Local measurement of lateral motion in erythrocyte membranes by photobleaching technique

The lateral diffusion coefficients ($\text{D}$) of the molecular fluorescence probe 3,3′-dioctadecylindocarbocyanine iodide (DII) in the membrane of discoid erythrocyte ghosts has been measured with the photobleaching technique between 7°C and 40°C. A fluorescence microscope which allows bleaching experiments within small local fields (approx. 1 μm²) at high magnification (X1600) has been used for these measurements. The diffusion coefficient increases from $\text{D = 9 · 10}{}^{\mathrm{?10}}\text{cm}{}^2\text{/s}$ to $\text{D = 7.5 · 10}{}^{\mathrm{?9}}\text{cm}{}^2\text{/s}$ from 7 to 40°C. An increase in membrane fluidity between 12°C and 17°C indicates a conformational change of the lipid bilayer moiety in this temperature region. The diffusion coefficient measured in the regions between the spicules of echinocytes is appreciably smaller than in the untransformed discoid ghosts. In the myelin tubes originating from cells, the lateral diffusion is somewhat larger (about a factor of 2) than in the non-transformed ghosts. With the fluorescence probe technique the rate of growth of myelin tubes of 0.3 μm diameter has been estimated.     

Carnitine uptake into human heart cells in culture

The uptake of radiolabeled carnitine and butyrobetaine has been studied in human heart cells (CCL 27). The uptake of carnitine is 3–10-fold higher in heart cells than in fibroblasts ($\text{pmol}\text{· μ}\text{g DNA}{}^{\mathrm{?1}}$). The uptake of carnitine increases with temperature coefficient $\text{K}{}_{\mathrm{<mtext>T</mtext>}}$ of 1.6 in the interval 10–20° C and with a negligible uptake at 4 and 10° C. The uptake of carnitine follows Michaelis-Menten kinetics with a $\text{K}{}_{\mathrm{<mtext>M</mtext>}}$ of $\text{4.8 ± 2.2 μ}\text{M}$ and $\text{V = 8.7 ± 3.2}\text{pmol}\text{· μ}\text{g DNA}{}^{\mathrm{?1}}\text{·}\text{h}{}^{\mathrm{?1}}$. Carnitine uptake is suppressed 90% by NaF (24 mM). Butyrobetaine is taken up into heart cells to the same extent as carnitine with a $\text{K}{}_{\mathrm{<mtext>M</mtext>}}$ of 5.7–17.3 μM and $\text{V = 8.7–9.3}\text{pmol}\text{· μ}\text{g DNA}{}^{\mathrm{?1}}\text{·}\text{h}{}^{\mathrm{?1}}$. Butyrobetaine inhibits competitively the uptake of carnitine and carnitine inhibits the uptake of butyrobetaine to the same extent. No conversion of radiolabeled butyrobetaine to carnitine, or carnitine to methyl choline was observed intra- or extracellulary during incubation. These data are compatible with a selective transport mechanism for carnitine which is also responsible for the uptake of butyrobetaine.     

Interaction of human fibrinogen with divalent metal chlorides

Precipitation of human fibrinogen in 0.15 m NaCl occurred at pH 7.4 (Tris-HCl buffer) when ZnCl₂, CuCl₂, NiCl₂, or CoCl₂ were added beyond their respective critical concentrations. The critical concentrations were about $\text{4 × 10}{}^{\mathrm{?5}}\text{m}\text{ZnCl}{}_2\text{, 6 × 10}{}^{\mathrm{?5}}\text{m}\text{CuCl}{}_2\text{, 3 × 10}{}^{\mathrm{?4}}\text{m}\text{NiCl}{}_2\text{and}\text{1 × 10}{}^{\mathrm{?3}}\text{m}\text{CoCl}{}_2$. At pH 5.8 2-(N-morpholino)-ethane sulphonic acid buffer, the critical concentrations were found only for CuCl₂ and ZnCl₂, and were about $\text{3 × 10}{}^{\mathrm{?5}}\text{and}\text{3 × 10}{}^{\mathrm{?4}}\text{m}$, respectively. CaCl₂ and MgCl₂ were not effective up to $\text{1 × 10}{}^{\mathrm{?2}}\text{and}\text{2 × 10}{}^{\mathrm{?2}}\text{m}$ at pH 7.4 and 5.8, respectively. At pH 7.4, precipitation was better in 0.015 m NaCl than in 0.15 m NaCl for both CuCl₂ and ZnCl₂. Little or no conformational change was indicated on binding Cu²⁺ ions. The fluorescence of tryptophan was quenched only by CuCl₂, while other metal ions (ZnCl₂, NiCl₂, CoCl₂ and CaCl₂) were ineffective as quenchers.     

Kinetics of phospholipid exchange between bilayer membranes

In an accompanying publication by Duckwitz-Peterlein, Eilenberger and Overath ((1977) Biochim. Biophys. Acta 469, 311–325) it is shown that the exchange of lipid molecules between negatively charged vesicles consisting of total phospholipid extracts from Escherichia coli occurs by the transfer of single lipid monomers or small micelles through the water. Here a kinetic interpretation is presented in terms of a rate constant, $\text{k}{}_{\mathrm{?}}$, for the escape of lipid molecules from the vesicle bilayer into the water. The evaluated rate constants are $\text{k}{}_{\mathrm{?}}{}^{\mathrm{<mtext>P</mtext>}}\text{= (0.86 ± 0.05) · 10}{}^{\mathrm{?5}}\text{s}{}^{\mathrm{?1}}$ and $\text{k}{}_{\mathrm{?}}{}^{\mathrm{<mtext>E</mtext>}}\text{= (1.09 ± 0.13) · 10}{}^{\mathrm{?6}}\text{s}{}^{\mathrm{?1}}$ for phospholipid molecules with $\text{trans-}\text{Δ}{}^9\text{-hexadecenoate}$ and $\text{trans-}\text{Δ}{}^9\text{-octadecenoate}$, respectively, as the predominant acyl chain component. The rate constants are discussed in terms of the acyl chain and polar head group composition of the lipids.     

Photophosphorylation in bacterial chromatophores entrapped in alginate gel: Improvement of the physical and biochemical properties of gel beads with barium as gel-inducing agent

The immobilization of Rhodopseudomonas capsulata chromatophores by entrapment in an alginate gel is described. Alginate beads were prepared with Ba²⁺, Sr²⁺ and Ca²⁺ as gel-forming agents and compared for their mechanical strength, chemical resistance against disruption by phosphate-induced swelling, and yield of photophosphorylation activity. Barium alginate beads proved to have better physico-chemical properties than the more commonly used calcium alginate beads. After embedding in barium alginate gel, R. capsulata chromatophores retained a high yield (up to 70%) of their photophosphorylation capacity. Alginate entrapment did not cause a large increase in the Michaelis constant for ADP and phosphate, the substrates of adenosinetriphosphatase (ATPase). These constants were $\text{K}{}^{\mathrm{ADP}}{}_{\mathrm{<mtext>m</mtext>}}\text{= 1.4 × 10}{}^{\mathrm{?5}}\text{m}$ and $\text{K}{}^{\mathrm{P}}{}_{\mathrm{i}}{}_{\mathrm{<mtext>m</mtext>}}\text{= 2.2 × 10}{}^{\mathrm{?4}}\text{m}$ for free chromatophores and $\text{K}{}^{\mathrm{ADP}}{}_{\mathrm{<mtext>m</mtext>}}\text{= 2.3 × 10}{}^{\mathrm{?4}}\text{m}$ and $\text{K}{}^{\mathrm{P}}{}_{\mathrm{i}}{}_{\mathrm{<mtext>m</mtext>}}\text{= 5.6 × 10}{}^{\mathrm{?4}}\text{m}$ for chromatophores entrapped in barium alginate gel. However, embedding gave no additional protection against rapid inactivation of chromatophores upon storage at 3°C. Preliminary results with a batch reactor for continuous ATP regeneration are presented. The barium alginate method has two features which are not generally encountered at the same time, extremely mild conditions for entrapment and excellent physical properties of the gels beads, which make this method a suitable tool for the construction of bioreactors with immobilized cells or organelles.     

A simple procedure for resolution of Escherichia coli RNA polymerase holoenzyme from core polymerase.

The association constant, K_A, for myosin subfragment-1 binding to actin was measured as a function of ionic strength [KCl, LiCl, and tetramethylammonium chloride (TMAC)]and temperature by the method of time-resolved fluorescence depolarization. The following thermodynamic values were obtained from solutions of 0.20 × 10^?6m S-1, 1.00 × 10^?6m actin in 0.15 m KCl, pH 7.0, at 25 °C: ΔG ° = ?39 ± 1 kJ M^?1, ΔH⁰ = 44 ± 2 kJ M^?1 and $\text{ΔS}{}^0\text{= 0.28 ± 0.01 kJ}\text{M}{}^{\mathrm{?1}}{}^0\text{K}{}^{\mathrm{?1}}$. For measurements in KCl (0.05 to 0.60 m), In $\text{K}{}_{\mathrm{a}}\text{= ?8.36 (KCl)}{}^{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$. Thus, the binding is endothermic and strongly inhibited by high ionic strength. When KCl was replaced by LiCl or TMAC the ionic effects on the binding were cation specific. The nature of actin-(S-1) binding in the rigor state is discussed in terms of these results.     

Histamine,theophylline and tryptamine transport through lipid bilayer membranes

Diffusion of histamine, theophylline and tryptamine through planar lipid bilayer membranes was studied as a function of pH. Membranes were made of egg phosphatidylcholine plus cholesterol (1 : 1 mol ratio) in tetradecane. Tracer fluxes and electrical conductances were used to estimate the permeabilities to nonionic and ionic species. Only the nonionic forms crossed the membrane at a significant rate. The membrane permeabilities to the nonionic species were: histamine, $\text{3.5 · 10}{}^{\mathrm{?5}}\text{cm}\text{· s}{}^{\mathrm{?1}}$; theophylline, $\text{2.9 · 10}{}^{\mathrm{?4}}\text{cm}\text{· s}{}^{\mathrm{?1}}$; and tryptamine, $\text{1.8 · 10}{}^{\mathrm{?1}}\text{cm}\text{· s}{}^{\mathrm{?1}}$. Chemical reactions in the unstirred layers are important in the transport of tryptamine and theophylline, but not histamine. For example, as pH decreased from 10.0 to 7.5 the ratio of nonionic (B) to ionic (BH⁺) tryptamine decreased by 300-fold, but the total tryptamine permeability decreased only 3-fold. The relative insensitivity of the total tryptamine permeability to the ratio, [B]/[BH⁺], is due to the rapid interconversion of B and BH⁺ in the instirred layers. Our model describing diffusion and reaction in the unstirred layers can explain some ‘anomalous’ relationships between pH and weak acid/base transport through lipid bilayer and biological membranes.     

Dopamine-stimulated cyclic AMP and binding of [3H]dopamine in acini from dog pancreas

Dispersed acini from dog pancreas were used to examine the ability of dopamine to increase cyclic AMP cellular content and the binding of [³H]dopamine. Cyclic AMP accumulation caused by dopamine was detected at 1·10^?8 M and was half-maximal at $\text{7.9±3.4·10}{}^{\mathrm{?7}}\text{M}$. The increase at 1·10^?5 M, (7.5-fold) was equal to the half-maximal increase caused by secretin at 1·10^?9 M. Haloperidol, a dopaminergic receptor antagonist inhibited cyclic AMP accumulation caused by dopamine. The IC₅₀ value for haloperidol, calculated from the inhibition of cyclic AMP increase caused by 1·10^?5 M dopamine was $\text{2.3±0.9·10}{}^{\mathrm{?6}}\text{M}$. Haloperidol did not alter basal or secretin-stimulated cyclic AMP content. [³H]Dopamine binding was studied on the same batch of cells as cyclic AMP accumulation. At 37°C, it was rapid, reversible, saturable and stereospecific. The $\text{K}{}_{\mathrm{<mtext>d</mtext>}}$ value for high affinity binding sites was $\text{0.43±0.1·10}{}^{\mathrm{?7}}\text{M}$ and $\text{4.7±1.6·10}{}^{\mathrm{?7}}\text{M}$ for low affinity binding sites. The concentration of drugs necessary to inhibit specific binding of dopamine by 50% was $\text{1.2±0.4·10}{}^{\mathrm{/t-7}}\text{M}$ noradrenaline, 2·10^/t-7 M epinine, $\text{4.1±1.8·10}{}^{\mathrm{/t-6}}\text{M}$ fluphenazine, $\text{8.0±1.6·10}{}^{\mathrm{/t-6}}\text{M}$ haloperidol, $\text{4.2±1.2·10}{}^{\mathrm{?6}}\text{M}$cis-flupenthixol, $\text{2.7±0.4·10}{}^{\mathrm{?5}}\text{M}$trans-flupenthixol, $\text{>1·10}{}^{\mathrm{?5}}\text{M}$ apomorphine, sulpiride, naloxone and isoproterenol.     

The use of 13C spin relaxation to investigate molecular motion in liquid tristearin

Longitudinal and transverse ¹³C spin relaxation times have been used to investigate the molecular motion of tristearin over a range of temperatures in the melt. Overall molecular rotational diffusion rates have been obtained as well as the diffusion rates about successive bonds in the stearoyl chains. The data can be explained using an anisotropic rotor model in which the fast and slow molecular diffusion rates are $\text{? 8 x 10}{}^9\text{sec}{}^{\mathrm{?1}}\text{and}\text{0.018 (2) x 10}{}^9\text{sec}{}^{\mathrm{?1}}$ respectively The alignment of the fast diffusion axis is close to the long chain axis of the ‘tuning fork’ model and the existence of such a configuration in the melt is supported by the observation of different relaxation times for the two chemically equivalent primary glyceryl carbons.The low flexibility gradient and high end group mobility of the acyl chain found at low temperatures in the melt is similar to that observed in lipid vesicle studies and suggest that the chains are aligned parallel. A break down of this short range order is apparent above 150°C.     

Weak acid-induced release of liposome-encapsulated carboxyfluorescein

Leakage of the entrapped anionic fluorophore carboxyfluorescein was used as a measure of the permeability of liposomes to several different acids. Carboxyfluorescein leakage increased with increasing buffer concentration at a given pH and depended on its chemical nature: apolar weak acids such as acetic or pyruvic acids induced fast leakage at relatively high pH (4 to 5), while glycine, aspartic, citric and hydrochloric acids induced leakage only at lower pH. Fluorescence leakage measurements reflected the acidification of the liposomes' aqueous spaces, which was primarily caused by the diffusion of undissociated acid molecules across the lipid bilayer. A simple mathematical model in accord with this hypothesis and assuming that carboxyfluorescein leakage was directly related to the proportion of its neutral lactone form, described satisfactorily the carboxyfluorescein leakage kinetics and allowed rough estimation of permeability coefficients for carboxyfluorescein (neutral lactone form; 9 · 10^?9 cm · s^?1), acetic acid ($\text{>1 · 10}{}^{\mathrm{?7}}\text{cm}\text{·}\text{s}{}^{\mathrm{?1}}$) and glycine (cation: 6 · 10^?9 cm · s^?1). These results are consistent with low effective proton permeability of liposomes ($\text{<5 · 10}{}^{\mathrm{?12}}\text{cm}\text{·}\text{s}{}^{\mathrm{?1}}$) and with the permeability coefficient of HCl (3 · 10^?3 cm · s^?1) reported by Nozaki and Tanford ((1981) Proc. Natl. Acad. Sci. U.S.A. 78, 4324–4328). Diffusion of weak acid molecules across lipid membranes has implications for drug encapsulation and delivery, and may be of biological significance.     

Electron transfer from pyridinyl radicals, hydrated electrons, CO2.- and O2.- to bacterial cytochrome P450.

Several rate constants for one-electron reduction of cytochrome P450 are more rapid in the absence than in the presence of the specific substrate. The respective values for methyl viologen, nicotinamide adenine dinucleotide and the 1-methyl-4-(and -3-)carbamidopyridinium radicals are 2.6, 3.4, 6 and 35 × 10⁷ M^?1 s^?1 without camphor, and 0.15, 0.1, 1.8 and 110 × 10⁷ M^?1 s^?1 for the camphor complex. Hydrated electrons react with cytochrome P450 with a rate constant of 3.0 × 10¹⁰ M^?1 s^?1 whether camphor is bound or not, but little of the reduction takes place at the haem iron. No reduction of the haem iron by $\text{CO}{}_2{}^{\mathrm{?-}}$ or $\text{O}{}_2{}^{\mathrm{?-}}$ could be detected, whether camphor is bound or not.     

Effect of angiotensin II on artificial lipid membranes

(5-Isoleucine)-angiotensin II applied to black lipid membranes produced current fluctuations varying between $\text{Δ>G = 5 · 10}{}^{\mathrm{?11}}\text{Ω}{}^{\mathrm{?}}$ and 3.5 · 10^?10 Ω^?1. These fluctuations depend on the voltage and the hydrostatic pressure. The membrane resistance is lowered by $\text{Δ>R = 6.1 · 10}{}^7\text{Ω · cm}{}^2$. With (5-isoleucine, 8-leucine)-angiotensin II the jumps are of a single amplitude ($\text{Δ>G = 2 · 10}{}^{\mathrm{?10}}\text{Ω}{}^{\mathrm{?1}}$). In both cases water and ions are transported across the membrane.     

Temperature dependence of N-phenyl-1-naphthylamine binding in egg lecithin vesicles

The temperature dependence of the binding of PhNapNH₂ ($\text{N-}\text{phenyl-1-naphthylamine}$) to vesicles of egg phosphatidylcholine has been determined. The Arrhenius plot of the association constant exhibits a discontinuity at 20.9 °C, some 30 °C above the broad phase transition region of the phospholipid. In the temperature range above 20 °C, $\text{ΔH}{}^0\text{= ?6100}\text{cal·mol}{}^{\mathrm{?1}}$ and $\text{ΔS}{}^0\text{= 9.7}\text{e. u.}$; in the temperature range below 20 °C, $\text{ΔH}{}^0\text{= 0}\text{cal · mol}{}^{\mathrm{?1}}$ and $\text{ΔS}{}^0\text{= 30.4}\text{e. u.}$ These values are consistent with the view that there are well ordered lipid-lipid bonds below 20 °C which are significantly less important above this temperature. The order in the temperature range of 5 to 20 °C, though significantly greater than that above 20 °C, is still significantly less than that in the crystalline state.     

The bimolecular decay rates of the flavosemiquinones of riboflavin,FMN and FAD

The bimolecular decay rates (2k) of the flavosemiquinones ($\text{FH}{}^{\mathrm{·}}\text{F}{}^{\mathrm{?}}$) of riboflavin, FMN and FAD have been determined using pulse radiolysis. The rates (defined as $\text{d}\text{[}\text{FH}{}^{\mathrm{·}}\text{F}{}^{\mathrm{?}}\text{]}\text{d}\text{t}\text{= ?2}\text{k}\text{[}\text{FH}{}^{\mathrm{·}}\text{F}{}^{\mathrm{?}}\text{]}{}^2$) for the neutral flavosemiquinones at zero ionic strength and pH 5.9 are (in units of mol^?1·dm³·s^?1): (1.2 ± 0.1)·10⁹, (5.0 ± 0.2)·10⁸ and (1.4 ± 0.1)·10⁸; and for the anionic flavosemiquinones at pH 11.2 (5.4 ± 0.9)·10⁸, (4.5 ± 0.3)·10⁷ and (8.5 ± 1.3)·10⁶, respectively. The kinetic salt effect has been used to formulate rate equations for each flavin to adjust for ionic strength effects.     

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.     

Interaction of anthracycline antibiotics with biopolymers: 9. Comparative study of the interaction kinetics of daunomycin,adriamycin and iremycin with DNA

The interaction kinetics of the three anthracycline antibiotics, daunomycin, adriamycin and iremycin, with calf thymus DNA has been investigated using the temperature-jump technique. Experimental data obtained at high binding ratio have been fitted by a kinetic theory which, for the binding of large ligands to a linear polymer chain, takes into account both nearest-neighbour ligand interaction and the overlap of potential binding sites. The kinetics of such cooperative binding according to a single-step mechanism can be described completely by two independent microscopic parameters, namely one rate constant and a kinetic cooperativity parameter. Both these parameters have been determined for the three anthracyclcine antibiotics, making use of the known equilibrium binding parameters. The association rate constant in the singly contiguous case turns out to be almost the same for all three antibiotics ($\text{7 × 10}{}^6\text{to 8 × 10}{}^6\text{1 mol}{}^{\mathrm{?1}}\text{s}{}^{\mathrm{?1}}$), while the corresponding dissociation rate constant ranges from 3.5 s^?1 for adriamycin to 10 s^?1 for daunomycin and about 35 s^?1 for iremycin. The different equilibrium binding constants thus correspond to different mean attachment times of the antibiotics at the polymer chain, which positively correlate with the inhibitory action of these drugs on in vitro DNA synthesis. Nearest-neighbour interaction in the case of adriamycin-DNA binding kinetics implies that adriamycin molecules dissociate from an isolated binding site nine times more frequently than from a site between two adjacent ligands.     

Cyclic AMP transport in human erythrocyte ghosts

10^?5 M cyclic AMP has high permeability in human erythrocyte ghosts ($\text{p = 0.061 · 10}{}^{\mathrm{?6}}\text{cm}\text{·}\text{s}{}^{\mathrm{?1}}$). Saturation of influx and efflux occurs. $\text{K}{}_{\mathrm{<mtext>z</mtext><mtext>t</mtext>}}{}^{\mathrm{<mtext>oi</mtext>}}\text{= 4.43}\text{mM}$. $\text{V}{}_{\mathrm{zt}}{}^{\mathrm{oi}}\text{= 259.6 μ}\text{M · min}{}^{\mathrm{?1}}$. $\text{K}{}_{\mathrm{<mtext>z</mtext><mtext>t</mtext>}}{}^{\mathrm{<mtext>io</mtext>}}\text{= 0.475 μ}\text{M}$. $\text{V}{}_{\mathrm{<mtext>z</mtext><mtext>t</mtext>}}{}^{\mathrm{<mtext>io</mtext>}}\text{= 28.3 μ}\text{M · min}{}^{\mathrm{?1}}$ at 30°C. Equilibrium exchange entry of cyclic AMP has similar kinetics to zero trans influx, though the system does show counterflow. Cythochalasin B is an apparent competitive inhibitor of cyclic AMP exit. ($\text{K}{}_{\mathrm{<mtext>i</mtext>}}\text{= 3.9 · 10}{}^{\mathrm{?7}}\text{M}$).Control experiments indicated that cyclic AMP remains intact during incubation with red blood cell ghosts and is contained within the intravesicular space during the transport experiments.     

Studies on the molecular weight of the adenovirus type 2 hexon and its subunit

The molecular weight of the adenovirus type 2 hexon was calculated from sedimentation equilibrium, light scattering and sedimentation and diffusion experiments. The extinction coefficient, E_{1 cm}^1%, was determined to be 14.3 at 279 nm, from quantitative nitrogen and carbon analyses combined with the N,C content calculated from the amino acid composition. Other parameters determined were: the partial specific volume, $\text{}\text{?}\text{gn = 0.738}\text{cm}{}^3\text{g}{}^{\mathrm{?1}}$; the refractive index increment, $\text{(}\text{?n}\text{?c}\text{)}{}_{\mathrm{<mtext>T,P</mtext><mtext>,\mu </mtext>}}\text{= 0.193}\text{cm}{}^3\text{g}{}^{\mathrm{?1}}$ at 435.8 nm; the sedimentation coefficient, s_20,w⁰ = 13.0 S; and the diffusion constant, D_{20, w}⁰ = 3.32 × 10^?7 cm² s^?1. All molecular weights were between 355,000 and 363,000. Crystal density measurements were made on native and glutaraldehyde cross-linked crystals and the molecular weights calculated from these data were compared with the precise molecular weight determined by physico-chemical methods.Only one polypeptide of molecular weight 120,000 was found in reduced, or reduced and alkylated, hexon. Four or six organomercurial molecules were bound per 120,000 molecular weight of native hexon upon titration with 2-chloromercuri-4-nitrophenol and 2-chloromercuri-4,6-dinitrophenol, respectively. With 5,5′-dithiobis (2-nitrobenzoic acid) only one SH-group per 120,000 could be titrated in native hexon, but after denaturation in 1% sodium dodeeyl sulphate five more SH-groups reacted per 120,000 molecular weight. Thus there are three identical polypeptides of molecular weight 120,000 per hexon of total molecular weight 360,000.