The yield of chlorophyll a fluorescence as a means to test the various deexcitation mechanisms in the antenna system of green plants

With the aid of measurements of the fluorescence yield, the efficiency of the various deexcitation mechanisms of an exciton in the light-harvesting system has been determined. For this purpose, the fluorescence of dark-adapted as well as of 3-(3,4-dichlorophenyl)-1,1-dimethylurea (DCMU)-treated and preilluminated leaves of Zea mays L. was excited by single ultrashort laser pulses of different energies. The experimental results have served for the fitting of solutions of rate equations, which describe the deexcitation by linear relaxation processes like fluorescence and radiationless transitions, by annihiation of excitons, and by traps both in the ground state and in an excited state. We have obtained the following results: a ratio of antenna chlorophyll molecules to Photosystem II traps of 600:1, an annihilation constant γ = 2·10^?8 cm³·s^?1, a mean trapping time of $\text{t}\text{?}\text{=0.5}\text{ns}$, a trapping probability for traps in the ground state of 2·10^?8 cm³·s^?1, and 6·10^?9 cm³·s^?1 for traps in an excited state.     

Electronic interactions between iron and the bound semiquinones in bacterial photosynthesis. EPR spectroscopy of oriented cells of Rhodopseudomonas viridis

Electron paramagnetic resonance (EPR) spectroscopy of the iron-semiquinone complex in photosynthetic bacterial cells and chromatophores of Rhodopseudomonas viridis is reported. Magnetic fields are used to orient the prolate ellipsoidal-shaped cells which possess a highly ordered internal structure, consisting of concentric, nearly cylindrical membranes. The field-oriented suspension of cells exhibits a highly dichroic EPR signal for the iron-semiquinone complex, showing that the iron possesses a low-symmetry ligand field and exists in a preferred orientation within the native reaction-center membrane complex. The EPR spectrum is analyzed utilizing a spin hamiltonian formalism to extract physical information describing the electronic structure of the iron and the nature of its interaction with the semiquinones. Exact numerical solutions and analytical expressions for the transition frequencies and intensities derived from a perturbation theory expansion are presented, and a computer-simulated spectrum is given. It has been found that, for a model which assumes no preferred orientation within the plane of the membranes, the orientation of the Fe²⁺ ligand axis of largest zero-field splitting (Z, the principal magnetic axis) is titled 64±6° from the membrane normal. The ligand field for Fe²⁺ has low symmetry, with zero-field splitting parameters of |D₁|=7.0±1.3 cm^?1 and |E₁|=1.7±0.5 cm^?1 and $\text{|}\text{E}{}_1\text{D}{}_1\text{|=0.26}$ for the redox state Q₁^?Fe²⁺Q^2?. The rhombic character of the ligand field is increased in the redox state Q₁Fe²⁺Q^?₂, where $\text{0.33>|}\text{E}{}_2\text{D}{}_2\text{|>0.26}$. This indicates that the redox state of the quinones can influence the ligand field symmetry and splitting of the Fe²⁺. There exists an electron-spin exchange interaction between Fe²⁺ and Q^?₁ and Q^?₂, having magnitudes |J₁|=0.12±0.03 cm^?1 and $\text{|J}{}_2\text{|?0.06}\text{cm}{}^{\mathrm{?1}}$, respectively. Such weak interactions indicate that a proper electronic picture of the complex is as a pair of immobilized semiquinone radicals having very little orbital overlap (probably fostered by superexchange) with the Fe²⁺ orbitals. The exchange interaction is analyzed by comparison with model systems of paramagnetic metals and free radicals to indicate an absence of direct coordination between Fe²⁺ and Q^?₁ and Q^?₂. Selective line-broadening of some of the EPR transitions, involving Q^? coupling to the magnetic sublevels of the Fe²⁺ ground state, is interpreted as arising from an electron-electron dipolar interaction. Analysis of this line-broadening indicates a distance of 6.2–7.8 ? between Fe²⁺ and Q^?₁, thus placing Q₁ outside the immediate coordination shell of Fe²⁺.     

Minimal functional unit for transport and enzyme activities of (Na+ + K+)-ATPase as determined by radiation inactivation

Frozen aqueous suspensions of partially purified membrane-bound renal (Na⁺ + K⁺)-ATPase have been irradiated at –135°C with high-energy electrons. (Na⁺ + K⁺)-ATPase and K⁺-phosphatase activities are inactivated exponentially with apparent target sizes of $\text{184 ± 4 kDa and 125 ± 3 kDa}$, respectively. These values are significantly lower then found previously from irradiation of lyophilized membranes. After reconstitution of irradiated (Na⁺ + K⁺)-ATPase into phospholipid vesicles the following transport functions have been measured and target sizes calculated from the exponential inactivation curves: ATP-dependent Na⁺?K⁺ exchange, $\text{201 ± 4}\text{kDa}$; (ATP + P_i)-activated Rb⁺?Rb⁺ exchange, $\text{206 ± 7}\text{kDa}$ and ATP-independent Rb⁺?Rb⁺ exchange, $\text{117 ± 4}\text{kDa}$. The apparent size of the α-chain, judged by disappearance of Coomassie stain on SDS-gels, lies between 115 and 141 kDa. That for the β-glycoprotein, though clearly smaller, could not be estimated. We draw the following conclusions: (1) The simplest interpretation of the results is that the minimal functional unit for (Na⁺ + K⁺)-ATPase is αβ. (2) The inactivation target size for (Na⁺ + K⁺)-dependent ATP hydrolysis is the same as for ATP-dependent pumping of Na⁺ and K⁺. (3) The target sizes, for K⁺-phosphatase (125 kDa) and ATP-independent Rb⁺?Rb⁺ exchange (117 kDa) are indistinguishable from that of the α-chain itself, suggesting that cation binding sites and transport pathways, and the $\text{p-}\text{nitrophenyl}$ phosphate binding site are located exclusively on the α-chain. (4) ATP-dependent activities appear to depend on the integrity of an αβ complex.     

Conversion of thyroxine to 3,3',5'-triiodothyronine (reverse-T3) by a soluble enzyme system of rat liver

Infrared spectra of N₂O in a variety of solvents and in the brain of a dog under typical conditions of halothane-N₂O anesthesia have been determined. The appearance or disappearance of N₂O in the brain was readily followed as N₂O was administered or withdrawn. The sites in brain were of two major types; one, with ν₃ = 2229.8 ± 0.4 cm^?1 and $\text{Δν}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{= 13.0 ± 0.6}\text{cm}{}^{\mathrm{?1}}$, is rather like the polar site in water and the other, with ν₃ = 2216.8 ± 0.8 cm^?1 and $\text{Δν}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{= 9.6 ± 1.0}\text{cm}{}^{\mathrm{?1}}$, is non-polar and is probably associated with membrane lipid. The significant variations in the antisymmetric stretch (ν₃) of N₂O as the polarity and other properties of the medium (solvent) vary make possible the characterization of $\text{in tissue}$ sites occupied by this anesthetic.     

Alkaline isomerization of ferricytochrome C from Euglena gracilis

$\text{Euglena gracilis}$ ferricytochrome $\text{c}$ has a small absorption maximum at about 700 nm having an extinction of 850 ± 10 M^?1cm^?1. This absorption band is analogous to the more commonly found maximum at 695 nm which is observed in ferricytochromes from other sources and which is characteristic of ligation of methionine 80 with the heme ion. The 700 nm band disappears upon raising the pH to 11 giving a transition involving a single proton having an apparent pK of about 10. These results demonstrate that the phenolic ionization of tyrosine 67 is not required to trigger the alkaline isomerization of ferricytochromes $\text{c}$ since Euglena cytochrome has a phenylalanine residue at position 67.     

Molar extinction coefficients and other properties of an improved reaction center preparation from Rhodopseudomonas viridis

Reaction centers have been purified from chromatophores of Rhodopseudomonas viridis by treatment with lauryl dimethyl amine oxide followed by hydroxyapatite chromatography and precipitation with ammonium sulfate. The absorption spectrum at low temperature shows bands at 531 and 543 nm, assigned to two molecules of bacteriopheophytin b. The 600 nm band of bacteriochlorophyll b is resolved at low temperature into components at 601 and 606.5 nm. At room temperature the light-induced difference spectrum shows a negative band centered at 615 nm, where the absorption spectrum shows only a weak shoulder adjacent to the 600 nm band. The fluorescence spectrum shows a band at 1000 nm and no fluorescence corresponding to the 830 nm absorption band. Two molecules of cytochrome 558 and three of cytochrome 552 accompany each reaction center. The differential extinction coefficient (reduced minus oxidized) of cytochrome 558 at 558 nm was estimated as 20 ± 2 mM^?1 · cm^?1 through a coupled reaction with equine cytochrome c. The extinction coefficient of reaction centers at 960 nm was determined to be 123 ± 25 mM^?1 · cm^?1 by measuring the light-induced bleaching of P-960 and the coupled oxidation of cytochrome 558. The corresponding extinction coefficient at 830 nm is 300 ± 65 mM^?1 · cm^?1. The absorbance ratio $\text{a}{}_{\mathrm{<mtext>280</mtext><mtext>nm</mtext>}}\text{a}{}_{\mathrm{<mtext>830</mtext><mtext>nm</mtext>}}$ in our preparations was 2.1, and there was 190 kg protein per mol of reaction centers. Sodium dodecyl sulfate-polyacrylamide gel electrophoresis showed three major components of apparent molecular weights 31 000, 37 000 and 41 000.     

Cytochalasin B inhibition and temperature dependence of 3-O-methylglucose transport in fat cells

The transport of $\text{3-O-}\text{methylglucose}$ in white fat cells was measured under equilibrium exchange conditions at $\text{3-O-}\text{methylglucose}$ concentrations up to 50 mM with a previously described method (Vinten, J., Gliemann, J. and Østerlind, K. (1976) J. Biol. Chem. 251, 794–800). Under these conditions the main part of the transport was inhibitable by cytochalasin B. The inhibition was found to be of competitive type with an inhibition constant of about 2.5 · 10^?7 M, both in the absence and in the presence of insulin (1μM). The cytochalasin B-insensitive part of the $\text{3-O-}\text{methylglucose}$ permeability was about 2 · 10^?9 cm · s^?1, and was not affected by insulin. As calculated from the maximum transport capacity, the half saturation constant and the volume/ surface ratio, the maximum permeability of the fat cell membrane to $\text{3-O-}\text{methylglucose}$ at 37°C and in the presence of insulin was 4.3 · 10^?6 cm · s^?1. From the temperature dependence of the maximum transport capacity in the interval 18–37°C and in the presence of insulin, an Arrhenius activation energy of $\text{14.8 ± 0.44}\text{kcal/mol}$ was found. The corresponding value was $\text{13.9 ± 0.89}$ in the absence of insulin. The half saturating concentration of $\text{3-O-}\text{methylglucose}$ was about 6 mM in the temperature interval used, and it was not affected by insulin, although this hormone increased the maximum transport capacity about ten-fold to 1.7 mmol · s^?1 per 1 intracellular water at 37°C.     

The primary photoreactions in the complex cytochrome-P-890 · P-760 (bacteriopheophytin760) of Chromatium minutissimum at low redox potentials

Experimental evidence for electron transfer, photosensitized by bacteriochlorophyll, from cytochrome c to a pigment complex P-760 (involving bacteriopheophytin-760 and also bacteriochlorophyll-800) in the reaction centers of Chromatium minutissimum has been described. This photoreaction occurs between 77 and 293 °K at a redox potential of the medium between ?250 and ?530 mV. Photoreduction of P-760 is accompanied by development of a wide absorption band at 650 nm and of an EPR signal with g = 2.0025±0.0005 and linewidth of 12.5±0.5 G, which are characteristic of the pigment radical anion.It is suggested that the photoreduction of P-760 occurs under the interaction of reduced cytochrome c with the reaction center state P⁺-890 · P^?-760 which is induced by light. The existence of short-lived state P⁺-890 · P^?-760 is indicated by the recombination luminescence with activation energy of 0.12 eV and $\text{τ}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{< 6}\text{ns}$. This luminescence is excited and emitted by bacteriochlorophyll and disappears when P-760 is reduced.At low redox potentials, the flash-induced absorbance changes related to the formation of the carotenoid triplet state with $\text{τ}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{= 6 μ}\text{s}$ at 20 °C are observed. This state is not formed when P-760 is reduced at 293 and 160 °K. It is assumed that this state is formed from the reaction center state P⁺-890 · P^?-760, which appears to be a primary product of light reaction in the bacterial reaction centers and which is probably identical with the state P^F described in recent works.     

Carbonic anhydrase catalyzed oxygen-18 exchange between bicarbonate and water

Oxygen-18 exchange techniques were applied to the dehydration of bicarbonate catalyzed by human carbonic anhydrase C. The rates of depletion of oxygen-18 from labeled bicarbonate were measured for both the catalyzed and uncatalyzed reactions at pH 9.4 and 25 °C. The equilibrium dissociation constant of the enzyme-substrate complex K is 0.321 ± 0.040 m and $\text{k}{}_{\mathrm{<mtext>enz</mtext>}}\text{=}\text{k}{}_2\text{K}{}_{\mathrm{m}}$ is (8.3 ± 1.9) × 10⁵m^?1 sec^?1 under these conditions. On the basis of these results it is demonstrated that the oxygen-18 exchange technique is capable of measuring K and k_enz for the carbonic anhydrase catalyzed dehydration of bicarbonate at a high pH range in which other kinetic techniques are not effective.It was also shown that the oxygen-18 exchange technique is an effective micromethod for the determination of carbonic anhydrase. Rates of isotopic depletion of labeled bicarbonate (in solutions of the enzyme) which fall outside the limits of error for the uncatalyzed rate of depletion demonstrate that this technique can detect concentrations of human carbonic anhydrase C as low as 5 × 10^?11m.     

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.     

Effect of bombesin-stimulated gastrin on gastric acid secretion in man

The effect of bombesin on gastrin release and gastric acid secretion was investigated in 10 healthy volunteers. Bombesin (0.6 μg · Kg^?1 · hr^?1) produced a significantly higher $\text{(}\text{p}\text{<}\text{0.001)}$ increase in plasma gastrin levels (86.7 11.1 pmo/1 than after a protein meal (39.6 ± 5.6 pmol1/1). The gastric acid secretory response to bombesin (12.1 ± 2.9 mEq · hr^?1) was however significantly lower $\text{(}\text{p}\text{<}\text{0.005)}$ than the maximal response produced by pentagostrin (20.9 ± 3.5 mEq · hr^?1) at the dose of 6 μg · Kg^?1. Atropine did not modify gastrin release induced by bombesin but significantly reduced gastric acid secretion $\text{(}\text{p}\text{<}\text{0.01)}$. From the data presented it may be hypothesized that less biologically active forms of gastrin and/or other peptides inhibiting the gastrin effect upon gastric acid secretion may be released by bombesin.     

Resonance raman spectroscopy of chemically modified and isotopically labelled purple membranes. I. A critical examination of the carbon-nitrogen vibrational modes

Resonance Raman spectra of bacteriorhodopsin are compared to the spectra of this protein modified in the following ways: (1) selective deuteration at the C-15 carbon atom of retinal, (2) full deuteration of the retinal, (3) the addition of a conjugated double bond in the β-ionone ring (3-dehydroretinal), (4) full deuteration of the protein and lipid components, (5) ¹⁵N enrichment of the entire membrane and (6) deuteration of the entire membrane (including the retinal). A detailed comparison of the ¹⁵N-enriched membrane and naturally occurring purple membrane from 800 cm^?1 to 1700 cm^?1 reveals that ¹⁵N enrichment affects the frequency of only two vibrational modes. These occur at 1642 cm^?1 and 1620 cm^?1 in naturally occurring purple membrane and at 1628 cm^?1 and 1615 cm^?1 in the ¹⁵N-enriched samples. Therefore, this pair of bands reflects the states of protonation of the Schiff base. However, our data also indicate that neither of these modes are simple, localized $\text{C}\text{=}\textcolor{red}{}\text{?}\text{H}$ or C=N stretching vibrations. In the case of the 1642 cm^?1 band motions of the retinal chain beyond C-15 are not significantly involved. On the other hand, in the 1620 cm^?1 band atomic motions in the isoprenoid chain beyond C-15 are involved.     

Kinetic studies of 18O exchange from inorganic phosphate catalyzed by Mg2+-activated unadenylylated glutamine synthetase (E. coli w).

Oxygen-18 exchange out of [¹⁸O]Pi catalyzed by Mg²⁺-activated unadenylated glutamine synthetase from $\text{E.}$$\text{coli}$ was followed by ³¹P-NMR in the presence of the other substrates, ADP and L-glutamine. The pattern of the ${}^{16}\text{O}{}^{18}\text{O}$ in the species P¹⁸O₄, P¹⁸O₃¹⁶O₁, P¹⁸O₂¹⁶O₂, P¹⁸O₁¹⁶O₃, P¹⁶O₄ during the exchange followed a binomial distribution consistent with indiscriminate removal of any of the four oxygens of P_i. The rate constant for ${}^{16}\text{O}{}^{18}\text{O}$ exchange was 410±40 min^?1 while the rate constant for net reaction (ATP formation) was 62±4 min^?1. Thus exchange proceeds ～7 times faster than net reaction, a finding in accord with that of Stokes and Boyer ($\text{J.}$$\text{Biol.}$$\text{Chem.}$ (1976) $\text{251}$, 5558) for the Mn²⁺-activated adenylylated glutamine synthetase. A model for the overall catalytic events first derived from rapid kinetic fluorescence experiments (Rhee and Chock, Proc. Natl. Acad. Sci. USA, (1976) $\text{73}$, 476) was successfully used to fit the oxygen exchange data in this paper.     

Zero field resonance and spin alignment of the triplet state of chloroplasts at 2°K

Microwave induced transitions in zero magnetic field have been observed in the photoinduced triplet of chloroplasts treated with dithionite by monitoring changes in the intensity of the 735 nm fluorescence band at 2°K. Similar results were obtained with chloroplasts treated with hydroxylamine plus 3-(3,4-dichlorophenyl)-1,1-dimethylurea and preillumination. The zero field parameters are $\text{D = 0.02794 ± 0.00007}\text{cm}{}^{\mathrm{?1}}$, $\text{E = 0.00382 ± 0.00007}\text{cm}{}^{\mathrm{?1}}$, i.e. equal to those of monomeric chlorophyll $\text{a}$ to within the experimental error. The photoinduced triplet appears to be linked to Photosystem II. This indicates that the low temperature 735 nm fluorescence band of chloroplasts is at least partly due to Photosystem II.     

Picosecond kinetics in reaction centers of Rps. sphaeroides and the effects of ubiquinone extraction and reconstitution.

Following picosecond light activation, the bacteriochlorophyll and bacteriopheophytin complement of $\text{Rps.}\text{sphaeroides}$ reaction centers depleted of ubiquinone behaves as though it has no primary electron acceptor; the excited intermediary $\text{BChl}\text{BPh}{}^2$ state formed in <10 ps lasts >1 ns. Addition of ubiquinone-10 reconstitutes the very rapid electron transfer rates from the excited intermediary $\text{BCh}\text{BPh}$ state to ubiquinone; the kinetics and rate are similar to that encountered in the untreated reaction centers. Interpretation of the data presented suggests that ubiquinone is the immediate electron acceptor from BPh^?. This is consistent with the model for the primary reactions leading to [(BChl)₂^?BPh]Q^?.     

Electrophoretic detection of reversible chlorpromazine · HCl binding at the human erythrocyte surface

The binding of chlorpromazine · HCl at the human erythrocyte surface has been detected through its effect on cellular electrophoretic mobility. Incubation of erythrocytes (approx. 5 · 10⁶/ml) in 23 μM chlorpromazine · HCl resulted in a reduction of negative electrophoretic mobility from the control value of $\text{?1.11 ± 0.01}$ (μm · s^?1)/(V · cm^?1) to $\text{?1.00 ± 0.02}$ (μm · s^?1)/(V · cm^?1) (pH 7.2, ionic strength 0.155). This mobility change was completely reversed when chlorpromazine · HCl was removed by centrifugal washing. Increasing the drug concentration to 70μM did not affect the mobility change, indicating saturation of the electrophoretically detectable drug binding sites over chlorpromazine · HCl concentration range studied here. The effect of the 23 μM chlorpromazine · HCl on electrophoretic mobility was also measured in isotonic media of reduced ionic strength. The drug-induced reduction in negative surface charge density was found to be independent of ionic strength over the range 0.155 (Debye length, 0.8 nm) to 0.00310 (Debye length, 5.7 nm).Fixation of erythrocytes with glutaraldehyde affected neither the normal electrophoretic mobility of discocytes nor the reduced electrophoretic mobility of chlorpromazine · HCl-induced stomatocytes. When these stomatocytes were first fixed with glutaraldehyde, then washed free of chlorpromazine · HCl, they retained the stomatocyte form while regaining a normal control electrophoretic mobility. Conversely, when discocytes fixed in that form were treated with chlorpromazine · HCl, they showed the same mobility change as did fixed or unfixed stomatocytes. The drug-induced mobility change is therefore independent of the shape change, but reflects a contribution to cellular surface charge density from the membrane-bound chlorpromazine · HCl molecules. From the charge reduction, it is estimated that about 10⁶ chlorpromazine · HCl molecules are bound at the electrokinetic cell surface and occupy approximately 0.4% of the total surface area.     

Greatly extended viability of rat brain storage vesicles in an intracellular medium based upon a non-permeant polyanion

The MgATP-stimulated accumulation of (-)-³H-nor- epinephrine (NE) by rat brain neuronal storage vesicles has been characterized in a new medium based upon polyacrylic acid (avg. MW 5,000). The medium allows careful regulation of K⁺ concentration (140 mM), has a large buffer capacity, and is non-permeant to membranes. Light scattering measurements have confirmed the osmotic stability of vesicles suspended in this medium. Vesicular accumulation of (-)-³ H-NE (Km 1 × 10^?6 M) in this system (37°) was examined under saturating (10^?5 M) and non-saturating (2 × 10^?7 M) concentrations of NE. At 10^?5 M NE, uptake saturated at 5 min and remained stable for periods up to one hour, with maximal uptake levels (pmol/mg protein) of 15.7±0.30 (37°), 3.0±0.49 (0°), 4.4±0.22 (reserpine pretreated $\text{in}$$\text{vivo}$) and 6.0±0.79 (without MgATP). At 2×10^?7 M NE uptake was biphasic with maximal uptake levels (pmol/mg protein) of 4.04±0.14 (37°), 0.19±0.01 (0°), 0.95±0.01 (reserpine) and 0.83±0.08 (without MgATP). Vesicle preparations refrigerated in this medium for 24 hrs displayed properties quite similar to those measured acutely (NE = 2.2x10^?7 M).     

Amino acid transport by the helicoidal colon of the new-born pig

The proximal colon of the new-born pig maintains a stable short-circuit current which is partly dependent upon the presence of methionine. This interaction between methionine and short circuit current shows Michaelis- Menten knetics with a $\text{K}{}_{\mathrm{<mtext>m</mtext>}}$ of 0.24 mM and a $\text{V}$ of 27 μA·cm^?2. The net flux of methionine to the serosal surface of proximal colons also shows a hyperbolic relation to the external concentration of methionine ($\text{K}{}_{\mathrm{<mtext>m</mtext>}}\text{0.38}\text{mM}$; $\text{V 10.4}\text{nmol}\text{·}\text{cm}{}^{\mathrm{?2}}\text{·}\text{min}{}^{\mathrm{?1}}$). The proximal colon concentrates methionine within its epithelium giving a mucosal to medium ratio of $\text{11.2 ± 1.9}$ (90 min incubation in 1 mM methionine).The ability of the colon to transport methionine across and concentrate methionine within its mucosa is maintained for at least 24 h after birth. Colonic transport of amino acids could be physiologically important in the pig, where the immediate post-natal transfer of immune globulins has been shown to cause a temporary inhibition of normal intestinal function.     

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.