Comparative studies on mitochondrial coupling factor B and FB.

Beef heart mitochondrial protein factor F_B [Higashiyama $\text{et}\text{al}$, Biochemistry $\text{14}$, 4117–4121 (1975)] was purified and its properties were compared with those of coupling factor B. Both proteins stimulated ATP-driven NAD⁺ reduction in ammonia and EDTA-treated (AE-) submitochondrial particles, but the extent of stimulation (maximum activity of particles) was very low with F_B. F_B was found to be ineffective in stimulating P_i-ATP exchange in either AE-particles or reconstituted oligomycin-sensitive ATPase vesicles. Furthermore, F_B failed to stimulate ATP-driven NAD⁺ reduction activity of AE-particles in the presence of saturating amounts of dithiothreitol (DTT). DTT alone stimulates the particle activity extensively as reported earlier. Rabbit antiserum to F_B did not show a precipitin band with purified Factor B, nor did the antibody inhibit Factor B stimulated activity of the AE-particles. The data suggest that F_B and Factor B are two different molecular species with different functions and fail to provide evidence that F_B is a coupling factor.     

Kinetics and thermodynamics of the P870+Q−A → P870+Q−B reaction in isolated reaction centers from the photosynthetic bacterium Rhodopseudomonas sphaeroides

The temperature dependences of the P870⁺Q^?_A → P870Q_A and P870⁺Q^?_B → P870Q_B recombination reactions were measured in reaction centers from Rhodopseudomonas sphaeroides. The data indicate that the P870⁺Q^?_B state decays by thermal repopulation of the P870⁺Q^?_A state, followed by recombination. ΔG° for the P870⁺Q^?_A → P870⁺Q^?_B reaction is ?6.89 kJ · mol^?1, while ΔH° = ?14.45 kJ · mol^?1 and ?TΔS° = + 7.53 kJ · mol^?1. The activation ethalpy, $\text{H}{}^3$, for the P870⁺Q^?_A Δ P870⁺Q^?_B reaction is +56.9 kJ · mol^?1, while the activation entropy is near zero. The results permit an estimate of the shape of the potential energy curve for the P870⁺Q^?_A → P870⁺Q^?_B electron transfer reaction.     

Enthalpy and volume changes accompanying electron transfer from P-870 to quinones in Rhodopseudomonas sphaeroides reaction centers

A capacitor microphone was used to measure the enthalpy and volume changes that accompany the electron transfer reactions, $\text{PQ}{}_{\mathrm{A}}\text{→}\text{hv}\text{P}{}^{\mathrm{+}}\text{Q}{}^{\mathrm{?}}{}_{\mathrm{A}}\text{and PQ}{}_{\mathrm{A}}\text{Q}{}_{\mathrm{B}}\text{→}\text{hv}\text{P}{}^{\mathrm{+}}\text{Q}{}_{\mathrm{A}}\text{Q}{}^{\mathrm{?}}{}_{\mathrm{B}}$, following flash excitation of photosynthetic reaction centers isolated from Rhodopseudomonas sphaeroides. P is a bacteriochlorophyll dimer (P-870), and Q_A and Q_B are ubiquinones. In reaction centers containing only Q_A, the enthalpy of P⁺Q^?_A is very close to that of the PQ_A ground state (ΔH_r = 0.05 ± 0.03 eV). The free energy of about 0.65 eV that is captured in the photochemical reaction evidently takes the form of a substantial entropy decrease. In contrast, the formation of P⁺Q_AQ^?_B in reaction centers containing both quinones has a ΔH_r of 0.32 ± 0.02 eV. The entropy change must be near zero in this case. In the presence of o-phenanthroline, which blocks electron transfer between Q^?_A and Q_B, ΔH_r for forming P⁺Q^?_AQ_B is 0.13 ± 0.03 eV. The influence of flash-induced proton uptake on the results was investigated, and the ΔH_r values given above were measured under conditions that minimized this influence. Although the reductions of Q_A and Q_B involve very different changes in enthalpy and entropy, both reactions are accompanied by a similar volume decrease of about 20 ml/mol. The contraction probably reflects electrostriction caused by the charges on P⁺ and Q^?_A or Q^?_B.     

A study of the surface-active properties of the Mg2+-activated ATPase from cytoplasmic membranes of Streptococcus faecalis

The surface activity and enzymic properties of the factor F₁, the catalytic moiety of Streptococcus faecalis H⁺-ATPase, has been studied at the air-water and phospholipid-water interfaces. F₁ does not interact with the monolayer phospholipids, hence its adsorption on a biological membrane must be due mainly to its recognition of proteins of the hydrophobic complex. The dimensions of the F₁ molecule at the air-water interface have been estimated. In the presence of Mg²⁺, base area is $\text{S = 1.8 · 10}{}^4\text{A}\text{?}{}^2$, height $\text{h = 27}\text{A}\text{?}$. Bearing in mind the size of a globular subunit, it follows from the measurements that the major F₁ subunits should all lie in the same plane. The ATPase activity of F₁ at the interface is inversely proportional to the monolayer density. With low density monolayer, the specific ATPase activity is higher at the interface than in the bulk of the solution.Adsorption of F₁ at the interface shifts the isoelectric point of the protein, apparently due to changes in its conformation. The findings are discussed relative to the proton-active transport mechanism.     

Computer-determined rate constants of hemolysis induced by Prymnesium parvum toxin

Rates of hemolysis of rabbit erythrocyte suspensions induced by P. parvum (prymnesin) have been measured colorimetrically at 25.5°C and pH 5.5. The data have been treated previously as consecutive first-order rate processes associated with the prolytic and lytic periods from which two specific rate constants have been obtained, k′ and kψ, respectively. These constants have been related to those obtained by a computer-generated fit of the rate data (absorbance A_t, as a function of time t) with the rate equation $\text{Y =}\text{D}\text{[1 +}\text{exp}\text{((X ? B)}\text{C)}\text{]}\text{+ E}$. Here Y equals A_t, X = time, t; D is equal to a spread factor, A_i ? A_∞; C is the slope of the curve at the inflection point; B is the midpoint time value, i.e., the time at which $\text{A}{}_{\mathrm{t}}\text{=}\text{D}\text{2}$; E is termed the off-set constant and is equal to A_∞. Of these constants, B is directly related to the length of the prolytic period, and C^?1 is directly related to the specific first-order rate constant for hemolysis, k_ψ.     

The dependence of reaction center and antenna triplets on the redox state of Photosystem I

The formation of chlorophyll triplet states during illumination of Photosystem I reaction center samples depends upon the redox state of P-700, X and ferredoxin Centers A and B. When the reaction centers are in the states P-700⁺A₁XFd_BFd^?_A and P-700 A₁XFd^?_BFd^?_A prior to illumination, we observe electron paramagnetic resonance (EPR) spectra from a triplet species which has zero-field splitting parameters (|D| and |E|) larger than those of either the chlorophyll a or chlorophyll b monomer triplet, and a polarization which results from population of the triplet spin sublevels by an intersystem crossing mechanism. We interpret this triplet as arising from photoexcited chlorophyll antenna species associated with reaction centers in the states P-700⁺Fd^?_A and P-700⁺X^?, respectively, which undergo de-excitation via intersystem crossing. When the reaction centers are in the states P-700A₁XFd^?_BFd^?_A and P-700A₁X^?Fd^?_BFd^?_A prior to illumination, we observe a triplet EPR signal with a polarization which results from population of the triplet spin sublevels by radical pair recombination, and which has a |D| value similar to that of chlorophyll a monomer. We interpret this triplet (the radical pair-polarized triplet) as arising from ³P-700 which has been populated by the process $\text{P-700}{}^{\mathrm{+}}\text{A}{}^{\mathrm{?}}{}_1\text{→}{}^3\text{P-700}\text{A}{}_1$. We observe both the radical pair-polarized triplet and the chlorophyll antenna triplet when the reaction centers are in the state P-700 A₁XFd^?_BFd^?_A, presumably because the processes P-700⁺A^?₁X → P-700⁺A₁X^? and $\text{P-700}{}^{\mathrm{+}}\text{A}{}^{\mathrm{?}}{}_1\text{X}\text{→}{}^3\text{P-700}\text{A}{}_1\text{X}$ have similar rate constants when Centers A and B are reduced, i.e., the forward electron transfer time from A^?₁ to X is apparently much slower in the redox state P-700 A₁XFd^?_BFd^?_A than it is in state P-700 A₁XFd_BFd_A. The amplitude of the radical pair-polarized triplet EPR signal does not decrease in the presence of a 13.5-G-wide EPR signal centered at g 2.0 which was recorded in the dark prior to triplet measurements in samples previously frozen under intense illumination. This g 2.0 signal, which has been attributed to phototrapped A^?₁ (Heathcote, P., Timofeev, K.N. and Evans, M.C.W. (1979) FEBS Lett. 101, 105–109), corresponds to as many as 12 spins per P-700 and can be photogenerated during freezing without causing any apparent attenuation of the radical pair-polarized triplet amplitude. We conclude that species other than A^?₁ contribute to the g 2.0 signal.     

Angles of nucleotides bound to cross-bridges in glycerinated muscle fiber at various concentrations of ϵ-ATP, ϵ-ADP and ϵ-AMPPNP detected by polarized fluorescence

The polarized fluorescence from nucleotides bound to myosin heads in glycerinated muscle fibers of rabbit psoas was measured as the number of myosin heads with bound nucleotides was varied by adding various concentrations of fluorescent ?-ATP, ?-ADP and ?-AMPPNP (1:N⁶-etheno-ATP, -ADP and -imido ATP). The angles of the absorption and emission dipoles of bound nucleotides to the fiber axis and their angular distribution were determined from the observed values of four components of the polarized fluorescence.The maximum amount of nucleotides bound to the myosin heads in the fiber, B_m, was 170 to 270 μm. The dissociation constant of nucleotides, $\text{K}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$, increased in the order ?-ATP, ?-ADP, ?-AMPPNP, and was four to six times larger at a sarcomere length (SL) of 2.1 μm than at 3.7 μm.The polarized fluorescence from bound ?-ADP at SL = 2.1 μm was independent of the amount of bound ?-ADP when it was lower than one-half of B_m, indicating a single helical array of myosin heads having ?-ADP. The angles of the absorption dipole, φ_A, and the emission dipole, φ_E, to the fiber axis were 69 ° and 66 °, respectively. As the amount of bound ?-ADP exceeded one-half of B_m, the values of the polarized fluorescence showed that the extra ?-ADP bound to myosin heads with a lower affinity and had different angles to the fiber axis: φ_A and φ_E were 49 ° and 54 °, respectively. The half-maximum width of the angular distribution of these bound ?-ADP molecules, $\text{θ}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$, was about 20 °.During development of isometric tension in the presence of ?-ATP with Mg²⁺, the polarized fluorescence was independent of the amount of bound ?-ATP when it was lower than one-third of B_m or when the concentration of free ?-ATP was lower than 100 μm, indicating a single helical array of myosin heads undergoing the ATPase reaction. The angles of bound nucleotides, φ_A and φ_E, were 68 ° and 64 °, respectively. The half-maximum width of the angular distribution, $\text{θ}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$, was about 22 °. As the amount of bound nucleotides exceeded one-third of B_m, the polarized fluorescence showed deviation from the values expected for the single helical array.The angles φ_A and φ_E for bound ?-AMPPNP were about 58 ° and 62 °, respectively, but the angular distribution was broad; that is, $\text{θ}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$ was about 42 °. These angles were independent of the amount of bound ?-AMPPNP.In a stretched fiber with SL = 3.7 μm, the polarized fluorescence showed that the angles of ?-ADP, ?-ATP and ?-AMPPNP bound to myosin heads had almost random distributions; $\text{θ}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$ was 90 ° to 100 °, independent of the amount of bound nucleotides. Similar results were obtained with the relaxed fiber in the presence of ?-ATP.     

The secondary attachment site for bacteriophage lambda in the proA/B gene of Escherichia coli

We have determined the nucleotide sequence of a secondary λ attachment site in $\text{pro}\text{A}\text{B}$, a site that accounts for 3% of lysogens isolated from Escherichia coli strains deleted for the primary site. Direct sequence analysis of the transducing bacteriophages carrying the left and right att junctions, as well as the recombinant pro⁺ phage reveals that the $\text{pro}\text{A}\text{B}$ site shares an 11-nucleotide interrupted homology with the core sequence of the primary site. We have compared the $\text{pro}\text{A}\text{B}$att site with other secondary attachment sites to gain insights into the structural features important for λ integration.     

Critical evaluation of electron transfer kinetics in P700–FA/FB, P700–FX, and P700–A1 Photosystem I core complexes in liquid and in trehalose glass

This work aims to fully elucidate the effects of a trehalose glassy matrix on electron transfer reactions in cyanobacterial Photosystem I (PS I). Forward and backward electron transfer rates from A_1A^? and A_1B^? to F_X, and charge recombination rates from A₀^?, A_1B^?, A_1A^?, F_X^?, and [F_A/F_B]^? to P₇₀₀⁺ were measured in P₇₀₀–F_A/F_B complexes, P₇₀₀–F_X cores, and P₇₀₀–A₁ cores, both in liquid and in a trehalose glassy matrix at 11% humidity. By comparing CONTIN-resolved kinetic events over 6 orders of time in increasingly simplified versions of PS I at 480?nm, a wavelength that reports primarily A_1A^?/A_1B^? oxidation, and over 9 orders of time at 830?nm, a wavelength that reports P₇₀₀⁺ reduction and A₀^? oxidation, assignments could be made for nearly all of the resolved kinetic phases. Trehalose-embedded PS I samples demonstrated partially arrested forward electron transfer. The fractions of complexes in which electron transfer did not proceed beyond A₀, A₁ and F_X were 53%, 16% and 22%, respectively, with only 10% of electrons reaching the terminal F_A/F_B clusters. The ~10?μs and ~150?μs components in both liquid and trehalose-embedded PS I were assigned to recombination between A_1B^? and P₇₀₀⁺ and between A_1A^? and P₇₀₀⁺, respectively. The kinetics and amplitudes of these resolved kinetic phases in liquid and trehalose-embedded PS I samples could be well-fitted by a kinetic model that allowed us to calculate the asymmetrical contribution of the A_1A^? and A_1B^? quinones to the electrochromic signal at 480?nm. Possible reasons for these effects are discussed.     

Synthesis and antitumor activity of platinum complexes of protonated diamines

Complexes of the formula cis-[Pt(H$\text{N}\text{+}$^～N)(L)Cl₂], where (H$\text{N}\text{+}$^～N) are the protonated diamines including 3-aminoquinuclidine, N-aminopiperidine, piperazine, N-methylpiperazine, 1,1,4-trimethylpiperazine, and N-methyl-1,4-diazabicyclo [2,2,2] octane (N-methyl-dabco) and L = SCN^?, NO₂^?, Br^?, and F^?, were synthesized from the protonated diamine complexes, [Pt(H$\text{N}\text{+}$^～N)Cl₃]. The antitumor activities of the complexes were evaluated in vitro against L1210 murine leukemia cells, and ID₅₀ values for the L-substituted complexes were compared to values of the parent complexes. In each case it was found that replacement of a chloride ion by SCN^?, NO₂^?, Br^?, or F^?, either reduced or completely eliminated antitumor activity. This effect is explained in terms of the trans-directing ability of the ligand, L, compared to chloride. The NO₂-substituted complex of 3- aminoquinuclidine was tested in vivo and found to exhibit little or no antitumor activity.     

Hydrophobic ion probe studies of membrane dipole potentials

Hydrophobic anions of dipicrylamine and of sodium tetraphenylborate have been employed as probes of interfacial dipole potential variations in lipid bilayer membranes. Systematic variation of dipole potentials has been achieved by introduction of compounds incorporating N⁺ and B^? charge centers. Distribution of hydrophilic and and hydrophobic groups relative to these charge centers has been shown to control the orientation in the membrane/solution interface of the electric dipole moment formed by these centers. Thus triphenyl-[4-trimethylphenylammonium] borate orients with the B^? center, surrounded by phenyl groups, embedded in the membrane, while the smaller methylated N⁺ center is directed toward the aqueous phases. This orientation has been confirmed using dipicrylamine probe ions. Results obtained in this system have been interpreted quantitatively using a previously developed model incorporating discrete charge effects. A second class of compounds, $\text{tri}\text{-n-}\text{alkylamine}$ borane (T_nAB) complexes having the generic formula (C_nH_{$\text{2n+1}$})₃N⁺B^?H₃, have also been synthesized for this study, using even-carbon alkyls ranging from ethyl to decyl. Molecular orientation of the complex is with the N⁺ center and its associated alkyl groups directed into the membranes, while the protonated B^? center is directed toward the aqueous phases, as confirmed by use of tetraphenylborate ions as probes.     

Analysis of chlorophyll fluorescence induction curves in the presence of 3-(3,4-dichlorophenyl)-1,1-dimethylurea as a function of magnesium concentration and NADPH-activated light-harvesting chlorophyll ab-protein phosphorylation

The effect of Mg²⁺ concentration and phosphorylation of light-harvesting chlorophyll $\text{a}\text{b-}\text{protein}$ on various chlorophyll fluorescence induction parameters of isolated pea thylakoids has been studied. (1) Lowering the Mg²⁺ concentration from 3 to 0.4 mM decreases only the variable fluorescence (F_v) and the area above the induction curve while at the same time increasing the slow exponential component of the rise (β_max). (2) A further decrease in Mg²⁺ concentration from 0.4 to 0 mM decreases the initial (F₀) fluorescence level such that the ratio $\text{F}{}_{\mathrm{<mtext>v</mtext>}}\text{F}{}_{\mathrm{<mtext>m</mtext>}}$ increases slightly as does the area above the induction curve and β_max. (3) Thylakoid membranes, phosphorylated at 5 mM Mg²⁺, show an equal decrease in F_v and F₀, no change in the area above the induction curve and an increase in β_max. At 2 mM Mg²⁺, however, phosphorylation induced a more extensive quenching of F_v so that the $\text{F}{}_{\mathrm{<mtext>v</mtext>}}\text{F}{}_{\mathrm{<mtext>m</mtext>}}$ ratio was lowered and the area above the induction curve decreased while β_max increased. (4) When phosphorylated membranes were subsequently suspended in an Mg²⁺-free medium the effect on F₀ due to phosphorylation was found to be additive to that due to the absence of Mg²⁺. The effect of membrane phosphorylation on fluorescence is discussed in relation to the control of excitation energy distribution and shows that different mechanisms operate depending on the background Mg²⁺ levels. At high Mg²⁺ the phosphorylation seems to affect the absorption cross-section of Photosystem II while at lower Mg²⁺ levels there is an additional effect of increased spillover from Photosystem II to I.     

Crystallographic study of plastocyanins

Crystals of plastocyanins from pea and corn leaves have been obtained. Both are suitable for X-ray structure analysis with a resolution up to 1.8 Å. The crystal form of plastocyanin from pea leaves belongs to the space group P2₁2₁2₁ with unit cell dimensions: $\text{a = 49.0}\text{A}\text{?}\text{, b = 53.3}\text{A}\text{?}\text{, c = 82.6}\text{A}\text{?}$. The assumed number of protein molecules per asymmetric unit of the unit cell is two. Crystals of the oxidized (Cu²⁺) and reduced (Cu⁺) forms are isomorphic. No essential differences in spot intensities for the main zone with a resolution of 3 Å were revealed. The crystal form of plastocyanin from corn leaves belongs to the space group P1 with unit cell parameters: $\text{a = 24.8}\text{A}\text{?}\text{, b = 30.0}\text{A}\text{?}\text{, c = 58.5}\text{A}\text{?}$ and α = 96° 10′, β = 87°08′, γ = 78°40′. The assumed number of protein molecules per asymmetric unit is two.     

Electron acceptors associated with P-700 in Triton solubilized Photosystem I particles from spinach chloroplasts

Flash-induced absorption changes of Triton-solubilized Photosystem I particles from spinach were studied under reducing and/or illumination conditions that serve to alter the state of bound electron acceptors. By monitoring the decay of P-700 following each of a train of flashes, we found that P-430 or components resembling it can hold 2 equivalents of electrons transferred upon successive illuminations. This requires the presence of a good electron donor, reduced phenazine methosulfate or neutral red, otherwise the back reaction of P-700⁺ with P-430 occurs in about 30 ms. If the two P-430 sites, designated Centers A and B, are first reduced by preilluminating flashes or chemically by dithionite under anaerobic conditions, then subsequent laser flashes generate a 250 μs back reaction of P-700⁺, which we associate with a more primary electron acceptor A₂. In turn, when A₂ is reduced by background (continuous) illumination in presence of neutral red and under strongly reducing conditions, laser flashes then produce a much faster (3 μs) back reaction at wavelengths characteristic of P-700. We associate this with another more primary electron acceptor, A₁, which functions very close to P-700. The organization of these components probably corresponds to the sequence $\text{P-700-}\text{A}{}_1\text{-}\text{A}{}_2\text{-P-430[}\text{A}\text{B}\text{]}$. The relation of the optical components to acceptor species detected by EPR, by electron-spin polarization or in terms of peptide components of Photosystem I is discussed.Preliminary experiments with broken chloroplasts suggest that an analogous situation occurs there, as well.     

Factors affecting the relative magnitudes of the ouabain-sensitive and the ouabian-insensitive fluxes of thallium ion in erythrocytes

A maximal rate of the ouabain-sensitive ²⁰⁴Tl influx in human erythrocytes can be attained at trace concentrations of Tl⁺ in Mg²⁺ isotonic media free of K⁺ and Na⁺. The maximal influx of Tl⁺ from isotonic Mg(NO₃)₂ at 20°C and pH 7.4 was $\text{0.45}\text{mM}\text{· 1}{}^{\mathrm{?1}}\text{· h}{}^{\mathrm{?1}}$ with a $\text{K}{}_{\mathrm{<mtext>m</mtext>}}$ of 0.025 mM. In contrast to the active influx of Tl⁺, the passive Tl⁺ fluxes were neither saturated nor influenced by external cations in the range of concentrations of Tl⁺ and K⁺ studied. The rate constants of Tl⁺ passive fluxes in human and cat erythrocytes can be related to pH by the equation $\text{log}\text{k}{}_{\mathrm{<mtext>in(out)</mtext>}}\text{= –A + B ·}\text{pH}$, where $\text{A}$ and $\text{B}$ are empirical constants for particular conditions. The apparent activation energy was 16 and 11 kcal/mol in sulphate and nitrate media, respectively. Tl⁺ and the alkali metal cations seem to overcome a common barrier in the erythrocyte membrane. Nevertheless, the rate of the passive penetration of Tl⁺ is about two orders of magnitude faster than those of K⁺ or Rb⁺. An extra non-Coulombic interaction between Tl⁺ and membrane ligands appears to be involved providing an accumulation of Tl⁺ somewhere in the vicinity of the membrane barrier and increasing the diffusion fluxes of Tl⁺ in both directions.     

Ultracentrifugation studies on early stage polymerization of tobacco mosaic virus protein

The effects of absolute temperature (T), ionic strength (μ), and pH on the polymerization of tobacco mosaic virus protein from the 4 S form (A) to the 20 S form (D) were investigated by the method of sedimentation velocity. The loading concentration in grams per liter (C) was determined at which a just-detectable concentration (β) of 20 S material appeared. It was demonstrated experimentally that under the conditions employed herein, an equilibrium concentration of 20 S material was achieved in 3 h at the temperature of the experiment and that 20 S material dissociated again in 4 h or less to 4 S material either upon lowering the temperature or upon dilution. Thus, the use of thermodynamic equations for equilibrium processes was shown to be valid. The equation used to interpret the results, log ($\text{C?β) =}\text{constant}\text{+ (}\text{ΔH}{}^1\text{2.3RT}$) + ($\text{Δ}\text{W}{}^1{}_{\mathrm{<mtext>el</mtext>}}\text{2.3RT}$) ? K′_sμ + ζpH, was derived from three separate models of the process, the only difference being in the anatomy of the constant; thus, the method of analysis is essentially independent of the model. $\text{ΔH}{}^1$ and ΔW¹_el are the enthalpy and the change in electrical work per mole of A protein (the trimer of the polypeptide chain), K^′_s is the salting-out constant on the ionic strength basis, ζ is the number of moles of hydrogen ion bound per mole of A protein in the polymerization, and R is the gas constant. The three models leading to this equation are: a simple 11th-order equilibrium between A₁ (the trimer of the polypeptide chain) and D, either the double disk or the double spiral of approximately the same molecular weight, designated model A; a second model, designated B, in which A₁ was assumed to be in equilibrium with D at the same time that it is in equilibrium with A₂, A₃, etc., dimers and trimers, etc., of A₁ in an isodesmic system; and a phase-separation model, designated model C, in which A protein is treated as a soluble material in equilibrium with D, considered as an insoluble phase. From electrical work theory, $\text{Δ}\text{W}{}_{\mathrm{el}}{}^1\text{/T}$ was shown to be essentially independent of T; therefore, in experiments at constant μ and constant pH the equation of log (C ? β) versus 1/T is linear with a slope of $\text{ΔH}{}^1\text{/2.3R}$. The results fit such an equation over nearly a 20 °C-temperature range with a single value of $\text{Δ}\text{H}{}^1$ of +32 kcal/mol A₁. Results obtained when T and pH were held constant but μ was varied did not fit a straight line, which shows that more than simple salting-out is involved. When the effect of ionic strength on the electrical work contribution was considered in addition to salting-out, the data were interpreted to indicate a value of $\text{Δ}\text{W}{}^1{}_{\mathrm{el}}$ of 1.22 kcal/mol A₁ at pH 6.7 and a value of 4.93 for K_s^′. When μ and T were held constant but pH was varied, and when allowance was made for the effect of pH changes on the electrical work contribution, a value of 1.1 was found for ζ. This means that something like 1.1 mol of hydrogen ion must be bound per mole of A₁ protein in the formation of D. When this is added to the small amount of hydrogen ion bound per A₁ before polymerization, at the pH values used, it turned out that for D to be formed, 1.5 H⁺ ions must be bound per A₁ or 0.5 per protein polypeptide chain. This amounts to 1 H⁺ ion per polypeptide chain for half of the protein units, presumably those in one but not the other layer of the double disk or turn of the double spiral. When polymerization goes beyond the D stage, as shown by previously published data, additional H⁺ ions are bound. Simultaneous osmotic pressure studies and sedimentation studies were carried out, in both cases as a function of loading concentration C. These results were in complete disagreement with models A and C but agreed reasonably well with model B. The sedimentation studies permitted evaluation of the constant, β, to be 0.33 g/liter.     

Reactions between primary and secondary acceptors of Photosystem II in Chlorella Pyrenoidosa under anaerobic conditions as studied by chlorophyll a fluorescence

The kinetics of the fluorescence yield Ф of chlorophyll a in Chlorella pyrenoidosa were studied under anaerobic conditions in the time range from 50 μs to several minutes after short ($\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{= 30}\text{ns}$ or 5 μs) saturating flashes. The fluorescence yield “in the dark” increased from $\text{Ф = 1}$ at the beginning to $\text{Ф ≈ 5}$ in about 3 h when single flashes separated by dark intervals of about 3 min were given.After one saturating flash, Ф increased to a maximum value (4–5) at 50 μs, then Ф decreased to about 3 with a half time of about 10 ms and to the initial value with a half time of about 2 s. When two flashes separated by 0.2 s were given, the first phase of the decrease after the second flash occurred within 2 ms. After one flash given at high initial fluorescence yield, the 10-ms decay was followed by a 10 s increase to the initial value. After the two flashes 0.2 s apart, the rapid decay was not follewed by a slow increase.These and other experiments provided additional evidence for and extend an earlier hypothesis concerning the acceptor complex of Photosystem II (Bouges-Bocquet, B. (1973) Biochim. Biophys. Acta 314, 250–256; Velthuys, B. R. and Amesz, J. (1974) Biochim. Biophys. Acta 333, 85–94): reaction center 2 contains an acceptor complex QR consisting of an electron-transferring primary acceptor molecule Q, and a secondary electron acceptor R, which can accept two electrons in succession, but transfers two electrons simultaneously to a molecule of the tertiary acceptor pool, containing plastoquinone (A). Furthermore, the kinetics indicate that 2 reactions centers of System I, excited by a short flash, cooperate directly or indirectly in oxidizing a plastohydroquinone molecule (A^2?). If initially all components between photoreaction 1 and 2 are in the reduced state the following sequence of reactions occurs after a flash has oxidised A^2? via System I: Q^?R^2? + A → Q^?R + A^2? → QR^? + A^2?. During anaerobiosis two slow reactions manifest themselves: the reduction of R (and A) within 1 s, presumably by an endogenous electron donor D₁, and the reduction of Q in about 10 s when R is in the state R^? and A in the state A^2?. An endogenous electron donor, D₂, and Q^? compete in reducing the photooxidized donor complex of System II in reactions with half times of the order of 1 s.     

IS50-mediated inverse transposition. Discrimination between the two ends of an IS element

The crystal and molecular structure of l-pyroglutamyl-β-(2-thienyl)-l-alanyl-l-prolinamide, < Glu-Thi-Pro-NH₂(Thi²-TRH), C₁₇H₂₂N₄O₄S, has been determined from X-ray diffraction data. Thi²-TRH is a highly active analogue of thyroliberin, a thyrotropin-releasing hormone (TRH), in which the imidazole ring of the central histidine moiety in the natural hormone has been replaced by a 2-thienyl group. Thi²-TRH crystallizes from water in the monoclinic space group P2₁, $\text{a = 9.340(1)}\text{A}\text{?}\text{, b = 21.961(3)}\text{A}\text{?}\text{, c = 9.449(1)}\text{A}\text{?}$ and β = 109.58(1) °, with two molecules per asymmetric unit. These independent molecules, A and B, have the same general backbone conformation with the φ₂, ψ₂ and ψ₃ torsional angles close to ?90 °, +120 ° and +150 °, respectively, but they show different magnitudes of rotational disorder in the thiophene ring as well as a certain disorder in the pyrrolidine ring. A and B are cross-linked by four interchain hydrogen bonds, forming a two-stranded antiparallel β-pleated sheet structure. The molecules in these dimer fragments are further hydrogen-bonded to successive translated molecules along the a and c axes, forming a pronounced two-dimensional predominantly hydrophobic layer structure. These layers, in which the atoms are almost equally arranged on both sides, are separated by ordinary van der Waals' distances. A close correlation between the molecular conformation in the solid state and the preferential conformation in solution is found. It is concluded that the crystalline structure of Thi²-TRH possesses structural features which may be of relevance in the hormone-receptor interaction process.