Comformation and absolute configuration of -methyllanthionine

If the bicyclic peptide ring proposed by Gross $\text{et}$$\text{al}$. (1,2) does in fact exist in nisin and related antibiotics, then the unusual β-methyllanthionine component must be significantly distorted from its conformation in the free state, as determined by x-ray structure analysis. The torsion angles about the SC_β bonds are 50–100° from the torsion angles in models of the sulfur-bridged peptide ring proposed for nisin. The chirality of the methylated β-carbon atom is (S). The conformation of the amino acid differs from that of $\text{meso}$-lanthionine only by a 180° rotation of a carboxyl group about the $\text{C}{}_{\mathrm{\alpha }}{}^{\mathrm{D}}\text{C}{}_{\mathrm{\beta }}\text{(CH}{}_3\text{)}$ bond.     

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.     

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.     

Defective PAPS-synthesis in epiphyseal cartilage from brachymorphic mice

Activity levels of sulfotransferases, requisite for the sulfation of chondroitin sulfate proteoglycan, were measured in cell-free homogenates prepared from neonatal epiphyseal cartilage of normal C57B1/6J or homozygous brachymorphic mice. In the presence of [³⁵S]-PAPS only or [³⁵S]-PAPS plus an exogenous sulfate acceptor, comparable amounts of ${}^{35}\text{SO}{}_4{}^{\mathrm{2?}}$ were incorporated into chondroitin sulfate by the normal and mutant types of cartilage. In contrast, the mutant cartilage catalyzed the conversion of only 30% of the ${}^{35}\text{SO}{}_4{}^{\mathrm{2?}}$ into chondroitin sulfate as compared to normal mouse cartilage when synthesis was initiated from ATP and H₂³⁵SO₄. These results suggest that the production of an undersulfated proteoglycan which has previously been reported in brachymorphic mice (Orkin, R.W. $\text{et}\text{al}$. (1976) Devel. Biol. $\text{50}$, 82–94) may result from a defect in the synthesis of the sulfate donor PAPS.     

Phospholipid exchange between bilayer membranes

The mode of interaction of aqueous dispersions of phospholipid vesicles is investigated. The vesicles (average diameter 950 Å) are prepared from total lipid extracts of Escherichia coli composed of phosphatidylethanolamine, phosphatidylglycerol and cardiolipin. One type of vesicle contains $\text{trans-}\text{Δ}{}^9\text{-octadecenoate}$, the other type $\text{trans-}\text{Δ}{}^9\text{-hexadecenoate}$ as predominant acyl chain component. The vesicles show order?disorder transitions at transition temperatures, $\text{T}{}_{\mathrm{<mtext>t</mtext>}}\text{= 42°}\text{C}$ and $\text{T}{}_{\mathrm{<mtext>t</mtext>}}\text{= 29°}\text{C}$, respectively. A mixture of these vesicles is incubated at 45° C and lipid transfer is studied as a function of time using the phase transition as an indicator. The system reveals the following properties: Lipids are transferred between the two vesicle types giving rise to a vesicle population where both lipid components are homogeneously mixed. Lipid transfer is asymmetric, i.e. $\text{trans-}\text{Δ}{}^9\text{-hexadecenoate}$-containing lipid molecules appear more rapidly in the $\text{trans-}\text{Δ}{}^9\text{-octadecenoate}$-containing vesicles than vice versa. At a given molar ratio of the two types of vesicles the rate of lipid transfer is independent of the total vesicle concentration. It is concluded that lipid exchange through the water phase by way of single molecules or micelles is the mode of communication of these negatively charged lipid vesicles.     

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.     

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.     

Characterization of the sub-transition of hydrated dipalmitoylphosphatidylcholine bilayers: X-ray diffraction study

The structural changes accompanying the recently described sub-transition of hydrated dipalmitoylphosphatidylcholine (Chen, S.C., Sturtevant, J.M. and Gaffney, B.J. (1980) Proc. Natl. Acad. Sci. USA 77, 5060–5063) have been defined using X-ray diffraction methods. Following prolonged storage at ?4°C the usual L_β′ gel form of hydrated dipalmitoylphosphatidylcholine (DPPC) is converted into a more ordered stable ‘crystal’ form. The bilayer periodicity is 59.1 Å and the most striking feature is the presence of a number of X-ray reflections in the wide angle region. The most prominent of these are a sharp reflection at $\text{1}\text{4.4}\text{A}\text{?}{}^{\mathrm{?1}}$ and a broader reflection at $\text{1}\text{3.9}\text{A}\text{?}{}^{\mathrm{?1}}$. This diffraction pattern is indicative of more ordered molecular and hydrocarbon chain packing modes in this low temperature ‘crystal’ bilayer form. At the sub-transition (T_rmsub = 15–20°C) an increase in the bilayer periodicity occurs ($\text{d=63.6}\text{A}\text{?}$) and a strong reflection at approx. $\text{1}\text{4.2}\text{A}\text{?}{}^{\mathrm{?1}}$ with a shoulder at approx. $\text{1}\text{4.1}\text{A}\text{?}{}^{\mathrm{?1}}$ is observed. This diffraction pattern is identical to that of the bilayer gel (L_β′) form of hydrated DPPC. Thus, the sub-transition corresponds to a bilayer ‘crystal’ → bilayer L_β′ gel structural rearrangement accompanied by a decrease in the lateral hydrocarbon chain interactions. Differential scanning calorimetry and X-ray diffraction show that on further heating the usual structural changes L_β′ → P_β′ and P_β′ → L_α occur at the pre- and main transitions, at approx. 35°C and 41°C, respectively.     

Crystallographic data for a penicillin receptor : exocellular DD-carboxypeptidase-transpeptidase from Streptomyces R61.

A pencillin-sensitive enzyme, the exocellular dd-carboxypeptidase-transpeptidase from Streptomyces R61, has been crystallized from polyethylene glycol (M_r = 6000 to 7500) solution at pH 7·6. X-ray examination of the orthorhombic crystals shows the space group is P2₁2₁2₁, with unit cell dimensions $\text{a = 51·1}\text{A}\text{?}\text{, b = 67·4}\text{A}\text{?}\text{,}\text{and}\text{c = 102·9}\text{A}\text{?}$. With four molecules of molecular weight 38,000, the $\text{A}\text{?}{}^3\text{/}\text{dalton}$ ratio for the cell is 2·33. The crystals are stable to irradiation for 75 hours and are suitable for structure analysis to at least 2·4 Å resolution. The radius of gyration of the molecule in solution at pH 6.8 is 20.8 Å.     

Kinetics of bidirectional active sodium fluxes in the toad bladder

The kinetics of isotopic Na⁺ flows was studied in urinary bladders of toads from the Dominican Republic. Initial studies of the potential dependence of passive serosal to mucosal ²²Na⁺ efflux demonstrated the absence of isotope interaction and/or other coupling with passive Na⁺ flow. The electrical current $\text{I}$ and mucosal to serosal ²²Na⁺ influx were then measured with transmembrane potential clamped at $\text{Δψ = 0, 25, 50, 75 or 100}\text{mV}$. Subsequent elimination of active Na⁺ transport mucosal amiloride permitted calculation of the rates of active Na⁺ transport $\text{J}{}_{\mathrm{<mtext>Na</mtext>}}{}^{\mathrm{<mtext>a</mtext>}}$ and active and passive influx and $\text{J}{}_{\mathrm{<mtext>Na</mtext>}}{}^{\mathrm{<mtext>a</mtext>}}$ and $\text{J}{}_{\mathrm{<mtext>Na</mtext>}}{}^{\mathrm{<mtext>p</mtext>}}$. The results indicate that for Dominican toad bladders mounted in chambers only Na⁺ contributes significantly to transepithelial active ion transport; hence $\text{J}{}_{\mathrm{<mtext>Na</mtext>}}{}^{\mathrm{<mtext>a</mtext>}}\text{= J}{}^{\mathrm{<mtext>a</mtext>}}$. $\text{J}{}^{\mathrm{<mtext>a</mtext>}}$ was abolished at $\text{Δψ = E = 96.3 ± 1.9}\text{(S.E.) mV}$. As Δψ approached $\text{E}$, active efflux $\text{J}{}^{\mathrm{<mtext>a</mtext>}}$ became demonstrable. At $\text{Δ = 100}\text{mV}\text{,}\text{J}{}^{\mathrm{<mtext>a</mtext>}}$ exceeded $\text{J}{}^{\mathrm{<mtext>a</mtext>}}$, so that $\text{J}{}^{\mathrm{<mtext>a</mtext>}}$ was negative. Experimental values of $\text{J}{}^{\mathrm{<mtext>a</mtext>}}$ agreed well with theoretical values predicted by a thermodynamic formulation: $\text{J}{}_{\mathrm{<mtext>exp</mtext>}}{}^{\mathrm{<mtext>a</mtext>}}\text{= 0.985}\text{J}{}_{\mathrm{<mtext>theor</mtext>}}{}^{\mathrm{<mtext>a</mtext>}}\text{(r = 0.993)}$. The dependence of $\text{J}{}^{\mathrm{<mtext>a</mtext>}}$ on Δψ is curvilinear.     

A high-affinity (Ca2+ + Mg2+)-ATPase in plasma membranes of rat ascites hepatoma AH109A cells

The activity of calcium-stimulated and magnesium-dependent adenosinetriphosphatase which possesses a high affinity for free calcium (high-affinity $\text{(Ca}{}^{\mathrm{2+}}\text{+ Mg}{}^{\mathrm{2+}}\text{)-ATPase}$, EC 3.6.1.3) has been detected in rat ascites hepatoma AH109A cell plasma membranes. The high-affinity $\text{(Ca}{}^{\mathrm{2+}}\text{+ Mg}{}^{\mathrm{2+}}\text{)-ATPase}$ had an apparent half saturation constant of $\text{77 ± 31}\text{nM}$ for free calcium, a maximum reaction velocity of $\text{9.9 ± 3.5}\text{nmol}$ ATP hydrolyzed/mg protein per min, and a Hill number of 0.8. Maximum activity was obtained at 0.2 μM free calcium. The high-affinity $\text{(Ca}{}^{\mathrm{2+}}\text{+ Mg}{}^{\mathrm{2+}}\text{)-ATPase}$ was absolutely dependent on 3–10 mM magnesium and the pH optimum was within physiological range (pH 7.2–7.5). Among the nucleoside trisphosphates tested, ATP was the best substrate, with an apparent $\text{K}{}_{\mathrm{<mtext>m</mtext>}}$ of 30 μM. The distribution pattern of this enzyme in the subcellular fractions of the ascites hepatoma cell homogenate (as shown by the linear sucrose density gradient ultracentrifugation method) was similar to that of the known plasma membrane marker enzyme alkaline phosphatase (EC 3.1.3.1), indicating that the ATPase was located in the plasma membrane. Various agents, such as K⁺, Na⁺, ouabain, KCN, dicyclohexylcarbodiimide and NaN₃, had no significant effect on the activity of high-affinity $\text{(Ca}{}^{\mathrm{2+}}\text{+ Mg}{}^{\mathrm{2+}}\text{)-ATPase}$. Orthovanadate inhibited this enzyme activity with an apparent half-maximal inhibition constant of 40 μM. The high-affinity $\text{(Ca}{}^{\mathrm{2+}}\text{+ Mg}{}^{\mathrm{2+}}\text{)-ATPase}$ was neither inhibited by trifluoperazine, a calmodulin-antagonist, nor stimulated by bovine brain calmodulin, whether the plasma membranes were prepared with or without ethylene glycol $\text{bis}\text{(β-}\text{aminoethyl ether}\text{)-N,N,N′,N′-}\text{tetraacetic acid}$. Since the kinetic properties of the high-affinity $\text{(Ca}{}^{\mathrm{2+}}\text{+ Mg}{}^{\mathrm{2+}}\text{)-ATPase}$ showed a close resemblance to those of erythrocyte plasma membrane $\text{(Ca}{}^{\mathrm{2+}}\text{+ Mg}{}^{\mathrm{2+}}\text{)-ATPase}$, the high-affinity $\text{(Ca}{}^{\mathrm{2+}}\text{+ Mg}{}^{\mathrm{2+}}\text{)-ATPase}$ of rat ascites hepatoma cell plasma membrane is proposed to be a calcium-pumping ATPase of these cells.     

Comparison of the three basic scattering functions of myoglobin in solution with those from the known structure in crystalline state

X-ray small-angle scattering of myoglobin in aqueous solutions enhances the probability that the structure of myoglobin is conserved on passing to the dissolved state. The agreement of measured and calculated results could be extended up to $\text{k = 1.2}\text{A}\text{?}{}^{\mathrm{?1}}$ which roughly corresponds to 5 Å resolution.     

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.     

Analysis of the kinetics of electron transfer reactions of hemoglobin and myoglobin with inorganic complexes.

The kinetics of methemoglobin reduction by Fe(EDTA)^2? have been studied and found to follow a second order rate law with k = 29.0 $\text{M}$^?1 s^?1 [25°C, μ = 0.2 $\text{M}$, pH 7.0 (phosphate)], $\text{ΔH}{}^3\text{= 5.5 ± 0.7 kcal/mol}$, and $\text{ΔS}{}^2\text{= ?33 ± 2 e.u.}$. The electrostatics-corrected self-exchange rate constant (k₁₁^corr) for hemoglobin based on the Fe(EDTA)^2? cross-reaction is 2.79×10^?3$\text{M}$^?1 s^?1. This rate constant is compared with others reported for a water-soluble iron porphyrin and calculated from published data for the reactions of myoglobin and hemoglobin with Fe(EDTA)^2? and Fe(CDTA)^2?/?. The k₁₁^corr values for these systems range over ten orders of magnitude with heme ? myoglobin > hemoglobin.     

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.     

The transepithelial shunt pathway in the renal proximal tubule of newt kidney

The transepithelial shunt pathway of newt proximal tubule was examined with glass micro-electrode and electron microscopic methods. The input resistance of the peritubular (basal) membrane and tubular wall were found to be $\text{4.2 ± 0.1 · 10}{}^6$ ($\text{mean ± S.E.}\text{, n = 16}$) and $\text{11.4 ± 0.2 · 10}{}^4\text{(n = 11)}$, respectively. The input resistance of the peritubular membrane was approximately 40-times larger than that of the tubular wall. When the kidneys were perfused in a lanthanum solution, the lanthanum ions were then observed in the junctional complexes and in the intercellular spaces on both the basal and apical sides. The results indicate that the electrical shunt pathway corresponds to the apical junctional complexes and the intercellular spaces, and that the tight junctions are not truly ‘tight’ for the transepithelial movement of small ions in the proximal tubule of the newt kidney.     

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.     

Ligand-dependent reactivity of (Na+ + K+)-ATPase with showdomycin

Showdomycin inhibited pig brain ($\text{Na}{}^{\mathrm{+}}\text{+}\text{K}{}^{\mathrm{+}}\text{)-}\text{ATPase}$ with pseudo first-order kinetics. The rate of inhibition by showdomycin was examined in the presence of 16 combinations of four ligands, i.e., Na⁺, K⁺, Mg²⁺ and ATP, and was found to depend on the ligands added. Combinations of ligands were divided into five groups in terms of the magnitude of the rate constant; in the order of decreasing rate constants these were: (1)$\text{Na}{}^{\mathrm{+}}\text{+}\text{Mg}{}^{\mathrm{2+}}\text{+}\text{ATP}$, (2) $\text{Mg}{}^{\mathrm{2+}}$, $\text{Mg}{}^{\mathrm{2+}}\text{+}\text{K}{}^{\mathrm{+}}$, $\text{K}{}^{\mathrm{+}}$ and none, (3) $\text{Na}{}^{\mathrm{+}}\text{+}\text{Mg}{}^{\mathrm{2+}}\text{,}\text{Na}{}^{\mathrm{+}}$, $\text{K}{}^{\mathrm{+}}\text{+}\text{Na}{}^{\mathrm{+}}$ and $\text{Na}{}^{\mathrm{+}}\text{+}\text{K}{}^{\mathrm{+}}\text{+}\text{Mg}{}^{\mathrm{2+}}$, (4) $\text{Mg}{}^{\mathrm{2+}}\text{+}\text{K}{}^{\mathrm{+}}\text{+}\text{ATP}\text{,}\text{K}{}^{\mathrm{+}}\text{+}\text{ATP}$ and $\text{Mg}{}^{\mathrm{2+}}\text{+}\text{ATP}\text{, (5)}\text{K}{}^{\mathrm{+}}\text{+}\text{Na}{}^{\mathrm{+}}\text{+}\text{ATP}$, $\text{Na}{}^{\mathrm{+}}\text{+}\text{ATP}$, $\text{Na}{}^{\mathrm{+}}\text{+}\text{ATP}$, $\text{Na}{}^{\mathrm{+}}\text{+}\text{K}{}^{\mathrm{+}}\text{+}\text{Mg}{}^{\mathrm{2+}}\text{+}\text{ATP}$ and ATP. The highest rate was obtained in the presence of Na⁺, Mg²⁺ and ATP. The apparent concentrations of Na⁺, Mg²⁺ and ATP for half-maximum stimulation of inhibition ($\text{K}{}_{0.5}{}^{\mathrm{<mtext>s</mtext>}}$) were 3 mM, 0.13 mM and 4μM, respectively. The rate was unchanged upon further increase in Na⁺ concentration from 140 to 1000 mM. The rates of inhibition could be explained on the basis of the enzyme forms present, including E₁, E₂, ES, E₁-P and E₂-P, i.e., E₂ has higher reactivity with showdomycin than E₁, while E₂-P has almost the same reactivity as E₁-P. We conclude that the reaction of ($\text{Na}{}^{\mathrm{+}}\text{+}\text{K}{}^{\mathrm{+}}\text{)-}\text{ATPase}$ proceeds via at least four kinds of enzyme form (E₁, E₂, E₁ · nucleotide and EP), which all have different conformations.     

Pyruvate flux into resealed ghosts from human erythrocytes

The kinetics of pyruvate transport across the isolated red blood cell membrane were studied by a simple and precise spectrophotometric method: following the oxidation of NADH via lactate dehydrogenase trapped within resealed ghosts. The initial rate of pyruvate entry was linear. Influx was limited by saturation at high pyruvate concentration. Pyruvate influx was greatly stimulated by increasing ionic strength in the outer but not the inner aqueous compartment. The $\text{K}{}_{\mathrm{<mtext>m</mtext>}}$ ranged from 15.0 mM at $\text{μ = 0.05}$ to 3.7 mM at $\text{μ = 0.01}$, while the $\text{V}$ went from $\text{0.611 · 10}{}^{-15}$ to $\text{0.137 · 10}{}^{-15}\text{mol}\text{·}\text{min}{}^{-1}\text{·}\text{ghost}{}^{-1}$. Ionic strength was shown to affect the translocation step and not pyruvate binding. The energy of activation of pyruvate flux into resealed ghosts was 25 kcal/mol, similar to that found in intact red blood cells. Inhibitors of pyruvate influx included such anions as thiocyanate, chloride, bicarbonate, α-cyanocinnamate, salicylate and ketomalonate (but not acetate); noncompetitive inhibitors were phloretin, 1-fluoro-2,4-dinitrobenzene, 4-acetamido-4′-isothiocyanate-stilbene-2,2′-disulfonic acid and o-phenanthroline/CuSO₄ mixtures. The last reagent, known to induce disulfide links in certain membrane proteins, blocked the ionic strength stimulation of pyruvate influx in this study.     

Effect of the cations sodium and potassium on the molecular weight of hyaluronate

The molecular weight of Na- and K-hyaluronate has been determined by low angle laser light scattering (LALLS) technique. Two preparations of hyaluronate from rooster comb ($\text{M}{}_{\mathrm{w}}\text{= 0.9 × 10}{}^6\text{and 4 × 10}{}^6$) were investigated. The LALLS was carried out both in a static mode and on the effluent from a column filled with porous gel. In contrast to Sheehan et al.¹, no significant difference was found in the molecular weight of viscosity of Na- and K-hyaluronate in 2.0 M salt solutions