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Stucki, Department of Pharmacology, University of Bern, Friedbu¨hlstrasse 49, CH-3010 Bern, Switzerland Fax: +41 31 632 4992 Tel: +41 31 632 3281 E-mail: joerg.stucki@pki.unibe.ch Websit

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What is optimized at steady state?

Jo¨rg W Stucki and Robert Urbanczik

Department of Pharmacology, University of Bern, Switzerland

Mitochondria are generally regarded as the

power-house of the cell having the main task of supplying

energy in the form of ATP produced during oxidative

phosphorylation from ADP and Pi Furthermore, it is

well known that mitochondria take up Ca2+ ions in

an energy-dependent manner Other important

reac-tions are the Krebs cycle, oxidation of fatty acids and

the urea cycle [1,2] One may ask, which of these

reac-tions are optimized and play the most important role?

There are probably no dominant tasks in liver

mito-chondria and we are therefore faced with multiple

optimizations, depending on the cellular demands

Mitochondria from liver and kidney contain

pyru-vate carboxylase and are actively involved in

gluconeo-genesis [3] The aim of this study was to discover the

importance of this first step in gluconeogenenesis, and

special conditions were therefore chosen to allow us to study the carboxylation of pyruvate, the Krebs cycle and ketone body production by ignoring the many other reactions also present in these organelles In this sense, the model and experiments of mitochondrial pyruvate metabolism are biased and do not consider the typical intracellular environment of hepatocytes Genomics has led to construction of the stoichio-metry matrices of several simple organisms such as Escherichia coli and Saccharomyces cerevisiae Apply-ing linear programmApply-ing methods, researchers have analysed the optimizations of different goals, the most prominent being the maximization of cellular growth [4–7] It goes without saying that this cannot be the major task of liver mitochondria Therefore, we inves-tigated the optimization of metabolic functions In

Keywords

dominant reactions; mitochondria;

optimization of metabolism; pyruvate

metabolism; stoichiometric network analysis

Correspondence

J W Stucki, Department of Pharmacology,

University of Bern, Friedbu¨hlstrasse 49,

CH-3010 Bern, Switzerland

Fax: +41 31 632 4992

Tel: +41 31 632 3281

E-mail: joerg.stucki@pki.unibe.ch

Website: http://www.cx.unibe.ch/pki/

index.html

(Received 17 August 2005, revised 28

September 2005, accepted 4 October 2005)

doi:10.1111/j.1742-4658.2005.05005.x

A representative model of mitochondrial pyruvate metabolism was broken down into its extremal independent currents and compared with experimen-tal data obtained from liver mitochondria incubated with pyruvate as a substrate but in the absence of added adenosine diphosphate Assuming no regulation of enzymatic activities, the free-flow prediction for the output of the model shows large discrepancies with the experimental data To study the objective of the incubated mitochondria, we calculate the conversion cone of the model, which describes the possible input⁄ output behaviour of the network We demonstrate the consistency of the experimental data with the model because all measured data are within this cone Because they are close to the boundary of the cone, we deduce that pyruvate is converted very efficiently (93%) to produce the measured extramitochondrial metabolites We find that the main function of the incubated mitochondria

is the production of malate and citrate, supporting the anaplerotic path-ways in the cytosol, notably gluconeogenesis and fatty acid synthesis Finally, we show that the major flow through the enzymatic steps of the mitochondrial pyruvate metabolism can be reliably predicted based on the stoichiometric model plus the measured extramitochondrial products A major advantage of this method is that neither kinetic simulations nor radioactive tracers are needed

Abbreviations

ACAC, acetoacetate; AcCoA, acetyl-CoA; AKG, 2-oxoglutarate; BOB, 3-OH-butyrate; CIT, citrate; FUM, fumarate; ICI, isocitrate; MAL, malate; OAA, oxaloacetate; SucCoA, succinyl-CoA; SUC, succinate.

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previous studies we analysed the efficiency of oxidative

phosphorylation and found different degrees of

coup-ling [8], which could be regulated by the metabolic

states of the liver, for example, feeding and starvation

[9]

In this study, we investigated whether the first step

of gluconeogenesis may also be a possible target for

optimization Finally, we wanted to see whether any

reasonable predictions about the behaviour of the

sys-tem could be made from knowledge of the

stoichio-metry matrix alone without any experimental data or

additional assumptions in what we called the free-flow

system

Experimental data and computational

procedures

Our experimental data were taken from a previous

publication in which computer-simulated fluxes were

compared with experimentally measured values [10] These procedures are not repeated here because an exhaustive description already exists Suffice it to men-tion that sodium [2-14C] pyruvate was used as a sub-strate, and allowed measurement of the pertinent metabolic flows in incubated mitochondria from rat liver The model investigated was somewhat simplified

by omitting activation of the pyruvate carboxylase by acetyl-CoA and its inhibition by ADP in order to get

an idea of the general properties of the unconstrained free-flow system and compare it with incubated mito-chondria The remaining reactions considered are listed

in Table 1 From these reactions the stoichiometry matrix was set up and the extremal currents were cal-culated using the mathematica program [11] Note that this program can deal directly only with irrevers-ible reactions and yields all extremal currents as defined by Clarke [12] It is based on the Nullspace approach and it is, in fact, an early version of a

Table 1 Major reactions involved in mitochondrial pyruvate metabolism rat liver The reactions are taken from a previously published model [10] and simplified as described in the text In addition to the numbering scheme the reactions and the enzymes catalysing them are listed together with their corresponding EC numbers The extramitochondrial pool is indicated by curly brackets.

2 Pyruvate + CoASH + NAD + fi Acetyl-CoA + NADH + H + + CO2 Pyruvate dehydrogenase 1.2.4.1

hydrolase

2.3.1.9 3.1.2.11

4 Acetoacetate + NADH + H + fi 3 -OH-Butyrate + NAD + 3-Hydroxybutyrate dehydrogenase 1.1.1.30.

5 3 -OH-Butyrate + NAD + fi Acetoacetate + NADH + H + 3-Hydroxybutyrate dehydrogenase 1.1.1.30.

10 Isocitrate + NAD + fi 2 -Oxoglutarate + NADH + H + + CO2 Isocitrate dehydrogenase 1.1.1.41.

11 2 -Oxoglutarate + NAD + + CoASH fi Succinyl-CoA + NADH + H + + CO2 Oxoglutarate dehydrogenase 1.2.4.2.

16 Malate + NAD+fi Oxaloacetate + NADH + H +

18 3 ADP + 3 P i + NADH + H + + 1 ⁄ 2 O 2 fi 3 ATP + NAD + + H 2 O Oxidative phosphorylation

19 2 ADP + 2 P i + FADH 2 + 1 ⁄ 2 O 2 fi 2 ATP + FAD + H 2 O Oxidative phosphorylation

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program by Urbanczik and Wagner [13] that handles

reversible reactions without splitting them into two

irreversible ones

Elementary flux modes [14], by contrast to extremal

currents, are able to deal with both reversible and

irre-versible reactions The extremal currents represent the

full solution of the system, whereas elementary flux

modes are generally a subset of them Only when all

reactions are irreversible, are the elementary flux

modes identical to the extremal currents, otherwise

they are a projection from the extremal current

poly-tope into a polypoly-tope with a lower dimension Because

a proper transformation operator exists [13], one can

switch from one representation to the other without

losing information

In order to arrive at a consistent presentation,

we use the same abbreviations for the metabolites

throughout

The free-flow system

As a first step we wanted to get a general idea about

mitochondrial pyruvate metabolism without any

experimental information, and to verify what

conclu-sions could be drawn at that stage Table 1 lists the

reactions we considered for pyruvate metabolism in

isolated mitochondria from rat liver Several reactions

were omitted for clarity First, the regulation of

pyru-vate carboxylase by acetyl-CoA and ADP is ignored

Second, different exchangers such as the citrate–malate

antiporter and the malate–oxoglutarate exchanger were

also omitted The main reason for this was not only to

simplify the model, but also because

extramitochond-rial counter ions were not added to the incubation

medium in the experiment, with the exception of Pi

Hence, all metabolites leaving the mitochondria do so

by simple efflux The same applies to pyruvate uptake,

because its exact mechanism remains unclear The

advantage of this procedure is that it provides

infor-mation about the unconstrained flows possible in this

scheme In other words, this simplified model furnishes

an idea about the general behaviour of the model

Fur-thermore, the metabolites Pi, O2, H2O and CO2 were

treated as external molecules in large excess and thus

as being essentially constant Because we are not

inter-ested in tracking these four metabolites they were

ignored in the stoichiometry matrix

For the intramitochondrial reactions in Table 1, the

corresponding stoichiometry matrix was set up (not

shown) This matrix was then further processed to find

all extremal currents by using the program

mathemat-ica The resulting matrix of the extremal currents is

shown in Fig 1 The 30 reactions listed in Table 1

produced 37 extremal currents all fulfilling the steady-state condition Note that the algorithm used is based

on the Nullspace approach, which eliminates all inde-pendent species automatically Therefore conservation conditions like NADH + NAD+¼ constant could be ignored The same goes for the free and bound CoA The matrix in Fig 1 shows all 37 extremal currents possible for the reactions listed in Table 1 Column 1 shows the entry of pyruvate and the last nine columns represent the different outputs of the produced meta-bolites (reactions 22–30 in Table 1) Four of these extremal currents produce no output because they rep-resent reversible reactions For example, row 3 stands for the reversible reaction of the fumarase and row 5 represents the reversible conversion of citrate to iso-citrate Furthermore, row 2 represents the Krebs cycle, which generates no output except CO2 and H2O but consumes pyruvate and dissipates ATP in reaction 21 Because, as mentioned above we are ignoring CO2,

H2O and Pi, in our notation the Krebs cycle appears

as simply consuming pyruvate but generating no out-put

The numbers in Fig 1 are not easy to visualize They could, for example, be drawn as reaction dia-grams, as done previously [12,15] Here, by simply adding the numbers in each column of the extremal current matrix, we obtain the free-flow diagram shown

in Fig 2 This gives a general graphical picture of the mutual interconnections of the flows

Of course, assigning an equal weight of unity to every extremal current is of questionable physiological meaning However, in the absence of experimental data determining the true weights, constructing the free-flow system may still be the best thing one can do

The incubated mitochondria

How does the free-flow system compare with incuba-ted rat liver mitochondria? To this end, we used the experimental results from a previous publication in which mitochondria were incubated with 2-[14 C]-pyru-vate [10] This allowed measurement of all intramito-chondrial fluxes including the citric acid cycle and ketone body production The measurements of the extramitochondrial metabolites are given in Table 2 and are compared in Fig 3 together with the free flow data

Obviously, there is a discrepancy between the two data sets Notably, in the free-flow system there is a large production of oxaloacetate, whereas none was found in the incubation The same goes for isocitrate Furthermore, there is a large difference in the cit-rate produced during incubation compared with the

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free-flow system This emphasizes the need for the

experimental data to get closer to the realistic

beha-viour of mitochondrial pyruvate metabolism

The conversion cone

When describing the metabolic model by the cone of extremal currents, flows through the internal reactions play an important role However, the experimental results in Table 2 provide information about the flows through the extramitochondrial exchange reaction of the network only Hence, in analysing the model, we consider only conversions between the external metab-olites, in effect treating the mitochondria as a black box input⁄ output system

Obtaining a description of the possible input⁄ output behaviour is straightforward We delete the columns (2–21) in the current matrix that correspond to the internal reactions Then, as a matter of convention, we invert the sign of the first column, as this represents an input exchange The projected current matrix thus obtained, which we call P is shown in Table 3 For instance, from the first row of the current matrix we obtain the first row of P as ()16 0 0 0 0 0 0 0 0 15), showing that 16 PYRfi 15 OAA is one of the

R

I C I

G A

A o C c S C S M U

F

L

A

M

A

6

0

0 9

8

4

8 5

0

9

3

1

1

6

0 3

0

8

Fig 2 Free, unconstrained flows at steady state This diagram was

constructed by using the information contained in the extremal

cur-rents matrix in Fig 1 (see text).

Fig 1 Extremal currents for the reactions listed in Table 1 These were calculated using the MATHEMATICA program [11] Because the 30 col-umns of this matrix correspond exactly to the numbering scheme used in Table 1 (from left to right) the last nine colcol-umns correspond to the metabolites leaving the mitochondria Similarly column 1 represents pyruvate uptake Note that of the 37 extremal currents, 5 produce

no output measured in the experiment (see text).

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conversions between the external metabolites that the

network can perform

Each row of P, the projected current matrix, thus

describes an allowed input⁄ output behaviour, and

indeed any possible input⁄ output behaviour is

obtained as a linear combination (with non-negative

scalar coefficients) of these 37 rows of P Such linear

combinations generate a convex cone, which we call the conversion cone C Unfortunately, although the conversion cone is obtained from P, this method of describing C is too complicated It would be simpler if

we just knew the edges of the cone C or, alternatively,

if we had a description of C by a set of linear inequal-ities, i.e a list of m vectors h(i)such that a point c is in

C if and only if

hðiÞc 0 for i ¼ 1; ; m ð1Þ For example the experimentally observed conversions

in Table 2 has

c¼ ð20:88;0:97;0:57;4:56;0:01;0:20;0:15;0:91;5:08;0:01Þ: The mathematical techniques used to obtain the edges

of the conversion cone C as well as the h(i) from the projected extremal current matrix P have been des-cribed elsewhere [16] Here, we state the results It turned out, as shown in Table 3, that of the 37 rows in

P only 28 are actually edges of C

The h(i) yielding the inequalities representation of C, Eqn (1) are given by the rows of the following matrix H:

H ¼

PYR ACAC BOB CIT ICI AKG SUC FUM MAL OAA

1 2 2 2 2 2 2 1 1 1

15 24 27 28 28 25 21 19 19 16

0 B B B B B B B B B B B

1 C C C C C C C C C C C

It is worth noting that the first nine rows of H state the obvious fact that all metabolites except pyruvate can only be produced but never consumed by the network Only the last two rows of H give nontrivial constraints on the allowed input⁄ output behaviour Using the matrix H makes it very easy to determine whether a given 10-dimensional point c lies in the con-version cone We just test if Hc ‡ 0 One easily verifies that the experimental result in Table 2 passes this test Hence, the experimental data lie within the conversion cone, thus demonstrating the consistency of our meta-bolic model However, although the experimentally observed conversion is in the interior of C, it actually lies quite close to the boundary of the conversion cone This can be illustrated by replacing the measured value

of 20.88 lmoles for the consumption of pyruvate in Table 2 by a variable uptake x while keeping the out-put metabolites at the measured values, i.e choosing

Table 2 Experimentally measured metabolites in the

extramitoch-ondrial medium Mitochondria from rat liver (18 mg mitochextramitoch-ondrial

protein) were incubated with pyruvate-2-[14C] and concentrations

were measured after incubation at 37 C for 10 min [10] The

pyru-vate used was calculated from the pyrupyru-vate added to the medium

at the beginning and that found after 10 min of incubation.

Extramitochondrial (used or found) lmol (10 min)

Fig 3 Comparison of extramitochondrial metabolites in incubated

mitochondria and in the free-flow system The data in Fig 2 and

Table 2 were converted into percentage on the basis of the

pyru-vate entering the mitochondria and plotted together in a bar graph.

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c¼ ðx; 0:97; 0:57; 4:56; 0:01; 0:20; 0:15; 0:91; 5:08; 0:01Þ:

We may then ask, for which minimal value of x this

choice of c is still within the conversion cone This

minimal pyruvate uptake is found to be x¼

19.25 lmoles because for this choice the last inequality

in H holds as an equality whereas the other

inequalit-ies are still strictly satisfied The minimal value of

19.25 lmoles is near the observed value of

20.88 lmoles and therefore shows that the

mitochon-dria are using pyruvate close to optimally (93%) in producing the metabolites measured in the experiment The remaining 1.63 lmoles of pyruvate are used to dissipate energy, probably to regulate the degree of coupling of oxidative phosphorylation (see below)

As already mentioned, the inequality given by the last row h(11)of H is the first one to be violated when decreasing x from 20.88 lmoles Now, the equation

h(11)c¼ 0 defines a subset of the 10-dimensional con-version cone C, viz a nine-dimensional facet of the

Table 3 The P matrix with its edges defining the conversion cone C The P matrix is obtained from columns 1 and 22–30 from the current matrix as explained in the text This matrix was then further processed as described previously [16] to find the edges of the conversion cone

C generated by its rows The 28 rows, which are edges, are marked with a + in the right column For example, 2 PYR fi FUM is not an edge because a multiple of this conversion is obtained as a linear combination with positive scalar coefficients from 19 PYR fi 15 FUM and PYR fi 0.

PYR ACAC BOB CIT ICI AKG SUC FUM MAL OAA

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conversion cone This situation is shown schematically

in Fig 4

Because this facet is the one closest to the

experimen-tal results we shall further pinpoint the location of the

observed conversion by computing its angles to the 21

edges of the facet The angles a were calculated

accord-ing to the standard formula from vector algebra

a b¼ jj a jj jj b jj cos a ð2Þ where a are vectors from the P matrix belonging to the

facet and b is the vector of the experimental data In

Table 4 we list the angles thus obtained and we also

show the angles between the free flow conversions and

the 21 edges A perusal of the angles of the free flow

system show that they are more or less uniformly

spread between 22 and 33 degrees and that none is

close to an edge This means, that there is no reaction

really dominating in this system, and all occur with

more or less the same probability By contrast, in

incu-bated mitochondria one conversion is 10 degrees closer

to one edge and the farthest edge is 46 degrees away

This means that the transformation number 1, two

citrates and one malate formed from five pyruvates,

dominates all other reactions, because it is closest to

the experiment This is also in accordance with the

data shown in Table 2 in which malate and citrate are

the main products This does not mean, however, that

no other conversions contribute to these metabolites,

as is evident from Table 4 in which these products

occur in different conversions

Predicting internal flows from extramitochondrial measurements

Given that the experimental findings for the extra-mitochondrial flows are consistent with our model, it

is interesting to ask in how many ways the model can reproduce these findings To this end, we modified the reaction system in Table 1, removing the 10 exchange

Table 4 Angles between edges and conversions in the facet for the free flow system as well as for the incubated mitochondria The calculation of the angles (in degrees) is described in the text.

Experiment

Free Flow

Fig 4 Schematic sketch of the conversion cone C in three

dimen-sions The vector lying squarely in the interior of the cone is

analog-ous to the conversion given by the free-flow system The second

vector that is close to the boundary of the cone lying nearly on the

front left facet corresponds to the experimental result In contrast

to this three-dimensional sketch in reality the nine-dimensional

facet is delimited by 21 of the 28 edges of the conversion cone.

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reactions for the external metabolites and replacing

them with the single pseudoreaction

0:97 ACACþ 0:2 AKG þ 0:57 BOB þ 4:56 CIT

þ 0:91 FUM þ 0:01 ICI þ 5:08 MAL þ 0:01 OAA

þ 0:15 SUC ! 20:88 PYR

Note, that this pseudoreaction is the experimentally

observed conversion (Table 2) with the roles of input

and output interchanged A study of this modified

network reveals that it has only five extremal currents

The first four are the futile cycles observed in the

ori-ginal model and only the fifth extremal current has a

nonzero flow through the above pseudoreaction But

because all other extremal currents of the modified

model are futile cycles that, based on thermodynamic

considerations, cannot run in a steady state, the fifth

extremal current is the only way by which the model

can explain the behaviour observed in the experiment

It is surprising that only one extremal current dictates

the behaviour of the system The flows for some

reac-tions were measured previously [10], and the measured

values are compared with the prediction from our

model in Fig 5 This shows that the extremal current

reliably describes the major flows

Furthermore, in the extremal current reaction 21 the

‘ATPase’ dissipates 158.7 nmoles ATPÆmin)1Æmg

mito-chondrial protein)1 (not shown in Fig 5) As

men-tioned above, the utilization of 19.25 lmoles of

pyruvate exactly fulfils inequality h(11), i.e the point c

lies precisely on the facet Taking this limiting value of

pyruvate utilization instead of the measured one

sur-prisingly shows that the ‘ATPase’ vanishes completely,

and no ATP is then dissipated So at this limiting

point there can no longer be any flow through the

complete Krebs cycle Hence, in the experiment the

excess 1.63 lmoles are destroyed by the Krebs cycle

One might, therefore, speculate about the physiological

role of these 1.63 lmoles of pyruvate leading to the

observed dissipation of ATP

In a previous study [8], we investigated the optimal

degrees of coupling q of oxidative phosphorylation

and found that in all cases q must be smaller than 1

In other words, full coupling (q¼ 1) was incompatible

with optimal efficiency at finite speed of oxidative

phosphorylation In these experiments an external load

utilizing ATP was present; this is not the case here

Furthermore, the efficiency of oxidative

phosphoryla-tion was defined as output power divided by input

power, calculated from the input and output reactions

of the mitochondria treated as a black box These

ingredients are absent in our experiment, but can we

still say something about the efficiency and the degree

of coupling of oxidative phosphorylation in the present system?

Such estimation requires some assumptions First,

we have to assume that oxidative phosphorylation is working at optimal efficiency, i.e that conductance matching is fulfilled [8] Second, we need to estimate the efficiency of oxidative phosphorylation as the ratio

of ATP utilized (reaction 7) divided by ATP produced The latter quantity can be obtained by adding the flows through reactions 7 plus 21, because these are the only ones consuming ATP which first must have been produced Taking the limiting value of 19.25 lmoles pyruvate used yields an efficiency of 1 and a degree of coupling q¼ 1 In other words, oxida-tive phosphorylation is fully coupled under these circumstances, which is incompatible with optimal effi-ciency

By contrast, doing the same calculation for the measured pyruvate utilization in the experiment yields

an efficiency of oxidative phosphorylation of 0.30 and

PYR AcCoA ACAC BOB

AKG

SUC FUM

MAL

(63.2) 62.2

(67.2) 68.1

(47.5) 42.9

(19.5) 14.4

(18.5) 13,2

(15.7) 19.2

(3.7) 3.5

(17.6) 12.2 (11.4)

6.5

(19.7) 25.1

Fig 5 Predicted and measured flows through some of the reac-tions The numbers in brackets are the measured flows (in nmolÆmin-1Æmg protein-1) taken from Stucki and Walter [10] In addition to these, the predictions of the extremal current analysis described in the text are given The extremal current was normal-ized to obtain the experimentally determined pyruvate uptake One

of the key junctions in the pathway is given by the flow of oxalo-acetate either directly to malate or, alternatively, into the Krebs cycle via citrate The predicted flow from oxaloacetate to citrate deviates from the measured value by 10% In absolute terms this relative error corresponds to some 5 units, and this absolute differ-ence must stay essentially the same throughout the Krebs cycle because the outflows are predetermined But this constant abso-lute error leads to increasingly large relative errors in the down-stream part of the Krebs cycle since the magnitude of the flows in the cycle decreases due to the outflows of the intermediates.

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a degree of coupling of q¼ 0.849 This degree of

coupling is between the values of optimal power

out-put and optimal flow of ATP production in oxidative

phosphorylation [8] An independent check with the

data in Stucki and Walter [10] (Table 3), yields an

effi-ciency of 0.293 with a value of q¼ 0.838 These results

show that the theoretical predictions and the data

taken from the experiment yield very similar values

This indicates that 1.63 lmoles of pyruvate are used

for the regulation of the degree of coupling, provided

that the assumptions mentioned above are indeed

valid Note, that the ‘ATPase’ is not a clearly defined

chemical reactions because it contains slips and leaks

of oxidative phosphorylation as well as the breakdown

of intra- and extramitochondrial ATP by unknown

ATPases, Thus we are not able to identify a single

pro-cess that would be responsible for the regulation of the

degree of coupling

Concluding remarks

The main results of this study are: first, the

transfor-mation of five pyruvates into two citrates plus one

malate is the dominating reaction of the system; and

second, the conversion of pyruvate into its products is

nearly optimal with 93% efficiency Hence, only 7%

of pyruvate is used for the dissipation of ATP,

prob-ably to regulate the degree of coupling of oxidative

phosphorylation

Predicting the dominating reactions in a network

is difficult This study has shown that a free-flow

diagram, although yielding the correct factors for a

steady state, can say nothing about which reactions

are important and which are not, thus there is (yet)

no simple recipe of reducing an extremal currents

matrix to its essential parts It is the impression of

the authors that there exist only two reasonable

pro-cedures possible at present to solve this question:

(a) imposing or assuming external constraints or

(b) the measurement of metabolite turnover in vitro,

or better still in vivo, under different metabolic

conditions

To illustrate this difficulty, we consider the study by

Stelling et al [4] as an example Successful splitting of

a large metabolic network into its independent currents

or elementary modes usually yields too much

informa-tion Thus Klamt and Stelling found 507 632

element-ary flux modes in a stylised partial model of E coli

[17] and one might indeed ask how to proceed further

From a practical point of view, it is convenient to

con-centrate on the functional aspects only, as done here,

and restrict analysis to the input⁄ output relationship

Note that by constructing the conversion cone one

loses no information because all other, less interesting, details are contained in the current matrix

Assuming external constraints makes sense for autonomous organisms such as E coli or S cerevisiae One might then ask under what conditions there is maximal growth [4–7] or maximal production of eth-anol, for example This approach, however, fails com-pletely for organelles such as mitochondria, which are

an integral part of a cell in an organ such as the liver

As already mentioned, such biochemical entities are tightly integrated in a constantly changing cellular environment In other words, the major role of these organelles is to act as servants rather than as inde-pendent, autonomic entities Mitochondria not only have to produce ATP but they play also an essential part in anaplerotic functions Under certain circum-stances, in starved rats for example, it is reasonable that they can take part in glucose production by pro-ducing malate Malate contains not only the carbon moieties for glucose synthesis, but it also shuttles the reducing equivalents into the cytosol where it is needed for glucose synthesis [3]

In concluding, it is instructive to compare our approach for estimating intramitochondrial flows from experimental observations with the full dynamic mod-elling of the reaction system employed previously [10] Whereas the latter approach yields somewhat more accurate results, it is not only much more involved as

it requires more computer time for the simulations, but it also needs a more detailed knowledge of the reaction kinetics By contrast, our approach is straight-forward and quick, needing only a minimum of bench work, notably without the use of radioactive tracers

Acknowledgements

The Swiss National Science Foundation has supported this study It is a pleasure to thank Dr Clemens Wag-ner for helpful comments

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