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The simple circadian oscillator found in cyanobacteria can be reconstituted in vitro using three proteins—KaiA, KaiB, and KaiC. The total phosphorylation level of KaiC oscillates with a circadian period, but the mechanism underlying its sustained oscillation remains unclear. We have shown that four forms of KaiC differing in their phosphorylation state appear in an ordered pattern arising from the intrinsic autokinase and autophosphatase rates of KaiC and their modulation by KaiA. Kinetic and biochemical data indicate that one of these phosphoforms inhibits the activity of KaiA via interaction with KaiB, providing the crucial feedback that sustains oscillation. A mathematical model constrained by experimental data quantitatively reproduces the circadian period and the distinctive dynamics of the four phosphoforms.
Circadian clocks coordinate metabolism and behavior with diurnal cycles in the environment (1). These clocks traditionally have been understood as transcriptional feedback oscillators in which clock genes repress their own synthesis, creating negative feedback that drives oscillation (1). However, pioneering work by Kondo and colleagues has shown that the circadian clock of the cyanobacterium Synechococcus elongatus requires neither transcription nor translation (2), and circadian oscillations can be reconstituted in vitro using only three proteins: KaiA, KaiB, and KaiC (3).
KaiC is a hexameric enzyme (4) that can autophosphorylate (5) and autodephosphorylate (6) at both serine 431 (S431) and threonine 432 (T432) (7, 8). The dimeric KaiA (9, 10) enhances the autophosphorylation of KaiC (11), whereas KaiB antagonizes the activity of KaiA (11-13). In the absence of KaiA, KaiC fully dephosphorylates (9). Complexes form between the Kai proteins (14), and the relative proportions of the KaiC-containing complexes oscillate (9, 15).
The amount of phosphorylated KaiC oscillates with a circadian period (11). However, the total level of phosphorylation cannot be the only dynamical variable controlling the oscillator since it traverses the same value twice each day, but each time in a different direction (increasing during the subjective day and decreasing during the subjective night). Previous mathematical models have treated both phosphorylation sites as functionally equivalent (16-24), and have proposed additional dynamical variables arising from persistent conformational changes (18, 20-24) or long-lived heterocomplexes (16, 17); we hypothesized that additional variables could be found by examining the pattern of multisite phosphorylation of KaiC during the circadian cycle.
We measured the time dependence of phosphorylation at S431 and T432 by SDS-PAGE (Fig. 1, A and B) and mass spectrometry (Fig. 1B), quantifying the four possible phosphorylation states: unphosphorylated (U-KaiC), phosphorylated only on S431 (S-KaiC), phosphorylated only on T432 (T-KaiC), and phosphorylated on both S431 and T432 (ST-KaiC). The concentration of each phosphoform oscillates with a circadian period but with different phases, creating an ordered pattern of phosphoform abundance during each cycle. Multisite phosphorylation of KaiC is required for oscillation since point mutations at either S431 or T432 abolish rhythmicity (7, 8) (fig. S1).
The predominance of distinct phosphoforms at different points in a cycle—T-KaiC during the phosphorylation phase and S-KaiC during the dephosphorylation phase—suggests that the phosphoform distribution (or a conformation tightly linked to the phosphorylation state) may determine the phase of the oscillator. If this is true, it should be possible to specify the initial phase by preparing KaiC with the appropriate phosphoform distribution and then adding KaiB and KaiA to initiate oscillations. Indeed, a reaction initiated with a KaiC pool enriched in T-KaiC begins in the phosphorylation phase, whereas a reaction initiated with high levels of S-KaiC begins in the dephosphorylation phase (Fig. 1C).
To investigate the origins of the ordered pattern of KaiC phosphoforms, we decomposed the oscillator into partial reactions. When KaiA is mixed with U-KaiC, T-KaiC accumulates first, followed by ST-KaiC, and eventually by S-KaiC (Fig. 2A). When highly phosphorylated KaiC is incubated alone, it autodephosphorylates, and the concentrations of T-KaiC and ST-KaiC decay monotonically (Fig. 2B). Concomitant with the decay of ST-KaiC, the abundance of S-KaiC transiently increases before eventually decaying, suggesting that S-KaiC is produced from ST-KaiC by dephosphorylation of T432. Neither the pattern of dephosphorylation nor its kinetics is affected by the presence of KaiB (fig. S2). These data are described well by a linear model of KaiC phosphoform interconversion (Fig. 2C). Based on the rate constants calculated by fitting these data (Fig. 2, fig. S3, and table S1), we conclude that KaiA both promotes KaiC phosphorylation (according to a hyperbolic dependence quantified in fig. S4) (11) and inhibits some dephosphorylation steps (6). Phosphoform interconversions occur on the same time scale as the oscillations themselves, consistent with the idea that these are the key slow dynamical processes underlying the oscillator.
Combining the phosphoform dynamics observed in the partial reactions (Fig. 2, A and B) yields the same qualitative pattern of phosphoform abundance observed in the full oscillating reaction, suggesting that each cycle of the oscillator is composed of a phosphorylation phase of high KaiA activity, followed by a dephosphorylation phase during which KaiA is inactive. To test this idea, which has been proposed previously [e.g., (9)], we introduced a small quantity of epitope-tagged, dephosphorylated KaiC into the oscillator at various times (Fig. 3A); the tagged KaiC will phosphorylate only if KaiA is active. We observe KaiA activity only during the phosphorylation phase. To rule out the alternative explanation that it is the sensitivity of KaiC to KaiA (21, 23)—rather than the activity of KaiA itself—that varies in a circadian cycle, we increased the concentration of KaiA in the middle of the dephosphorylation phase (Fig. 3B). The phosphorylation level of KaiC immediately increased, indicating that KaiC had not become insensitive to KaiA.
Inactivation of KaiA requires KaiB, as no oscillations occur in its absence (9) (Fig. 2A). Since previous studies have shown that KaiA-KaiB-KaiC complexes form during the clock reaction and that KaiB preferentially binds phosphorylated KaiC (9), we conjectured that inactivation of KaiA and hence initiation of the dephosphorylation phase occurs through a physical interaction between a specific phosphoform of KaiC and KaiA and KaiB. We found that the fraction of KaiC and KaiA complexed with KaiB closely follows the abundance of S-KaiC (Fig. 3C), suggesting that S-KaiC mediates a negative feedback loop through inactivation of KaiA via KaiB. As S431 and T432 are buried within the KaiC oligomer (25), the specific preference of KaiB for S-KaiC suggests that changes in KaiC phosphorylation may be closely tied to conformational changes sensed by KaiB. To isolate the effects of phosphorylation at each site on KaiB-mediated feedback, we studied single-site nonphosphorylatable KaiC mutants and found that KaiB interacts preferentially with the mutant phosphorylatable only on S431 (fig. S1B), and also preferentially inhibits its phosphorylation (fig. S1A).
To further investigate the timing of KaiB function, we introduced it to a KaiA-KaiC reaction at various points (Fig. 3D). Adding KaiB early in the reaction, when S-KaiC levels are low, does not induce any measurable deviation from the KaiA-KaiC control until S-KaiC has reached at least ~10% abundance. In contrast, introduction of KaiB when S-KaiC levels are already high (~15%) rapidly induces dephosphorylation. Hence, S-KaiC plays a special role in promoting inactivation of KaiA. Indeed, the similarity between the dephosphorylation pattern caused by adding KaiB when S-KaiC levels are high and that induced by removing KaiA (fig. S5) demonstrates that adding KaiB in the presence of substantial S-KaiC is equivalent to removing KaiA.
To determine if our understanding of the phosphoform kinetics and feedback mechanism can quantitatively account for the circadian oscillation of KaiC phosphorylation, we created a simple mathematical model (Fig. 4A and fig. S6A) constrained by our experimental measurements. The key assumptions of this minimal model are (i) the concentrations of the three phosphorylated species are the only slow dynamical variables; (ii) the interconversions between phosphoforms are first-order reactions with rates (table S2) that depend hyperbolically on the concentration of active KaiA (Fig. 4A and fig. S4); and (iii) each S-KaiC monomer (together with KaiB) inactivates one KaiA dimer. The phosphorylation and dephosphorylation rates are thus nonlinear functions of the concentration of S-KaiC—the source of the crucial nonlinear feedback (Fig. 4A).
Using rate constants and a KaiA concentration dependence (table S2) derived solely from data on the non-oscillatory partial reactions (Fig. 2 and figs. S3 and S4), this simple model predicts (Fig. 4B) essential features of the circadian oscillator—period (~21 hours in the model), amplitude of total phosphorylation, sequential appearance of the phosphoforms, the larger magnitude of the T-KaiC peak (see also fig. S7). This predictive ability suggests that the model captures the key elements of the in vitro oscillator. Modifying the model to explicitly treat the formation of KaiA-KaiC complexes (9) likely responsible for promoting KaiC phosphorylation makes it consistent with the observation that the oscillations are rather insensitive to the total concentration of Kai proteins (9) (supporting online text and fig. S8).
The following picture of the origin of stable oscillations emerges (fig. S6A). Starting from the unphosphorylated state, KaiA promotes phosphorylation that is kinetically favored at T432; subsequent phosphorylation at S431 produces ST-KaiC. ST-KaiC can decay via dephosphorylation of T432 to produce S-KaiC, but S-KaiC accumulation is slow because KaiA both inhibits that dephosphorylation and promotes rephosphorylation of S-KaiC to ST-KaiC. Thus, S-KaiC levels remain low until a substantial pool of ST-KaiC has formed. When S-KaiC levels do rise, KaiA activity is reduced, promoting dephosphorylation of ST-KaiC and thereby causing it to rapidly decay into S-KaiC. Thus, S-KaiC accelerates its own production (from ST-KaiC), which causes its concentration to overshoot the point at which KaiA is completely inactivated; this overshoot yields a reservoir of S-KaiC that permits extended inactivation of KaiA even as S-KaiC concentrations decrease through dephosphorylation. In the absence of KaiA activity, T-KaiC and ST-KaiC both dephosphorylate, and S-KaiC—which dephosphorylates more slowly—becomes the dominant remaining phosphorylated species. Eventually enough S-KaiC dephosphorylates for KaiA activity to return, and the cycle begins anew.
To focus on the essential slow dynamics and to be able to derive model parameters directly from our experimental data, our model ignores some known biochemical properties of the Kai proteins and abstracts others into the rate constants. KaiC exists as a hexamer (4), and we have neglected possible effects that depend on the state of the entire hexamer. Further, monomer exchange between hexamers (9) is not explicitly included, and we assume that inhibition of KaiA via KaiB occurs instantaneously upon formation of S-KaiC. In actuality, inhibition appears to take approximately one hour (fig. S9), possibly due to slow interaction between KaiB and KaiC or slow exchange of monomers between hexamers. These neglected effects have the potential to increase both the tendency of the system to oscillate and the amplitude of oscillation, but the success of our simplified model suggests that they are not part of the fundamental mechanism.
A recent report from the Kondo group (26) describes the differential phosphorylation of S431 and T432 during the circadian cycle and the interaction of KaiB with KaiC phosphorylated on S431. By using phosphomimetic KaiC mutants, they provide information about ordered phosphorylation complementary to and consistent with our kinetic study of wild-type KaiC.
The most striking behavior of the cyanobacterial circadian oscillator in vivo is its precision: Even with asynchronous cell division and an absence of external cues, the clock of a single cell and its offspring maintains precision to a small fraction of a day over several weeks (27). A reductive understanding of the various aspects of the clock—especially that of the core Kai oscillator presented here—should enable us to understand the effects of random fluctuations and variable environments. The Synechococcus clock provides an ideal model system for understanding how cells perform quantitative functions in highly variable intra- and extracellular environments.
We thank B. Budnik, J. Neveu, and R. Robinson for assistance with mass spectrometry; T. Mori and C. Johnson for SDS-PAGE conditions for phosphoform separation; J. Ferrell for helpful discussions; and B. Stern, R. Losick, M. Ebert, S. Douglas and T. Schmidt for comments on the manuscript. This work was supported by an NSF Graduate Research Fellowship (J.S.M.), NSF grant DMR-0229243 (D.S.F.), and the HHMI (E.K.O.).