Effects of temperature on cytochrome oxidase activity in solubilized form and in lipid vesicle systems.

Isolated mammalian cytochrome oxidase gave an Arrhenius plot with a break (Tb) at about 20 degrees C when assayed in a medium containing Emasol. The activation energies above and below 20 degrees C were 9.3 (EH) and 18.9 kcal/mol (EL), respectively. Isolated cytochrome oxidase was also incorporated into vesicles of dipalmitoyl phosphatidylcholine (DPPC, phase transition temperature Tt = 40 degrees C), dimyristoyl phosphatidylcholine (DMPC, Tt = 23 degrees C) and dioleoyl phosphatidylcholine (DOPC, Tt = -22 degrees C). The DPPC system showed a nearly linear Arrhenius plot between 9 and 36 degrees C with E = 22.8 kcal/mol. When cytochrome oxidase was resolubilized from the DPPC vesicles and assayed in solution a biphasic plot was obtained again. Cytochrome oxidase-DOPC was more active than the solubilized enzyme and exhibited a biphasic Arrhenius plot with Tb = 23 degrees C. EH and EL were 6.6 and 15.8 kcal/mol, respectively. The plot for the oxidase-DMPC also showed a break (Tb = 26 degrees C) with EH = 6.6 and EL = 26.6 kcal/mol. These results indicate that the break in the Arrhenius plot reflects primarily a structural transition in the cytochrome oxidase molecule between the "hot" and "cold" conformations, as proposed previously. This transition, as well as the molecular state of cytochrome oxidase, is affected by the physical state of the membrane lipids as reflected by changes in the kinetic properties.     

Temperature dependence of D-glucose transport in reconstituted liposomes

Sodium-dependent D-glucose uptake into proteoliposomes reconstituted from dimyristoylphosphatidylcholine (DMPC) and hog kidney brush border membrane extract is strongly affected by temperature and the physical state of the membranes. This dependence is defined by a nonlinear Arrhenius plot with a break point at 23 degrees C, a temperature not significantly different from the phase transition temperature of the pure lipid (24 degrees C). The transport process is characterized by different activation energies: 35.1 kcal/mol below and 5.5 kcal/mol above the transition temperature. The shift in the break point for the D-glucose transport activity from 15 degrees C, in the brush border membranes, to 23 degrees C in the reconstituted system leads us to conclude that the lipids surrounding the sodium/D-glucose cotransport system can exchange readily with the bulk lipid used for reconstitution. The results thus provide no evidence for the presence of an annulus of specific lipids surrounding the transport system.     

Temperature dependence of the energy-linked monosaccharide transport across the cell membrane of Rhodotorula gracilis.

The temperature dependence of the active monosaccharide transport across the cell membrane of the yeast Rhodotorula gracilis has been studied between 0 and 55 degrees C with D-xylose as the transported substrate: (i) Between 0 and 10 degrees C there is virtually no transport. (ii) The initial velocity of transport increases exponentially from 15 to 30 degrees C (deltaE equal to 32 plus or minus 2 kcal/mol). (iii) At 30 degrees C a sharp "break" occurs in the Arrhenius plot and with increasing temperature the transport becomes inactivated, with a positive slope of the corresponding straight line ("deltaE equal to minus 15 kcal/mol"). (iv) In the temperature range of 50-55 degrees C, both the transport and the metabolic activity cease. In order to account for the abrupt changes of the membrane permeability, we attempted to ascribe them to phase transitions in the membrane structure: the first one, between 10 and 15 degrees C, to the crystalline: liquid-crystalline phase change; the second one, around 30 degrees C, to a change from highly ordered (low entropy) to less ordered (high entropy) membrane structure. Whereas the former phase transition is reversible, the latter appears to be irreversible. Arrhenius plots of the cell respiration exhibit a "break" at 30 degrees C, as well. However, at higher temperatures there is no thermal inactivation of the respiratory activity. The importance of a proper organization of the cell membrane constituents for the efficient transport function is discussed.     

Temperature dependence of unitary properties of an ATP-dependent potassium channel in cardiac myocytes.

The temperature dependence of the properties of unitary currents in cultured rat ventricular myocytes has been studied. Currents flowing through an ATP-dependent K+ channel were recorded from inside-out patches with the bath temperature varied from 10 degrees to 30 degrees C. The channel conductance was 56 pS at room temperature (22 degrees C), and the amplitudes of unitary currents and the channel conductance exhibited a relatively weak (Q10 from 1.4 to 1.6) dependence on temperature. The temperature dependence of channel mean open times was biphasic with the low temperature (10-20 degrees C) range showing a relatively stronger temperature dependence (Q10 of 2.3) than the high temperature (20-30 degrees C) range (Q10 of 1.6). The activation energies for the two regions were determined from an Arrhenius plot with the activation energy, corresponding to the lower temperature range, near 16 kcal/mol. Thermodynamic analysis, using transition rate theory, indicated that the formation of a transition state prior to channel closure to be associated with a positive entropy component for the high Q10 region.     

The effect of temperature on monoxygenase reactions in the microsomal membrane

The effect of temperature on the rates of monoxygenase reactions was studied with microsomes prepared from phenobarbital pretreated rats. The rates of the N-demethylation of ethylmorphine, benzphethamine, aminopyrine, and p-nitroanisole were studied. Breaks at temperatures around 24 degrees C were observed in the Arrhenius plots of all these reactions. The energy of activation of these reactions has values of 10-12 and 19-21 kcal per mol at temperature ranges above and below the break temperature, respectively. The break, however, was not observed if 30% glycerol was added to the microsomes. The Arrhenius plot of the microsomal NADPH-cytochrome c reductase activity also did not show any break. The implications of these observations in relationship to the fluidity of the membrane, the translational mobility of membrane enzymes, and the rate of monoxygenase reactions are discussed.     

A jump in an Arrhenius plot can be the consequence of a phase transition. The binding of ATP to myosin subfragment 1

The temperature dependence of the kinetics of the binding of ATP to myosin subfragment-1 was studied by an ATP chase technique in a rapid-flow-quench apparatus: (formula; see text) A temperature range of 30 degrees C to -15 degrees C was obtained with ethylene glycol as antifreeze. The Arrhenius plot of k2 is discontinuous with a jump at 12 degrees C. Above the jump delta H+ = 9.5 kcal/mol, below delta H+ = 28.5 kcal/mol. Few such Arrhenius plots are recorded in the literature but they are predicted from theory. Thus, we explain our results as a phase change of the subfragment 1-ATP system at 12 degrees C. This is in agreement with certain structural studies.     

Temperature dependence of anion transport in the human red blood cell

Arrhenius plots of chloride and bromide transport yield two regions with different activation energies (Ea). Below 15 or 25 degrees C (for Cl- and Br-, respectively), Ea is about 32.5 kcal/mol; above these temperatures, about 22.5 kcal/mol (Brahm, J. (1977) J. Gen. Physiol. 70, 283-306). For the temperature dependence of SO4(2-) transport up to 37 degrees C, no such break could be observed. We were able to show that the temperature coefficient for the rate of SO4(2-) transport is higher than that for the rate of denaturation of the band 3 protein (as measured by NMR) or the destruction of the permeability barrier in the red cell membrane. It was possible, therefore, to extend the range of flux measurements up to 60 degrees C and to show that, even for the slowly permeating SO4(2-) in the Arrhenius plot, there appears a break, which is located somewhere between 30 and 37 degrees C and where Ea changes from 32.5 to 24.1 kcal/mol. At the break, the turnover number is approx. 6.9 ions/band 3 per s. Using 35Cl- -NMR (Falke, Pace and Chan (1984) J. Biol. Chem. 259, 6472-6480), we also determined the temperature dependence of Cl- -binding. We found no significant change over the entire range from 0 to 57 degrees C, regardless of whether the measurements were performed in the absence or presence of competing SO4(2-). We conclude that the enthalpy changes associated with Cl- - or SO4(2-)-binding are negligible as compared to the Ea values observed. It was possible, therefore, to calculate the thermodynamic parameters defined by transition-state theory for the transition of the anion-loaded transport protein to the activated state for Cl-, Br- and SO4(2-) below and above the temperatures at which the breaks in the Arrhenius plots are seen. We found in both regions a high positive activation entropy, resulting in a low free enthalpy of activation. Thus the internal energy required for carrying the complex between anion and transport protein over the rate-limiting energy barrier is largely compensated for by an increase of randomness in the protein and/or its aqueous environment.     

Effects of temperature on the mitochondrial malate dehydrogenase of adult muscle of Toxocara canis

Purified mitochondrial malate dehydrogenase isoenzyme (m-MDH) of Toxocara canis muscle presented maximum activity at 48 degrees C. A clear change in slope of the Arrhenius plot was observed. The energy of activation calculated for the catalytic process showed values of 3.2 kcal/mol and 10.5 kcal/mol. Thermal inactivation of m-MDH showed that it is more thermolabile than the s-isoenzyme. The inactivation of the enzyme by heat could be reduced at least in part by the addition of 0.1 mM NADH. The heat denaturation showed to be a first-order process. The rate constant (k) was calculated as being of the order of 5.28 X 10(-4) s-1 at 40 degrees C. The activation energy for the heat inactivation process was 16.45 kcal/mol between 30 degrees C and 40 degrees C and 13.79 kcal/mol between 40 degrees C and 48 degrees C.     

Catalytic and thermodynamic properties of the urocanate hydratase reaction.

Urocanate hydratase (4-imidazolone-5-propionate hydro-lyase, EC 4.2.1.49) isolated from Pseudomonas putida contains covalently bound alpha-ketobutyrate as its cofactor. In the process of examining the mechanism by which alpha-ketobutyrate serves in this capacity, various thermodynamic parameters and temperature effects on urocanate hydratase activity were determined. As the equilibrium constant at 15 degrees C for imidazooone propionate formation from urocanate is approximately 69, regardless of whether urocanic acid or chemically synthesized imidazolone propionate is used as the initial substrate, it is concluded that the reaction is freely reversible. DeltaG degrees ', deltaH degrees ' and deltaS degrees ' were --2.5 kcal/mole, +5.2 kcal/mole and +26 cal/deg mole, respectively. Measurement of first-order reaction rates at various temperatures, in order to calculate the Arrhenius activation energy, showed a sharp break in the Arrhenius plot at 29 degrees C. Further examination of this phenomenon by determining s20,w values of urocanate hydratase as a function of temperature revealed a dramatic change at 31 degrees C. Since the enzyme in both experiments reverts to its original state when the temperature is lowered back below the transition point, it is proposed that urocanate hydratase undergoes a reversible conformational change or partial dissociation which affects its catalytic properties in the range of 29--31 degrees C.     

Temperature dependence of endocytosis mediated by the asialoglycoprotein receptor in isolated rat hepatocytes. Evidence for two potentially rate-limiting steps

The rate of endocytosis of cell surface-bound [3H]-asialo-orosomucoid was determined as a function of temperature. Freshly isolated rat hepatocytes were allowed to bind [3H]asialo-orosomucoid at 4 degrees C, washed to remove nonbound ligand, and internalization was then assessed by the resistance of cell-associated radioactivity to release by the Ca2+ chelator EDTA. At 10 degrees C or below, endocytosis is negligible. Above 10 degrees C, the rate of endocytosis is proportional to temperature but the increase of the rate of endocytosis with increasing temperature changes sharply at about 20 degrees C. From 10-20 degrees C, the apparent activation energy for endocytosis, calculated from an Arrhenius plot, is 45.9 kcal/mol and the temperature coefficient, Q10, is 15.6. However, between 20 and 41 degrees C, the calculated activation energy is 17.0 kcal/mol and the Q10 is 2.6. Although the rate of endocytosis of previously bound [3H]asialo-orosomucoid is very dependent on the temperature, the final extent of endocytosis is essentially temperature-independent between 14 and 37 degrees C. The results suggest that there are at least two steps in the overall process of endocytosis mediated by the asialoglycoprotein receptor on isolated hepatocytes which can be potentially rate-limiting, one at 10 degrees C and another at approximately 20 degrees C.     

Temperature dependence of d-glucose transport in reconstituted liposomes

Sodium-dependent d-glucose uptake into proteoliposomes reconstituted from dimyristoylphosphatidylcholine (DMPC) and hog kidney brush border membrane extract is strongly affected by temperature and the physical state of the membranes. This dependence is defined by a nonlinear Arrhenius plot with a break point at 23°C, a temperature not significantly different from the phase transition temperature of the pure lipid (24°C). The transport process is characterized by different activation energies: 35.1 kcal/mol below and 5.5 kcal/mol above the transition temperature. The shift in the break point for the d-glucose transport activity from 15°C, in the brush border membranes, to 23°C in the reconstituted system leads us to conclude that the lipids surrounding the sodium/d-glucose cotransport system can exchange readily with the bulk lipid used for reconstitution. The results thus provide no evidence for the presence of an annulus of specific lipids surrounding the transport system.     

Alterations in phospholipid-dependent (Na+ +K+)-ATPase activity due to lipid fluidity. Effects of cholesterol and Mg2+.

The (Na+ +K+)-activated, Mg2+-dependent ATPase from rabbit kidney outer medulla was prepared in a partially inactivated, soluble form depleted of endogenous phospholipids, using deoxycholate. This preparation was reactivated 10 to 50-fold by sonicated liposomes of phosphatidylserine, but not by non-sonicated phosphatidylserine liposomes or sonicated phosphatidylcholine liposomes. The reconstituted enzyme resembled native membrane preparations of (Na+ +K+)-ATPase in its pH optimum being around 7.0, showing optimal activity at Mg2+:ATP mol ratios of approximately 1 and a Km value for ATP of 0.4 mM. Arrhenius plots of this reactivated activity at a constant pH of 7.0 and an Mg2+: ATP mol ratio of 1:1 showed a discontinuity (sharp change of slope) at 17 degrees C, with activation energy (Ea) values of 13-15 kcal/mol above this temperature and 30-35 kcal below it. A further discontinuity was also found at 8.0 degrees C and the Ea below this was very high (greater than 100 kcal/mol). Increased Mg2+ concentrations at Mg2+:ATP ratios in excess of 1:1 inhibited the (Na+ +K+)-ATPase activity and also abolished the discontinuities in the Arrhenius plots. The addition of cholesterol to phosphatidylserine at a 1:1 mol ratio partially inhibited (Na+ +K+)-ATPase reactivation. Arrhenius plots under these conditions showed a single discontinuity at 20 degrees C and Ea values of 22 and 68 kcal/mol above and below this temperature respectively. The ouabain-insensitive Mg2+-ATPase normally showed a linear Arrhenius plot with an Ea of 8 kcal/mol. The cholesterol-phosphatidylserine mixed liposomes stimulated the Mg2+-ATPase activity, which now also showed a discontinuity at 20 degrees C with, however, an increased value of 14 kcal/mol above this temperature and 6 kcal/mol below. Kinetic studies showed that cholesterol had no significant effect on the Km values for ATP. Since both cholesterol and Mg2+ are known to alter the effects of temperature on the fluidity of phospholipids, the above results are discussed in this context.     

Fluidity of human erythrocyte membrane and effect of chlorpromazine on fluidity and phase separation of membrane

The fluidity of human erythrocyte membrane, and the effect of chlorpromazine at prelytic and lytic concentrations on the fluidity have been studied by using three kinds of fatty acid spin labels and measuring the temperature dependence of Mg2+-ATPase activity. The Arrhenius plot of the apparent rotational correlation time, tau c, for probes I(12,3) and I(5,10) showed an abrupt discontinuity at about 30 degrees C, and the plot for I(1,14) at 25 degrees C, indicating that a large difference in the fluidity exists between the interior and the outer surface of the lipid bilayer. The portions of the fatty acid chain near the ten carbon bond lengths removed from the bilayer surface became more fluid by chlorpromazine treatment; there was a decrease in the break point to around 26 degrees C following treatment with 0.6 or 1 mM of the drug. Two breaks at 21 and 30 degrees C in the Arrhenius plot of the Mg2+-ATPase activity were observed in normal erythrocyte membrane. The activation energy of the Mg2+-ATPase reaction has the values of 3.0 and 22.1 kcal/mol above the upper break and below the lower break, respectively. The drug exposure induced only a slight shift in the break temperatures, while the treatment significantly enhanced the associated activation energies of the reaction. These results suggest that the boundary phospholipids of the Mg2+-ATPase in the membrane are probably more rigid than the bulk lipids.     

Effect of NaCl addition on nanosecond O2 escaping reaction of myoglobin: evidences for the transition of myoglobin dynamic structure at 20 degrees C.

We studied the nanosecond (ns) geminate O2 escape reaction from the protein interior of myoglobin (Mb) to the solvent phase in the temperature range of 5-40 degrees C containing 0-0.1 M NaCl. In the flash photolysis experiments, we found that both the rate constant, kout, and its Arrhenius plot changed upon the variation of the NaCl concentration. In particular, it was noteworthy that the Arrhenius plot of kout dramatically changed in its slope, keeping the break at 20 degrees C, upon the addition of NaCl, indicating that the thermodynamic parameters such as an enthalpy of activation (delta H not equal to) and an entropy of activation (delta S not equal to) are different between above and below 20 degrees C, and that they are further altered upon the NaCl addition to the sample solution. From these results, we suggested that the Mb dynamic structure in the ns geminate O2 escape reaction is sensitively regulated by the interaction of the protein surface and the salt. The present study also showed that an inconsistency of the Arrhenius plot of kout between Chatfield et al. ((1990) J. Am. Chem. Soc. 112, 4680-4687) and us ((1990) J. Biol. Chem. 265, 18823-18828) is probably due to the difference in the solution condition.     

Conformational change in bacterio-opsin on binding to retinal.

The detailed mechanism of retinal binding to bacterio-opsin is important to understanding retinal pigment formation as well as to the process of membrane protein folding. We have measured the temperature dependence of bacteriorhodopsin formation from bacterio-opsin and all-trans retinal. An Arrhenius plot of the apparent second-order rate constants gives an activation energy of 11.6 +/- 0.7 kcal/mol and an activation entropy of -4 +/- 2 cal/mol deg. Comparison of the activation entropy to model compound reactions suggests that chromophore formation in bacteriorhodopsin involves a substantial protein conformational change. Cleavage of the polypeptide chain between residues 71 and 72 has little effect on the activation energy or entropy, indicating that the connecting loop between helices B and C is not involved in this conformational change.     

Characteristics of light-induced H+ transport in spinach chloroplast at lower temperatures II. A possible role of structured water in H+ transport of chloroplast near 0{degrees}C

Light-induced H⁺ transport in spinach chloroplasts at lowertemperatures was investigated with a glass electrode. Half-decaytime of the H⁺ transport on turning off the illumination increasedwith lowering of the temperature. However, near the freezingpoint of bulk water, the H⁺ transport showed no dependency ontemperature. An Arrhenius plot of the apparent first-order rate constantof H⁺ transport showed a break at about 8°C. Below thatcritical temperature, activation energy was about 0 kcal/mole. The break temperature in the Arrhenius plot shifted by 2–3°Cto a higher temperature in the presence of 10% glycerol, aneffective water structure-enhancing agent. On the other hand,addition of 5 mM NaSCN, known as a potent water structure breaker,abolished the break and a constant activation energy was obtainedover the entire low temperature range. A similar effect wasobserved in the presence of 50 mM urea. On the basis of these results, we propose a mechanism for theH⁺ transport of chloroplasts at lower temperatures involvingstructured water, where rapid proton transfer between hydrogen-bondedstructured water molecules takes place. (Received September 11, 1975; )     

Thermohemolysis of erythrocytes in the temperature range including physiologic (autohemolysis)]

The activation energy of thermohemolysis of erythrocytes changes from 36 +/- 5 kcal/mol (35-45 degrees C) to 97 +/- 5 kcal/mol (45-55 degrees C) at the temperature about 45 degrees C in isotonic buffer. The break on Arhenius' plot is preserved also when erythrocytes are placed into plasma. The character of Arhenius' plot is the same when erythrocyte hemoglobin is totally oxidated into methemoglobin by chemical way, though thermal stability of such erythrocytes is decreased. The scheme is presented in which thermohemolysis of erythrocytes occurs by two independent ways: thermodenaturation of hemoglobin (limiting stage of the process when t greater than 45 degrees C) and modification of membrane proteins by hemin, the last being a product of hemoglobin oxidation (limiting stage of the process when t less than 45 degrees C).     

Studies on the special properties of actomyosin in the gel form. I. Unusual features of the Mg2+-ATPase activity

The hydrolysis of MgATP by actomyosin gel at low ionic strength is known to show two unusual features: (1) an Arrhenius plot with a shallow slope in the higher temperature range (35-16 degrees C) and a steep slope in the lower temperature range (16-0 degrees C); (2) a rate curve of hydrolysis that begins with a 'burst' and falls to a lower steady-state level. Both of these can now be interpreted in terms of a specific, relatively slow transformation in the gel (t 1/2 = 9 s at 25 degrees C), induced by the binding of MgATP to the active sites of the myosin filaments. In the rate curves, this transformation is reflected in the transition from the burst rate (catalyzed by the original gel) to the steady-state rate (catalyzed by the modified gel). Importantly, this transition does not occur to a significant extent at low temperatures. Thus, in the typical nonlinear Arrhenius plot, where steady-state rates are used, the shallow slope in the high temperature range is a property of the modified gel, whereas the steep slope at low temperatures is a property of the original gel. Consistent with this interpretation, when the burst rates (presumably due to the original gel) were used in the high temperature range (and when substrate inhibition of hydrolysis by high levels of MgATP was avoided), the Arrhenius plot was linear over the entire temperature range (40-0 degrees C); the steep slope of this plot gives a high apparent heat of activation (25-30 kcal), similar to that reported for actin-activated hydrolysis by the soluble subfragment, heavy meromyosin. It is the steady-state form of the gel at high temperatures that gives a low apparent heat of activation (6-10 kcal). It was found that the regulatory proteins with calcium activate hydrolysis by the original form but have no effect on the steady-state form of the gel. Oxygen exchange measurements made during the burst and steady state at 25 degrees C indicate that the mechanism of hydrolysis is essentially the same for both, but that there is a higher effective actin concentration around the myosin sites in the original form.     

Factors influencing survival and growth of mammalian cells exposed to hypothermia. I. Effects of temperature and membrane lipid perturbers

The Arrhenius plot of the rate of V79 Chinese hamster cell inactivation due to hypothermia has a "break" around 7-10 degrees C with optimum storage temperature for unprotected cells being about 10 degrees C. Addition of the membrane lipid perturber, butylated hydroxytoluene, improves survival of cells when compared to controls at temperatures below this break but not above. Arrhenius plots of growth rates of the cells show breaks at 30 and 40 degrees C. Measurements of membrane fluidity by electron spin resonance or membrane polarization anisotropy by fluorescence spectrophotometry techniques as a function of temperature in these cells also reveal "breaks" centered around 8 and 30 degrees C. Hence, the changes in the rate of cell inactivation and growth as a function of temperature may be related to membrane lipid phase changes.     

Temperature-dependence of rapid axonal transport in sympathetic nerves of the rabbit.

Stop-flow techniques were used to determine how temperature affected the axonal transport of dopamine-beta-hydroxylase (DBH) activity in rabbit sciatic nerves in vitro. These nerves were cooled locally to 2 degrees C for 1.5 hr, which caused a sharp peak of DBH activity to accumulate above the cooled region. Accumulated DBH was then allowed to resume migration at various temperatures. From direct measurements of the rate of migration, we found that the axonal transport velocity of DBH was a simple exponential function of temperature between 13 degrees C and 42 degrees C. Over this range of temperatures, the results were well described by the equation: V=0.546(1.09)T, where V is velocity in mm/hr, and T is temperature in degrees centigrade. The Q10 between 13 degrees and 42 degrees C was 2.33, and an Arrhenius plot of the natural logarithm of velocity versus the reciprocal of absolute temperature yielded an apparent activation energy of 14.8 kcal. Transport virtually halted when temperature was raised to 47 degrees C, although only about half of the DBH activity disappeared during incubation at this temperature. Another transition occurred at 13 degrees C; below this temperature, velocity fell precipitously. This was not an artifact peculiar to the stop-flow system since the rate of accumulation of DBH activity proximal to a cold-block also decreased abruptly when the temperature above the block was reduced below 13 degrees C.