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Dynamic Structure of Lipid Bilayers Studied by ... - glia.cu-tokyo.ac.jp

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KAWATO. KINOSITA. AXD IKEGAMl“microviscosity” should be in the difference between the twoanalyses. In the present analysis, contributions <strong>of</strong> the anisotropicequilibrium on r(t) are considered separately; that is,qc is the viscosity only in the cone where probes can diffusepr<strong>ac</strong>tically. The “microviscosity” was estimated from thesteady-state anisotropy rs without regarding the restrictionson the rotational motion. Rather higher values <strong>of</strong> the “microviscosity”reported for DPPC suggest restrictions in therotational motion <strong>of</strong> perylene in the bilayer. In f<strong>ac</strong>t, preliminaryresults show that r(t) <strong>of</strong> perylene in DPPC vesicles followseq 14 indicating restrictions.Fluorescence Lifetime and Steady-State Intensity. Thefluorescence lifetime and the quantum yield Q are directlyrelated to the rates <strong>of</strong> emission k, and internal quenching k,<strong>by</strong> the relation:Therefore the sharp decrease <strong>of</strong> 7 at Tt may be induced <strong>by</strong> theincrease in thermal motion and in polarity around DPH dueto the transition, because k, is generally affected <strong>by</strong> thesef<strong>ac</strong>tors.As the natural lifetime 70 Ilk, is supposed to be constantin these experimental conditions, the quantum yield Q is proportionalto 7 and the ratio IrS/7 gives the relative number <strong>of</strong>DPH embedded in vesicles. The relative number <strong>of</strong> DPH in thebilayer increases about 10% at TI as shown in Figure 6.<strong>Dynamic</strong> Aspects <strong>of</strong> <strong>Lipid</strong> <strong>Bilayers</strong>. As DPH has a rod-likeshape, very similar to a hydrocarbon chain <strong>of</strong> lipid, DPH in thelipid bilayer should oc<strong>cu</strong>py just the same positions <strong>of</strong> chainsand their mole<strong>cu</strong>lar motion should reflect directly the motion<strong>of</strong> hydrocarbon chains.The estimated values <strong>of</strong> 8, shown in Figure 4 are about 20’even at the crystalline state, sufficiently below T,, and about70° above TI. These values indicate that the fairly large sp<strong>ac</strong>emust be attributed to the cone used to describe the wobblingdiffusion. It is very unnatural to consider that such a largesp<strong>ac</strong>e leaves a va<strong>cu</strong>um around e<strong>ac</strong>h DPH. A major part <strong>of</strong> thesp<strong>ac</strong>e should be oc<strong>cu</strong>pied <strong>by</strong> hydrocarbon chains to reduce voidvolume. DPH is permanently in collision with these chains andwobbles around <strong>ac</strong>cording to the thermal motion <strong>of</strong> hydrocarbonchains, and vice versa. The cone-like potential forwobbling diffusion is a conceptual one which indicates thetime-averaged arrangement <strong>of</strong> chains around DPH. Ratherlarge values <strong>of</strong> 8, at temperatures above Tr indicate a highlydisordered state <strong>of</strong> hydrocarbon chains.The wobbling diffusion constant is determined <strong>by</strong> the frequency<strong>of</strong> collisions between DPH and hydrocarbon chains and<strong>by</strong> the mean free rotational angle between successive collisions.As the density <strong>of</strong> hydrophobic region is not so much changed<strong>by</strong> the transition, the temperature dependence <strong>of</strong> D, shownin Figure 5 mainly indicates the change in the frequency <strong>of</strong>collisions, that is, the rate <strong>of</strong> chain motion. It should be notedthat no drastic change in the rate <strong>of</strong> chain motion was apparentat Tr and its temperature dependence was like the exponentialfunction. However, the orientational freedom <strong>of</strong> chains, or O,,changed like a sigmoidal transition.Contrary to this wobbling diffusion constant, a sigmoidaltransition in the lateral diffusion constant <strong>of</strong> lipids in DPPCvesicles at Tr was reported recently (Naqvi et al., 1974). Therate <strong>of</strong> lateral diffusion <strong>of</strong> lipids may be determined mainly b)the number <strong>of</strong> structural defects in the two-dimensional arrangements<strong>of</strong> lipids. Such defects should increase drasticallqat Tr corresponding to the increase <strong>of</strong> 0,.AcknowledgmentThe authors thank Pr<strong>of</strong>essor S. Ebashi for kindly makinghis apparatus available for the experiment.ReferencesAndrich, M. P., and Vanderkooi, J. M. (1976), Biochemistr).15, 1257.Badley, R. A., Martin, W. G., and Schneider, H. (1973).Biochemistry 12, 268.Chapman, D. (1975), Q. Rec. Biophys. 8, 185.Cogan, U., Shinitzky, M., Weber, G., and Nishida, T. ( I973),Biochemistry 12, 52 1.Hubbell, W. L., and McConnell, H. M. (197 l), J. Am. Chem.Soc. 93, 314.Inesi, G., Millman, M., and Eletr, S. (I 973), J. Mol. Bid. 81,483.Israel<strong>ac</strong>hvili, J., Sjosten, J., Eriksson, L. E. G., Ehrstrom, M..Graslund, A,, and Ehrenberg, A. (1975), Biochim. Biophys.Acta. 382, 125.J<strong>ac</strong>obson, K., and Papahadjopoulos, D. (1975), Biochemistr~,14, 152.Kinosita, K., Jr., Kawato, S., and Ikegami. A. (1977). Biophys.J. (to be published).Kinosita, K., Jr., Mitaku, S., Ikegami. A., Ohbo, N., and Kunii.T. L. (1976), Jpn. J. Appl. Phys. 15, 2433.Lentz, B. R., Barenholz, Y., and Thompson. T. E. (1976a).Biochemistry 15, 4521.Lentz, B. R., Barenholz, Y., and Thompson, T. E. (1976b).Biochemistry 15, 4529.Naqvi, K. R., Behr, J. P., and Chapman, D. (1974), Chem.Phys. Lett. 26, 440.R<strong>ac</strong>ker, E., and Hinkle, P. C. (1974), J. Membr. Biol. 17,181.S<strong>ac</strong>kmann, E., Trauble, H., Galla, H. J., and Overath, P.(1973), Biochemistry 12, 5360.Shinitzky M., and Barenholz, Y. (I 974), J. Biol. Chem. 249,2652.Shinitzky, M., Dianovx, A. C., Gitler, C., and Weber, G.(1971), Biochemistry IO, 2106.Tao, T. (l969), Biopolymers 8, 609.Trauble, H., and Eibl, H. (1974), Proc. Nufl. A<strong>cu</strong>d. Sci. 0.S.A.71, 214.Wahl, Ph., Auchet, J. C., and Donzel, B. (1974), Reu. Sci.Instrum. 45, 28.Whal, Ph., Kasai, M., and Changeux, J. P. (1971). Eur. J.Biochem. 18, 332.Weber, G., and Teale, F. W. J. (1957), Trans. Faraday SOC.53, 640.2324 BIOCHEMISTRY. VOL. 16, NO. 11, 1977

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