BioSystems, 24 (1990) 127-133 127
Elsevier Scientific Publishers Ireland Ltd.
Does a
cell perform isoelectric focusing?
Jaroslav Flegr
(Received February l9th,1990)
(Revision received May 2nd,1990)
A model
of intracellular electrical sorting of enzymes and organelles in the cytosol,
based on isoelectric focusing, is proposed. The focusing is suggested to take
place over a centrally symmetric pH gradient which in the cytosol of the yeast
Saccharomyces cerevisiae is known to be 7.2-6.4. From published data on the
energetic capacity and from the computed electric resistance of the S.
cerevisiae cell, the maximum value of the electric field that can be maintained
in the cytosol was estimated. The results showed that the strength of a
centrally symmetric intracytosolic electric field could be as high as 90 mV/cm,
which is sufficient to account for sorting of cytosolic proteins according to
their isoelectric points. Although direct experimental evidence for
intracellular isoelectric focusing is still missing, several phenomena of
physiological importance can be understood on the assumption of its real
existence.
Kegwords: Hypothesis; pH gradient; Electrophoretic sorting;
Structure of cytosol.
1.
Introduction
The
physiological importance of electrophoretic transport of molecules and
organelles in a manner analogous to
zone electrophoresis has been stressed
by many authors; for reviews see DeLoof
(1985, 1986), Robinson
(1985),
Harold et al. (1985,1986) and Nuccitelli
(1988). The existence of a pH gradient in the cytosol (Slavik,1983; Slavik and Kotyk, 1984; Tsien and
Poenie,1986; Ross and Slavik,1987;
Paradiso et al.,1987) suggests that also some analogy with isolectric focusing could be functioning in a living cell. It is obvious
that if both an electric field and a pH gradient exist in the interior of the cell, then cytosolic ampholytes (e.g. proteins) are sorted
according to their isoelectric points (pI) to occupy stable positions in distinct regions within the cell. The rates of many, if not all,
biochemical reactions in the cytosol are
supposed to be limited by the rates of
diffusion of the reactants (Snol,1979). The importance of a process which could
concentrate the reactants into small
and distinct regions of the cell interior
and thus overcome the limitation is evident.
In this
paper, the possibility of intracellular
isoelectric focusing operating in the S. cerevisiae cell is considered
from an energetic point of view. Experimental data supporting the existence of
intracellular isoelectric focusing are reviewed and its possible impacts on
different physiological processes in the cell are discussed..
2. The
expenditure on intracellular isoelectric focusing in the energetic budget of
the yeast cell
Slavik
and Kotyk (1984) have demonstrated the presence of a continuous pH gradient
ranging from pH 72 (cell centre) to pH 6.4 (cell periphery) in the cytosol of a
living Saccharomyces cerevisiae cell. If such a gradient were to be utilised
for isoelectric focusing of cell components, a centrally symmetric electric
field with a negative potential in the cell centre would have to exist. One of
a number of alternative models of electric field generation is shown in Fig. 1.
It assumes that positive
|
Fig.1. Model of generation of an electric field in the cell interior and
of an isoelectric focusing of a protein, pH 6.8.
ions are pumped into cisterns of the endoplasmic reticulum, from which
the nuclear envelope is formed and whose lumen is known to communicate through
transport vesicles or through channels with the extracellular space
(Franke,1974).
The model
does not take into consideration the influence of cytoskeleton and organelles
such as lysosomes, mitochondria and microbodies. An interior of these
organelles has often different pH from the rest of the cell, suggesting that
they are electrically isolated from the cytosol. Such structures, of course,
could highly influence on the geometry of the field in the real livin cell.
Also the
cytoskeleton could play a big role in the real cell. Many cells, especially
animal cells, show movements due to the activity of the cytoskeleton. It could
be possible that the cytoskeleton keeps structures containing ion pumps in
place in the cell interior so that the movements would not disturb the
gradients too much.
The maximal
strength of the field could be estimated using the published experimental data
on S. cerevis;ae metabolism. To
maintain a steady state, as required for efficient isoelectric focusing, a
constant power would have to be invested to compensate for the electric current
(. between electrodes. This power ( T can be expressed as
W = UI
where U is the difference of potentials between electrodes. From Ohm's
law we obtain
W =U2/R (1)
where R is the resistance of the electrophoretic chamber. The
resistance of a thin spherical layer of electrolyte in a spherical
electrophoretic chamber with two concentric spherical electrodes (a highly
simplified and idealised model of the S. cerevisiae
cell) can be expressed as
dR = (r dX/(4pXz) (2)
where r is the resistivity of the electrolyte in a steady state of
isoelectric focusing and X is the radius of the infinitesimally thin spherical
layer. The total resistance of the electrolyte between electrodes (R) can be
calculated as an integral
ò B r/(4 pX2) dX
A
hence
R=(r (1/B-1/A))/ 4 p (3)
where A and B are the radii of the outer and inner electrode,
respectively. During isoelectric focusing, all electrically charged particles
migrate toward the electrodes, which results in a continual increase of
resistivity of the electrolyte. Finally, when only H+ and OH are left to
transfer the electric current, the resistivity increases up to the value of
pure water; for an electrolyte of pH near 7 this is about 1.8 x 10E7 W/cm (Svensson, 1962). For the S. cerevisiae
cell, we can estimate the radius of the outer and inner electrode as 3.1 x 10-4
cm and 0.62 x 10-4 cm,
respectively (Slavik and Kotyk, 1984). Substituting these values into Eqn. (3),
we find that the resistance of the interior of the S. cerevisiae cell is about 1.85 x 1010 W. The maximum power which S. cerevisiae
can invest into isoelectric focusing is 4.4 x 10-12 J/s, the power
which the yeast spends on unidentified functions different from the known
metabolic processes (Lagunas,1976). From Eqn. (1) we obtain that this power is
sufficient to maintain an intracellular difference of electric potentials equal
to about 0.29 V, which represents an electric field of about 1.5 kV/cm.
This
electric field strength seems to be rather low in comparison with the strength
of electric fields used for separation of proteins in laboratory devices for
isoelectric focusing. The question arises, how much and how quickly could the
cellular proteins be focussed in this field. The efficiency of isoelectric
focusing in directly proportional to two parameters, namely electric field
strength and the value of the pH gradient. The former is more than three orders
of magnitude higher in man-made apparatus for isoelectric focusing; the latter
(3200 pH/cm), however, is nearly four orders of magnitude higher in the living
S. cerevisiae cell. Also the distance
which the proteins are expected to migrate (< 2.5 x 10-4 cm) is
about five orders of magnitude less in the cell. Therefore, an electric field
strength of 1.5 kV/cm would be more than sufficient for effective isoelectric
focusing of intracellular components and their redistribution would be
accomplished within seconds.
3. Evidence for existence of intracellular isoelectric focusing
Although the existence of intracellular isoelectric focusing has not
been proved experimentally, the actual existence of this phenomenon can be
inferred from the following facts:
(1) An
intracytosolic pH gradient has been shown to exist in different cells (Slavik,1983;
Slavik and Kotyk, 1984; Tsien and Poenie, 1986; Ross and Slavik, 1987; Paradiso
et al., 1987). The simplest mechanism whereby a cell could set up such a
gradient is to generate an electric field between the centre and the periphery
by some sort of electrogenic transport. The electric field than gives rise to a
natural pH gradient (Svennson, 1961) and this, in turn, should lead to
isoelectric focusing of ampholytes.
(2)
Proteins labeled with fluorescent dyes injected into a cell often form distinct
spherical zones in the cytosol (Wehland and Weber, 1980; Wodsworth and
Sloboda, 1983; Glacy, 1983). Some results even suggest that the shapes of these
zones are spherical layers (Wehland and Weber, 1980), which agrees with
predictions based on the model of intracellular isoelectric focusing.
(3) The
hypothesis of intracellular isoelectric focusing is strongly supported by the
results of 31P nuclear magnetic resonance studies (NMR). When
cytosolic pH was estimated by NMR using inorganic phosphate and intermediates
of glycolysis, values of pH 7.2 and 7.0 were obtained, respectively (Navon et
al., 1979). This difference could be explained by different molecules being
focused into different regions of the cytosol; the region of maximal
accumulation of glycolytic intermediates probably coincides with the region of
maximal occurrence of glycolytic enzymes.
A pH
gradient has been demonstrated in S. cerevisiae
cytosol using a pH-specific fluorescent probe (Slavik and Kotyk, 1984). In contrast,
the sharp resonance peaks of most intracellular pH-sensitive molecules obtained
with NMR studies would suggest that one distinct pH value rather than a pH
continuum exists in the cytosol of the S. cerevisiae
cell (Salhany et al., 1975; Navon et al., 1979; Barton et al., 1980). This
discrepancy can be explained if the presence of intracellular isoelectric
focusing is taken into consideration. The molecule which is used for monitoring
pH is not homogeneously distributed throughout the cytosolic compartment but is
concentrated, according to its pI or its electric charge, in a distinct region
of the cytosol, displaying the pH of that particular region rather than the
average pH of the cytosol. It is worth mentioning that the resonance peak of
highly diffusible (and, consequently, poorly electrofocusable) ions of
inorganic phosphate is far broader than expected from theory and than observed
for other 31P-containing molecules (Busby et al., 1970; Busby et
al., 1978; Roberts and Jardetzky, 1981). This phenomenon, suggesting the
existence of an intracytosolic pH gradient, can be detected in the intact cell
only, not in a cell homogenate.
(4) On the basis of the
structure of the genetic code, the properties of amino acids, and the character
of the process of mutagenesis, a model describing the evolution of proteins has
been constructed (Graur, 1986). The model shows that in the absence of strong
selection constraints the pIs of proteins should converge toward mildly basic
values. The large diversity in pIs among real proteins suggests that this
parameter has its biological meaning and that it is controlled by natural
selection. Experimental evidence supports the same conclusion. Studies with
proteins injected into living cells have shown that a parameter controlling
the entry of a protein into a nucleus is its pI (Kreis and Birchmeier,1982). A
similar study has shown that a strong correlation also exists between the pI of
a protein and the rate of its degradation in vivo (Dice and Goldberg, 1975).
The process of intracellular isoelectric focusing could easily be the missing
link between the physical constant, i.e. pI, and the biological properties of
the protein.
(5) There is a growing
body of evidence suggesting that the cytosol of a living cell exists in a
highly organized state. Different cytosolic molecules are separated into
distinct regions of the cell rather than homogeneously distributed throughout
the cytosol. The rates of diffusion of proteins, but not of polysaccharides of
the same molecular weight, are much lower in the cytosol of living cells than
in a water solution of the same viscosity. Enzymatic-reaction rates are often
different in cell homogenates than in living cells. For a review of this topic
see Bhargava (1985) and Kaprelyants (1988).
4. Possible significance of intracellular iaoelectric f ocusing f or
cell physiology
Data suggest that a cell could generate an electric field of the
strength of 1.5 kV/cm, which appears sufficient for efficient isoelectric
focusing of intracellular ampholytes. This section shows that existence of
this process would be advantageous from the point of view of cell physiology.
In a biochemist's test tube, the molar concentrations of enzymes are usually
much lower than the concentrations of substrates, so the reactions follow a
pseudo-first-order reaction kinetics. By contrast, the concentrations of
enzymes and substrates in a living cell are often nearly identical
(Lehninger,1978). Under such conditions the reaction follows the second-order
reaction kinetics and the rate of diffusion of the reactants, rather than
turnover number of the enzyme, would be the factor limiting the reaction rate.
A process which could overcome this limitation would highly improve the
efficiency of intracellular enzymatic reactions. Intracellular isoelectric
focusing could be such a process. Of course, this would require a spatial
coincidence of enzymes and corresponding substrates. While electrofocusing of
enzymes is very likely, this is not the case with the low molecular weight,
highly diffusible substrates, mostly lacking ampholytic character (Svensson,
1962). The results of Bernhard (1988), however, show that once trapped by the
first enzyme of a particular biochemical pathway, the substrate seldom leaves
the molecule of the enzyme to diffuse freely to the second enzyme of the
enzymatic cascade. Substrates are rather transported between enzymes, being
bound on their surfaces, via enzyme-enzyme collisions (Srivastava and Bernhard,
1985; Weber and Bernhard, 1982). In such a way, the focusing of enzymes would
be sufficient zor an enhancement of the rate of biochemical processes.
Electrofocusing
of enzymes could not only speed up biochemical processes: it also offers a
powerful tool for the regulation of cell metabolism. A cell could avoid futile
cycles simply by focusing enzymes of different biochemical pathways into
different parts of its interior. Furthermore, phosphorylation,
dephosphorylation, glycosylation, or other modifications that could change an
enzyme's pI would automatically result in its translocation into a new cell
region. This could switch particular biochemical processes on or off. In this
case both reactants, i.e. the regulating enzyme and the regulated enzyme, are
ampholytes and so they could be electrofocused into the same part of the cell.
Theoretically, the substrate specificity of the regulating enzyme could be
based on the very fact that both enzymes share the same pI value.
Isoelectric
focusing could also participate in processes of intracellular molecular transport.
It has been estimated (Whetley,1985) that the time required for an average
protein molecule to move across the interior of a HeLa cell by a simple
diffusion would be about 26 or 27 min. Proteins introduced into a cell by
microinjection are, however, seen to spread through the cell within seconds
(Stacey and Allfrey, 1977). Similar velocities (0.1- 2.0 mm/ s) could be expected for proteins electromigrating in an electric
field of 90 mV/cm. Electrophoretically driven transport has been demonstrated
in many biological systems (Jaffe, 19fi6; Jaffe et al., 1974; Woodruff and
Telfer,1974; Jaffe and Woodruff,1979; Woodruff and Telfer, 1980; Cooper et
al., 1989). Intracellular isoelectric focusing appears to offer a more
versatile tool for assembling sophisticated material-transporting systems than
zone electrophoresis. While the latter is just capable of separating intracellular
particles into two regions and the values of the electric charges of the
particles merely influence the migration rates, isoelectric focusing could
sort the particles into a number of distinct cell regions, thus establishing a
finely tune-up distribution of proteins and organelles. For the transport of a
molecule from one cell region to another by isoelectric focusing, only one
substrate-specific step, i.e. a modification leading to a change of pI of the
transported molecule, is necessary. The following step, translocation of the
molecule, could be performed by the substrate-non-specific mechanism of
intracellular isoelectric focusing.
In the preceding
paragraphs, intracellular isoelecric focusing of macromolecules, namely
proteins, has been considered. There is no reason, however, to exclude higher
structures, e.g. subcellular particles and organelles, from these
considerations. Because of their low diffusion coefficients, the transport or
stabilisation of these structures in particular cell regions could be very
efficiently controlled by isoelectric focusing (Vesterberg and Svensson,
196fi). Considering that proteins of different pI values could be inserted
into different parts of organelle membranes, one might propose that the shape,
orientation, and spatial distribution of intracellular membrane structures
could all be controlled by the process of intracellular isoelectric focusing.
5. Concluding remarks
Processes
analogous to isoelectric focusing have been proposed to participate in the spatial
arrangement of intracellular components. The presumed processes have been shown
to fall within the range of the energetic capacity of the cell. Some possible
physiological functions of intracellular isoelectric focusing have been
discussed and some experimental data suggesting its existence have been
reviewed.
Intracellular
isoelectric focusing could play important roles in many different
intracellular processes connected with
compartmentalisation of the cell interior, transport of material, or
transmission of physiological signals. Such processes could be especially
important in a large cell. In nature two distinct types of cell architecture
exist - the small prokaryotic cell of bacteria and generally about three
orders of magnitude larger eukaryotic cell of other organisms. The presence of
endosymbiotically originated organelles, mitochondria and plastids, is often
considered a principal difference between the two types of cells. The
discrepancy between monophyletical origin of the eukaryotic cell and probably
polyphyletical origin of its endosymbionts, however, suggests a possible
existence of a more fundamental difference. Such a difference could
theoretically be the presence of intracellular isoelectric focusing in the preeukaryotic
cell and its absence in the prokaryotic one. This mechanism could enable the
functioning of large cells; the large size is a necessary precondition for
endosymbiosis. For this reason, it could be speculated that the origin of the
eukaryotic cell was associated with the evolutionary emergence on the life
scene of the mechanism of intracellular isoelectric focusing.
Acknowledgements
I am grateful
for the helpful comments of several colleagues, especially Dr. Jiri Cerkasov
and Dr. Apolena Cerkasovova, Charles University. Prague, and an anonymous referee
for the suggestion concerning the possible role of the cytoskeleton in
intracellular isoelectric focusing.
Corrigendum
to „Does a cell perform isoelectric focusing?“[BioSystems 24 (1990) 127]
Jaroslav
Flegr
The
Author regrets that there was a serious numeric error in abowe paper. The
correct value for a resistance of S. cerevisiae interior is 1.85 10E10 , i.e. approximately in eight orders of
magnitude higher then originally claimed. If the correct value is substituted
into Eq. 1, we find that S. cerevisiae
cell can maintain an intracellular difference of electric potential equal to
about 0.29 V which represents an electric field of about 1.15 kV/cm. The
correct value suggests that the cell can achieve a highly effective isoelectric
focusing of intracellular proteins and organelles by using less then 1% of its
energy reserves.
The author thanks to Dr
Stephen Bolsover of University College London for finding the error.
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