Dynorphin induced magnetic ordering in lipid bilayers as studied by 31P NMR spectroscopy

AbstractLipid bilayers of dimyristoyl phosphatidylcholine (DMPC) containing opioid peptide dynorphin A(1–17) are found to be spontaneously aligned to the applied magnetic field near at the phase transition temperature between the gel and liquid crystalline states (Tm=24°C), as examined by 31P NMR spectroscopy. The specific interaction between the peptide and lipid bilayer leading to this property was also examined by optical microscopy, light scattering, and potassium ion-selective electrode, together with a comparative study on dynorphin A(1–13). A substantial change in the light scattering intensity was noted for DMPC containing dynorphin A(1–17) near at Tm but not for the system containing A(1–13). Besides, reversible change in morphology of bilayer, from small lipid particles to large vesicles, was observed by optical microscope at Tm. These results indicate that lysis and fusion of the lipid bilayers are induced by the presence of dynorphin A(1–17). It turned out that the bilayers are spontaneously aligned to the magnetic field above Tm in parallel with the bilayer surface, because a single 31P NMR signal appeared at the perpendicular position of the 31P chemical shift tensor. In contrast, no such magnetic ordering was noted for DMPC bilayers containing dynorphin A(1–13). It was proved that DMPC bilayer in the presence of dynorphin A(1–17) forms vesicles above Tm, because leakage of potassium ion from the lipid bilayers was observed by potassium ion-selective electrode after adding Triton X-100. It is concluded that DMPC bilayer consists of elongated vesicles with the long axis parallel to the magnetic field, together with the data of microscopic observation of cylindrical shape of the vesicles. Further, the long axis is found to be at least five times longer than the short axis of the elongated vesicles in view of simulated 31P NMR lineshape

Morphological Behavior of Lipid Bilayers Induced by Melittin near the Phase Transition Temperature

Morphological changes of DMPC, DLPC, and DPPC bilayers containing melittin (lecithin/melittin molar ratio of 10:1) around the gel-to-liquid crystalline phase transition temperatures (Tc) were examined by a variety of biophysical methods. First, giant vesicles with the diameters of ∼20 μm were observed by optical microscopy for melittin-DMPC bilayers at 27.9°C. When the temperature was lowered to 24.9°C (Tc = 23°C for the neat DMPC bilayers), the surface of vesicles became blurred and dynamic pore formation was visible in the microscopic picture taken at different exposure times. Phase separation and association of melittin molecules in the bilayers were further detected by fluorescent microscopy and mass spectrometry, respectively. These vesicles disappeared completely at 22.9°C. It was thus found that the melittin-lecithin bilayers reversibly undergo their fusion and disruption near the respective Tcs. The fluctuation of lipids is, therefore, responsible for the membrane fusion above the Tc, and the association of melittin molecules causes membrane fragmentation below the Tc. Subsequent magnetic alignments were observed by solid-state (31)P NMR spectra for the melittin-lecithin vesicles at a temperature above the respective Tcs. On the other hand, additional large amplitude motion induced by melittin at a temperature near the Tc breaks down the magnetic alignment

Conformation and Dynamics of the [3-(13)C]Ala, [1-(13)C]Val-Labeled Truncated pharaonis Transducer, pHtrII(1–159), as Revealed by Site-Directed (13)C Solid-State NMR: Changes Due to Association with Phoborhodopsin (Sensory Rhodopsin II)

We have recorded (13)C NMR spectra of the [3-(13)C]Ala, [1-(13)C]Val-labeled pharaonis transducer pHtrII(1–159) in the presence and absence of phoborhodopsin (ppR or sensory rhodopsin II) in egg phosphatidylcholine or dimyristoylphosphatidylcholine bilayers by means of site-directed (amino acid specific) solid-state NMR. Two kinds of (13)C NMR signals of [3-(13)C]Ala-pHtrII complexed with ppR were clearly seen with dipolar decoupled magic angle spinning (DD-MAS) NMR. One of these resonances was at the peak position of the low-field α-helical peaks (α(II)-helix) and is identified with cytoplasmic α-helices protruding from the bilayers; the other was the high-field α-helical peak (α(I)-helix) and is identified with the transmembrane α-helices. The first peaks, however, were almost completely suppressed by cross-polarization magic angle spinning (CP-MAS) regardless of the presence or absence of ppR or by DD-MAS NMR in the absence of ppR. This is caused by an increased fluctuation frequency of the cytoplasmic α-helix from 10(5) Hz in the uncomplexed states to >10(6) Hz in the complexed states, leading to the appearance of peaks that were suppressed because of the interference of the fluctuation frequency with the frequency of proton decoupling (10(5) Hz), as viewed from the (13)C NMR spectra of [3-(13)C]Ala-labeled pHtrII. Consistent with this view, the (13)C DD-MAS NMR signals of the cytoplasmic α-helices of the complexed [3-(13)C]Ala-pHtrII in the dimyristoylphosphatidylcholine (DMPC) bilayer were partially suppressed at 0°C due to a decreased fluctuation frequency at the low temperature. In contrast, examination of the (13)C CP-MAS spectra of [1-(13)C]Val-labeled complexed pHtrII showed that the (13)C NMR signals of the transmembrane α-helix were substantially suppressed. These spectral changes are again interpreted in terms of the increased fluctuation frequency of the transmembrane α-helices from 10(3) Hz of the uncomplexed states to 10(4) Hz of the complexed states. These findings substantiate the view that the transducers alone are in an aggregated or clustered state but the ppR-pHtrII complex is not aggregated. We show that (13)C NMR is a very useful tool for achieving a better understanding of membrane proteins which will serve to clarify the molecular mechanism of signal transduction in this system