E degradation in Xic1-treated embry-os does not depend upon transient cyclin EyCdk2activityWhen embryos are microinjected with 5 ng of

D34Xic1, cyclin EyCdk2 activity is inhibited bymore than 90% without inhibition of Cdk1 activityw25x. Intuitively, we would predict that cyclin Edegradation would be blocked indefinitely(or untilembryos died by necrosis) in D34Xic1-injectedembryos. However, the degradation of cyclin Edoes occur, only several hours delayed, when

embryos have reached the nucleocytoplasmic ratioof the MBT w25x. This observation challenges thehypothesis that cyclin E degradation is directlylinked to cyclin EyCdk2 activity.One possible explanation for the eventual deg-

radation of cyclin E inD34Xic1-injected embryosis that cyclin EyCdk2 activity resumes transiently,prior to the degradation of cyclin E, at approxi-mately 9 h post-fertilization(pf). This scenarioplayed a central role in a preliminary mathematicalmodel that simulated the delay in degradation ofcyclin E in D34Xic1-injected embryos. However,kinase assays performed on embryos injected withD34Xic1 detected no transient peak of Cdk2 activ-ity (Fig. 2), even when samples were collected at30-min intervals(not shown), ruling out this par-ticular model.

4.1.3. Cyclin E degradation in Xic1-treated embry-os does not depend upon zygotic transcriptionIt could be that degradation of cyclin E in

embryos injected withD34Xic1 is initiated byzygotic transcription at the MBT, since transcrip-tion initiates coincident with cyclin E degradationin D34Xic1-injected embryosw25x. To determinewhether a product of zygotic transcription turnedon degradation of maternal cyclin E, independentof cyclin EyCdk2 activity, embryos were injectedwith H O, a-amanitin (an inhibitor of transcrip-2

tion), D34Xic1, or a combination ofa-amanitinand D34Xic1 (Fig. 3). In embryos injected withH O or a-amanitin, cyclin E disappeared between2

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Fig. 4. A theoretical molecular mechanism of the cyclinEyCdk2 developmental timer was used to construct the math-ematical model. The hatched box represents a mechanism forremoving cyclin EyCdk2 from the oscillatory subsystem. ‘Deg’represents the cyclin E degradation system, which we assumeis activated by the ‘removed’ form of cyclin EyCdk2. Noticethat the removal step is cooperative, i.e. the more cyclinEyCdk2 is bound to the hatched box, the faster is the associ-ation reaction. A kinase(‘Kin’ ) is introduced between cyclinEyCdk2 and Wee1 to create a time lag in the negative feedbackloop.

5 and 7 h pf, consistent with previous reports thatdegradation of maternal cyclin E at the MBT doesnot depend on transcriptionw25,32x. As predictedw25x, degradation of cyclin E was delayed inembryos injected withD34Xic1 and was completeby 10 h pf. In embryos injected with botha-amanitin andD34Xic1, cyclin E was degraded atthe same time as in embryos injected withD34Xic1 alone, ruling out the possibility of redun-dant degradation mechanisms, one dependent upontranscription and the other upon cyclin EyCdk2activity. These results indicate that transcription atthe MBT is not required for the eventual degra-dation of cyclin E in embryos lacking cyclin EyCdk2 activity.

4.2. Kinetic model of the cyclin EyCdk2 develop-mental timer

Based on the information summarized in Section1 and the new data presented in Figs. 1–3, aworking model of the cyclin EyCdk2 controlsystem was developed(Fig. 4). The model iscomposed of three modules: a negative feedbackoscillator, a positive feedback switch and an irre-versibly activated pathway for cyclin Edegradation.

4.2.1. Negative feedback oscillatorA maternal store of cyclin E combines with free

Cdk2 monomers to form active cyclin EyCdk2dimers. In the model, we assume cyclin EyCdk2dimers can be transformed between an inactive,phosphorylated form(PCdk2:CycE) and an active,non-phosphorylated form(Cdk2:CycE) by theaction of a kinase, Wee1, and a phosphatase,Cdc25A. This assumption is based on evidencethat Cdk2 is regulated by tyrosine phosphorylationw37,40x. For simplicity, we assume that Cdc25A ispresent at constant activity in the early embryo,and that Wee1 is periodically activated by cyclinEyCdk2, indirectly through the action of a hypo-thetical kinase, Kin.(Cdc25C was not included inthe model because dominant-negative Cdc25Cdoes not affect cell cycle length in embryosw36x.)In the model, Kin phosphorylates and inactivatesWee1, and cyclin EyCdk2 phosphorylates andinactivates Kin. These interactions create a delayednegative feedback loop, consisting of three inacti-

vating phosphorylation steps in sequence(Cdk2—±Kin—±Wee1—±Cdk2). (A delayed feedback inwhich Kin activates Cdc25A would be an alter-native possibility.) The parameters in the modelare adjusted to create limit cycle oscillations witha period of approximately 15 min(two peaks permitotic cycle). Because a two-component negativefeedback loop (Cdk2—±Wee1—±Cdk2) cannotoscillate w43x, we are compelled to introduce thehypothetical kinase(as the simplest case of someprocess that provides a delay between the actionsof Cdk2 and Wee1).

4.2.2. Positive feedback switchTo model the abrupt degradation of cyclin E at

approximately 7 h pf, it is proposed that cyclin Ey

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Cdk2 is removed from the oscillatory subsystemin a cooperative fashion through a positive feed-back loop. Subsequently, the removed form ofcyclin E is degraded, probably by the SCFyproteasome pathway. ‘Removed’ cyclin EyCdk2could correspond to a change in phosphorylationstate, localization or some other property of cyclinE. Qualitatively, it is predicted that, during the first7 h of embryonic development, most cyclin E willcycle between active(unphosphorylated) and inac-tive (Cdk2-phosphorylated) forms. During theseoscillations, an increasing fraction of cyclin EyCdk2 dimers is removed from the oscillatingforms, eventually stimulating rapid, cooperative(autocatalytic) removal of cyclin EyCdk2, whichquenches the oscillation.

4.2.3. Cyclin E degradationAfter a further delay, the cyclin E degradation

machinery (‘Deg’) activates, and the wholeremoved pool of cyclin E is degraded. We sup-pose that Deg is activated by the unphosphorylatedform of removed cyclin EyCdk2 dimers(Cdk2:CycE ) and that only removed cyclin Erem

is targeted by Deg. Furthermore, the concentrationof Cdk2:CycE must exceed a certain thresholdrem

wTable 2,u in Eq. (7)x before it can activate Deg.As cyclin E is destroyed, we presume that Degremains active.

4.2.4. Effect of D34Xic1We assume that(1) Xic1 binds strongly to all

forms of cyclin EyCdk2 and blocks any catalyticactivity they may have; nonetheless,(2) Xic1binding does not interfere with removal of cyclinEyCdk2. Furthermore, we assume that Xic1 boundto removed forms of cyclin EyCdk2 is slowlydegraded, possibly in association with chromatinw44–46x. As Xic1 is degraded,wCdk2:CycE xrem

increases and subsequently activates cyclin E deg-radation. Under these assumptions, Xic1 injectionsare expected to quench oscillations of cyclin EyCdk2 activity and to delay(but not eliminate)cyclin E degradation.

4.2.5. Further assumptionsThe removed forms of cyclin EyCdk2 are not

subject to phosphorylation and dephosphorylationby Wee1 and Cdc25 and do not phosphorylate

Kin. These assumptions make the model slightlyeasier to understand, but they are not necessary.Models in which these assumptions are not madebehave very similarly to the model simulated here(not shown).

4.2.6. The modelA mathematical model(the differential equa-

tions in Table 2) can be derived from the molecularwiring diagram(Fig. 4) using standard rate lawsof biochemical kinetics. Basal parameter valuesare proposed in Table 3. These values were chosento reproduce the basic quantitative characteristicsof the cyclin EyCdk2 timer in normal frog embry-os. We assume that, atts0 (fertilization, or shortlythereafter), the cyclin EyCdk2 oscillator is in fullswing and no cyclin E is removed from theoscillatory system.

4.3. Numerical simulations and experimental val-idation: testing the model

4.3.1. The model reproduces the fundamental fea-tures of the cyclin EyCdk2 timerFig. 5 presents a numerical solution of the

kinetic equations(Table 2) using the basal param-eter values proposed for unperturbed embryos(Table 3). The model reproduces the fundamentalobservations driving this study:(1) cyclin E is astable protein at first and then rapidly degraded atthe MBT w25,32x; and(2) cyclin EyCdk2 activityoscillates twice per cell cycle before the MBTw25x(Fig. 5a). We did not attempt to model cycle 1,which is longer than cycles 2–12 and involvescyclin E degradationw26x.An appreciation of the regulatory mechanisms

behind the oscillations in kinase activity and theabrupt degradation of cyclin E unfolds from graph-ing the concentrations of the four forms of cyclinEyCdk2 over time(Fig. 5b). Oscillations in cyclinEyCdk2 activity prior to the MBT derive from theperiodic phosphorylation and dephosphorylation ofCdk2, as a consequence of the negative feedbackloop with Wee1. As removed dimers accumulate,Deg is activated and removed cyclin E is degraded.Because no steps in the model(Fig. 4) involve

protein synthesis, the model is consistent with thefact that oscillations in cyclin EyCdk2 activityw25x and disappearance of cyclin E at a fixed time

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580 A. Ciliberto et al. / Biophysical Chemistry 104 (2003) 573–589

Table 2Differential equations describing the model in Fig. 3

1wCdk2:CycExsyk wWee1*xwCdk2:CycExqk wPCdk2:CycExyk fwCdk2:CycEx

dwee 25A ondt

qk wCdk2:CycE xyk wXicxwCdk2:CycExqk wXic:Cdk2:CycExremoff assoc dissoc

2wPCdk2:CycExsqk wWee1*xwCdk2:CycExyk wPCdk2:CycExyk fwPCdk2:CycEx

dwee 25A ondt

qk wPCdk2:CycE xyk wXicxwPCdk2:CycExqk wXic:PCdk2:CycExremoff assoc dissoc

3

w x w xk Wee1 yWee1* w xw xk Kin* Wee1*wact totalŽ . winactdw xWee1*sq y

w x w x w xdt J qWee1 yWee1* J qWee1*wact total winact

4wKin* x s q

k 1ywKin* xŽ .iactd k wCdk2:CycExwKin* xiinactydt J q1ywKin* x J qwKin* xiact iinact

5wCdk2:CycE xsqk fwCdk2:CycExyk wCdk2:CycE xyk wDegxwCdk2:CycE x

d rem rem remon off edegdt

qk wXic:Cdk2:CycE xyk wXicxwCdk2:CycE xqk wXic:Cdk2:CycE xrem rem remxdeg assoc dissoc

6wPCdk2:CycE xsqk fwPCdk2:CycExyk wPCdk2:CycE x

d rem remon offdt

yk wDegxwPCdk2:CycE xqk wXic:PCdk2:CycE xrem remedeg xdeg

yk wXicxwPCdk2:CycE xqk wXic:PCdk2:CycE xrem remassoc dissoc

7wDeg*xsk Heav(wCdk2:CycE xyu)

d remdactdt

8wXicxsyk wXicx(wCdk2:CycExqwPCdk2:CycExqwCdk2:CycE xqwPCdk2:CycE x)

d rem remassocdt

qk (wXic:Cdk2:CycExqwXic:PCdk2:CycExqwXic:Cdk2:CycE xqwXic:PCdk2:CycE x)rem remdissoc

9wXic:Cdk2:CycExsqk wXicxwCdk2:CycExyk wXic:Cdk2:CycEx

dassoc dissocdt

yk fwXic:Cdk2:CycExqk wXic:Cdk2:CycE xremon off

yk wWee1*xwXic:Cdk2:CycExqk wXic:PCdk2:CycExwee 25A

10wXic:PCdk2:CycExsqk wXicxwPCdk2:CycExyk wXic:PCdk2:CycEx

dassoc dissocdt

yk fwXic:PCdk2:CycExqk wXic:PCdk2:CycE xremon off

qk wWee1*xwXic:Cdk2:CycExyk wXic:PCdk2:CycExwee 25A

11wXic:Cdk2:CycE xsqk wXicxwCdk2:CycE xyk wXic:Cdk2:CycE x

d rem rem remassoc dissocdt

qk fwXic:Cdk2:CycExyk wXic:Cdk2:CycE xremon off

yk wDegxwXic:Cdk2:CycE xyk wXic:Cdk2:CycE xrem remedeg xdeg

12wXic:PCdk2:CycE xsqk wXicxwPCdk2:CycE xyk wXic:PCdk2:CycE x

d rem rem remassoc dissocdt

qk fwXic:PCdk2:CycExyk wXic:PCdk2:CycE xremon off

yk wDegxwXic:PCdk2:CycE xyk wXic:PCdk2:CycE xrem remedeg xdeg

13wXic xsqk wDegxwXic:Cdk2:CycE xqk wDegxwXic:PCdk2:CycE xyk wXic x

d rem rem rem remedeg edeg xdegdt

All concentration variables are expressed in arbitrary units, i.e. they are dimensionless numbers. Hence, all rate constants(kvalues) have units time . In the text, 1 AU of Xic and CycE concentration is estimated to be approximately 33 nM.y1 fs

, . wPoolxswCdk2:CycE xqwPCdk2:CycE xqwXic:Cdk2:CycE xqnw x´qPool

rem rem remµ ∂Heav xs 0, if x-0; 1, if xG0Ž .n nw xL qPoolwXic:PCdk2:CycE x. f is a Hill function describing the cooperativity of Cdk2:CycE removal. It depends onwPoolx, the ‘total pool’rem

of removed cyclin E. Heav(x) is the Heaviside function, a common mathematical expression for a switch.u is the threshold Cdk2activity for turning on the switch. The activation kinetics of Wee1 and Kin are assumed to be zero-order ultrasensitive switchesw51x.

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581A. Ciliberto et al. / Biophysical Chemistry 104 (2003) 573–589

Table 3Basal parameter values for the differential equations in Table 1

Rate constants(min )y1

k s1.5, k s0.1, k s0.02,k s0.0001,k s0.1, k s0.001,k s0.75,k s1.5,wee 25A on off assoc dissoc wact winact

k s0.15,k s0.6, k s0.017,k s0.01,k s0.023iact iinact edeg xdeg dact

Other constants(dimensionless)J s0.01,J s0.01,J s0.01,J s0.01,us0.3, ´s0.001,Ls0.4, ns4, wWee1 xs8wact winact iact iinact total

Initial concentrations(arbitrary units)wCdk2:CycExs0.06,wPCdk2:CycExs0.94,wWee1*xs1.02,wKin* xs0.60, wDeg*xs0,wall ‘removed’ formsxs0, wall Xic-bound formsxs0, wXicxsadjustable

Fig. 5. The mathematical model is consistent with the dynamics observed for cyclin EyCdk2 in normal frog embryos.(a) Numericalsimulation of the equations in Table 2, given the parameter values in Table 3. The control system exhibits rapid oscillations in Cdk2activity (period approx. 15 min) followed by abrupt degradation of cyclin E at approximately 6 h pf. (b) The four forms of cyclinEyCdk2.

post-fertilizationw25,32x occur, even when embry-os are treated with cycloheximide to block proteinsynthesis, a critical constraint from the experimen-tal literaturew25x.

4.3.2. Exogenous D34Xic1 is degraded prior tothe disappearance of cyclin EA major challenge in developing the model was

the experimental result that embryos microinjectedwith D34Xic1 eventually degrade cyclin E, with adelay of only several hoursw25x. If cyclin Edegradation were intrinsically linked to cyclin EyCdk2 activity as we assume, and ifD34Xic1inhibits cyclin EyCdk2 activity by more than 90%w25x, then cyclin E levels might persist indefinitelyin D34Xic1-injected embryos. That this is not the

case suggests that Xic1 is eventually lost from thetreated embryos. In the model, we assume thatXic1 bound to the removed forms of cyclin EyCdk2 is subject to steady degradation. Simulationsshow that this reasonable assumption is sufficientto account for Xic1 and cyclin E fates in treatedembryos(Fig. 6). To simulate the effect of inject-ing D34Xic1, the initial concentration of Xic1 inthe model was set to 3.{ In simulations of unper-turbed embryos(Fig. 5), wtotal Xic1xs0, basedon the data ofw33,50x.} Simulations indicate thatmost cyclin EyCdk2 associates with Xic1, and thiscomplex gradually shifts to the pool of removedforms, peaking approximately 7 h pf(Fig. 6a).Once in the removed pool, Xic1 is degraded there,consistent with experiments in egg extracts

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582 A. Ciliberto et al. / Biophysical Chemistry 104 (2003) 573–589

Fig. 6. ExogenousD34Xic1 is degraded prior to the destruction of cyclin E.(a,b,c) Simulation. wXic1x s3. In panel(c),initial

wXic1 xywXic1x is plotted.(d) Experiments. Embryos were injected with 5 ng of Xic1-C orD34Xic1, collected at the indicatedtotal initial

time points and analyzed by immunoblotting for content of cyclin E and Xic1. The migration of molecular weight standards isindicated on the left.Note: Xic1-C reacts weakly with the Xic1 antibody, but is detected and is degraded at the same time asD34Xic1.

w44,45x. As long as free Xic1 is present in the cell,cyclin EyCdk2 complexes that lose their Xic1partner will quickly pick up another. Between 5and 9 h, a steady drop in concentration of freeXic1 is observed, with only a modest rise inremoved cyclin EyCdk2 (Fig. 6b). Once the sup-ply of Xic1 is exhausted, the unphosphorylatedform of removed cyclinEyCdk2 can turn on Deg(Fig. 6b) and cyclin E is degraded(Fig. 6c). Weassume that removed cyclin EyCdk2 is not immu-

noprecipitated and detected in H1 kinase assaysbecause we do not detect a transient peak in cyclinEyCdk2 activity between the degradation ofmicroinjected D34Xic1 and the degradation ofcyclin E (Fig. 2 and data not shown). Alternatively,the peak in removed cyclin EyCdk2 may be tootransient or too low in amplitude to be detected inour kinase assays.Plotting levels ofD34Xic1 and cyclin E over

time (Fig. 6c) indicates that(1) cyclin E is

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Fig. 7. Timing of cyclin E degradation is dependent upon the dose ofD34Xic1. (a) Simulation. Total cyclin E for different amountsof Xic1 added to the system. As in Fig. 6, Xic1 is degraded prior to cyclin E. The times when one-half of the original Xic1 hasbeen degraded are 6.4, 7.6 and 10 h forwXic1x s1.5, 3 and 6, respectively The times when one-half of the original cyclin Einitial

has been degraded are 7, 7.7, 10.3 and 15.4 h forwXic1x s0, 1.5, 3 and 6, respectively.(b) Experiment. Embryos were injectedinitial

with 0, 2.5, 5 or 10 ng ofD34Xic1, collected at the time points indicated, and analyzed by immunoblotting for content of cyclinE. Arrows denote the position of cyclin E.

degraded abruptly at approximately 10 h pf, con-sistent with observationsw25x, and(2) D34Xic1 isdegraded a few hours before cyclin E.Since the content ofD34Xic1 over time had not

been monitored in previous studies ofD34Xic1-injected embryos, the theoretical prediction thatD34Xic1 would be degraded prior to the degrada-tion of cyclin E was tested experimentally. Embry-os were injected with 5 ng of Xic1-C orD34Xic1at the one-cell stage, collected at multiple timepoints and analyzed for content of cyclin E andXic1 (Fig. 6d). The level of D34Xic1 droppedsharply between 6 and 8 h pf, prior to the degra-dation of cyclin E between 8 and 10 h pf, confirm-ing this prediction of the model.

4.3.3. Cyclin E degradation is progressivelydelayed by increasing amounts of D34Xic1As a final test of the model, the dose ofD34Xic1

was altered in simulations to determine the effecton cyclin E degradation. Simulations(Fig. 7a)suggested that the timing of cyclin E degradationshould be inversely correlated to the quantity ofD34Xic1 injected over at least a four-fold range.

To test this prediction experimentally, embryoswere injected with 0, 2.5, 5 or 10 ng ofD34Xic1.The total injection volume was kept constant.Embryos were analyzed for the degradation ofcyclin E at multiple time points(Fig. 7b). Inembryos lackingD34Xic1, most cyclin E degra-dation occurred between 5 and 7 h pf. In embryosinjected with 2.5 or 5 ng ofD34Xic1, cyclin Edegradation occurred 7–8 and 9–10 h pf, respec-tively. Little degradation of cyclin E was detectedin embryos injected with 10 ng ofD34Xic1, evenas late as 11 h pf. The simulations and experimen-tal data correlate well, further supporting the theo-retical basis of the model.These observations allow us to estimate the

‘arbitrary units’ of Xic1 concentration in the mod-el. wTotal Xic1xs1 AU corresponds to 1.67 ng ofD34Xic1 per embryo(1.5 AU simulates activityof 2.5 ng of D34Xic1; 3 AU simulates 5 ng ofD34Xic1, etc.), which is a concentration of approx-imately 33 nM (assuming one embryo is equiva-lent to 1.0ml and the molecular weight ofD34Xic1is 50 000 gymol). Since Xic1 and cyclin EyCdk2bind in 1:1 stoichiometry, this means thatwtotal

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cyclin Exs1 AU also corresponds to approximate-ly 33 nM.

5. Discussion

By combining computational and experimentalapproaches, we have built a model of the cyclinEyCdk2 developmental timer in earlyXenopusembryos. Development of the model was con-strained by experimental evidence obtained fromintactXenopus embryos:(1) oscillations in cyclinEyCdk2 occur twice per cell cycle prior to theMBT w25x; (2) the level of cyclin E remainsconstant during this timew25,32x; and (3) cyclinE is degraded at a fixed time post-fertilization,independent of cell number, protein synthesis,nucleocytoplasmic ratio and zygotic transcriptionw25,32x. The model faithfully reproduces 22 oscil-lations in cyclin EyCdk2 activity and degradationof cyclin E at approximately 6–7 h pf, independentof protein synthesis. Experimental evidence thatthe degradation of cyclin E is delayed in embryosmicroinjected with 5 ng ofD34Xic1 w25x alsoagrees with the simulations.The model is composed of three ‘modules’: an

oscillatory module, based on a delayed negativefeedback loop; a switching module, based oncooperative removal of cyclin EyCdk2; and aproteolysis module, based on irreversible activationof the cyclin E degradation pathway.

5.1. Oscillatory module

In the oscillatory module, oscillations in cyclinEyCdk2 activity do not depend on cyclin E syn-thesis or degradation, because total cyclin E levelis quite constant throughout the early stages offrog embryogenesisw25x. Nor are these oscillationsattributable to periodic fluctuations in a stoichio-metric inhibitor, Xic1, because Xic1 is not nor-mally present in the early embryow33x. That leavesreversible inhibitory phosphorylation of Cdk2 asthe prime suspect for generating oscillations incyclin EyCdk2 activity. To the best of our knowl-edge, oscillations in the phosphorylation state ofCdk2 have not been measured in intact embryosand may be difficult to observe because the oscil-lations are rapid and may be localized within

nuclei. On the other hand, Cdk2 activity is regu-lated by reversible phosphorylation in extractsw37x, and embryos microinjected with XChk1,which promotes tyrosine phosphorylation of Cdks,have reduced cyclin EyCdk2 activityw40x. If cyclinEyCdk2 oscillations derive from reversible phos-phorylation alone, then the components must beinvolved in a negative feedback loop, with cyclinEyCdk2 either promoting Wee1 activity or inhib-iting Cdc25. This supposition is in sharp contrastto the case of cyclin ByCdk1, which inhibits Wee1and activates Cdc25. In that case, oscillationsdepend on Cdk1 turning on cyclin B degradationby activating FizzyyAPC w12x. Therefore, Cdk2oscillations are fundamentally different from Cdk1oscillations.At this point, the oscillatory module in Fig. 4 is

purely hypothetical and awaits experimental vali-dation. It should also be kept in mind that anegative feedback loop, whereby cyclin EyCdk2indirectly inhibits Cdc25, might be an alternativebasis for oscillations in Cdk2 activity.

5.2. Switching module

The second major assumption in the model isthat the timing of cyclin E degradation dependsupon cyclin EyCdk2 activity, in particular uponremoved cyclin EyCdk2. In support of thisassumption, degradation of cyclin E is delayedwhen Cdk2 activity is inhibited by eitherD34Xic1w25x or XChk1 (Fig. 1). However, inD34Xic1-injected embryos, cyclin E is eventually degraded.The model incorporates the idea that cyclin EyCdk2 promotes chromatin association and subse-quent degradation of Xic1, as suggested by theexperiments of Furstenthal et al.w45x. In simula-tions of D34Xic1-injected embryos, cyclin E isdegraded some hours after degradation ofD34Xic1(Fig. 6c). This prediction was validated experi-mentally(Fig. 6d).Initially, we assumed that ‘removed’ cyclin E

was chromatin-bound cyclin E, and that associationof cyclin E with chromatin was cooperative. Thisassumption was based on data indicating thatcyclin EyCdk2 associates with chromatinw47x andis responsible for loading Xic1 onto chromatin,where Xic1 is then degradedw44,45x. However,

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585A. Ciliberto et al. / Biophysical Chemistry 104 (2003) 573–589

Table 4Differential equations used for bifurcation analysis in Fig. 8

1wCdk2:CycExsyk wWee1*xwCdk2:CycExqk (E yH–wCdk2:CycEx)

dwee 25A totdt

3

w x w xk Wee1 yWee1* w xw xk Kin* Wee1*wact totalŽ . winactdw xWee1*s y

w x w x w xdt J qWee1 yWee1* J qWee1*wact total winact

4

w x w xw xk 1yKin* k Cdk2:CycE Kin*iact iinactŽ .dw xKin* s y

w x w xdt J q1yKin* J qKin*iact iinact

5

nd ´qHHsqk = E yH yk HŽ .on tot offn ndt L qH

In the simplified model, cyclin E degradation and Xic1 binding are ignored. These equations are carried over from Table 2, withthe understanding thatHswremoved forms of Cdk2:CycEx andE swall forms of Cdk2:CycEx.tot

binding of cyclin EyCdk2 to chromatin dependsupon DNA replication cyclesw47x, inconsistentwith observations that degradation of cyclin Eoccurs at a fixed time, even in cycloheximide-treated embryos(in which DNA replication isblocked indirectly) w25,41x. Therefore, we aban-doned the specific model of chromatin binding.Alternatively, ‘removed’ cyclin EyCdk2 could

be a posttranslationally modified form. Whencyclin E is autophosphorylated by cyclin EyCdk2,it binds an F-box protein and becomes ubiquitin-ated and degraded by the SCF(reviewed inw48x).If autophosphorylated cyclin EyCdk2 were rapidlydegraded, then the removal step would not becooperative. Therefore, a sufficient time delay isneeded between autophosphorylation and degra-dation of cyclin E. Since cyclin E needs to bephosphorylated at a second site prior to degrada-tion w49x, the time delay could exist if autophos-phorylated cyclin EyCdk2 were to phosphorylateand activate another kinase(e.g. Deg). One dis-crepancy with our model is that Xic should inhibitthe removal of cyclin E in this case, since ‘remov-al’ depends upon cyclin EyCdk2 catalytic activity.A key assumption of the model is that removal isnot inhibited by Xic. Clearly, the details of theremoval step are speculative and need to be deter-mined by future experimentation. Therefore, theremoval mechanism remains deliberately generalin the model.

5.3. Degradation module

We have not attempted to model the molecularmachinery of cyclin E degradation, because it does

not feedback, as far as we know, on the dynamicsof the oscillatory and switching modules. To keepthis part of the model as simple as possible, weuse a ‘Heaviside function’ to switch on cyclin Edegradation in an irreversible fashion, after asufficient amount of Cdk2:CycE has accu-rem

mulated.

5.4. Bifurcation analysis of the mathematicalmodel

To understand better the fundamental behaviorof the cyclin EyCdk2 developmental timer, bifur-cation analysis was applied to a simplified versionof the model.(A primer on bifurcation analysis isavailable inw15x.) Because our aim was to uncoverthe dynamics of the oscillatory and switchingmodules, we have eliminated Xic1 binding andcyclin E degradation from the network(see Table4). A numerical simulation of these equations ispresented in Fig. 8a. Removed cyclin EyCdk2(dashed line) increases abruptly at approximately6 h pf, indicative of cooperativity, as postulatedby the model. Oscillations in active free cyclin EyCdk2 (solid line) are created by the negativefeedback loop involving Wee1 and quenched bythe cooperative removal of cyclin EyCdk2.In Fig. 8b, we consider the behavior of the

negative feedback loop as a function of the fractionof removed cyclin E. That is, we fixwCdk2:CycE xqwPCdk2:CycE xsHsconstant, andrem rem

study the behavior of the negative feedback loopas a function of the value ofH. For 0-H-0.45,the steady-state solution of the negative feedback

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586 A. Ciliberto et al. / Biophysical Chemistry 104 (2003) 573–589

Fig. 8. Bifurcation analysis of the cyclin EyCdk2 developmental timer.(a) Simulation of the equations in Table 4. Removed cyclinEyCdk2 (dashed line; HswCdk2:CycE xqwP Cdk2:CycE x) and active, unremoved cyclin EyCdk2 (solid line) as functions ofrem rem

time. (b) Dependence of negative feedback oscillations onH. The ordinate iswCdk2:CycEx, except for the open diamonds, whichindicate the period of oscillation(scale on right). Solid line, stable steady state; dashed line, unstable steady state; black circles,maximum and minimum values ofwCdk2:CycEx during the course of an oscillation at fixedH. The control system undergoes aHopf bifurcation atHs0.45. (c) Bistability in the positive feedback module. We plot dHydt as a function ofH for two values ofk . The system is monostable(one steady state, where dHydts0) for k s0.0001(solid line) and bistable(three steady states)off off

for k s0.01 (dashed line). (d) Oscillations in the negative feedback module,Hs0. Symbols as in panel(b). The steady state isoff

unstable between the two points of Hopf bifurcation atts4=10 and 12(see text).y4

loop (dashed line) is unstable, and the networkexecutes sustained oscillations(the black circlesindicate the maximum and minimum values ofactive cyclin EyCdk2 over the course of an oscil-

lation) with period close to 14 min(open dia-monds). For 0.45-H-1, the negative feedbackloop has a stable steady state(solid line) and nosustained oscillations. AtHs0.45, the negative

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feedback loop is said to undergo a Hopf bifurca-tion. Now, comparing Fig. 8a,b, we observe thatasH increases from 0 to 0.45(during the first 5h pf), the negative feedback loop oscillates with aperiod of approximately 14 min. However, as soonasH exceeds the Hopf-bifurcation point, the oscil-lations are quickly lost.To see whyH increases as in Fig. 8a, we plotted

the rate of change ofH (dHydt) as a function ofH in Fig. 8c. When dHydt is positive,H increases;when dHydt is negative,H decreases. Steady statesexist wherever dHydts0. For the parameter setused here(solid line), a single stable steady stateexists atH close to 1. Hence, starting withHs0(no removed cyclin EyCdk2), H must increaseuntil it reaches the steady state, where most cyclinEyCdk2 is removed. Note, however, that the rateof increase ofH is, at first, very small(dHydtf0.0008) and then accelerates rapidly by nearly10-fold. This acceleration is a reflection of thecooperative removal of cyclin EyCdk2 in themodel.Cooperative removal is a form of positive feed-

back(autocatalysis) that can easily create bistablebehavior. If the dissociation rate constant,k , isoff

increased from 0.0001 to 0.01, then dHydt as afunction of H is modified (dashed line) so thatthere now exist two stable steady states: one withHf0.1 (little removed cyclin E), and another withHf0.7 (most cyclin E removed). At the lowersteady state, the negative feedback loop will be inits oscillatory regime, and at the upper steady state,the negative feedback loop will be quiescent. Thisbehavior of the control system is entirely differentfrom what is observed. We have chosen our param-eter set(Table 3) to bring the control system closeto but not within its region of bistability. With thischoice, H increases slowly at first, pulling theoscillatory module past its Hopf bifurcation, andthenH increases rapidly, as most of the cyclin Eis removed from the oscillatory system.Finally, we have mentioned several times that

oscillations in the negative feedback loop requirean intermediate, Kin, between cyclin EyCdk2 andWee1. Kin introduces a time delay between acti-vation of cyclin EyCdk2 and subsequent increasein Wee1 activity. This time delay depends on thecharacteristic time,t, required for cyclin EyCdk2

to inactivate Kin(ts1yk ). The basal value ofiinact

t is 1.67 (see Table 3). As t decreases, the timedelay in the negative feedback loop becomesnegligible, and oscillations disappear at a Hopfbifurcation, atts4=10 in Fig. 8d. (To keepy4

the relative activity of Kin fixed, we steadilyincrease bothk and k , keeping their ratioiact iinact

constant atk yk s0.25.) The amplitude ofiact iinact

oscillation becomes quite small, even fort-0.05.In other words, oscillations in the negative feed-back loop require an intermediate that introducesa minimal time lag between cyclin EyCdk2 andWee1. Fig. 8d shows that oscillations are also lostif t becomes too large(t)12).

5.5. Future developments

The model presented here will be refined asnew experimental data become available. Mostimportantly, experiments are needed to identifywhether Kin exists and functions in a negativefeedback loop between cyclin EyCdk2 and Wee1.Alternatively, does negative feedback existbetween cyclin EyCdk2 and Cdc25? In addition,the specific nature of ‘removed’ cyclin E needs tobe determined.

Acknowledgments

We are grateful to Dr Rebecca Hartley(Univer-sity of New Mexico Health Sciences Center) forthe cyclin E antibody, and to Dr James Maller(Howard Hughes Medical Institute, University ofNew Mexico Health Sciences Center) for the Xic1protein and cyclin antibodies. The experiment inFig. 1 was performed by JCS while in Dr Maller’slab. We appreciate Dr Monica Murakami’s(National Cancer Institute; NIH) help with prelim-inary Wee1 studies. This work has been supportedby the National Institutes of Health(Grant Num-bers R01-GM59688 to JCS, R01-GM64339 toJJT), the Defense Advanced Research ProjectsAgency—Biocomputation Program (AFRL�F30602-02-0572), the National Science Foun-dation—Biocomplexity Program(MCB-0083315),and the Research Division of Virginia Tech.

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