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Biophysical Journal 74: 175-181 (1998)
© 1998 the Biophysical Society
Biophys J, January 1998, p. 175-181, Vol. 74, No. 1
*Department of Zoology, University of Cambridge, Cambridge CB2 3EJ, United Kingdom, and #Department of Microbiology and Immunology, University of North Carolina, Chapel Hill, North Carolina 27599-7290 USA
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ABSTRACT |
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Cells in a cloned population of coliform bacteria exhibit
a wide range of swimming behaviors
a form of non-genetic
individuality. We used computer models to examine the proposition that
these variations are due to differences in the number of chemotaxis signaling molecules from one cell to the next. Simulations were run in
which the concentrations of seven gene products in the chemotaxis
pathway were changed either deterministically or stochastically, with
the changes derived from independent normal distributions. Computer
models with two adaptation mechanisms were compared with experimental
results from observations on individuals drawn from genetically
identical populations. The range of swimming behavior predicted for
cells with a standard deviation of protein copy number per cell of 10%
of the mean was found to match closely the experimental range of the
wild-type population. We also make predictions for the swimming
behaviors of mutant strains lacking the adaptational mechanism that can
be tested experimentally.
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INTRODUCTION |
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If you watch them closely, tethered by their flagellae to the surface of an antibody-coated slide, you can tell them from each other by the way they twirl, as accurately as though they had different names. Lewis Thomas, Medusa and the Snail
The term "non-genetic individuality"
has been applied to organisms from a genetically identical population
that display differences in phenotype from individual to individual.
This phenomenon has been observed repeatedly in both prokaryotic and
eukaryotic organisms (McAdams and Arkin, 1997
). The individuality in
the swimming behavior of Escherichia coli (Spudich and
Koshland, 1976
) is of particular interest because the underlying cell
signaling pathway is uniquely well characterized in terms of the
concentrations of the components and the rate constants of the
reactions in which they participate. This has spurred the development
of a number of computer models of chemotaxis that illuminate particular
aspects of the pathway (Bray et al., 1993
; Bray and Bourret, 1995
;
Hauri and Ross, 1995
; Barkai and Leibler, 1997
; Spiro et al., 1997
).
Motility in a coliform bacterium is generated by up to six motors
attached to long filamentous flagella. When the motors rotate in a
counterclockwise direction, the flagella form a bundle and the cell
swims smoothly (runs) with a high degree of directionality. On the
other hand, when the motors rotate in a clockwise direction, the
flagellar bundle flies apart and the cell tumbles, randomly reorienting
the direction of the subsequent run (reviewed in Eisenbach, 1990
). The
behavior of a flagellar motor is commonly quantified in terms of
its bias, defined as the fraction of time that the motor
rotates in a counterclockwise direction. Movement of a cell up a
concentration gradient of attractant increases the bias of the motors
and, hence, the persistence of movement in this favorable direction
(Block et al., 1983
), with the result that the cell performs a biased
random walk toward the source of attractant (Berg and Brown, 1972
).
In 1976, Spudich and Koshland described the pronounced differences that
exist in the swimming behavior of individual cells in a cloned
population of bacteria (Spudich and Koshland, 1976
). They gave the
cells, which were either free-swimming or tethered to the surface of
microscope coverslips by antibodies to individual flagella, a brief
chemotactic stimulus of attractant and measured their adaptational
response
the time taken to return to the original pattern of runs and
tumbles. The cells showed major and persistent differences in their
individual adaptation times, as well as related differences in their
resting-state pattern of runs and tumbles. These differences were
independent of nutritional state and position of the cell in its
division cycle.
In their original paper, Spudich and Koshland proposed that the variations could be generated by stochastic fluctuations in small numbers of molecules controlling the direction of flagellar rotation. The identity of these molecules was not known at the time, but now, two decades later, we have detailed information not only on the proteins themselves but also on their average numbers in the cell and their functions in controlling the rotation of flagella. It is, therefore, possible to use detailed computer models of the signal pathway to survey, in a systematic fashion, how changes in the number of signaling molecules, either singly or coordinately with other proteins, influence flagellar rotation. We can also ask whether some proteins have a greater effect than others and whether certain mutants, especially those affecting the adaptational response, may be expected to show more or less individual variation.
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METHODS |
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Signal pathway
The chemotactic response pathway consists of a set of
transmembrane receptor proteins (e.g., Tar) and the products of four chemotaxis genes, CheW, CheA, CheY, and CheZ. The latter four convey
information on the binding of attractants or repellents at the
receptors to the flagellar motor, and thereby modify its direction of
rotation (reviewed in Parkinson, 1993
; Eisenbach, 1996
; Stock and
Surette, 1996
). The receptors are bound in a complex to the
autophosphorylating protein kinase CheA via the linking protein CheW.
Phosphoryl groups are transferred from phosphorylated CheA, CheAp, to
CheY, and phosphorylated CheY, CheYp, then diffuses to the switch
complex of the flagellar motor, causing a reversal in the direction of
rotation from counterclockwise (the default direction) to clockwise.
CheZ terminates the response by stimulating the dephosphorylation of
CheYp. Two other gene products are involved in adaptation of the
chemotactic response: the methyltransferase CheR methylates up to six
specific sites on each receptor, and the methylesterase CheB performs
the reverse demethylation reaction. The phosphorylation of CheB to
CheBp, again by phosphotransfer from CheAp, causes a large increase in
its esterase activity (Fig. 1).
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Theory
A detailed computer model of the signal response pathway in
bacterial chemotaxis has been described previously (Bray and Bourret, 1995
). This model includes the phosphorylation reactions in which CheYp
is formed, together with the network of binding steps through which the active receptor complex (TTWWAA) is assembled from the starting material of Tar dimers (TT), CheW monomers (W), and CheA dimers (AA). For the purposes of the present study, we have expanded the model to implement the adaptation reactions mediated by CheR and
CheB in both a "robust" and a "fine-tuned" manner. Robust systems intrinsically maintain certain properties, for example exact
adaptation, when the system parameters
concentration and kinetic
data
vary over a wide range. In fine-tuned systems, however, the
system parameters are adjusted, usually through an optimization procedure, to obtain the desired property, which is likely to be lost
when even small changes in the system parameters are made.
In the implementation of the "fine-tuned" algorithm, the rates of
the adaptation reactions depend solely on the current
concentrations of modified or unmodified receptor according to
bimolecular mass-action laws. This mechanism is similar to one
originally proposed by Segel et al. (1986)
and later used in a more
detailed fashion by Hauri and Ross (1995)
and Spiro et al. (1997)
. In
the implementation of the second "robust" algorithm (a copy of the
robust version of the program is available from the website
http://www.zoo.cam.ac.uk/zoostaff/levin/index.htm), the receptor is
assumed to exist in either an active or an inactive conformation
depending on its ligand occupancy and state of methylation (Asakura and
Honda, 1984
). Methylation by CheR in this case occurs at a constant
rate, whereas demethylation by CheB takes place only when the receptor
is in its active state. It has been shown that under these conditions
the system will always return to its original level of activity
regardless of the nature or magnitude of the stimulus or the rate
constants or concentrations of the reactants (Barkai and Leibler,
1997
).
The "output" of the computer simulations is the cytoplasmic
concentration of the phosphorylated species CheYp, which interacts with
a switching complex on the cytoplasmic face of the flagellar motor to
reverse its direction of rotation. Present evidence suggests that this
is a cooperative interaction in which many CheYp molecules bind to FliM
molecules in the switch complex of the motor (Welch et al., 1993
). In
this study, we assume that the relationship between the CheYp
concentration and motor bias is of the form:
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(1) |
Tethering experiments
E. coli cells wild-type for chemotaxis (RP437) were
tethered to glass coverslips by their shorn flagella (Bray et al.,
1993
). The movements of individual cells, along with a
computer-readable timecode, were recorded onto videotape for a minimum
of 30 s, using a rate of 60 frames per second. The tape was played
back at 12 frames per second, while changes in the direction of
rotation were manually logged using specialized computer software
(Observer, Noldus Information Technology, The Netherlands). Rotational
bias was calculated as the fraction of time the cell was rotating
counterclockwise. A comparison of bias distributions from different
cultures demonstrated there was no significant variation between
cultures.
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RESULTS |
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Changing individual proteins
An important feature of the computer model used in this study is
that it includes the network of binding steps leading to the formation
of the receptor complex (Bray and Bourret, 1995
). Other models of
chemotaxis (Hauri and Ross, 1995
; Barkai and Leibler, 1997
) lack this
feature, and treat the receptor complex as a fixed unit in their
simulations. We have used the greater flexibility our model provides to
examine the effects of mutations in receptor function, and adaptation
mechanism, on the individuality question. This gives us the opportunity
to examine the effects of changing the levels of all seven individual
components of the pathway on the steady-state levels of CheYp,
including Tar, CheA, and CheW.
As a first step, we considered the effect of changing the concentration of each protein in turn while keeping the concentrations of the other six proteins constant. The results for the fine-tuned adaptational pathway over a range of expression from zero to 10× wild-type are presented in Fig. 2 A. Three proteins (Tar, CheW, and CheA) display a maximum CheYp concentration when expressed at, or close to, the wild-type level; two proteins (CheZ and Che B) display a negative gradient (that is, a decrease in CheYp concentration with increasing protein level); and the two remaining proteins (CheR and CheY) display a positive gradient.
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The existence of a maximum CheYp in the case of Tar, CheW, and CheA is
consonant with the experimental observation that both null and
overexpression mutants affecting these proteins display a high bias
(Liu and Parkinson, 1989
; Sanders et al., 1989
). The mechanistic basis
for this maximum has been proposed to lie in the network of binding
reactions leading to formation of the Tar complex (Bray and Bourret,
1995
). The negative gradient obtained with CheZ and CheB may also be
understood on the basis of the signal transduction pathway shown in
Fig. 1. Since CheZ is the specific phosphatase of CheY, high levels of
CheZ will reduce the levels of CheYp and thereby increase the bias.
CheB catalyzes the removal of methyl groups from the Tar complex, and
this lowers the rate of phosphorylation of CheY. Increasing CheB,
therefore, leads to a decrease in CheYp.
In the case of the two positive gradients, that of CheR has a similar
explanation to CheB
high levels increase methylation of the Tar
complex and hence increase CheYp. Increases in CheY expression,
however, operate by a more subtle mechanism. Since CheA
autophosphorylation is rate-limiting with respect to phosphotransfer, and almost all of the phosphate flux is directed toward CheY rather than CheB, a large increase in CheY will increase CheYp only
marginally, but reduce CheBp by a substantial amount. As CheBp is many
times more active than CheB, this reduction in total methylesterase activity with unchanged methyltransferase activity will increase the
degree of methylation of the Tar complex, which will feed through into
the observed increase in CheYp.
The fine-tuned and robust adaptational mechanisms produced similar but not identical results in the deterministic simulations (Fig. 2, B and C, respectively). The more limited range of protein expression in comparison with Fig. 2 A reveals differences in the respective positions of the maxima for Tar, CheW, and CheA.
Changing proteins in concert
It is evident from the data in Fig. 2 that individual chemotaxis
proteins may have opposite effects on the CheYp levels. The question
therefore arises whether increases or decreases in multiple proteins
simultaneously would result in these effects canceling out. We
therefore examined the consequences of increasing or decreasing all
seven signaling proteins in concert. Changes of this kind could occur
naturally as the mocha and meche operons, which
carry the structural genes for all of the proteins under investigation, are expressed at different levels through changes in the nutritional status of the bacterium (Silverman and Simon, 1974
).
The effect of coordinate changes was found, in fact, to lie within the extremes of the range shown by individual proteins (Fig. 3). There was, however, an unexpected sensitivity to the method of adaptation incorporated in the program. As the coordinate concentration is increased from zero, both pathways initially display increasing CheYp concentrations, but it is only with the robust algorithm that the CheYp concentration passes through a maximum before declining. At high coordinate concentrations, this results in the fine-tuned algorithm producing a response at the opposite end of the bias spectrum to that produced by the robust algorithm.
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With the exception of some earlier studies of the effects of CheY
overexpression on swimming behavior (Kuo and Koshland, 1989
), there has
been no systematic investigation of the effects of different levels of
expression of the chemotaxis signaling proteins on resting bias. Our
results suggest that such a study would be highly informative, and in
particular might help to distinguish between the possible models of the
adaptation process.
Changing proteins randomly
The most likely origin of individuality in coliform swimming
behavior lies in independent variation in each chemotaxis protein from
cell to cell. Although there is little direct evidence for this
conjecture, it is well known that the protein content of individual
cells, even from a cloned population, shows substantial variation.
Experiments using flow cytometry typically reveal that the protein
content per cell has a standard deviation in excess of 10% of the mean
(see, for example, Darzynkiewicz et al., 1982
; Crissman et al., 1985
).
Changes of this kind could arise as a consequence of unequal
partitioning of protein molecules at cell division (Sennerstam, 1988
);
or they could be due to stochastic mechanisms in gene expression (Ko,
1992
), with occasional large bursts of signal proteins activating or
suppressing controlled genes, thereby triggering cascades or affecting
the decision between switching alternatives (McAdams and Arkin, 1997
).
To simulate this effect we selected the concentrations of all the
chemotaxis proteins at random from independent normal distributions
with equal relative standard deviations.
The range of CheYp concentration was computed for a population of bacteria in which each of the seven chemotaxis proteins was subject to independent variation in concentration (Fig. 4 A). In Fig. 4 B, we have used these CheYp values to calculate the expected rotational bias of the flagellar motors of the cells according to Eq. 1. It may be seen that the spread of CheYp values and bias values increases markedly with increasing relative standard deviation of protein copy number.
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Thus, if we arbitrarily define a bias falling between 0.8 and 0.9 as wild-type, then with 5% standard deviation of protein copy number ~55% of cells will be wild-type, whereas with 10% standard deviation only 28% will be wild-type. The above distributions were calculated using the robust adaptational algorithm, but the fine-tuned algorithm gave very similar results (not shown).
The strength of any computer model lies in its ability to reproduce experimental results. As a consequence, we determined experimentally the bias distribution of a large sample of wild-type cells drawn from a genetically identical population (see Methods), and compared this data with the computer-generated result. In Fig. 5 A, we present the distribution of bias values obtained from 500 individual cells compared to the distribution predicted from the computer program with a standard deviation of 10% of the mean (from Fig. 4 B). In Fig. 5 B, the experimental data have been used to deduce the probable concentration of CheYp in each cell from Eq. 1, and this is shown together with the computed distribution with the same standard deviation of 10% (from Fig. 4 A).
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In both Fig. 5 A and 5 B, it may be seen that the experimental and computed distributions are broadly similar. The number of cells with a nominal wild-type swimming bias, for example, was 26% in the experimental population and 28% for the computed distribution. On the basis of this result, therefore, we are able to say that the observed variation in swimming behavior from cell to cell in this population of bacterial cells could have arisen if the numbers of seven chemotaxis proteins fluctuated randomly with a standard deviation of 10% of the mean.
Mutant distributions
We were curious to know whether mutant bacteria in which one or
more of the proteins controlling swimming have been altered by mutation
would show more or less individual variation than wild-type cells. The
comparison is especially informative in mutant strains that, while
being unable to respond correctly to attractants or repellents,
nevertheless have an average unstimulated bias close to wild-type
values. Two mutants of this kind were modeled in this study: the first
is an R
B
strain that lacks both the
methylating enzyme CheR and the demethylating enzyme CheB and is,
therefore, defective in the adaptation response; the second is a
T
W
Z
strain lacking the Tar
receptor, CheW and CheZ.
Predicted CheYp distributions for populations of these two mutants
compared to those of the wild-type strain are shown in Fig.
6 A (the robust adaptation
algorithm) and Fig. 6 B (the fine-tuned algorithm). These
results were calculated for a 10% standard deviation in protein
numbers per cell. In general, as shown in Fig. 6 and Table
1, the difference between the mutant and
the wild-type cells is not very great. The
T
W
Z
strain displays a
slightly narrower distribution of CheYp concentrations than the
R
B
strain with both the fine-tuned and
robust algorithms. The R
B
strain only
displays a narrower distribution of CheYp concentrations than the
wild-type strain with the robust algorithm
there is little difference
between the two distributions produced with the fine-tuned algorithm.
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For the mutant strains, both the robust and fine-tuned adaptation
algorithms produce almost identical distributions of CheYp concentrations because of the absence of receptor modification activity: the T
W
Z
strain
lacks receptor complexes, while the R
B
strain lacks the modification enzymes themselves. The difference between the two mutant strains lies in the mechanism for generating the
phosphate flux: in the T
W
Z
strain, by the slow autophosphorylation of free CheA dimers; in the
R
B
strain, by the rapid autophosphorylation
of methylated Tar complexes. The magnitude of the flux in the
T
W
Z
strain is linearly
dependent on the CheA concentration, but in the
R
B
strain it is a nonlinear function of the
Tar, CheW, and CheA concentrations determined by the
Kd values of the network of binding steps. The
synergistic effect of random changes in the concentration of all three
components of the complex widens the CheYp distribution with respect to
the T
W
Z
strain (Fig. 2
illustrates the deterministic effect with each of these components
taken in turn).
Experimental predictions
An important feature of the detailed, molecular-based computer
simulations used in this study is that they readily provide specific
predictions that can be tested experimentally. For example, the bias
distribution seen in populations of both the
R
B
strain and the
T
W
Z
strain should have a
comparable standard deviation to that of a population of wild-type
cells. Until recently, it has not been feasible to perform such
experiments due to the inordinate amount of time involved in
quantifying the biases of large numbers of tethered cells. The use of
automated tracking equipment on this task would enable large sets of
bias data to be obtained in much shorter periods of time.
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ACKNOWLEDGMENTS |
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This work was supported by a grant from the UK Medical Research Council to Dennis Bray.
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FOOTNOTES |
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Received for publication 7 July 1997 and in final form 29 September 1997.
Address reprint requests to Dr. Matthew Levin, Department of Zoology, University of Cambridge, Downing Street, Cambridge CB2 3EJ, UK. Tel.: 44(0)1223336623; Fax: 44(0)1223336676; E-mail: mdl22{at}cus.cam.ac.uk.
Walid N. Abouhamad's present address is Laboratory of Pharmacology and Chemistry, National Institute of Environmental Health Sciences, Research Triangle Park, NC 27709.
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REFERENCES |
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Biophys J, January 1998, p. 175-181, Vol. 74, No. 1
© 1998 by the Biophysical Society 0006-3495/98/01/175/07 $2.00
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