| Literature DB >> 23230424 |
Rainis Venta1, Ervin Valk, Mardo Kõivomägi, Mart Loog.
Abstract
The G1/S transition is a crucial decision point in the cell cycle. At G1/S, there is an abrupt switch from a state of high cyclin-dependent kinases (CDK) inhibitor (CKI) levels and low S-phase CDK activity to a state of high S-phase CDK activity and degraded CKI. In budding yeast, this transition is triggered by phosphorylation of the Cdk1 inhibitor Sic1 at multiple sites by G1-phase CDK (Cln1,2-Cdk1) and S-phase CDK (Clb5,6-Cdk1) complexes. Using mathematical modeling we demonstrate that the mechanistic basis for the abruptness of the G1/S transition is the highly specific phosphorylation of Sic1 by S-phase CDK complex. This switch is generated by a double-negative feedback loop in which S-CDK1 phosphorylates Sic1, thus targeting it for destruction, and thereby liberating further S-CDK1 from the inhibitory Sic1-S-CDK1 complex. Our model predicts that the abruptness of the switch depends upon a strong binding affinity within the Sic1-S-CDK inhibitory complex. In vitro phosphorylation analysis using purified yeast proteins revealed that free Clb5-Cdk1 can create positive feedback by phosphorylating Sic1 that is bound in the inhibitory complex, and that Sic1 inhibits Clb5-Cdk1 with a sub-nanomolar inhibition constant. Our model also predicts that if the G1-phase CDK complex is too efficient at targeting Sic1 for destruction, then G1/S becomes a smooth and readily reversible transition. We propose that the optimal role for the G1-phase CDK in the switch would not be to act as a kinase activity directly responsible for abrupt degradation of CKI, but rather to act as a priming signal that initiates a positive feedback loop driven by emerging free S-phase CDK.Entities:
Keywords: CDK; CKI; Cdk1; G1/S; Sic1; cell cycle; cyclin-dependent kinases; switch
Year: 2012 PMID: 23230424 PMCID: PMC3515773 DOI: 10.3389/fphys.2012.00459
Source DB: PubMed Journal: Front Physiol ISSN: 1664-042X Impact factor: 4.566
Figure 1Inhibition of Clb5-Cdk1 and Cln2-Cdk1 by Sic1. (A) Autoradiograph of a Clb5-Cdk1 and Cln2-Cdk1 inhibition assay. Sic1 is extensively phosphorylated by Cln2-Cdk1 whereas no detectable phosphorylation is seen with Clb5-Cdk1. (B) Inhibition curves for Clb5-Cdk1 and Cln2-Cdk1 are presented as the initial rates of histone H1 phosphorylation in the presence of different concentrations of Sic1. (C) Calculated IC50 values from the experiment in panel (A). (D) The values of IC50 change in parallel with Clb5-Cdk1concentrations when both Sic1 and the kinase are varied in the picomolar or low nanomolar ranges.
Figure 2Sic1 is efficiently phosphorylated within the Sic1/Clb5-Cdk1 complex, when an excess of Clb5-Cdk1 is added. Assays with Cln2-Cdk1 complexes are included for comparison. (A) Autoradiography showing the phosphorylation of purified Sic1wt and Sic1ΔC by Clb5-Cdk1 and Cln2-Cdk1 complexes using 15 nM Sic1 and 30 nM cyclin-Cdk1 complexes. (B) The activity of Clb5-Cdk1 was determined using 2.5 μM histone H1, with and without 15 nM Sic1wt in the assay mixture. (C,D) Quantification of the experiment presented in panel (A). For comparison, phosphorylation rates were normalized using cyclin-Cdk1 activity units obtained in panel (B).
Figure 3Minimal model of the G1/S switch. Parameters used for diagrams and simulations presented in the figures below are listed in Tables 1 and 2. Black crosses designate the phospho-dependent degradation of Sic1 via the SCF-proteasome pathway. Gray crosses designate basal degradation of Sic1.
Equations describing the minimal model of the G1/S switch.
| Conservation equations: |
| Kinetic constants (the values presented below are those used in Figure |
The description of the system is presented in Figure 3. For the phase diagrams presented in Figures 5–7, the steady-state solutions for the dependencies between Sic1TOTAL and Clb5-Cdk1TOTAL and Clb5-Clb5-Cdk1FREE and Clb5-Cdk1TOTAL were derived.
Equation system used for numerical simulation of the time courses at G1/S in Figures .
| The kinetic constants (values presented below are those used in Figure |
The initial values for y1 (Sic1FREE) and y5 (Sic1TOTAL) in two simulations were 1 μM.
Figure 5(A–D) The steady state phase diagrams showing the effect of the inhibition strength on the bistability of the G1/S switch. The dissociation rates of the inhibitory complex were increased in 10-fold increments from 0.01 to 10 min−1 as indicated. In the model, these values correspond to K values of 0.1–100 nM. Arrows indicate the paths of the system at the G1/S transition.
Figure 7Phase diagrams showing the potential effect of Cln2-dependent priming phosphorylation on the bistability of the system. The rate constant value of 0.001 nM×min−1 for Clb5-Cdk1 exemplifies a system with no Cln2-dependent priming while increasing values of this constant mimic increased levels of Cln2-dependent priming effect. (A) Phase diagrams showing the dependence of free Clb5-Cdk1 activity on total Clb5-Cdk1 levels. (B) Phase diagrams showing the dependence of total Sic1 concentration on total Clb5-Cdk1. The color coding is the same for both panels.
Figure 4Phase diagrams showing the bistability of the system at steady state. Parameter values are provided in Table 1. The dark gray arrows show possible paths for a gradual increase of free Clb5-Cdk1 while entering the S-phase, and possible reversible paths (light gray arrows) in the event of stochastic decreases in Clb5 levels. (A) Phase diagram showing the dependence of free Clb5-Cdk1 activity on total Clb5-Cdk1 levels. When a threshold is reached, the system switches itself into the state corresponding to S-phase, as indicated by the upward pointing arrow. (B) Phase diagram for the same system with the same parameter values as in panel (A), showing the dependence of total Sic1 concentration on total Clb5-Cdk1. The threshold level for a drop of Sic1 corresponds to the same threshold level of total Clb5-Cdk1 that triggers the jump in steady state levels of free Clb5-Cdk1 in panel (A).
Figure 6(A–C) Phase diagrams showing the effect of changes in the relative ability of Cln2-Cdk1 to directly cause the degradation of Sic1. The rate constant values for Cln2-Cdk1 were gradually increased as indicated.
Figure 8Time course simulations to analyze the abruptness of the transition. The equation system and parameter values are provided in Table 2. (A) The simulation with the basic set of key parameters for inhibition and phosphorylation, similar to those used in the phase diagrams in Figure 4. (B) The effect of faster Cln2-dependent phosphorylation rate on the switch. The rate constant value for Cln2-Cdk1 was taken to be equal to the “k” value of Clb5-dependent phosphorylation. (C) The effect of weaker inhibition strength on the switch. The dissociation rate of the inhibitory complex was raised to 10 min−1, which in the model corresponds to a K value of 100 nM.
Figure 9Time course simulations showing the potential effect of Cln2-dependent priming phosphorylation on the abruptness of the switch. The equation system and parameter values are provided in Table 2. (A) A system with no priming effect in the absence of Cln2. The basal rate constant value of 0.001 nM−1 × min−1 for Clb5-Cdk1 was used. (B–D) Different priming effects were mimicked by using the following “k” values for Clb5-Cdk1: 0.01 nM−1 × min−1 (B), 0.03 nM−1 × min−1 (C), and 0.1 nM−1 × min−1 (D).
Figure 10Time course simulations for systems where only Cln2 is responsible for phosphorylation and degradation of Sic1. (A) A model similar to that in Figures 8 and 9 was used, except that the rate constant value for Clb5-Cdk1 toward Sic1 was taken to be zero. The rate constant for Cln2-Cdk1 was 0.001 nM−1 × min−1, which is the same value used for Clb5-Cdk1 in Figure 8A. (B) A system that requires Cln2-dependent multisite phosphorylation for degradation of Sic1. The sequential phosphorylation of six sites in Sic1 was taken to be the output signal for degradation of Sic1.
Equation system used for simulation of the time course for Cln2-dependent multisite phosphorylation of Sic1presented in Figure .
| kon = 0.1;—the association rate of the inhibitory complex. To lower the complexity, the dissociation rate was considered very slow and not included in this version of the model. |
| The initial value for 0P-Sic1 ( |