In previous articles (Diederichs, [6,10]) a new phenomenological type of flux equation to describe not only membrane transport reactions but also enzyme-catalyzed reactions as they occur in the living cell, was introduced. The new formalism combines some characteristics known from enzyme-catalyzed reactions with energetic relations of NET. They are comparable to several other linear relationships between corresponding flows and forces such as electric current flow, heat flow, or diffusional flow. The main difference to these latter phenomenological laws and to NET is brought about by introducing a variable instead of a constant conductance into flux equations. Conductances may be varied by substrate and ion concentrations as is known from enzyme kinetics [11], leading to the following expression:

A (J/mol) denotes the affinity or driving force of a given reaction. It is defined as A = −dG/dξ (G = Gibbs free energy (J/mol), ξ = extent of reaction (mol)). A is not constant, but depends on the mass action quotient of variable nonequilibrium activities (≈concentrations). L(c₁,c₂,...) (μM/ms × mol/J) denotes the conductance of that reaction. It is treated here as a variable, which can be varied by concentrations of metabolites, cofactors, and inorganic ions like Ca²⁺ (c’s).

When applied to membrane transport reactions, flux J is given by

or

respectively. Both G’s denote conductances (in pS), Δμ̃ and Δμ (both in mV) are the electro-chemical and chemical potential differences, respectively, of the transported substance. α represents a conversion factor converting electric current I into flux J (see Section 3).

Equation (1a) and (1b) are based on the following relationship derived from the Second Law of Thermodynamics: entropy production per unit time and volume of an irreversible chemical or biochemical reaction of a system (‘i’) like the cytosolic compartment is related to the reaction’s affinity and velocity by

(T = absolute temperature (K), V = system volume (L), d_iS/dt = entropy produced during time interval dt). For T = const., an equivalent form of this equation is given by

Φ is the dissipation function per unit volume, it is given in units of power dissipated per unit volume. It is identical to the heat dissipated by the irreversible reaction per unit time and volume. Analogous to electrical power P = I × U and current I = L × U, the expression of flux J then is given by Equation (1a). This latter formulation, which is used throughout this paper, may be advantageous in view of its similarity to relations known from techniques such as electric circuits and heat flow. It should be noticed, however, that A is not identical to a conjugated force X, which according to Equation (2a) is defined by X = A/T.

In the following, the relationship to a Michaelis-Menten type reaction is shown. The flux through an enzyme-catalyzed reaction may be expressed as

(V_Enz^max = maximal reaction rate of an enzyme-catalyzed reaction; K_M = Michaelis-Menten (analogue) constant). For k = 1 Equation (3a) represents the well known Michaelis-Menten formula, and for k > 1, (3a) changes to Hill’s Equation [31]). Comparison of Equations (1a) and (3a) shows that the new formalism is obtained by replacing V_Enz^max of (3a) by L_Enz^max × A, yielding

with

The S (S = substrate or effector) containing term of Equation (3a) and (3b) represents a dimensionless activation/inhibiting factor, which can be regarded as a concentration-dependent probability, by which the maximal conductance L_Enz^max of an enzyme-catalyzed reaction may be reached. If several activating and/or inhibiting factors were involved with the catalytic process, then, according to probability calculus, these factors must appear as products in the respective flux Equation [6].

On the other hand, Equation (3a) can be regarded as a special case of flux equation derived from the more fundamental rate Equations (1a) or (3b). In Equation (3a) the variable term L_Enz^max × A of Equation (3b) is replaced by the constant V_Enz^max of (3a), which can be expressed as a product consisting of two constant factors L_Enz^max and A_const, respectively. In contrast to the variable affinity A, A_const does not depend on variables given by the mass action quotient. Subsequently, all flux equations of the Michaelis-Menten type and of NET can be regarded as special cases of the new flux equation given in Equation (1a). The former contain variable conductances, but constant affinities, whereas the opposite is true for equations of NET; these contain constant conductances, but variable affinities.

The great advantage of flux equations containing both variable conductances as well as variable affinities, is that they are remarkably well-suited for metabolic network modeling. So flux control by activating or inhibiting effectors is made possible as it is known from enzyme kinetics [11]. The inclusion of driving forces has the advantage that energetic parameters like power output or efficiency of coupled processes as they occur in metabolic pathways can be calculated.

As was shown in reference [6], the new formalism is applicable to reactions under “far from” as well as under “near” equilibrium conditions. Far from equilibrium, the flux equation is dominated by activation factors. This is brought about by the logarithmic nature of A, which remains fairly constant in large logarithmic arguments. Under these conditions, the flux equation approaches Michaelis-Menten kinetics [6] and, therefore may be suitable to describe far from equilibrium reactions, which is demonstrated by present simulations (most reactions are far from equilibrium). Theoretically, it is possible to reverse such an irreversible flux, but only at extreme substrate and/or product concentrations which do not occur in living cells.

Under near equilibrium conditions, the flux equation becomes dominated by A, because the logarithmic function then approaches zero. In this region the slope of this function becomes markedly increased. Under these conditions, the flux equation approaches the NET formalism. This approach is all the more complete, the more the K_M value of this reaction approaches zero.

In Figure 1 the behavior of flux equations is demonstrated for conditions of [Ca²⁺]_c induced forced oscillations (see Section 2.3.2). At high A’s (panels A and B), flux oscillations are brought about mainly by activation factors, whereas at near zero driving forces, flux oscillations follow the oscillations of respective A’s about zero. The Second Law of Thermodynamics demands that the reaction rate of a spontaneously proceeding reaction goes against zero continuously. The oscillations about zero (Figure 1) do not violate this law, because these oscillations of the driving force are forced by the oscillating sarcosolic/cytosolic ADP concentration ([ADP]_c).

To demonstrate the different behavior between pathway fluxes composed of constant and variable L’s respectively, a metabolic pathway composed of n in series enzyme-catalyzed reactions may be regarded. If, e.g., L_i is increased by a factor f at constant L’s, the pathway flux J expectedly would be increased by a factor f′ < f. Then, according to Ohm’s law, the fractional increase of J is equal to the fractional increases of all n − 1 affinities at the n − 1 remaining conductances. Only the fractional change of A_i at L_i (fractional increase of L_i is imposed and given by f − 1) must be different from all others. It is given by ΔA/A₀ = (ΔJ/J₀ − (f − 1))/f.

The above conditions of constant conductances are equivalent to a simple electric network, but are probably not compatible with a metabolic pathway. Since, under these latter conditions, variable enzyme activities determine conductances and thus might be responsible for a quite different behavior. The n − 1 fractional changes of affinities are not equal as is to be expected for constant conductances. This fact is associated with a remarkably different quality. Pathway fluxes containing variable conductances, after a given perturbation, can reach a new steady state much more rapidly than those having constant conductances. This is verified with a simple simulation (SIM_GLY, see App. A14, the maximal conductance of the first reaction step, L_GK^max, is increased by a factor f = 2.0). Under variable conditions a new steady state is reached already after 3.0 min (see Figure 2), whereas with constant L’s the new steady state develops only after 160 min (not shown).

In this context, it seems worth mentioning that Michaelis-Menten type formulations of pathway flux (const. A’s to yield L_Enz^max × A_const = V_Enz^max =const. ), under the same conditions are unable to produce a new steady state. Obviously, in addition to variable conductances, the inclusion of variable driving forces in pathway fluxes is indispensible for the toleration of non-infinitesimal changes of conductances as they occur in living cells, for instance during activation of glucose metabolism, to increase power output.

With the new formalism, however, it is possible to describe metabolic networks as was shown recently with the known phenomena of stimulus-secretion coupling of β-cells [6,10]. In simulations the increase of only one single parameter, the glucose concentration, is necessary and sufficient to induce β-cell activation, as is known from experiments.

In a metabolic pathway, which may be composed of a source and a sink and several in series enzyme-catalyzed reactions at steady state, the pathway flux can be expressed as

This follows from Φ = ∑J_iA_i, and at steady state Φ = J∑A_i = JA_ov. Furthermore, due to the similarity of the flux equation to Ohm’s law, in series conductances generate an equivalent conductance L_ov. A constant overall affinity of the pathway A_ov = ∑A_i is then determined by the constant concentrations of metabolites of the source and sink, respectively. So, it is possible to contract several in series reactions of a given reaction sequence to one single step. In cellular metabolism this principle is used for metabolic channeling [32,33], which is brought about by aggregating several different enzyme molecules of a sequence to one catalytic complex. Because respective intermediates do not appear in solution, this may cause an appreciable increase of the overall conductance of the catalytic complex.

Since chemical and electro-chemical potentials are potential functions, their line integral over a closed path must vanish, i.e., Kirchhoff’s loop rule is applicable also to metabolic networks [2]. Kirchhoff’s second rule, the junction rule, however is not always valid. For instance, the aldolase reaction splits the first part of GLY into two equal fluxes, which merge again to the second part of GLY. The flux of this latter pathway is not equal to that of the first part, as is to be expected for an electric network (conservation of charge), but is increased by a factor of two. If, however a given flux is split up into several parallel fluxes, the junction rule is obeyed [2]. In any case, the law of mass conservation has to be fulfilled.

This latter fact has to be taken into account, when A_ov and L_ov are to be determined. Equation (4) is applicable only if a constant flux of given magnitude through the entire pathway is realized. With regard to GLY this would mean that for instance the flux of the second part (J_Ga, A3) has to be transformed to yield the same magnitude as the flux of the first part. Since a given Φ can be expressed by any other reliable product of J and A, and consequently also by a product containing a J of desired magnitude, e.g., J_GK (which is a measure of glucose utilization), an altered affinity has to be determined in such a way that Φ remains unchanged. This transformed affinity is given by

and the associated transformed conductance by

Such transformed values have to be used, when the steady state pathway flux of a metabolic network containing one or several fluxes of different magnitude is to be determined. To develop a simulation of a metabolic network like coupled glucose oxidation, it is not necessary to know all parameters exactly. If glucose utilization and/or oxygen consumption are known from experiments, conductances can be adjusted for a maximal power output. Affinities of single reactions often are given or may be estimated from Gibbs energies of formation [Alb]. With known stoichiometric coefficients the simulation must yield correct results also with respect to thermodynamic constraints, even if the steepness of flux equations is not precisely met. This means that the use of adjusted constants like K_M values and other modeling parameters may suffice to fulfill reliability requirements.

In Metabolic Control Analysis (MCA) several dimensionless coefficients are defined, to quantify metabolic control at steady state [34]. One of these coefficients is the flux control coefficient C_Ex^J, which is defined as

(E_x = one particular enzyme concentration of a metabolic pathway of several reaction steps in series; ΔJ_x = change of pathway flux produced by a perturbation ΔE_x/E_x = f − 1). According to MCA, the sum of flux control coefficients ( ∑ C E n z J) approaches 1.0, for ( f − 1) → 0.

To demonstrate changes of a pathway flux after a small perturbation, a simulation of GLY is used, in which the reduced nicotinamide adenine dinucleotide concentration ([NAD_red]) is fixed (SIM_GLY, A14). As a source and sink, glucose ([Glu]) and pyruvate ([Pyr]) concentrations (4 mM and 43 μM, respectively) are both held constant. The new steady states are produced by multiplying successively respective maximal conductances by the same factor f. In all cases a new steady state can be obtained, in which all individual fluxes of the pathway have changed by the same degree, including that with the imposed change. In addition, affinities and intermediates have changed, but to a different extent in each case. From the newly adjusted pathway fluxes J, the initial flux J₀, and the imposed f, all flux control coefficients can be calculated. For f = 1.01 this yields C_GK^J = 0.1258, C_Ald^J = 0.0021, C_Ti^J = 0.00037, C_G^J = 0.0068, and C_W^J = 0.8623, yielding ∑ C E n z J = 0.9974.

In Figure 2 the behavior of all fluxes after increasing L_GK^max of J_GK (A1) by a markedly more pronounced perturbation (f = 2.0) is shown. After a new steady state has been reached, all fluxes are equally increased. To achieve this, the initially increased one (J_GK from 2 × 1.8084 × 10⁻³) must decrease, whereas the other ones (J_Ald, J_Ti, and J_Ga) must all increase until all individual fluxes of the first part of GLY (J_GK, J_Ald, and J_Ti) are equal and a new steady state pathway flux is produced. All new fluxes are in fact increased, but the relative increase is much less than f − 1 (0.0694 compared to 1.0).

For conditions of constant conductances, the same simulation as described above but with constant L’s is used. For these conditions, the sum of C_Enz^J can be obtained analytically. It is derived from Equation (4) by building n fractional changes of pathway flux (n = number of individual in series fluxes of a pathway), of which each individual one contains in each case a conductance, which has been changed by f. Summarizing and dividing by f − 1 yields ∑ C E n z J ( f ) (not shown).

For infinitesimal changes, ∑ C E n z J ( f ) → 1.0, and at f = 1.0, a singularity appears. For f > 1.0, this function is always smaller than 1.0, whereas the opposite occurs for f < 1.0 (Figure 3).

For variable L’s, the above relation cannot be solved analytically. The output values of the simulation, however, show that respective points follow roughly the analytical function. At small perturbations (f →1.0) the summation theorem seems to be sufficiently approached, as is shown above for f = 1.01. For larger changes, however, as they normally occur in cellular metabolism, deviations from 1.0 have to be expected (Figure 3).

In a more complex pathway like whole coupled glucose oxidation, coupled reactions and, in addition, load reactions (‘load’ usually designates the output affinity A₁ of a cytosolic reaction coupled to ATP_c splitting) are involved, both of which may impair the constancy of A_ov. As a result, fractional changes of the pathway flux are also influenced by a changed A_ov. This is given by

According to Equations (5a) and (5b), transformed values have to be used, which are designated A⃗_tot and L⃗_tot, respectively, to describe more complex networks. Such influences become most pronounced, when uncoupled reactions are involved (see Section 2.3.1).

During oxidative glucose metabolism hydrogen of glucose is transferred to oxidized hydrogen carriers like NAD_ox, which in turn transfer their hydrogen to the respiratory chain of the mitochondrial inner membrane, where it reacts with oxygen to form H₂O and reoxidized carrier. This reoxidation of redox carriers (NAD_red and FAD_red, respectively) at the inner side of the mitochondrial inner membrane is coupled to the transport of protons from the mitochondrial matrix space to the outer side of the inner membrane. At the interface between the outer aspect of the inner membrane and the bulk solution of the intermembrane space (solution between inner and outer mitochondrial membranes) these protons may exchange with other cations like K⁺ ions of the intermembrane space, so that an electrochemical potential difference of protons over the inner membrane, Δμ̃_H, is produced by coupled proton transport. It is composed of a chemical potential difference of protons over the inner membrane, Δμ_H, plus an electrical potential difference, the membrane potential Δ_mφof the inner membrane, yielding in mV

For simulations presented in this and foregoing articles [6,10] it was assumed that the pH of the intermembrane space is identical to the cytosolic pH_c and that outwards pumped and inward flowing protons only affect matrix pH_m, but have no effect on pH_c (e.g., J_NA or J_SY, A7 or A9). The same holds for proton symport and exchange reactions at the inner membrane: only pH_m can be changed, pH_c remains unaffected (e.g., J_Pi and J_HC, see [2]). In contrast, Δ_mφ is changed by both, in - and outgoing electrogenic membrane fluxes like J_CU (see [2]) or J_SY.

Such behavior might be realized for real mitochondria in situ by a further compartmentation of the intermembrane space. From recent morphological studies [35–38], it is known that cristae membranes form flat sacs with narrow openings to the intermembrane space. If proton cycling (outwards pumping and inwards flow) would preferentially occur at these structures, then primarily the luminal pH of cristae would be affected. This means that Δμ̃_H of the inner membrane might be transformed into a potential difference with a more pronounced (more negative) chemical component (Δμ_H) and an appropriately less pronounced (less negative) electrical component (Δ_mφ) at cristae membranes than at the rest of the inner membrane. A low buffering power of these regions would further increase this effect. Strauss et al. [36] could demonstrate that ATP synthase complexes are located preferentially at the rims of cristae sacs where they may be involved with shaping the rim structure. These morphological facts are consistent with the idea that pH_c under physiological conditions may be affected only to a negligible degree by proton fluxes across the inner membrane. So, an amount of Δμ̃_H × n (J) of energy is dissipated, when n moles of protons move without coupling across the inner membrane from the bulk phase of the intermembrane space to the bulk phase of the matrix.

Redox reactions (J_NA and J_FA, A7 and A8) are coupled to proton transport with a stoichiometry of 10.0 and 6.0 mol H⁺ per mol of NAD_red or FAD_red oxidized [18], respectively. Thus, 6.0 mol O₂ and 12.0 mol reducing equivalents are consumed per mol of oxidized glucose. These chemical constraints are fulfilled by all simulations. But not all protons transported by J_NA and J_FA enter oxidative phosphorylation (OP). Some leak back into the matrix (J_PL), some are needed for Ca/H exchange (J_HCE), and some for the malate-aspartate shuttle (J_MS). In addition, in real mitochondria H⁺ influx may be required for transhydrogenation. This membrane reaction, however, is not addressed in present simulations. The remaining proton flux is used by ATP synthase (J_SY) and ATP/ADP exchange (J_AE) plus H/Pi symport (J_Pi). At steady state, the stoichiometry of coupled J_SY is assumed to be 3.0 mol H⁺ per mol of matrix ATP (ATP_m) produced [18]. ATP_m is transferred into the cytosol and ADP_c plus Pi are delivered to the matrix by two further in series reaction steps (via J_AE and J_Pi, respectively). Both reactions are coupled to inward transport of 1.0 mol of positive charge (via J_AE) and 1.0 mol of electrically neutralized protons (by symport via J_Pi) per mol of exchanged ATP_m, i.e., one additional Δμ̃_H is consumed to exchange ATP_m from the matrix with ADP_c and P_i from the cytosol. Thus, under near static head conditions, OP would require 4.0 Δμ̃_H to overcome in series affinities of ATP synthesis in the matrix (−A_ATPm, A13) and of ATP exchange (A_AdPi, A13). Under more physiological conditions, however, ATP_c consumption occurs permanently to drive load reactions of the cytosol. Mainly these reactions lower the ratio A_ATPc |Δμ̃_H below 4.0 (if ATP production by GLY and CAC were included, this value would be slightly higher).

When ATP splitting by load reactions is added, the whole process may be considered as two interconnected cycles: a proton cycle J_H^coup coupled to an ATP cycle J_ATP^coup through the ATP synthase reaction, ATP/ADP exchange, and H/Pi symport. At steady state (all individual fluxes of a given cycle are of same magnitude), both cyclic flows produce no dissipation (or entropy), because their respective sums of affinities taken over a closed path in both cases must be equal to zero.

In the above derivation proton fluxes from proton sources to proton sinks at the outer and inner sides of the mitochondrial inner membrane are not included in calculations. Under real conditions, however, in order to allow proton cycling, such fluxes must be present, and thus, also a certain amount of dissipation of free energy. In addition, during ATP cycling free energy is dissipated by diffusional fluxes of ATP, ADP, and P_i species (see Section 2.4). It can be concluded, therefore, that under real conditions OP must be always slightly uncoupled, even if all respective inner membrane reactions of OP would proceed at q = 1.0.

The flux ratio of coupled cycles, J_H^coup | J_ATP^coup must always be equal to 4.0 under totally coupled as well as under uncoupled conditions, as long as the ATP synthase reaction (J_SY) remains coupled. In addition to the coupling between cycles, the proton cycle is coupled to J_Rop^o, and the ATP cycle to J_Wop^ld (A13), respectively. Both respective affinities, A_R^o (input force) and A_W^ld (negative output force), are the only forces, which do not vanish at steady state cycling.

The reaction sequence of OP is given by the following in series reactions: J_R^o denotes the resultant input flux of OP of parallel input reactions (fraction Q_H of J_NA plus J_FA, A13a). From total J_R^o only the coupled fraction without leak flux can be used for proton pumping, while J_R^h (coupled flux minus leak flux) is the effective proton efflux. At steady state it is equal to proton influx J_SY^h plus (J_AE − J_CAC). From total J_SY^h only the coupled fraction is used for ATP_m synthesis, but only J_SY^p (coupled flux minus leak flux) is exported from the mitochondrion to produce ATP_c. It must be equal to (J_AE − J_CAC) and coupled J_R^o.

Equation (10) cannot give any information about the mechanisms of coupling and uncoupling, respectively. However, from their derivation [39] it follows that uncoupling leak fluxes must flow through the coupling device, i.e., through the respective multi-enzyme complex involved, because they are added to input and output fluxes, respectively. In contrast to this direct uncoupling an indirect uncoupling may occur through additional parallel leak fluxes like the proton leak flux J_PL at the inner mitochondrial membrane, or the flux of Na⁺ and K⁺ ions through sodium and potassium channels or other Na⁺ and/or K⁺-permeable channels of the cell membrane. The relevant coupled reaction for these latter uncoupling fluxes is given by the reaction sequence of the Na-K pump. Also Ca²⁺pumps must be mentioned in the context of such pump and leak fluxes. Remarkably, dissipation of free energy is used further by these systems for signal transduction.

In principle, to avoid static head production, coupled reactions are controlled in addition to parallel leak fluxes by their own substrates. For instance, Na-K pumps are kinetically controlled by [Na⁺]_c, and Ca²⁺ pumps by [Ca²⁺]_c, so that pump fluxes slow down when substrate concentrations become sufficiently lowered.

Stucki suggested that energy coupling through OP may be described as a two-flux-system in the same way as for a single coupled reaction [40]. He identified the oxygen utilizing redox reaction as the input and the ATP_c yielding reaction as the output flux. Including an additional attached ATP_c consuming load reaction, he could show that the dissipation function (entropy production in his article) of such a system possesses a minimum at a reduced force ratio given by x_min = − q/(1 + L₃₃/L₁₁) (x = A₁/A₂ × Z), L₃₃ and L₁₁ are Stucki’s load and input conductances, respectively). Equating this value with the x coordinate of maximal efficiency, x max = - q / ( 1 + 1 - q 2 ), shows that a minimal dissipation and a maximal efficiency would coincide, if the ratio of the load (L₃₃) and the input (L₁₁) conductance of whole OP fulfilled the condition L 33 / L 11 = 1 - q 2. This relation was termed conductance matching by Stucki [40]. It is derived for uncoupled systems only, because under totally coupled conditions the above relationship requires that L₃₃ vanishes. This, however, would generate a static head state, which is not compatible with conditions of metabolizing cells.

It seems already worth mentioning that all simulations presented here and those published recently [6,10] do not adjust to such a value. Moreover, they all allow total coupling without producing a static head.

To prove Stucki’s hypothesis of conductance matching, a simulation of OP fuelled by pyruvate was developed (SIM_OP^Pyr, A16). Under such conditions OP may be better comparable to conditions of isolated mitochondria, especially because activation of PFK by cytosolic adenosine monophosphate concentration [AMP]_c is absent.

At first, it is demonstrated that experimental results of Stucki can be principally reproduced by the present simulation of OP. Figures 4 and 5 show that under uncoupled conditions a linear relationship exists between J₁ and X₁ (J_NA^h and A_NA^h, and J_SY^p and A_SY^p, respectively), as well as between J₂ and X₁ (J_NA^o and A_NA^h, and J_SY^h and A_SY^p, respectively, A7 and A9). From this linear behavior Stucki concluded that for a given q_ov (overall value of q for whole OP), X₁ may be the only variable of this two-flux-system, and that all other parameters, i.e., X₂, L₁₁, and L₁₂ are constant and can be derived from experimental results [40].

The simulation demonstrates, however, that linearity under such conditions can be produced with variable conductances and variable forces as well. It can be taken from Figures 4 and 5 (panels A and B) that the fluxes J₁₁ and J₁₂, whose sum yields J₁, are slightly curved with opposite curvature, but that their sum yields a straight line. The same holds for J₂. The slight deviation from linearity shows that some results of the simulation only approximately obey flux equations of NET. Under coupled conditions, fluxes J₁ and J₂ are equal and linear (not shown).

Figures 4d and 5d demonstrate that uncoupling of individual reactions of OP fulfill the analytical efficiency equation (10). Panels D-F of Figure 4 show that for this individual two-flux-system (A_NA is far from equilibrium) efficiency is close to the maximum, but that dissipation is not minimal, whether at the reduced force ratio x_max (where efficiency is maximal), nor for that obtained from the simulation. Power output of this reaction is 67.5% at q_n = 0.952. In contrast, panels D-F of Figure 5 show that efficiency of this near equilibrium reaction (A_SY is near zero) is not maximal. Dissipation is close to a minimum for the x value obtained from the simulation, but not for the η_max related x. As can be expected, power output for this near equilibrium reaction is much lower, only 11.7% at q_s = 0.971.

The results of Figures 4 and 5 demonstrate that individual reactions of OP fulfill exactly the equations of NET. If, however, whole OP were formulated as a two-flux-system with A_R^o as input force, and −A_ATPc as output force, A_W^p =A_ATPc (positive) would be the input force of the attached load reaction. Because both affinities cancel, the reduced force ratio x of such a system would be zero, so that the dissipation function would be given merely by the term L_OP(λ2_ov + 1)(A_R^o)² (A19b) For this expression, efficiency cannot be formulated as a function of x. It must be zero, because the output force is zero under all conditions. A conductance matching, as demanded by Stucki, therefore does not exist in simulations presented here, and, since the reaction sequence of ATP formation and ATP consumption must be present as an indispensible part of energy metabolism, this mechanism may also not be realized in a living cell.

Furthermore, from a teleological perspective, Stucki’s conductance matching seems highly unlikely to occur in energy metabolism of living cells, since such behavior would lead to the paradoxical situation that most favorable conditions of energy conversion – namely power output without losses of free energy by uncoupling – must result in cell death by the inevitable emergence of a static head.

When dissipation functions are formulated up to −A_ATPc or A_W^ld, all forces but the input force (A⃗_R^o) and the output force (−A_ATPc or A_W^ld, respectively) must vanish to describe the involved reactions as a two-flux-system. Although this is possible, unreliable results are produced, which often show negative λ_ov’s and a q_ov > 1.0, respectively. This might be caused by the cyclic mode of operation of the coupling system. It is concluded, therefore, that it is impossible to describe OP as a two-flux-system according to NET, although individual reactions of this complex coupling system may fulfill those equations.

Hexokinase of heart muscle has a very low K_M value compared to that of glucokinase of β-cells. It is this kinetic difference of the first glycolytic reaction step, which is necessary to allow high pathway fluxes of glucose oxidation in muscle cells. In addition, the low K_M prevents that the intracellular glucose concentration ([Glu]) might become limiting as in β-cells (see below). Because [Glu] activation of hexokinase is saturated at resting concentrations ([Glu] = 4.0 mM), its conductance cannot vary which makes it more difficult if not impossible to develop a new steady state after a perturbation. This can be avoided by introducing a feedback inhibition of hexokinase by the concentration of glucose-6-phosphate ([G6P]), which in simulations can be expressed by the concentration of fructose-6-phosphate ([F6P]), since both intermediates are virtually at equilibrium through the phosphoglucose isomerase reaction (A2). Such a feedback can also avoid an extreme increase of [G6P] and [F6P]. So [F6P] appears as an additional variable in simulations of glucose oxidation in VMs. As a consequence, and in contrast to β-cell simulations, the PFK reaction is incorporated as an individual reaction step (not part of several in series reactions contracted to one single step as in β-cells) into the glycolytic reaction sequence of VMs. It is activated by [F6P] and in addition by [AMP]_c, and is inhibited by [ATP]_c. Also the pyruvate kinase (PK) reaction, which is part of several contracted in series reactions, is inhibited in VMs by [ATP]_c (A3).

To see which reactions of the glucose oxidation pathway must be activated to increase power output of ATP splitting reactions of the cytosol, MCA has been applied to these pathways. A simultaneous change of all conductances yields a value of C^J = 1.0. When conductances are changed successively, C^J does not reach 1.0. A pronounced change can already be obtained by changing simultaneously merely two conductances, that of J_W (G_Wser^max, L_Wcrbr^max, L_Wb^max, A4 – A6), and that of J_PFK (L_PFK^max; A2). For f = 2.0, ∑C_Enz^J under these conditions reaches a value of 0.8725. Interestingly, this value can be appreciably increased further to 0.9757 by including the indirect uncoupling flux J_PL. In contrast, when all remaining conductances of these pathways are increased simultaneously by f = 2, this yields a ∑C_Enz^J value of 0.0112 only. It seems noteworthy that also a direct uncoupling can appreciably augment ∑C_Enz^J. For instance, increasing conductances of only [Ca²⁺]_c dependent load reactions by f = 1.1, yields a ∑C_Enz^J of 0.248. When under the same conditions the ATP synthase reaction is slightly uncoupled (λ_sp = λ_sh = 0.01), a ∑C_Enz^J of 2.77 is obtained. This large increase of the sum of control coefficients by uncoupling is brought about by an appreciable increase of A⃗_tot (see Equation (7)). Therefore, if a ∑C_Enz^J >> 1.0 were found with a pathway containing coupled reactions, this may indicate a significant uncoupling.

The above results of control analysis show that increasing only two conductances may be sufficient to appreciably increase pathway flux and thus, also power output. A simultaneous increase of all maximal conductances is not necessary; the variability of conductances obviously is able to produce the demanded increase of whole pathway flux. Moreover, also fluxes through J_AE and J_Pi must not be specifically activated. Ca²⁺ activation of pyruvate dehydrogenase (PDH), and dehydrogenases of the citric acid cycle (fluxes J_PDH and J_CAC, respectively) is virtually without effect on power output and O₂ consumption in present simulations, because respective conductances (L_PDH^max and L_CAC^max) are adjusted to rather high values.

In real VMs, these conductances might be appreciably lower, so that a [Ca²⁺]_m activation becomes indispensable at an increasing power output [23,24,41–43]. Also ATP synthase of VMs is known to be activated by [Ca²⁺]_m [44]. In present simulations, activation of ATP synthase (J_SY) by [Ca²⁺]_m cannot increase power output, but reduces dissipation of free energy of this reaction. Beside these latter effects of [Ca²⁺]_m, mitochondrial Ca²⁺ fluxes may be needed to synchronize free energy flows of several mitochondria during contraction cycles. Otherwise an optimal interplay of all involved reactions might not be guaranteed.

In the present simulation as well as in real VMs, important load reactions like muscular contraction or Ca²⁺ transport by SERCA pumps are activated by an increase of [Ca²⁺]_c. This in turn leads to an increase of ATP_c consumption with a concomitant elevation of [ADP]_c and [Pi]_c. Because the adenylate kinase (AK) reaction is near equilibrium, this means that also [AMP]_c must increase and PFK becomes activated, with the result that all pathway fluxes associated with glucose oxidation become activated too. So activation of ATP_c utilization is followed by an appropriately adjusted ATP_c delivery. In this way load reactions not only deliver useful work, but concomitantly generate [AMP]_c, which quasi as a third messenger activates ATP_c production, so that a drastic decrease of [ATP]_c and associated A_ATPc may be prevented, even under conditions of a markedly increased power output. Present simulations demonstrate that the increase of only [Ca²⁺]_c dependent load conductances and [AMP]_c dependent L_PFK is needed, to switch from low to a high power output.

O₂ consumption of working hearts shows linear dependence on mechanical power output over a wide range of delivered power [23–25]. Such behavior can be simulated, supposing that pressure development of whole hearts is mechanically produced by the contractile machinery of single VMs, i.e., by ATP- driven cross-bridge cycling. To formulate this process as a two-flux-system, a molar torque τ^m (generated by cross-bridge cycling) is defined as output force A_τ coupled to the input force A_ATPc (A5). An increasing pressure development of the activated heart is considered in simulations through a [Ca²⁺]_c dependent change of τ^m. From NET it is clear that increasing A_τ must reduce the resultant force A_coup, so that the associated flux must be reduced too. This does not only decrease velocity of contraction, but also increases efficiency of this reaction.

Figure 6A shows that results of simulation are consistent with experiments: over a wide range of power P_Wτ,= −Φ_Wτ= −J_WτA_Wτ, J_O2 depends linearly on this variable. Only at very high [Ca²⁺]_c’s, O₂ consumption begins to be larger than would be expected from linearity. Panel B shows that J_O2 depends linearly on [ADP]_c and [AMP]_c. These results of simulations, however, do not support the conclusion that O₂ consumption may be activated by [ADP]_c at the level of ATP/ADP exchange of mitochondria. Even a tenfold increase of this flux conductance (L_AE^max) could not further increase O₂ consumption, which underlines above mentioned results of MCA. With permeabilized cardiomyocytes it could be shown [28] that the activation effect may be caused by a limited availability of ADP for OP, since ADP³⁻ cannot permeate with sufficient rapidity the voltage dependent anion channel (VDAC) [45]. The demonstrated Pi activation of O₂ consumption [46,47] presumably cannot be explained by a limited availability of H₂PO⁴⁻, since, in contrast to ADP³⁻, this Pi species may easily permeate the VDAC pore of the outer membrane. It was suggested that Pi may activate dehydrogenases of the matrix and in addition may be needed to activate electron transport of the respiratory chain [46].

But even if the above mentioned activation effects of [ADP]_c and/or [Pi]_c were operative also in coupled glucose oxidation of real VMs, an activation of whole pathway flux is absolutely necessary to deliver free energy under conditions of an increased consumption of free energy. Since it is not stored sufficiently in glucose metabolism itself including OP, it must be delivered by other stores, that is, mainly from the extracellular space in the case of VMs. So the controlled flow of free energy through the whole metabolic pathway is necessary to satisfy changing free energy demands. As is demonstrated with simulations, the most effective points of control are given by [Ca²⁺]_c dependent load reactions and PFK. The flow of information from load to delivery is brought about by the feedback via AK of [AMP]_c on PFK.

Up till now all results were related to steady state conditions, intrinsic oscillations do not occur under these conditions and forced oscillations were excluded. VMs in heart tissue, however, contract rhythmically at various frequencies and variable pressure developments. These oscillating contractions are known to be induced by rhythmic depolarizations of the membrane potential (Δ_cφ), which in turn trigger periodic Ca²⁺ release from and accumulation into the sarcoplasmic reticulum (SR). The oscillating [Ca²⁺]_c then may initiate—beside other activations—periodic contraction and relaxation of myofibrils. Thus, such [Ca²⁺]_c oscillations are not generated by an intrinsic oscillator, but rather are forced by rhythmic depolarizations of Δ_cφ It seems justified, therefore, to simulate rhythmic behavior by simple sinusoidal oscillations of [Ca²⁺]_c (A18). Figure 7 shows that many variables and parameters are forced to oscillate in the presence of [Ca²⁺]_c oscillations. The arithmetic means of such oscillations deviate slightly from steady state results. For instance, when results of Figure 6 are compared with results found under the same conditions, but in the presence of oscillations, they yield the following: at [Ca²⁺]_c = 0.18 μM J_O2 and P_Wτ are 0.121 μM/ms and 3.273 J/Ls, respectively, in the absence of oscillations. In the presence of forced oscillations, respective means are 0.122 μM/ms and 3.432 J/Ls. Values at 0.72 μM [Ca²⁺]_c are 0.570 μM/ms and 96.45 J/Ls, and 0.553 μM/ms and 95.18 J/Ls, respectively. Therefore, it seems justified to conclude that deductions made with respect to steady state are valid also under conditions of forced oscillations.

Because OP cannot be formulated as a two-flux-system, Equation (10o) would be inappropriate to show that power output of coupled glucose oxidation is near maximal. The problem of non-reliable overall parameters can be circumvented, however, if transformed conductances were taken into account.

It is well known in electrical engineering that power output of a battery becomes maximal when the internal conductance L_i matches the conductance of the outer circuit, L_e. A battery can be regarded as a coupled two-flux-system, in which a chemical reaction with affinity A₂ is coupled to an electrical potential difference, Δφ = −U, with affinity A₁. Coupled glucose oxidation, when transformed to equal flux velocities, can be regarded analogously: the input force is given by A⃗_ov, while the coupled output force is given by −A⃗_ATPc. Both forces and conductances L⃗_i and L⃗_e can be obtained from respective dissipation functions as described above. In analogy to a simple electric circuit consisting of a battery whose poles are connected by an electrical resistance (R_e = 1/L_e) with an attached load, L⃗_i is related to the whole pathway of glucose oxidation including coupled ATP_c production, and L_e to ATP_c utilizing reactions, i.e., all cytosolic ATPases. As in an electric circuit, only the electrical resistance (R_e) of an energy converter is involved with power maximation. In energy metabolism it is therefore only that part of L⃗_W, which is associated with ATP splitting. That is, the flux through A_ATPc (J_W^p) is the relevant flux, and L_e therefore has to be derived from the input dissipation function Φ_W^p, and not from total dissipation function Φ_W = Φ_W^ld + Φ_W^p. It is given by

L⃗_i is given by

Delivery of free energy from coupled glucose oxidation in the form of ATP_c, i.e., power output, is identical to the input dissipation function of the load reaction

Analogous to I = E R e + R i (I = electrical current, and E = electromotive force), the respective flux is given by

and

Power output can be expressed then as

or with Λ = L → e L → i

If L⃗_i and A⃗_ov were both constant, then Φ_W ^p would be a function of Λ alone with a maximum at Λ = 1.0, or at L⃗_e = L⃗_i

With η = - ( - A → A T P c ) A → o v, and using (10d) and (10f), efficiency in terms of Λ is given by

and Λ = 1, yields η = 0.5.

These relations are verified with a simplified simulation (SIM_GLY, A14) with constant conductances (Figure 8). The results show that a maximum does in fact exist at Λ = 1.0 under these conditions and that η is equal to 0.5 at this value of Λ.

A simulation of whole glucose oxidation with variable conductances (SIM_GlOx, A15) and, in addition, with a feed back by [AMP]_c on PFK leads however to entirely different results, when Λ is increased by an increase of [Ca²⁺]_c (Figure 8) (conductances of load reactions become increased at an elevated [Ca²⁺]_c, A4 and A5). Only one point at Λ = 0.82 ([Ca²⁺]_c = 0.18 μM) fulfils Equation (13g), all other values for Φ_W^p, and especially those found for higher [Ca²⁺]_c’s are markedly elevated above that curve, but are all at nearly the same value of Λ (Figure 9A). In contrast, when PFK activation by [AMP]_c is omitted, power output cannot be increased by increasing L⃗_e (Figure 9C) and, because conductances are not constant, points do not fulfill Equation (13g).

Obviously, the feedback by [AMP]_c on PFK can activate whole coupled glucose oxidation to appropriately increase ATP production to meet the demands of an increased ATP consumption. Λ remains remarkably constant at about 0.79 over a nine fold range of power output. It is close to maximal power output. Consequently, also efficiency must be approximately constant and, as follows from Equation (13g), near a value of 0.5 (0.56) (Figure 9B, D). Interestingly, also efficiency of the glycolytic span from glucose to pyruvate lies near this value.

The respective points of Φ_W^p must always fulfill the associated hypothetical power curve calculated each time for a given pair of values L⃗_i; and A⃗_ov. These curves are hypothetical insofar as especially L⃗_i (changes of A⃗_ov are negligible under all conditions) is not constant at varying L⃗_e. That is, only one single point of the curve related to a given particular condition is of significance.

Larger deviations of Λ from 1.0 can be obtained by uncoupling OP. Figure 9F shows that efficiency obeys exactly Equation (13h) over a very wide range of Λ’s. Both conductances, L⃗_e as well as L⃗_i, are increased by uncoupling OP, but L⃗_e to a much higher degree, so that Λ increases and thus efficiency decreases. Figure 9E shows that also under conditions of markedly increased Λ’s, power output points are close to their hypothetical respective power curve. Comparison of these uncoupled values with those obtained for coupled conditions shows that larger losses of useful power obviously can be prevented. This power preservation is associated, however, with a marked reduction in efficiency (Figure 9E,F).

These results demonstrate in a striking manner, how serious deteriorations of energy coupling can be compensated by an [AMP]_c mediated increase of pathway flux. In addition, for the metabolism of VMs they show that maintenance of power output obviously has priority over conservation of efficiency.