Kinetics of reduction of the oxidized primary electron donor of Photosystem II in spinach chloroplasts and in Chlorella cells in the microsecond and nanosecond time ranges following flash excitation

Absorption changes (ΔA) at 820 nm, following laser flash excitation of spinach chloroplasts and Chlorella cells, were studied in order to obtain information on the reduction time of the photooxidized primary donor of Photosystem II at physiological temperatures.In the microsecond time range the difference spectrum of ΔA between 750 and 900 nm represents a peak at 820 nm, attributable to a radical-cation of chlorophyll a. In untreated dark-adapted material the signal can be attributed solely to P⁺?700; it decays in a polyphasic manner with half-times of 17 μs, 210 μs and over 1 ms. The oxidized primary donor of Photosystem II (P⁺_II) is not detected with a time resolution of 3 μs. After treatment with 3–10 mM hydroxylamine, which inhibits the donor side of Photosystem II, P⁺_II is observed and decays biphasically (a major phase with $\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{= 20–40 μ}\text{s}$, and a minor phase with $\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{? 200 μ}\text{s}$), probably by reduction by an accessory electron donor.In the nanosecond range, which was made accessible by a new fast-response flash photometer operating at 820 nm, it was found the P⁺_II is reduced with a half-time of 25–45 ns in untreated dark-adapted chloroplasts. It is assumed that the normal secondary electron donor is responsible for this fast reduction.     

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.     

Changes in the redox state of the secondary acceptor of Photosystem II associated with light-induced thylakoid protein phosphorylation

Thylakoid membrane protein phosphorylation affects photochemical reactions of Photosystem II. Incubation of thylakoids in the light with ATP leads to: (1) an increase in the amplitude of three components (4–6, 25–45 and 280–300 μs) of delayed light emission after a single flash without any change in their kinetics; (2) a reduction of the flash-dependent binary oscillations of chlorophyll a fluorescence yield associated with electron transfer from the primary quinone acceptor, Q, to the secondary quinone acceptor, B; (3) an increase in the $\text{B}{}^{\mathrm{?}}\text{B}$ ratio resulting from an increase in stability of the semiquinone anion during dark adaptation; and (4) no change in the redox state of the plastoquinone pool as determined by flash-induced photooxidation of the Photosystem I reaction center, P-700. All the above observations are reversible upon dephosphorylation of the thylakoid membranes. These data are explained by a protein phosphorylation-induced stabilization of the bound semiquinone anion, B^?. It is proposed that this increased stability may be due to an alteration in the accessibility of an endogenous reductant to B, or to an increase in dissipative cycling of charge around Photosystem II.     

Picosecond time-resolved study of MgCl2-induced chlorophyll fluorescence yield changes from chloroplasts

The MgCl₂-induced chlorophyll fluorescence yield changes in broken chloroplasts, suspended in a cation-free medium, treated with 3,-(3′,4′-dichlorophenyl)-1,1-dimethylurea and pre-illuminated, has been investigated on a picosecond time scale. Chloroplasts in the low fluorescing state showed a fluorescence decay law of the form exp $\text{?At}{}^{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$, where A was found to be 0.052 $\text{ps}{}^{\mathrm{<mtext>?1</mtext><mtext>2</mtext>}}$, and may be attributed to the rate of spillover from Photosystem II to Photosystem I. Addition of 10 mM MgCl₂ produced a 50% increase in the steady-state fluorescence quantum yield and caused a marked decrease in the decay rate. The fluorescence decay law was found to be predominantly exponential with a 1/e lifetime of 1.6 ns. These results support the hypothesis that cation-induced changes in the fluorescence yield of chlorophyll are related to the variations in the rate of energy transfer from Photosystem II to Photosystem I, rather than to changes in the partitioning of absorbed quanta between the two systems.     

Flash-induced photophosphorylation in chloroplasts with activated ATPase

Chloroplasts which were rapidly isolated from illuminated leaves showed activity of ATP hydrolysis at a level much higher than that of the dark control. Under the high-intensity illumination or under repetitive flash excitation, the activated chloroplasts synthesized more ATP than those with a low ATP hydrolysis activity. formed under repetitive flashes was smaller in the activated chloroplasts than in the inactive chloroplasts. The inhibition of ATP yield per flash by valinomycin or nigericin in the presence of K⁺ was stronger in the inactive chloroplasts than in the activated chloroplast. ATP synthesis in the activated chloroplasts seems to have a lower threshold.     

Redox titration of electron acceptor Q and the plastoquinone pool in Photosystem II

The primary photochemical quencher Q and the secondary electron acceptor pool in Photosystem II have been titrated. We used particles of Scenedesmus mutant No. 8 that lack System I and allowed the system to equilibrate with external redox mediators in darkness prior to measurement of the fluorescence rise curve.The titration of Q, as indicated by the dark level of F_i, occurs in two discrete steps. The high-potential component (Q_h) has a midpoint potential of +68 mV (pH 7.2) and accounts for ～67% of Q. The pH sensitivity of the midpoint potential is ?60 mV, indicating the involvement of 1 $\text{H}{}^{\mathrm{+}}\text{e}$. The low-potential component (Q₁) accounts for the remaining 33% of Q and shows a midpoint potential near?300 mV (pH 7.2).The plastoquinone pool, assayed as the half-time of the fluorescence rise curve, titrates as a single component with a midpoint potential 30–40 mV more oxidizing than that of Q_h, i.e., at 106 mV (pH 7.2). The E_m shows a pH sensitivity of ?60 mV/pH unit, indicating the involvement of 1 $\text{H}{}^{\mathrm{+}}\text{e}$. The observation that all 12–14 electron equivalents in the pool titrate as a single component indicates that the heterogeneity otherwise observed in the secondary acceptor system is a kinetic rather than a thermodynamic property.Illumination causes peculiar, and as yet unclarified, changes of both Q and the secondary pool under anaerobic conditions that are reversed by oxygen.     

A one microsecond component of chlorophyll luminescence suggesting a primary acceptor of system II of photosynthesis different from Q

The kinetics of the luminescence of chlorophyll a in Chlorella vulgaris were studied in the time range from 0.2 μs to 20 μs after a short saturating flash ($\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{= 25}\text{ns}$) under various pretreatment including anaerobiosis, flashes, continuous illumination and various additions. A 1 μs luminescence component probably originating from System II was found of which the relative amplitude was maximum under anaerobic conditions for reaction centers in the state SPQ^? before the flash, about one third for centers in the state S⁺PQ^? or SPQ before the flash, and about one tenth for centers in the state S⁺PQ before the flash. S is the secondary donor complex with zero charge; S⁺ is the secondary donor complex with 1 to 3 positive charges; P, the primary donor, is the photoactive chlorophyll a, P-680, of reaction center 2; Q^? is the reduced acceptor of System II, Q. Under aerobic conditions, where an endogenous quencher presumably was active, the luminescence was reduced by a factor two.The 1 μs decay of the luminescence is probably caused by the disappearance of P⁺ formed in the laser flash according to the reaction ZP⁺ → Z⁺P in which Z is the molecule which donates an electron to P⁺ and which is part of S. After addition of hydroxylamine, the 1 μs luminescence component changed with the incubation time exponentially (τ = 27 s) into a 30 μs component; during the same time, the variable fluorescence yield, measured 9 μs after the laser flash, decreased by a factor 2 with the same time constant. Hereafter in a second much slower phase the fluorescence yield decreased as an exponential function of the incubation time to about the dark value; meanwhile the 30 μs luminescence increased about 50% with the same time constant (τ = 7 min). Heat treatment abolished both luminescence components.The 1 μs luminescence component saturated at about the same energy as the System II fluorescence yield 60 μs after the laser flash and as the slower luminescence components. From the observation that the amplitude is maximum if the laser flash is given when the fluorescence yield is high after prolonged anaerobic conditions (state SQ^?), we conclude that the 1 μs luminescence is probably caused by the reaction

$\text{PWQ}{}^{\mathrm{?}}\text{+hv →}\text{P}\text{1}\text{WQ}{}^{\mathrm{?}}\text{→}\text{P}{}^{\mathrm{+}}\text{W}{}^{\mathrm{?}}\text{Q}{}^{\mathrm{?}}\text{→}\text{P}\text{1}\text{WQ}{}^{\mathrm{?}}\text{→ PWQ}{}^{\mathrm{?}}\text{+hv}$

in which W is an acceptor different from Q. The presence of S⁺ reduced the luminescence amplitude to about one third. Two models are discussed, one with W as an intermediate between P and Q and another, which gives the best interpretation, with W on a side path.     

Covalent modification of chloroplast Photosystem II polypeptides by p-nitrothiophenol

Illumination of the chlorophyll $\text{a}\text{b}$ light-harvesting complex in the presence of $\text{p-}\text{nitrothio}\text{[}{}^{14}\text{C]phenol}$ caused quenching of fluorescence emission at 685 nm (77 K) relative to 695 nm and covalent modification of light-harvesting complex polypeptides. Fluorescence quenching saturated with one p-nitrothiophenol bound per light-harvesting complex polypeptide (10–13 chlorophylls); $\text{1}\text{2}$ maximal quenching occurred with one p-nitrothiophenol bound per light-harvesting complex polypeptides (190–247 chlorophylls). This result provides direct evidence for excitation energy transfer between light-harvesting complex subunits which contain 4–6 polypeptides plus 40–78 chlorophylls per complex.Illumination of chloroplasts or Photosystem II (PS II) particles in the presence of $\text{p-}\text{nitrothio}\text{[}{}^{14}\text{C]phenol}$ caused inhibition of PS II activity and labeling of several polypeptides including those of 42–48 kilodaltons previously identified as PS II reaction center polypeptides. In chloroplasts, inhibition of oxygen evolution accelerated p-nitrothiophenol modification reactions; DCMU or donors to PS II decreased p-nitrothiophenol modification. These results are consistent with the hypothesis that accumulation of oxidizing equivalents on the donor side of PS II creates a ‘reactive state’ in which polypeptides of PS II are susceptible to p-nitrothiophenol modification.     

Flash-induced absorption changes of the primary donor of photosystem II at 820 nm in chloroplasts inhibited by low pH or tris-treatment

A comparative study is made, at 15 °C, of flash-induced absorption changes around 820 nm (attributed to the primary donors of Photosystems I and II) and 705 nm (Photosystem I only), in normal chloroplasts and in chloroplasts where O₂ evolution was inhibited by low pH or by Tris-treatment.At pH 7.5, with untreated chloroplasts, the absorption changes around 820 nm are shown to be due to P-700 alone. Any contribution of the primary donor of Photosystem II should be in times shorter than 60 μs.When chloroplasts are inhibited at the donor side of Photosystem II by low pH, an additional absorption change at 820 nm appears with an amplitude which, at pH 4.0, is slightly higher than the signal due to oxidized P-700. This additional signal is attributed to the primary donor of Photosystem II. It decays ($\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$ about 180 μs) mainly by back reaction with the primary acceptor and partly by reduction by another electron donor. Acid-washed chloroplasts resuspended at pH 7.5 still present the signal due to Photosystem II ($\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$ about 120 μs). This shows that the acid inhibition of the first secondary donor of Photosystem II is irreversible.In Tris-treated chloroplasts, absorption changes at 820 nm due to the primary donor of Photosystem II are also observed, but to a lesser extent and only after some charge accumulation at the donor side. They decay with a half-time of 120 μs.     

Damping of oscillations in the semiquinone absorption in reaction centers after successive flashes. Determination of the equilibrium between QA−QB and QAQB−

A quantitative model for the damping of oscillations of the semiquinone absorption after successive light flashes is presented. It is based on the equilibrium between the states Q_A^?Q_B and Q_AQ_B^?. A fit of the model to the experimental results obtained for reaction centers from Rhodopseudomonas sphaeroides gave a value of $\text{α =}\text{[}\text{Q}{}_{\mathrm{<mtext>A</mtext>}}{}^{\mathrm{?}}\text{Q}{}_{\mathrm{<mtext>B</mtext>}}\text{]}\text{([}\text{Q}{}_{\mathrm{<mtext>A</mtext>}}{}^{\mathrm{?}}\text{Q}{}_{\mathrm{<mtext>B</mtext>}}\text{] + [}\text{Q}{}_{\mathrm{<mtext>A</mtext>}}\text{Q}{}_{\mathrm{<mtext>B</mtext>}}{}^{\mathrm{?}}\text{])}\text{= 0.065 ± 0.005}$ (T = 21°C, pH 8).     

Localization at the ultrastructural level of maternality derived enzyme and determination of the time of paternal gene expression for acid phosphatase-1 in Drosophila melanogaster.

Ultrastructural histochemistry instead of acrylamide gel electrophoresis (see R. Yasbin, J. Sawicki, and R. J. MacIntyre, 1978, Develop. Biol. 63, 00-00) is used to determine the time of paternal gene expression for the enzyme acid phosphatase-1 of Drosophila melanogaster in $\text{Acph-1}{}^{\mathrm{n}}\text{Acph-1}{}^{\mathrm{B}}$ embryos in which the null allele is derived from the female parent. Timed embryos were histochemically stained for acid phosphatase activity according to the lead phosphate method of Gomori and were examined at the ultrastructural level. Enzyme activity, resulting from activation of the paternal Acph-1 gene, is detected as early as 5 hr after fertilization. Maternally derived enzyme in $\text{Acph-1}{}^{\mathrm{B}}\text{Acph-1}{}^{\mathrm{B}}$ embryos is found principally in the yolk regions and around invaginations. This suggests that acid phosphatase-1 functions in yolk digestion and in cell movements during early embryogenesis.     

Reconstitution of b-type cytochrome oxidase from Rhodopseudomonas capsulata in liposomes and turnover studies of proton translocation

Purified b-type cytochrome oxidase from Rhodopseudomonas capsulata was incorporated into phospholipid vesicles to measure proton extrusion with pulses of ferrocytochrome c for one oxidase turnover. In accordance with the pH shift of its midpoint potential, the purified oxidase showed a proton extrusion of 0.24 $\text{H}{}^{\mathrm{+}}\text{e}{}^{\mathrm{?}}$ with uptake of 1 $\text{H}{}^{\mathrm{+}}\text{e}{}^{\mathrm{?}}$ from the liposomes for the reduction of oxygen to water. This proton translocation could only be observed in the presence of valinomycin +K⁺ and was not inhibited by DCCD. Oxidase preparations from the first purification step, which contain other protein compounds especially a membrane-bound cytochrome c but not the ubiquinol-cytochrome c₂-oxidoreductase showed a pumping activity of 0.9 $\text{H}{}^{\mathrm{+}}\text{e}{}^{\mathrm{?}}$, which was inhibited by DCCD for nearly 75%. Inhibition of the electron transfer was not observed, which could be explained by a ‘molecular slipping’ of proton extrusion and electron transfer. Proton extrusion from two oxidase-turnovers was only 80% of that from one turnover. The proton pumping of the b-type oxidase strongly depended on the enzyme/phospholipid ratio.     

Photosystem II energy coupling in chloroplasts with H2O2 as electron donor

NH₂OH-treated, non-water-splitting chloroplasts can oxidize H₂O₂ to O₂ through Photosystem II at substantial rates (100–250 μequiv · h^?1 · mg^?1 chlorophyll with 5 mM H₂O₂) using 2,5-dimethyl-p-benzoquinone as an electron acceptor in the presence of the plastoquinone antagonist dibromothymoquinone. This H₂O₂ → Photosystem II → dimethylquinone reaction supports phosphorylation with a $\text{P}\text{e}{}_2$ ratio of 0.25–0.35 and proton uptake with $\text{H}{}^{\mathrm{+}}\text{e}$ values of 0.67 (pH 8)–0.85 (pH 6). These are close to the $\text{P}\text{e}{}_2$ value of 0.3–0.38 and the $\text{H}{}^{\mathrm{+}}\text{e}$ values of 0.7–0.93 found in parallel experiments for the H₂O → Photosystem II → dimethylquinone reaction in untreated chloroplasts. Semi-quantitative data are also presented which show that the donor → Photosystem II → dibromothymoquinone (→O₂) reaction can support phosphorylation when the donor used is a proton-releasing reductant (benzidine, catechol) but not when it is a non-proton carrier (I^?, ferrocyanide).     

New experimental approach to the estimation of rate of electron transfer from the primary to secondary acceptors in the photosynthetic electron transport chain of purple bacteria

A method for calculating the rate constant ($\text{K}{}_{\mathrm{<mtext>A</mtext><mtext>1</mtext><mtext>A</mtext><mtext>2</mtext>}}$) for the oxidation of the primary electron acceptor (A₁) by the secondary one (A₂) in the photosynthetic electron transport chain of purple bacteria is proposed.The method is based on the analysis of the dark recovery kinetics of reaction centre bacteriochlorophyll (P) following its oxidation by a short single laser pulse at a high oxidation-reduction potential of the medium. It is shown that in Ectothiorhodospira shaposhnikovii there is little difference in the value of $\text{K}{}_{\mathrm{<mtext>A</mtext><mtext>1</mtext><mtext>A</mtext><mtext>2</mtext>}}$ obtained by this method from that measured by the method of Parson ((1969) Biochim. Biophys. Acta 189, 384–396), namely: $\text{(4.5±1.4) · 10}{}^3\text{s}{}^{\mathrm{?1}}$ and $\text{(6.9±1.2) · 10}{}^3\text{s}{}^{\mathrm{?1}}$, respectively.The proposed method has also been used for the estimation of the $\text{K}{}_{\mathrm{<mtext>A</mtext><mtext>1</mtext><mtext>A</mtext><mtext>2</mtext>}}$ value in chromatophores of Rhodospirillum rubrum deprived of constitutive electron donors which are capable of reducing P⁺ at a rate exceeding this for the transfer of electron from A₁ to A₂. The method of Parson cannot be used in this case. The value of $\text{K}{}_{\mathrm{<mtext>A</mtext><mtext>1</mtext><mtext>A</mtext><mtext>2</mtext>}}$ has been found to be $\text{(2.7±0.8) · 10}{}^3\text{s}{}^{\mathrm{?1}}$.The activation energies for the A₁ to A₂ electron transfer have also been determined. They are 12.4 kcal/mol and 9.9 kcal/mol for E. shaposhnikovii and R. rubrum, respectively.     

Determination of H+e− ratios in chloroplasts with flashing light

Using a rapid pH electrode, measurements were made of the flash-induced proton transport in isolated spinach chloroplasts. To calibrate the system, we assumed that in the presence of ferricyanide and in steady-state flashing light, each flash liberates from water one proton per reaction chain. We concluded that with both ferricyanide and methylviologen as acceptors two protons per electron are translocated by the electron transport chain connecting Photosystem II and I. With methyl viologen but not with ferricyanide as an acceptor, two additional protons per electron are taken up due to Photosystem I activity. One of these latter protons is translocated to the inside of the thylakoid while the other is taken up in H₂O₂ formation. Assuming that the proton released during water splitting remains inside the thylakoid, we compute $\text{H}{}^{\mathrm{+}}\text{e}{}^{\mathrm{?}}$ ratios of 3 and 4 for ferricyanide and methyl viologen, respectively.In continuous light of low intensity, we obtained the same $\text{H}{}^{\mathrm{+}}\text{e}{}^{\mathrm{?}}$ ratios. However, with higher intensities where electron transport becomes rate limited by the internal pH, the $\text{H}{}^{\mathrm{+}}\text{e}{}^{\mathrm{?}}$ ratio approached 2 as a limit for both acceptors.A working model is presented which includes two sites of proton translocation, one between the photoacts, the other connected to Photosystem I, each of which translocates two protons per electron. Each site presents a ≈ 30 ms diffusion barrier to proton passage which can be lowered by uncouplers to 6–10 ms.     

Photoconversion and regeneration of active protochlorophyll(ide) in mutants defective in the regulation of chlorophyll synthesis

Seedlings carrying mutations in regulatory genes for protochlorophyll(ide) synthesis accumulate protochlorophyll(ide) in darkness in amounts exceeding the wildtype level. Thus, +/tig-d¹² and $\text{tig-b}{}^{24}\text{tig-b}{}^{24}$accumulate 2-fold, $\text{tig-o}{}^{34}\text{tig-o}{}^{34}$ 5- to 6-fold, and $\text{tig-d}{}^{12}\text{tig-d}{}^{12}$ 15-fold more protochlorophyll(ide) than the wild type.The amount of photoconvertible protochlorophyll(ide) accumulated in darkness is the same in all genotypes, despite the large differences in total protochlorophyll(ide) content, indicating a constant number of photoconversion sites.When briefly illuminated leaves are returned to darkness, regeneration of active protochlorophyll(ide) from the pool of inactive protochlorophyll(ide) takes place in wild-type and mutant leaves. Compared to the wild type, the rate of protochlorophyll(ide) activation during 4- and 10-min dark periods is higher in +/tig-d¹², $\text{tig-b}{}^{24}\text{tig-b}{}^{24}$, and $\text{tig-o}{}^{34}\text{tig-o}{}^{34}$, but lower in $\text{tig-d}{}^{12}\text{tig-d}{}^{12}$.There was no indication that the accumulation of protochlorophyll(ide) influences the conversion sites of the protochlorophyll(ide) holochrome, as the kinetics of photoconversion of initially active protochlorophyll(ide) in leaves with the genotypes +/+, +/tig-o³⁴, and $\text{tig-o}{}^{34}\text{tig-o}{}^{34}$ are similar or identical.     

A flash photolysis ESR study of Photosystem II Signal IIvf, the physiological donor to P-680+

In flash-illuminated, oxygen-evolving spinach chloroplasts and green algae, a free radical transient has been observed with spectral parameters similar to those of Signal II ($\text{g ≈ 2.0045}$, $\text{ΔH}{}_{\mathrm{<mtext>pp</mtext>}}\text{≈ 19}\text{G}$). However, in contrast with ESR Signal II, the transient radical does not readily saturate even at microwave power levels of 200 mW. This species is formed most efficiently with “red” illumination ($\text{λ < 680}\text{nm}$ and occurs stoichiometrically in a 1 : 1 ratio with $\text{P-700}{}^{\mathrm{+}}$. The Photosystem II transient is formed in less than 100 μs and decays via first-order kinetics with a halftime of 400–900 μs. Additionally, the $\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$ for radical decay is temperature independent between 20 and 4 °C; however, below 4 °C the transient signal exhibits Arrhenius behavior with an activation energy of approx. 10 kcal · mol^?1. Inhibition of electron transport through Photosystem II by $\text{o-}\text{phenanthroline}$, 3-(3,4-dichlorophenyl)-1,1-dimethylurea or reduced $\text{2,5-}\text{dibromo}\text{-3-}\text{methyl}\text{-6-}\text{isopropyl}\text{-p-}\text{benzoquinone}$ suppresses the formation of the light-induced transient. At low concentrations (0.2 mM), $\text{2,5-}\text{dibromo}\text{-3-}\text{methyl}\text{-6-}\text{isopropyl}\text{-p-}\text{benzoquinone}$ partially inhibits the free radical formation, however, the decay kinetics are unaltered. High concentrations of $\text{2,5-}\text{dibromo}\text{-3-}\text{methyl}\text{-6-}\text{isopropyl}\text{-p-}\text{benzoquinone}$ (1–5 mM) restore both the transient signal and electron flow through Photosystem II. These findings suggest that this “quinoidal” type ESR transient functions as the physiological donor to the oxidized reaction center chlorophyll, $\text{P-680}{}^{\mathrm{+}}$.     

The repetitive sequence structure of component alpha DNA and its relationship to the nucleosomes of the African green monkey.

An analysis of the repeat structure of the highly repetitive sequence, component α DNA of the African green monkey, shows that the DNA contains restriction sites for EcoRI, $\text{Eco}\text{RI}{}^1$, HindIII and HaeIII. All four restriction enzyme activities indicate a basic repeat length of 176 ± 4 base-pairs. In addition to primary $\text{Eco}\text{RI}{}^1$ and HindIII sites, about 59% of the repeat sequences contain secondary $\text{Eco}\text{RI}{}^1$ sites and about 36% of the repeat sequences contain secondary HindIII sites. The secondary sites are located less than 176 base-pairs from the primary sites and their cleavage yields several complex series of minor, intermediate segments in gels of the partial $\text{Eco}\text{RI}{}^1$ or HindIII digests. Cleavage at the secondary sites yields segments shorter than the unit monomer in the limit digests. The sites for EcoRI, $\text{Eco}\text{RI}{}^1$, HindIII and HaeIII have been mapped within the repeat unit.Treatment of the monkey nuclei with micrococcal nuclease at 2 °C and in the presence of 80 mm-NaCl reveals two distinct populations of nucleosomes. One population contains bulk DNA sequences, and after cleavage with micrococcal nuclease this population yields heterogeneous segments of DNA spanning 180 to 200 base-pairs in length. The other population contains component α sequences and after cleavage with micrococcal nuclease yields homogeneous segments of component α DNA that are exact multiples of the basic sequence repeat unit of 176 base-pairs. Thus, the cleavage by micrococcal nuclease of nucleosomal arrays containing component α sequences is as regular and precise as the cleavage of the purified DNA by the restriction enzymes. The resolution of the two distinct subsets of nucleosomes in the monkey nuclei is dependent upon the conditions of ionic strength and temperature employed during the nuclear isolation and the micrococcal nuclease digestion.These observations are consistent with a phase relation between the component α repeat sequences and the associated nucleosomal proteins (Musich et al., 1977b). They are also in accord with the hypothesis that the subunit structure of constitutive heterochromatin modulates or determines the repeat sequence structure and hence, the evolution of many highly repetitive mammalian DNAs (Maio et al., 1977).     

Synthesis of phosphatidylglycerol by chloroplasts from leaves of Spinacia oleracea L. (spinach)

Purified chloroplasts from leaves of Spinacia oleracea L. (spinach) incorporated glycerol 3-phosphate into diacylglycerol, monoacylglycerol, phosphatidylglycerol, phosphatidic acid, and lysophosphatidic acid. The omission of ATP or CTP, CoA or illumination decreased the incorporation markedly. The fraction of incorporated glycerol 3-phosphate found in phosphatidylglycerol was greatly reduced by the omission of bicarbonate, acetate, and ATP, or in darkness, low-osmolarity medium, or high magnesium ion concentration (10 mM). Incorporation of glycerol 3-phosphate into lipid and specifically into phosphatidylglycerol was optimal at a $\text{Mg}{}^{\mathrm{2+}}\text{CTP}$ ratio of 1, whereas the optimal ratio for $\text{Mg}{}^{\mathrm{2+}}\text{ATP}$ was closer to 2. The $\text{Mg}{}^{\mathrm{2+}}\text{CTP}$ gave lower total incorporation but a higher fraction of incorporation in phosphatidylglycerol. Triton X-100 inhibited incorporation of glycerol 3-phosphate into lipid, especially into phosphatidylglycerol.