Phase transitions in phospholipid vesicles Fluorescence polarization and permeability measurements concerning the effect of temperature and cholesterol

We have studied the solid to liquid-crystalline phase transition of sonicated vesicles of dipalmitoylphosphatidylglycerol and dipalmitoylphosphatidylcholine. The transition was studied by both fluorescence polarization of perylene embedded in the vesicles, and by the efflux rate of trapped ²²Na⁺.Fluorescence polarization generally decreases with temperature, showing an inflection in the region 32–42°C with a mid-point of approximately 37.5 °C. On the other hand, the perylene fluorescence intensity increases abruptly in this region. To explain this result, we have proposed that, for $\text{T < T}{}_{\mathrm{<mtext>c</mtext>}}$ where $\text{T}{}_{\mathrm{<mtext>c</mtext>}}$ is the transition temperature, perylene is excluded from the hydrocarbon interior of the membranes, whereas, $\text{T < T}{}_{\mathrm{<mtext>c</mtext>}}$ this probe may be accommodated in the membrane interior to a large extent.The self-diffusion rates of ²²Na⁺ through dipalmitoylphosphatidylglycerol vesicles exhibit a complex dependence on temperature. There is an initial large increase in diffusion rates (approximately 100-fold) between 30 and 38 °C, followed by a decrease (approximately 4-fold) between 38 and 48 °C. A monotonic increase is then observed at temperatures higher than 48 °C. The local maximum of ²²Na⁺ self-diffusion rates at approximately 38 °C coincides with the mid-point of phase transition as detected by changes in fluorescence polarization of perylene with the same vesicles. Vesicles composed of dipalmitoylphosphatidylcholine show the same general behavior in terms of ²²Na⁺ self-diffusion rates at different temperatures, except that the local maximum occurs at approximately 42 °C.The temperature dependence of the permeability and the appearance of a local maximum at the phase transition region could be explained in terms of a domain structure within the plane of the membranes. This explanation is based on the possibility that boundary regions between liquid and solid domains would exhibit relatively high permeability to ²²Na⁺.Mixed vesicles composed of equimolar amounts of dipalmitoyl phospholipids and cholesterol show no abrupt changes in the temperature dependence of either perylene fluorescence polarization or ²²Na⁺ diffusion rate measurements. This is taken to indicate the absence of agross phase transition in the presence of cholesterol.     

Acid dissociation of cyclohexaamylose and cycloheptaamylose

Acid dissociation constants of aqueous cyclohexaamylose (6-Cy) and cycloheptaamylose (7-Cy) have been determined at 10–47 and 25–55°C, respectively, by pH potentiometry. Standard enthalpies and entropies of dissociation derived from the temperature dependences of these pK_a's are ΔH⁰ = 8.4 ± 0.3 kcal mol^?1, $\text{Δ}\text{S}{}^0\text{= ?28. ± 1}\text{cal mol}{}^{\mathrm{?1}}{}^0\text{K}{}^{\mathrm{?1}}$ for 6-Cy and ΔH⁰ = 10.0 ± 0.1 kcal mol^?1, $\text{Δ}\text{S}{}^0\text{= ?22.4 ±0.3}\text{cal mol}{}^{\mathrm{?1}}{}^0\text{K}{}^{\mathrm{?1}}$ for 7-Cy. Intrinsic ¹³C nmr resonance displacements of anionic 6- and 7-Cy were measured at 30°C in 5% D₂O ($\text{v}\text{v}$). These results indicate that the dissociation of 6- and 7-Cy involves both C2 and C3 2⁰-hydroxyl groups. The thermodynamic and nmr parameters are discussed in terms of interglucosyl hydrogen bonding.     

Membrane lipid fluidity as rate limiting in the concanavalin A-mediated agglutination of pyBHK cells

The initial rate of concanavalin A-mediated agglutination of polyoma transformed Baby Hamster Kidney (pyBHK) cells follows Arrhenius kinetics. There is a smooth decrease in the agglutination rate from 37°C to 22°C with an activation energy of $\text{11.8 ± 0.2}\text{kcal/mol}$ in this region. There is a sharp decrease in agglutination rate below 22°C. The addition of 0.1 mM 1,3-di-tert-2-hydroxyl-5-methylbenzene, a lipid perturber, increases the agglutination rate by a factor of two and increases the membrane lipid fluidity as determined by the spin label method. The rotational correlation time of the spin label 2N14 $\text{(2,2-}\text{dimethyl-5-dodecyl-5-methyloxazolidine}\text{-N-}\text{oxide}$) was measured. The sum of the enthalpy of activation of rotational diffusion and the enthalpy of activation of translational diffusion is very nearly equal to the enthalpy of activation of agglutination. This is consistent with the rate limiting step of agglutination being receptor diffusion, which is probably limited in pyBHK cells by membrane lipid fluidity.     

Calorimetric investigations of the helix-coil conversion of phenylalaninespecific transfer ribonucleic acid

The enthalpy of the helix-coil conversion of phenylalaninespecific transfer ribonucleic acid from brewer's yeast (tRNA^Phe_{brewer's yeast}) has been measured using both an LKB 10700-2 batch miciocalorimeter and an adiabatic differential scanning calorimeter. In the mixing calorimeter the conversion from coil to helix was induced by mixing a tRNA^Phe solution with a solution containing an excess of MgSO₄. We measured the enthalpy of this reaction stepwise in the temperature range from +9 to +60° C. For the enthalpy of folding of tRNA^Phe from coil to helix this method yielded the remarkably high value of ?310 $\text{kcal}\text{mole}$ of tRNA^Phe. With the differential scanning calorimeter in which the helix-coil conversion is simply induced by raising the temperature we found a value of +240 $\text{kcal}\text{mole}$ of tRNA^Phe at a Tm value of 76° C and a value of +200 $\text{kcal}\text{mole}$ of tRNA^Phe at a T_m value of 50° C. A comparison of the apparent van't Hoff enthalpies with the calorimetrically measured enthalpies shows, that the cooperativity of the system increases continually with rising melting temperatures - which are achieved by increasing Mg²⁺ concentrations - reaching a constant value at about 57° C. Above this temperature value the thermodynamic behaviour of the helix-coil conversion of tRNA^Phe may be approximately described by the model of an all-or-none process.     

Thermodynamics of the interaction of daunomycin with DNA

The association constant for the interaction of daunomycin with DNA was determined as a function of temperature (using [³H] daunomycin in conventional equilibrium dialysis cells) and ionic strength (using a spectrophotometric titration method). The association constant varied between 3.1 × 10⁶ M^?1 (4°C) and 3.9 × 10⁵ M^?1 (65°C). The free energy change was ?8.2 to ?8.8 $\text{kcal}\text{mol}$, the enthalpy change ?5.3 $\text{kcal}\text{mol}$ and the entropy change +10 to +11 eu, all values being consistent with that expected of an intercalation process. The apparent number of intercalation sites detected (0.15 to 0.16 per nucleotide) was independent of temperature. The large positive entropy change accompanying the interaction appeals to be due to extensive release of water from the DNA and daunomycin. The apparent number of binding sites increased dramatically with decrease of ionic strength, although the apparent association constant remained largely unaffected by ionic strength.     

Heat stabilization dependence on redox state of cytochrome cd1 oxidase from Pseudomonas aeruginosa

The irreversible thermal denaturation of cytochrome cd₁ oxidase from $\text{P.}\text{aeruginosa}$ as a function of the oxidation-reduction states of its hemes was observed with a differential scanning calorimeter. Upon full reduction of the four hemes, the apparent denaturation temperature decreases by about 10° and the denaturation enthalpy decreases slightly: oxidized, 5.9 cal/gm; reduced, 5.4 cal/gm. At pH 7.5, the first order rate constants for denaturation at 90°C are: reduced, 33 × 10^?3s^?1; oxidized, 3 × 10^?3s^?1. Thus, oxidation of the hemes reuults in heat stabilization of the cytochrome oxidase. The activation energy for denaturation of fully reduced oxidase, 53 kcal/mol, is less than that for fully oxidized protein (73 kcal/mol).     

Thermodynamics of the glutamate dehydrogenase catalytic reaction

The enthalpy change for the oxidative deamination of glutamate by NADP⁺ catalyzed by bovine liver glutamate dehydrogenase has been determined calorimetrically. The ΔH^o values are 64.6 ± 1.2 $\text{kJ}\text{mol}$ and 70.3 ± 1.2 $\text{kJ}\text{mol}$ at 25 and 35°C respectively. The equilibrium constants for the reaction at the two temperatures were determined spectrophotometrically. This enabled the determination of ΔG^o and ΔS^o of the reaction as well. ΔH^ovalues were also determined for the reaction using an alternative coenzyme and the deuterated substrate.     

Cytochalasin B inhibition and temperature dependence of 3-O-methylglucose transport in fat cells

The transport of $\text{3-O-}\text{methylglucose}$ in white fat cells was measured under equilibrium exchange conditions at $\text{3-O-}\text{methylglucose}$ concentrations up to 50 mM with a previously described method (Vinten, J., Gliemann, J. and Østerlind, K. (1976) J. Biol. Chem. 251, 794–800). Under these conditions the main part of the transport was inhibitable by cytochalasin B. The inhibition was found to be of competitive type with an inhibition constant of about 2.5 · 10^?7 M, both in the absence and in the presence of insulin (1μM). The cytochalasin B-insensitive part of the $\text{3-O-}\text{methylglucose}$ permeability was about 2 · 10^?9 cm · s^?1, and was not affected by insulin. As calculated from the maximum transport capacity, the half saturation constant and the volume/ surface ratio, the maximum permeability of the fat cell membrane to $\text{3-O-}\text{methylglucose}$ at 37°C and in the presence of insulin was 4.3 · 10^?6 cm · s^?1. From the temperature dependence of the maximum transport capacity in the interval 18–37°C and in the presence of insulin, an Arrhenius activation energy of $\text{14.8 ± 0.44}\text{kcal/mol}$ was found. The corresponding value was $\text{13.9 ± 0.89}$ in the absence of insulin. The half saturating concentration of $\text{3-O-}\text{methylglucose}$ was about 6 mM in the temperature interval used, and it was not affected by insulin, although this hormone increased the maximum transport capacity about ten-fold to 1.7 mmol · s^?1 per 1 intracellular water at 37°C.     

Effects of temperature and molecular interactions on the vibrational infrared spectra of phospholipid vesicles

Infrared spectra were obtained as a function of temperature for a variety of phospholipid/water bilayer assemblies (80% water by weight) in the 3000-950 cm^?1 region. Spectral band-maximum frequency parameters were defined for the 2900 cm^?1 hydrocarbon chain methylene symmetric and asymmetric stretching vibrations. Temperature shifts for these band-maximum frequencies provided convenient probes for monitoring the phase transition behavior of both multilamellar liposomes and small diameter single-shell vesiclesof dipalmitoyl phosphatidylcholine/water dispersions. As examples of the effects of bilayer lipid/cholesterol/water (3 : 1 mol ratio) and lipid/cholesterol/amphotericin B/water (3 : 1 : 0.1 mol ratios) vesicles were examined using the methylene stretching frequency indices. In comparison to the pure vesicle form, the transition width of the lipid/cholesterol system increased by nearly a factor of two (to 8°C) while the phase transition temperature remained approximately the same (41° C). For the lipid/cholesterol/amphotericin B system, the phase transition temperature increased by about 4.5° C (to 45.5°C) with the transition width increasing by nearly a factor of four ($\text{to}\text{≈ 15°}\text{C}$) above that of the pure vesicles. The lipid/cholesterol/amphotericin B data were interpreted as reflecting the formation below 38°C of a cholesterol/amphotericin B complex whose dissociation at higher temperature (38–60°C range) significantly broades the gel-liquid crystalline phase transition.     

Orientational order in the choline headgroup of sphingomyelin: A 14N-NMR study

An aqueous dispersion of fully hydrated bovine sphingomyelin was studied using ¹⁴N-NMR spectroscopy. Spectra were obtained as a function of temperature over the range 15–80°C, in both the liquid crystal and gel phases. In the liquid crystal phase, powder pattern lineshapes were obtained, whose quadrupolar splitting slowly decreases with increasing temperature. The spectra are increasingly broadened as the temperature is lowered through the phase transition into the gel phase. The linewidths and the second moments of these spectra indicate that the onset of a broad phase transition occurs at approx. 35°C, in agreement with previous calorimetric and ³¹P-NMR measurements. There is no evidence from the lineshapes for an hexagonal phase in this system, and this conclusion is supported by X-ray diffraction measurements carried out on aqueous dispersions of sphingomyelin in both phases. Assuming that the static nitrogen quadrupole coupling constant is the same for both sphingomyelin and dipalmitoyl-l-α-phosphatidylcholine (DPPC), the decrease observed in the quadrupolar splitting of sphingomyelin compared to that of DPPC indicates that the orientational order of the choline headgroup in liquid crystalline sphingomyelin is not the same as that of its counterpart in DPPC. Preliminary relaxation time measurements of $\text{T}{}_1$ and $\text{T}{}_2$ are presented which suggest that there are also dynamic differences between sphingomyelin and DPPC in the choline headgroup.     

Phase transition characteristics of diphosphatidylglycerol (cardiolipin) and stereoisomeric phosphatidyldiacylglycerol bilayers: Mono- and divalent metal ion effects

Synthesis and phase transition characteristics of aqueous dispersions of the homologous (12 : 0, 14 : 0, 16 : 0) diphosphatidylglycerols (cardiolipins) and phosphatidyldiacylglycerols are reported. Electron microscopy of the negatively stained aqueous dispersions reveals a characteristic lamellar structure suggesting that these phospholipid molecules are organized as bilayers in the aqueous dispersions. The phase transition temperature ($\text{T}{}_{\mathrm{<mtext>m</mtext>}}$) and the enthalpy of transition ($\text{ΔH}$) increase monotonically with chain length in the cardiolipin and phosphatidyldiacylglycerol series; $\text{T}{}_{\mathrm{<mtext>m</mtext>}}$ for phosphatidyldiacylglycerol is higher than that for cardiolipin of the same chain-length. The transition temperatures for the enantiomeric $\text{sn-3,3-}\text{and}\text{sn-1,1-}\text{phosphatidyldiacylglycerol}$ and for the diastereomeric, $\text{meso}\text{-sn-1,3-}\text{phosphatidyldiacylglycerol}$ are approximately the same. The molar enthalpy for the transition of cardiolipin-NH₄⁺ bilayers is approximately twice the value for the phosphatidylcholines of the same chain length, i.e., the molar enthalpy per acyl chain is approximately the same in the two systems. The transition temperatures for metal ion salts of C_{1 6}-cardiolipin exhibit a biphasic dependence upon the unhydrated ionic radii, i.e. the highest $\text{T}{}_{\mathrm{<mtext>m</mtext>}}$ is observed for Ca²⁺- cardiolipin and decreases for the salts of ions with smaller and larger ionic radii than that of Ca²⁺. The lowest $\text{T}{}_{\mathrm{<mtext>m</mtext>}}$ is observed for Rb⁺-cardiolipin. Monovalent metal salts of cardiolipin exhibit two phase transitions. This effect may result from different conformational packing of the four acyl chains due to differences in metal-phosphate binding.     

Increase in temperature induces the Z to B transition of poly[d(G-C)] in water-ethanol solution

An increase in temperature from 20 to 50° C results in the complete transition from the Z to B form of poly(d(G-C)], dissolved in a 55% ethanol-water solution. The transition is fully reversible and displays a slow kinetics. The transition profiles for the free polynucleotide and for that in the presence of ethidium bromide, which is known to stabilize the B form, are obtained by circular dichroism. Based on these data the enthalpy value for the B-Z transition in our conditions is estimated to be ΔH_BZ = ?0.7 $\text{kcal}\text{mol}$.     

Thermodynamic and kinetic parameters of an oligonucleotide hairpin helix

The thermodynamics of the hairpin helix-single strand transition of A₆C₆U₆ has been analyzed by a staggering zipper model with consideration of single strand stacking. This analysis yields an enthalpy change of +11 kcal/mole for the formation of a first, isolated base pair. The stability constant of a first (intramolecular) base pair in A₆C₆U₆ is around 2 × 1O^?5 at 25°C, whereas a first (intermoleciilar) base pair in an A₆ · U₆ helix is characterised by a stability constant of about 4 × 10^?3M^?1 (25°C, extrapolated from A_n · V_n oligomer measurements). These data indicate a destabilizing effect of the C₆ loop.The rate constant of hairpin helix formation is 2 to 3 × 10⁴ sec^?1 associated with an activation enthalpy of +2.5 kcal/mote. The rate of helix dissociation of the A₆C₆U₆ hairpin is in the range of 10³ to lO⁵ sec^?1 with an activation enthalpy of 21 $\text{kcal}\text{mole}$. A comparison with the kinetic parameters obtained for A · U oligomer helices shows a specific influence of the C₆ loop due to the stacking tendency of the cytosine residues. This intluence is preferentially reflected in the relatively low value of the rate constant of helix formation.     

Kinetics of monensin complexation with sodium ions by 23Na NMR spectroscopy

The kinetics of the sodium binding to the ionophore monensin (Mon) in methanol has been studied by ²³Na NMR spectroscopy. Fast quadrupole relaxation of the bound sodium affected the relaxation rate of the free sodium through an exchange process between these two species. The exchange was found to be dominated by the reaction: Na⁺ + Mon^? ? MonNa. The dissociation rate constant at 25°C is 63 s^?1, with an activation enthalpy of 10.3 $\text{kcal}\text{mol}$ and activation entropy of ?15.8 $\text{cal}\text{mol}$ deg. These results indicate that the specificity of the binding of sodium ions to monensin is reflected in the relatively slow dissociation process. The entropy changes indicate that the activated monensin-sodium complex undergoes a conformational change, but the existence of a conformational change in monensin anion prior to complexation is excluded.     

Thermal phase transitions in the polar lipids of plant membranes. Their induction by disaturated phospholipids and their possible relation to chilling injury

The phase behaviour of leaf polar lipids from three plants, varying in their sensitivity to chilling, was investigated by differential scanning calorimetry. For the lipids from mung bean (Vigna radiata L. var. Berken), a chilling-sensitive plant, a transition exotherm was detected beginning at $\text{10 ± 2°}\text{C}$. No exotherm was evident above 0°C with polar lipids from wheat (Triticum aestivum cv. Falcon) or pea (Pisum sativum cv. Massey Gem), plants which are insensitive to chilling. The enthalpy for the transition in the mung bean polar lipids indicated that only about 7% w/w of the lipid was in the gel phase at ?8°C. The thermal transition of the mung bean lipids was mimicked by wheat and pea polar lipids after the addition of 1 to 2% w/w of a relatively high melting-point lipid such as dipalmitoylphosphatidylcholine, dipalmitoylphosphatidylglycerol or dimyristoylphosphatidylcholine. Analysis of the polar lipids from the three plants showed that a dipalmitoylphosphatidylglycerol was present in mung bean (1.7% w/w) and pea (0.3% w/w) but undetected in wheat, indicating that the transition exotherm temperature of 10°C in mung bean, 0°C in pea and about ?3°C in wheat correlates with the proportion of the high melting-point disaturated component in the polar lipids. The results indicate that the transition exotherm, observed at temperatures above 0°C in the membranes of chilling-sensitive plants, could be induced by small amounts of high melting-point lipids and involves only a small proportion of the membrane polar lipids.     

Analysis of protein self-association by combined calorimetric and molecular sieve studies: application to beta-lactoglobulin A

The application of isothermal calorimetry to the study of self-association reactions between identical protein subunits has been explored to assess the types of information obtainable from heat of dilution curves (i.e., the molar heat of dilution as a function of total solute concentration). Relationships between the heat of dilution, subunit association constants, and enthalpies of formation for the various association complexes in a self-associating system have been formulated. A method is described for constructing heat of dilution curves from sequential step-wise dilution experiments in a batch-type calorimeter. The relationship between calorimetric and van't Hoff enthalpies is formulated for systems undergoing self-association reactions. Comparison between the two is shown by numerical simulation to provide a very sensitive test for the presence of intermediate species.Calorimetric measurements were made on the self-association of β?lactoglobulin-A at 5.0 °C, pH 4.65, in 0.1 m NaCl and in 0.1 m acetate. Heat of dilution curves constructed from these data were used to estimate the equilibrium constant and enthalpy of formation, assuming a monomer-tetramer association process. Values of 31 ± 4 kcal/mole tetramer for the enthalpy and 1.3 ± 1.0 × 10¹¹ liter³/mole³ for the constant of tetramerization were determined from the calorimetric measurements in NaCl. The corresponding values for calorimetric measurements in acetate were 33 ± 4 kcal/mole and 1.6 ± 1.0 × 10¹¹ liter³/mole³.The calorimetric results were compared with thermodynamic information obtained from association data between 5 and 25 °C in 0.1 m acetate using molecular sieve chromatography. Within experimental error, the molecular sieve data at 5 °C could be fit to a monomer-tetramer association reaction with a monomer molecular weight of 36,000. From these studies a van't Hoff enthalpy of 38 ± 4 kcal/mole tetramer and an equilibrium constant of 4.6 ± 1.0 × 10¹¹ liter³ mole³ at 5 °C were obtained. Comparison between calorimetric and van't Hoff enthalpies indicates that the self-association of β-lactoglobulin-A under these conditions can be adequately described by a monomer-tetramer reaction. The results suggest that, a small fraction (e.g., 5–10%) of species having intermediate states of aggregation may be present, but preclude the presence of large fractions of intermediate species having appreciable enthalpies of association.     

Characterization of the phase behavior of phosphonolipids in model and biological membranes by 31P-NMR

³¹P-NMR is used to characterize the phase behavior of phosphonolipids in both model and biological membranes. ($\text{1′,2′-}\text{Dipalmitoyl}\text{-sn-}\text{glyceryl)-2-aminoethylphosphonate}$ gives rise to static chemical shift tensor elements (?87, 5 and 63 ppm) which differ considerably from those reported for the analogous phospholipid, $\text{1,2-}\text{dipalmitoyl}\text{-sn-}\text{glycero-3-phosphoethanolamine}$ (?81, ?20 and 105 ppm). Phosphonolipid, as well as a mixture of phosphonolipid and $\text{1,2-}\text{dipalmitoyl}\text{-sn-}\text{glycero-3-phosphocholine}$, in aqueous dispersion gives rise to ³¹P spectra which may be interpreted in terms of lamellar structures. A mixture of phosphonolipid and egg phosphatidylethanolamine exhibits a bilayer-to-hexagonal phase transition with a concomitant decrease by one-half in the value of the ³¹P chemical shift anisotropies of both the phosphonate and phosphate resonances. The chemical shift anisotropy associated with phosphonolipid has been found to be consistently smaller than that observed for the analogous phospholipid. ³¹P-NMR spectra of total lipid extracts of Tetrahymena sp. indicate that both phospho- and phosphonolipids have a bilayer organization between ?20 and 20°C.     

Effect of pH,mono- and divalent cations on the mixing of phosphatidylglycerol with phosphatidylcholine. A monolayer (π, ΔV) and fluorescence study

The mixing of various molecular species of phosphatidylglycerol and phosphatidylcholine differing in their acyl chain lengths has been studied both in monolayers (π, Δ$\text{V}$), and in water dispersions (fluorescence polarization) with varying pH and ionic strength of the aqueous phase and in the presence of the divalent cations Mg²⁺ and Ca²⁺. In dilauroylphosphatidylglycerol/dipalmitoylphosphatidylcholine mixtures, both in monolayers and in water dispersions, no phase separation was detected at pH 2.9 where phosphatidylglycerol was protonated. With dipalmitoylphosphatidylglycerol/dipalmitoylphosphatidylcholine mixtures, in monolayers and at the same pH, no phase separation was detected for surface pressures below $\text{π = 40}\text{mN}\text{·}\text{m}{}^{\mathrm{?1}}$. In monolayers, and under ionic conditions such that phosphatidylglycerol was ionized (pH 5.6, 10 mM NaCl) miscibility was observed with dilauroylphosphatidylglycerol and dipalmitoylphosphatidylcholine and also with dipalmitoylphosphatidylglycerol and dilauroylphosphatidylcholine. Varying the ionic strength did not alter the miscibility of these lipids. The divalent cations Mg²⁺ and Ca²⁺ did not modify that of dilauroylphosphatidylglycerol with dilauroylphosphatidylcholine or with dipalmitoylphosphatidylcholine. Both in monolayers and in water dispersions, dipalmitoylphosphatidylglycerol and dilauroylphosphatidylcholine appeared to be at least partly miscible, in the presence of magnesium. Only in the presence of calcium and at high surface pressure might the monolayer data account for phase separation between these two lipids. The data presented demonstrate the existence of strong cohesive forces between phosphatidylcholine and phosphatidylglycerol with a marked influence of the former on the physical state of the latter. From an analysis of the Δ$\text{V}$ data, it is suggested that intrafacial hydrogen bonds may play a significant role in stabilizing phosphatidylcholine/phosphatidylglycerol mixtures.     

Investigations on purine and pyrimidine bases stacking associations in aqueous solutions by the fluorescence quenching method: III. Intramolecular association of 9,9'-[1,3-propylene]-bis-2-aminopurine

General equations relating fluorescence quantum yield and lifetime of a compound with its intramolecular stacking equilibrium and kinetics were derived. Intramolecular stacking association of 9,9'-[1,3-propylene]-bis-2-aminopurine in aqueous solution was examined within the range of temperatures from 0 to 90°C. A two-state thermodynamic model of the association was verified. The stacking enthalpy and entropy can be taken, with a good approximation, as temperature-independent (δH = ?2.0 $\text{kcal}\text{mol}$, ΔS = ?3.25 e.u.) although the function ΔG = ?0.00886 T² + 8.847 T ?2876 describes more precisely the observed changes of stacking free enthalpy with temperature. The association rate constants were determined. Activation energy of the reaction (2 $\text{kcal}\text{mol}$) is the same as in the case of association between free 2-aminopurine molecules. It confirms a two-step mechanism of the process. The advantages and shortcomings of the fluorescence quenching method are discussed.