TY - JOUR
T1 - Vesicle-micelle transformation of phosphatidylcholine/octyl-β-D-glucopyranoside mixtures as detected with titration calorimetry
AU - Wenk, Markus R.
AU - Seelig, Joachim
PY - 1997/6/26
Y1 - 1997/6/26
N2 - The vesicle - micelle transition of lipid bilayers induced by the addition of the nonionic detergent octyl-β-d-glucopyranoside (OG) was studied with high-sensitivity titration calorimetry and spectroscopic methods. Sonified phospholipid vesicles composed of 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC) were titrated into OG solutions with concentrations between 15 and 22 mM. The critical OG concentration for bilayer micellization was determined as cD* = 15.4 ± 0.3 mM whereas the critical micellar concentration of pure OG was ccmc = 23.7 mM (in buffer). All calorimetric titrations were performed below the cmc of pure OG solutions. The titration curves can be explained by a superposition of three processes, namely (i) a partitioning of surfactant molecules into the lipid membrane, (ii) a membrane micellization, and (iii) a membrane re-formation. The basic process is a partitioning of OG molecules into the phospholipid vesicles which occurs during the whole titration experiment. It can be described according to Xb = KcD,f where Xb is the degree of binding (effective surfactant-to-lipid ratio) and cD,f is the equilibrium detergent concentration free in solution. The thermodynamic parameters were determined as K = 88 ± 3 M-1 and ΔHD° = 1.7 ± 0.4 kcal/mol for the transfer of OG from the aqueous phase to the membrane (15 mM ≤ cD° ≤ 22 mM). OG partitioning entails a bilayer micellization in the initial phase of the lipid-into-detergent titration experiment. Bilayer micellization is an endothermic process with ΔHmic = +1.85 ± 0.1 kcal/mol lipid. With continuous addition of lipid, bilayer micellization comes to a halt and is replaced by the reverse process. The demicellization process is exothermic with ΔHdemic = -1.84 ± 0.1 kcal/mol lipid. Micellization and demicellization are thus symmetrical processes. Once the free OG concentration falls below the critical limit of cD* = 15.4 mM, the titration curves follow the predictions of the partition model. A quantitative model is proposed to describe the excess heat, ΔH̄DE, of the bilayer ⇄ micelle equilibrium. To a first approximation, ΔH̄DE, follows the symmetrical mixing behavior of two closely related nonpolar liquids. Phosphorus-31 nuclear magnetic resonance and right-angle light scattering were used to monitor the structural changes of the OG/POPC mixtures. They confirm a phase boundary between the bilayer phase and the bilayer/micelle coexistence phase at cD* = 15.4 ± 0.3 mM and Xb = 1.36 ± 0.04. The phase boundary between the bilayer/micelle coexistence phase and the pure micellar phase is found for Xb ≥ 2.8. The calorimetric titrations can be used to construct a rather precise phase diagram of the POPC/OG system as the discontinuities of the titration curves define the critical concentrations of detergent and lipid at the phase boundaries.
AB - The vesicle - micelle transition of lipid bilayers induced by the addition of the nonionic detergent octyl-β-d-glucopyranoside (OG) was studied with high-sensitivity titration calorimetry and spectroscopic methods. Sonified phospholipid vesicles composed of 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC) were titrated into OG solutions with concentrations between 15 and 22 mM. The critical OG concentration for bilayer micellization was determined as cD* = 15.4 ± 0.3 mM whereas the critical micellar concentration of pure OG was ccmc = 23.7 mM (in buffer). All calorimetric titrations were performed below the cmc of pure OG solutions. The titration curves can be explained by a superposition of three processes, namely (i) a partitioning of surfactant molecules into the lipid membrane, (ii) a membrane micellization, and (iii) a membrane re-formation. The basic process is a partitioning of OG molecules into the phospholipid vesicles which occurs during the whole titration experiment. It can be described according to Xb = KcD,f where Xb is the degree of binding (effective surfactant-to-lipid ratio) and cD,f is the equilibrium detergent concentration free in solution. The thermodynamic parameters were determined as K = 88 ± 3 M-1 and ΔHD° = 1.7 ± 0.4 kcal/mol for the transfer of OG from the aqueous phase to the membrane (15 mM ≤ cD° ≤ 22 mM). OG partitioning entails a bilayer micellization in the initial phase of the lipid-into-detergent titration experiment. Bilayer micellization is an endothermic process with ΔHmic = +1.85 ± 0.1 kcal/mol lipid. With continuous addition of lipid, bilayer micellization comes to a halt and is replaced by the reverse process. The demicellization process is exothermic with ΔHdemic = -1.84 ± 0.1 kcal/mol lipid. Micellization and demicellization are thus symmetrical processes. Once the free OG concentration falls below the critical limit of cD* = 15.4 mM, the titration curves follow the predictions of the partition model. A quantitative model is proposed to describe the excess heat, ΔH̄DE, of the bilayer ⇄ micelle equilibrium. To a first approximation, ΔH̄DE, follows the symmetrical mixing behavior of two closely related nonpolar liquids. Phosphorus-31 nuclear magnetic resonance and right-angle light scattering were used to monitor the structural changes of the OG/POPC mixtures. They confirm a phase boundary between the bilayer phase and the bilayer/micelle coexistence phase at cD* = 15.4 ± 0.3 mM and Xb = 1.36 ± 0.04. The phase boundary between the bilayer/micelle coexistence phase and the pure micellar phase is found for Xb ≥ 2.8. The calorimetric titrations can be used to construct a rather precise phase diagram of the POPC/OG system as the discontinuities of the titration curves define the critical concentrations of detergent and lipid at the phase boundaries.
UR - https://www.scopus.com/pages/publications/0031163529
U2 - 10.1021/jp9707955
DO - 10.1021/jp9707955
M3 - Article
AN - SCOPUS:0031163529
SN - 1520-6106
VL - 101
SP - 5224
EP - 5231
JO - Journal of Physical Chemistry B
JF - Journal of Physical Chemistry B
IS - 26
ER -