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               360                                                                                 Membrane Structure


                                                                 face moves the N end of the headgroup −P-N dipole
                                                                                +
                                                                                                        +
                                                                 away from the membrane surface, and a negative charge
                                                                            +
                                                                 moves the N end towards the hydrocarbon phase. The
                                                                 out-of-plane movement of the phospholipid headgroup
                                                                 dipole creates a local electric field across the membrane,
                                                                                                    5
                                                                 which can easily reach a field strength of 10 V/cm. Such
                                                                 high electric fields can, in principle, entail conforma-
                                                                 tional changes of membrane-bound proteins, and the lipid
                                                                 dipole field could thus play a regulatory role in membrane
                                                                 function.
                                                                   If the membrane contains negatively charged lipids to
                                                                 begin with, the concentration of cationic compounds at
                                                                 the membrane surface is drastically enhanced, facilitating
                                                                 the binding and also providing an additional mechanism
                                                                 of electric modulation.


                                                                 D. Headgroup Orientation in Glycolipids and
                                                                    Glycosphingolipids and Their Influence on
                                                                    Phospholipid Headgroups
                                                                 The deuterium order parameter of headgroup-labeled
                                                                 glycolipids and glycosphingolipids generally show a
                                                                 headgroup orientation in which the sugar residues project
                                                                 essentially straight up from the bilayer surface into the
                                                                 aqueousregion,permittingmaximumhydrationoftheglu-
                                                                 cose hydroxyl groups by water. The glucosyl headgroup
                                                                 appears to be rather rigid, but rotates with a rotational
                                                                                      8 −1
                                                                 diffusion constant of ∼10 s .
                                                                   The headgroup conformational changes of deuterium-
               FIGURE 2 Deuterium magnetic resonance spectra of sn-2 and
                                                                 labeled PC observed in the presence of glycolipids and
               sn-3 phosphatidylcholine bilayers deuterated at different po-
               sitions (50 wt% lipid, 50 wt% H 2 O). (A) 1,2-dipalmitoyl-sn-  glycosphingolipids were shown to be qualitatively similar
               glycero-3-phosphocholine deuterated in both chains at the C-2 
  to those of negatively charged ions (cf. Fig. 4). However, in
               segment [Seelig and Seelig (1975). Biochim. Biophys. Acta 406,  comparison to the effects induced by charged substances,
                             
 2
               1]; (B) 1,3-bis-([2 ,2 - H 2 ]palmitoyl)-sn-glycero-2-phosphocholine

               [Seelig et al. (1980). Biochemistry 19, 2215); (C) 1,2-dipalmitoyl-  these effects were modest.
               sn-glycero 3-phosphocholine deuterated in both chains at the
               C-3 segment; (D) 1,2-dipalmitoyl-sn-glycero-3-phosphocholine


               deuterated in both chains at the C-10 segment [Seelig and Seelig  IV. HYDROPHOBIC CORE REGION
               (1974). Biochemistry 13, 4839].
                                                                 A. Fatty Acyl Chain Order in Saturated
                                                                    Lipid Membranes
               hydrophobic cations and anions, amphiphiles, and lipids
               have been shown to yield similar results when incorpo-  The hydrocarbon chains of the lipid bilayer are in a
               rated as guest molecules into PC or PE membranes. This  liquid-like state as evidenced by X-ray diffraction, elec-
               is demonstrated in Fig. 4, which summarizes the experi-  tron spin resonance spectroscopy, and differential scan-
               mental results in a rather condensed representation. If a  ning calorimetry studies. A quantitative characterization
               guest molecule is added to a headgroup deuterated phos-  of the hydrocarbon chain order in lipid bilayers by means
                                                                    2
               pholipid, the α- and β-quadrupole splittings ( ν α , ν β )  of H-NMR became possible by selectively deuterating
               change linearly with increasing concentration. In Fig. 4  both fatty acyl chains in a lipid molecule. Measurement
               the slopes, m α and m β , of such  ν α and  ν β versus  of the deuterium quadrupole splittings,  ν Q , allowed
               concentration plots are shown. A linear correlation ex-  calculation of the order parameter of the C D bond vec-
               ists between m α and m β , with a slope of −0.5 for cations  tor at each labeled carbon atom. The variation of the order
               and −1 for anions. The molecular interpretation is as fol-  parameter |S CD | with the position of the labeled carbon
               lows: A positive electric charge on the membrane sur-  atom in the membrane is the so-called “order profile.” An
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