The effect of CO2 on the timing of cell cycle events in fission yeast Schizosaccharomyces pombe B. NOVAK, J. HALBAUER and E. LASZL6 Department of Agricultural Chemical Technology, Technical University of Budapest, 1521 Budapest Gellert ter 4, Hungary Summary The effect of CO2 removal on the cell cycle phases of Schizosaccharomyces pombe has been examined in minimal, aspartate-containing and complete medium. The removal of CO2 shortened the G2 phase of the cell cycle and arrested the cells in Gi phase in minimal medium. The Gx block caused by C0 2 deprivation was demonstrated by transition-point and flow-cytometry analyses. The slow-down of anapleurotic CO2 fixation might be responsible for this effect, as aspartic acid could abolish the Gi block. The shortening of G2 phase in the wild-type cells was observed in every medium irrespective of whether the growth rate was changed or not. The experiments in which growth rate was not changed by CO2 shift-down suggest that this CO2 effect can be independent from its action on CO2-fixing steps in metabolism. Introduction There are basically two different ways of looking at the cell cycle (Mitchison, 1971; Kirschner et al. 1985). The first sees it as a dependent sequence of events leading to DNA synthesis and mitosis and the size controls over them (Fantes & Nurse, 1981). The other sees it as a master oscillator which can be described as a limit cycle type oscillation (Kauffman & Wille, 1975). There is a substantial amount of evidences that cell size controls the cycle time of growing systems (see e.g. Fantes, 1977), therefore size control models are more preferable (Mitchison, 1977). However there are some clear indications for persistent periodicities after the cell division cycle has been blocked, which fits into the clock model (Mitchison, 1984; Novak & Mitchison, 1986, 1987). We have tried to resolve this discrepancy between the models in a limit cycle type oscillation model, which is based on the tricarboxylic acid (TCA) cycle completed Journal of Cell Science 89, 433-439 (1988) Printed in Great Britain © The Company of Biologists Limited 1988 Therefore we propose that CO2 inhibits mitosis in fission yeast and we explain the proportionality between growth rate and cell size at mitosis found by Fantes & Nurse by this CO2 inhibition. The larger CO2 production in fast-growing cells leads to a higher CO2 concentration, which could exert a stronger inhibition of mitosis. A wee mutant, which has lost its mitotic size control, also shows the Gi block after CO2 deprivation, but its mitosis is insensitive to CO2. Comparing the respiration of wee and wild-type cells we conclude that CO2 inhibits the citric acid cycle in the wild type. The consequence of these results in the regulation of fission yeast cell cycle is discussed. Key words: CO2, fission yeast, Schizosaccharomyces pombe, cell cycle, wee mutant, size control. by the CC>2-fixing anapleurotic reactions (Novdk & Liszl6, 1986). In this model the cell size influences the period of the oscillator through the intracellular CO 2 concentration in a negative manner (the larger cells have shorter cycle times). A very simple consequence of this model is that the reduction of intracellular CO 2 concentration switches off the oscillator and stops the cell cycle. Therefore we have examined the effect of CO2 removal on the proliferation of Schizosaccharomyces pombe. The fission yeast is a very attractive organism for studying the effect of CO 2 because it does not have the two characteristic enzymes of the glyoxalate shunt (Flury, 1973), which is an alternative way for filling up the TCA cycle, e.g. in budding yeast (Beck & von Meyenburg, 1968). The regulation of the fission yeast cell cycle can be described by two size controls (Nurse & Fantes, 1981; Fantes, 1984). One acts just before DNA synthesis, at the start of the cycle, and it is cryptic in fast-growing cells (Nurse & Thuriaux, 1977; Nasmyth et al. 1979). 433 The cells also have to attain a critical size before mitosis but the actual size is a function of nutritional status or growth rate (Fantes & Nurse, 1977). Our results support these findings, but they also show that the relation between the critical cell size for mitosis and growth rate could be indirect, because the growth rate could influence mitosis through the intracellular CO2 concentration. Materials and methods Strains and nutrients The wild-type and the wee 1.6 mutant of Scizosaccharomyces pombe was a gift from James Creanor (Department of Zoology, University of Edinburgh). The wild-type strain 972 h~ was originally obtained from Professor U. Leupold (Bern). The mutant weel.6 divides at about half the size of the wild-type cell (Thuriaux et al. 1978). Edinburgh Minimal Medium (EMM3) was used in most of the experiments (Creanor & Mitchison, 1982). In some experiments the NH4CI in EMM3 was replaced by aspartic acid at 5 g l " ' and the pH adjusted to 5-4 (EMM+ASP). In others, the medium was supplemented with 5 g l ~ ' yeast extract (EMM + YE). Strategy of experiments Cultures were grown overnight in a fermentor at 35°C to mid-exponential phase (to 5X 10 5 -lXl0 6 cellsml" 1 ). The fermentor containing about 0 5 1 yeast suspension was stirred and aerated, and the change in dissolved O2 and CO2 concentration was measured as described below. The exponential growth was followed for about one generation time, which seemed to be enough to determine the specific growth rate of the culture. The dissolved O2 concentration was held constant at 80 % of saturation value by changing the aeration intensity. After this time the CO2 was flushed out by aflowof N2 (flow rate ~4001 h" 1 ) through the medium. The dissolved O2 concentration was not changed during the experiment so some air was mixed with the N2 flow. Elimination of the CO2 in the medium reduces the intracellular CO2 concentration by increasing the diffusion flux between the cell and its environment. Measurements of cell number and cell size distribution Cell number was measured after mild sonication with a Laborscale (Medicor, Hungary) electronic particle counter with a 70-^m aperture. The mean cell volume (V) was estimated from the cell volume distribution obtained with the PSA-1 channel-analyser (Medicor, Hungary) by the following equation: V = '-^-L where iV, is the number of cells and A", the cell volume in the / channel (0 < / < 64): A, = 3-265/. DNA flow cytometry Up to now the DNA content of fission yeast has only been analysed by flow cytometry in one laboratory (Beach et al. 434 B. Novak et al. 1985; Costello et al. 1986): our sample preparation procedure is basically the same as described in these papers. Samples of cells (~10 7 cells) were mildly sonicated, collected by centrifugation, washed free of growth medium and suspended in 40 % ethanol. The cells were fixed in 70 % ethanol for at least 24 h at 4°C. Thereafter the cells were washed with lml 005 M-phosphate buffer (pH 7-5) and resuspended in 1 ml of the same buffer. They were treated with preboiled RNase (Reanal, Hungary) at 1 mgrnl" concentration for 90min at 37°C. After centrifugation the cells were stained at 4°C for at least 15min in 2ml solution containing: l g l ~ ' sodium citrate, 0-58gl~' NaCl and 50mgl~' ethidium bromide. Total fluorescence intensities were measured in an FC 200/4800A-50 instrument (Biophysics Inc) equipped with a 5W argon-ion laser giving 120 mW at 488 nm. Light to the fluorescence amplifier was filtered using a 600 nm filter and the analyses were based on the accumulation of 10s cells. The mean DNA content of the cells was calculated from the distribution with a similar equation used for calculating the mean cell size. In some experiments the digestion by RNase was omitted on a portion of the sample to obtain the total ethidium bromide fluorescence of nucleic acids. The comparison of two samples showed that fluorescence from DNA is negligible compared to the RNA. It is not surprising since the DNA/RNA ratio is 1/100 in fission yeast (Mitchison & Lark, 1962). Other techniques The dissolved O2 and CO2 concentration was determined with electrodes sensitive to these gases (Radelkis, Hungary). The aeration of the culture was disrupted for a short time (~10min) and the rate of respiration was determined from the slope of O2 concentration decrease. It is impossible to measure the respiration rate during the intensive aeration period. The optical density (o.D.) of the culture was measured at 595 nm on a Specord M40 photometer (Zeiss, Jena). Results Fig. 1 shows the reaction of wild-type yeast to the removal of CO2 after some time in exponential growth in three independent experiments. The downward pointing arrow indicates the start of flushing out and the upward pointing arrow marks the time at which the N2 flow was switched off. The CO2 concentration and the mean cell size curves belong with the lower cell number curve. The reduction of CO2 concentration causes two dramatic changes in the cell density curves. The rate of cell division accelerates and the cell number remains constant after it has reached about double the value it had at the start of the CO2 reduction. Thus all the cells divide once again in the absence of CO2 with a rate higher than normal. In parallel the mean cell size decreases from the 90 fim value characteristic of balanced growth to 60 /im 3 . 64, 2 32 E 16at X> E 3 C 3H 4' o| 3 £J 2 on « j 100- •3-9- O U I2'6 1-3- Time (h) Fig. 1. The growth of wild-type cells in EMM3 at 35 °C in the presence and in the absence of CO^. The N2 flow was switched on at the downward pointing arrows and switched off at upward pointing arrows. Curves A-C, cell number; 1 arbitrary unit = 10s cells ml" 1 . Curve D, specific respiration rate; 1 arbitrary unit = 10~8^l C^celF 1 min" 1 . Curve E, mean cell volume. Curve F, partial pressure of CO2 in the medium. After switching off the N 2 flow, the CO 2 starts to increase together with the cell size, but the cell number remains constant for about a cycle time (~2-5h). Curve D in Fig. 1 shows the specific respiration of wild-type before CO2 deprivation and after the CO2 shift up. The stage in the cell cycle at which a cell cycle block arrests the cells can be estimated from the residual cell number increase after the block, based on a theoretical age distribution (Cook & James, 1964). Cells that at the time of shift are before this 'transition' point cannot divide, but cells that are over this stage can complete their cycle and divide (Nurse et al. 1976). The mean residual cell number increase after CO 2 reduction from eight independent experiments gives a —0-18 transition point, which is a good estimate for a Gi block. This conclusion is strengthened by DNA flowcytometry analysis of the population. Fig. 2 shows the change in the cell number and in the mean DNA content of the cells calculated from flow-cytometry data in another experiment. In fast-growing fission yeast populations, almost all the cells have a 2C (G 2 ) DNA content, because the time of DNA synthesis coincides with cell division (Mitchison & Creanor, 1971). Therefore the decrease of the cellular DNA content to nearly half of its original value is a clear indication that most of the cells have changed to a Gi DNA content. Fig. 3 shows the cellular DNA distribution of the exponentially growing and the CO2-deprived cultures. The bottom curve on Fig. 2 shows the fraction of the cells in the population carrying a septum (Septal Index, SI). This septum is formed shortly after mitosis, therefore the SI gives an estimate similar to the mitotic index. The rapid increase in SI after the reduction of CO 2 indicates that the cells accelerate into mitosis. It means that the faster division rate is due to the shortened G 2 phase rather than to the shortened period between mitosis and cell division. After switching off the N 2 flow, the mean DNA content and the SI rise transiently above the value characteristic for the balanced growth, because the culture shows some degree of synchrony. The top curve in Fig. 2 is the change in the optical density, which gives an estimate proportional to cell number and cell size. After the CO 2 shift-down the optical density reaches a plateau after a transient and slight increase in its slope. During the transient increase in slope the cell number and the cell size change in the opposite way (see Fig. 1), therefore the optical density curve does not give a real estimate for the specific growth rate. However the lack of increase in optical density indicates that the absence of CO 2 inhibits cell growth and reduces the specific growth rate to zero or very close to it. A plausible explanation for this is that the reduced level of CO 2 limits the Effect of CO2 on cell cycle events in S. pombe 435 80 *^A 0-15 40 units t I 0-10 / B Z Arbitr £20 a 0-05 10 1C 2C 4C Fig. 3. The distribution of cellular DNA content estimated by flow cytometry of exponentially growing (A) and CO2 deprived (B) cells. 5 12- / c u §10. / < Z Q 8 c u vz s \ \ 6- ~ 30 X 1 20 » 10 • / \ /*7 /c 16 1 / /A / r A s^. . . ._* 6 Time (h) 10 12 Fig. 2. The growth of wild-type cells in EMM3 at 35°C in the presence and in the absence of CO2. Curve A, optical density; 1 arbitrary unit = 2X 10~3A. Curve B, cell number; 1 arbitrary unit = 105 cells nil"'. Curve C, mean DNA content. Curve D, septal index. growth rate through CO2-fixing reactions. The acceleration into the mitosis could be a consequence of the reduced growth rate, according to the model of Fantes & Nurse (1977). The experiments with EMM + ASP medium were done to test the hypothesis that anapleurotic CO2 fixation is the rate-limiting step at the reduced CO2 level. Aspartic acid can be transaminated to oxaloacetate and so it can fill up the TCA cycle independently of the CO2 fixating anapleurotic reactions. Fig. 4 shows the effect of CO2 on proliferation of wild type in EMM + ASP. The reduction of CO2 makes little difference to the slope of the optical density and does not stop the cell number increase. Thus the presence of aspartate abolished the G| block caused by CO2 436 B. Novak et al. 10 Fig. 4. The growth of wild-type cells in EMM + ASP medium at 35 °C in the presence and in the absence of CO2. Curve A, optical density; 1 arbitrary unit = 10~ A. Curve B, cell number; 1 arbitrary unit = 8 5 X 10s cells ml"'. Curve C, mean cell volume. Curve D, septal index. 16 10 10 Fig. 5. The growth of wild-type cells in EMM+YE medium at 35 CC in the presence and in the absence of CO2. Curve A, optical density; 1 arbitrary unit = \0~zA. Curve B, cell number; 1 arbitrary unit = 5x 105 cells ml" 1 . Curve C, mean cell volume. Curve D, septal index. deprivation. However the drop in CO2 caused a rise in SI and a transient acceleration in cell division, indicating that the reduction of CO2 shortened the G2 phase as in minimal medium. There is no parallel relationship between the growth rate change and the extent of acceleration into mitosis after the CO 2 shift down. In Fig. 4 the acceleration into mitosis is nearly as large as in Fig. 2, while there is only about a 10% fall in growth rate in EMM+ASP in contrast to the 100% decrease in growth rate in EMM. This suggested that the level of mitotic size control is not growth rate related but it is a function of the CO2 concentration. We tried to test this in the following way. The minimal medium was supplemented with yeast extract. This complete medium contains the precursors of biosynthetic reactions; the CC>2-fixing reactions cannot therefore be rate limiting even though they are slowed down. Fig. 5 shows the growth of cells Fig. 6. The growth of iveel.6 cells in the presence and in the absence of CO2. Curve A, cell number; 1 arbitrary unit = 2'5X 10°. Curve B, cell number; 1 arbitrary unit = 6-66X 105 cells ml" 1 . Curve C, cell number; 1 arbitrary unit = 10 cells ml" . Curve D, mean cell size. Curve E, specific respiration rate; 1 arbitrary unit = in EMM+YE; CO 2 deprivation has no effect on the slope of optical density and cell number increase. The only thing that happened was that the cells were advanced into mitosis and there was a rise in SI and a step in cell number. This result shows that the CO^ concentration influences the mitotic size control independently from its action on the growth rate. It was interesting to examine the effect of CO2 on wee cells, which have lost their mitotic size control because of a mutation in a single gene (Nurse, 1975). Fig. 6 shows the results with weel.6 cells in three independent experiments. The mean cell size and the specific respiration curves belong with the bottom cell number curve. The cell number increase after the CO2 reduction is less than in wild type. The mean of five experiments give a 0-39 transition point which agrees well with the position of S phase in these cells (Dickinson, 1983). It means that the absence of CO 2 Effect of CO2 on cell cycle events in S. pombe 437 causes a Gi block in wee cells similar to that in wild-type cells. However the shift-down in CO2 did not cause any increase in division rate and SI (data not shown), thus wee cells were not advanced into mitosis. The genetic lesion in the mitotic size control makes the mitosis insensitive to CO2. The bottom curve on Fig. 6 shows the specific respiration rate of weel.6 cells before CO2 deprivation and after the CO2 shift up. The initial low value of this rate after CO2 deprivation indicates that respiration has been slowed down by the reduced CO2 level. This can be explained by the limited rate of anapleurotic reactions which fill up the TCA cycle responsible for generating NADH. The rise in CO2 results in a fast increase in respiration which can be due to the acceleration of the TCA cycle caused by CO2 fixation. A comparison of Fig. 1 and Fig. 6 shows that the specific respiration rate of wild type is almost half that of ivee cells. It is interesting that the specific CO2 production rate of wild type is exactly double that of wee 1.6 (Novdk & Mitchison, 1986). It means that the respiration quotient of wee (RQ = 3) is much smaller than that of wild type (RQ = 10). Therefore the TCA cycle is more active compared to glycolysis in wee cells than in wild type. Discussion Our results indicate that CO2 has a dual effect on the fission yeast cell cycle in minimal medium. Reduction of CO2 in the medium rapidly accelerates the cells into mitosis by shortening of the G% phase of the cell cycle. Depriving the cells of CO2 also causes them to accumulate in Gi phase as we have shown with the transition points of wild-type and ivee cells and with the flowcytometry data. The Gi block seems to be a nutrientdeprivation response because it correlates with the cessation of growth. COvfixing reactions, which slow down at reduced CO2 concentration, could be behind this effect. CO2 fixing steps occur at different points in the metabolism of a heterotrophic cell: TCA cycle filling up (anapleurotic) reactions, in lipid biosynthesis and degradation, in purine and pyrimidine biosynthesis (see e.g. Biggers & Bellve, 1974). Since aspartic acid almost completely abolishes the G\ block caused by CO2 deprivation, anapleurotic reactions may be the most sensitive among these reactions. This suggests that the replenishment of the TCA cycle is necessary to complete the Gi and to initiate the S phase. The other observed effect of CO2 decrease is the shortening of G2 phase. The acceleration of cells into mitosis by shift-down of CO2 has been observed in every medium in wild type cells, but not in wee cells. It has been also detected when CO2 was decreased to a value that did not lengthen the cycle time. 438 B. Novak et al. A similar shortening of G 2 and acceleration of mitosis has been found in nitrogen shift-down experiments (Fantes & Nurse, 1977). These were consistent with the mitotic delay found in shift-up experiments done by changing the nitrogen, carbon or phosphate source. Fantes & Nurse (1977) interpreted these results as showing that the cell size control over mitosis could be modulated by the nutritional status or growth rate. They did not find any mitotic acceleration or delay in weel cells in shift experiments (Fantes & Nurse, 1978), so they concluded that the signal generated by growth rate is transmitted by the weeJ+ gene product to control the entry into mitosis. Our results confirm these findings and their interpretation with the one exception where growth rate is not changed by CO2 shift-down in Fig. 5. Therefore we propose that CO2 could be an element of the growth rate monitoring system and it could mirror the nutritional status. It is well known that the specific rate of metabolic reactions is a function of the specific growth rate, showing a minimal (maintenance) value in the non-growing state. It means that in faster growing and dividing cells the CO2-production rate is larger than in slow growing cells. The larger CO2 production leads to a higher CO2 concentration in the cell and the intracellular CO2 concentration is proportional to the specific growth rate. Thus the cells could 'measure' their growth rate through the intracellular CO2 concentration. Since CO2 inhibits mitosis, the faster-growing cells might divide their nuclei only at a larger cell size. Although the molecular mechanism of this mitotic inhibition caused by CO2 is completely unknown, CO2 is a well-known inhibitor of decarboxylases (Jones & Greenfield, 1982). The TCA cycle from pyruvate to succinyl-CoA contains three decarboxylating enzymes, which could be the targets of CO2 action. The derepressed TCA cycle activity found in ivee 1.6 cells fits into the picture well, because the mitosis of wee cells is insensitive to CO2 and their TCA cycle is more active compared to wild type. We thank Professor Murdoch Mitchison for his continuous interest during the work, useful suggestions and for reading the manuscript. We thank Dr Paul Nurse and Dr P. A. Fantes for critical reading the manuscript. We also thank Dr Zolt<in Marcsek at United Research Organization of the Hungarian Academy of Sciences and the Semmelweis Medical University for the flow cytometry measurements and Liszld SzilSk for technical assistance. References BEACH, D., RODGERS, L. & GOULD, J. (1985). 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