Theoretical insights into the effects of molar ratios on stabilities,mechanical properties,and detonation performance of CL-20/HMX cocrystal explosives by molecular dynamics simulation

To research and estimate the effects of molar ratios on structures, stabilities, mechanical properties, and detonation properties of CL-20/HMX cocrystal explosive, the CL-20/HMX cocrystal explosive models with different molar ratios were established in Materials Studio (MS). The crystal parameters, structures, stabilities, mechanical properties, and some detonation parameters of different cocrystal explosives were obtained and compared. The molecular dynamics (MD) simulation results illustrate that the molar ratios of CL-20/HMX have a direct influence on the comprehensive performance of cocrystal explosive. The hardness and rigidity of the 1:1 cocrystal explosive was the poorest, while the plastic property and ductibility were the best, thus implying that the explosive has the best mechanical properties. Besides, it has the highest binding energy, so the stability and compatibility is the best. The cocrystal explosive has better detonation performance than HMX. In a word, the 1:1 cocrystal explosive is worth more attention and further research. This paper could offer some theoretical instructions and technological support, which could help in the design of the CL-20 cocrystal explosive.     

Theoretical investigation of the effects of the molar ratio and solvent on the formation of the pyrazole–nitroamine cocrystal explosive 3,4-dinitropyrazole (DNP)/2,4,6,8,10,12-hexanitrohexaazaisowurtzitane (CL-20)

The effects of the molar ratio, temperature, and solvent on the formation of the cocrystal explosive DNP/CL-20 were investigated using molecular dynamics (MD) simulation. The cocrystal structure was predicted through Monte Carlo (MC) simulation and using first-principles methods. The results showed that the DNP/CL-20 cocrystal might be more stable in the molar ratio 1:1 near to 318 K, and the most probable cocrystal crystallizes in the triclinic crystal system with the space group P\( \overline{1} \). Cocrystallization was more likely to occur in methanol and ethanol at 308 K as a result of solvent effects. The optimized structure and the reduced density gradient (RDG) of the DNP/CL-20 complex confirmed that the main driving forces for cocrystallization were a series of hydrogen bonds and van der Waals forces. Analyses of the trigger bonds, the charges on the nitro groups, the electrostatic surface potential (ESP), and the free space per molecule in the cocrystal lattice were carried out to further explore their influences on the sensitivity of CL-20. The results indicated that the DNP/CL-20 complex tended to be more stable and insensitive than pure CL-20. Moreover, an investigation of the detonation performance of the DNP/CL-20 cocrystal indicated that it possesses high power.

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Graphical abstract DNP/CL-20 cocrystal models with different molar ratios were investigated at different temperatures using molecular dynamics (MD) simulation methods. Binding energies and mechanical properties were probed to determine the stability and performance of each cocrystal model. Solvated DNP/CL-20 models were established by adding solvent molecules to the cocrystal surface. The binding energies of the models in various solvents were calculated in order to identify the most suitable solvent and temperature for preparing the cocrystal explosive DNP/CL-20

     

Molecular dynamics calculation on structures,stabilities, mechanical properties,and energy density of CL-20/FOX-7 cocrystal explosives

In this article, different CL-20/FOX-7 cocrystal models were established by the substitution method based on the molar ratios of CL-20:FOX-7. The structures and comprehensive properties, including mechanical properties, stabilities, and energy density, of different cocrystal models were obtained and compared with each other. The main aim was to estimate the influence of molar ratios on properties of cocrystal explosives. The molecular dynamics (MD) simulation results show that the cocrystal model with molar ratio 1:1 has the best mechanical properties and highest binding energy, so the CL-20/FOX-7 cocrystal model is more likely to form in 1:1 M ratio. The detonation parameters show that the cocrystal explosive exhibited preferable energy density and excellent detonation performance. In a word, the 1:1 cocrystal model has the best comprehensive properties, is very promising, and worth more theoretical investigations and experimental tests. This paper gives some original theories to better understand the cocrystal mechanism and provides some helpful guidance and useful instructions to help design CL-20 cocrystal explosives.     

Mesoscopic simulation of aggregate behaviour of fluoropolymers in the TATB-based PBX

The aggregate behaviours of fluoropolymers F₂₃₁₁, F₂₃₁₂, F₂₃₁₃ and F₂₃₁₄ in TATB-based PBX were studied using the dissipative particle dynamics method. All of these four different fluoropolymers form the mesh-ball-like structure, in which the triaminotrinitrobenzene (TATB) explosive is wrapped. The self-aggregate behaviour and the poor wrap property of fluoropolymers in the TATB-based PBX are consistent with the experimental observation. Simulations with various chlorotrifluoroethylene (CTFE) contents were made. Results indicate that some fluoropolymers are disengaged from the main spherical phases forming a new small spherical phase with the increasing of CTFE content in fluoropolymers. The fluoropolymers form mesh and honeycomb structures at 350 and 400 K, respectively. In addition, the dynamic behaviour of fluoropolymers in TATB-based PBX was also studied and analysed in detail.     

Molecular dynamics study on the correlation between structure and sensitivity for defective RDX crystals and their PBXs

Molecular dynamics simulation was applied to investigate the sensitivities of perfect and defective RDX (cyclotrimethylene trinitramine) crystals, as well as their PBXs (polymer-bonded explosives) with the polymeric binder F₂₃₁₁, in the NPT (constant number of particles, constant pressure, constant temperature) ensemble using the COMPASS force field. Five kinds of defects—two dislocations, one vacancy, and two types of doping—were considered separately. The bond length distribution and the maximum (L _max) and average (L _ave) bond lengths of the N–NO₂ trigger bonds in RDX were obtained and their relationships to the sensitivities of RDX and PBXs are discussed. L _max was found to be an important structural parameter for judging the relative sensitivity, and defects were observed to have little effect on the sensitivities of PBXs, due to the strong desensitizing effect of the polymer F₂₃₁₁.     

Theoretical investigation of the safety of nitroguanidine-based PBXs containing the nonpolar desensitizing agent polytetrafluoroethylene

In order to elucidate why the inclusion of a nonpolar desensitizing agent in polymer-bonded explosives (PBXs) affects their sensitivity and safety, the intermolecular interactions between nitroguanidine (NQ: a high-energy-density compound used as a propellant and in explosive charges) and F₂C=CF₂ were investigated theoretically at the B3LYP/6–311++G(2df,2p) and M06-2X/6–311++G(2df,2p) levels of theory, focusing especially on the influence of intermolecular interactions on the strength of the trigger bond in NQ. The binding energies and mechanical properties of various β-NQ/polytetrafluoroethylene PBXs were also studied via molecular dynamics simulation. The results indicated that the weak intermolecular interactions between NQ and F₂C=CF₂ have almost no effect on the strength of the trigger bond or the energy barrier to the intramolecular hydrogen-transfer isomerization of NQ, as also confirmed by an AIM (atoms in molecules) analysis. However, the mechanical properties of the β-NQ/polytetrafluoroethylene PBXs were found to be significantly different from those of pure β-NQ: the PBXs showed reduced rigidity and brittleness, greater elasticity and plasticity, and—in particular—better ductility. Thus, β-NQ-based PBXs with polytetrafluoroethylene are predicted to be less sensitive to external mechanical stimuli, leading to reduced explosive sensitivity and increased safety.

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Only mechanical properties influence the safety of nitroguanidine-based PBXs

     

A novel model for the molecular dynamics simulation study on mechanical properties of HMX/F2311 polymer-bonded explosive

The ‘insert’ model for β-octahydro-1,3,5,7-tetranitro-1,3,5,7-tetrazocine (HMX)-based polymer-bonded explosive (PBX) was proposed for finding the relation of temperatures with mechanical properties. This model was simulated by using molecular dynamics models. The elastic constants and the effective moduli were calculated with static analysis method. Cauchy pressure was also calculated. It is found that the rigidity is weakened and the ductibility is improved by adding a small amount of F₂₃₁₁ in the crystalline HMX. The rigidity is also weakened with increasing temperature. However, the ductibility of HMX/F₂₃₁₁ PBX changes as a parabola with increasing temperature duo to the enhancement of F₂₃₁₁ molecular chain movement and simultaneously the increment of high energy conformation ratio in this molecular chain, i.e. the increment of the molecular chain rigidity.     

Growth morphology of CL-20/HMX cocrystal explosive: insights from solvent behavior under different temperatures

A 2,4,6,8,10,12-hexanitro-2,4,6,8,10,12-hexaazaisowurtzitane (CL-20) /1,3,5,7-tetranitro-1,3,5,7-tetrazacyclooctane (HMX)-isopropanol (IPA) interfacial model was constructed to investigate the effect of temperature on cocrystal morphology. A constant volume and temperature molecular dynamics (NVT-MD) simulation was performed on the interfacial model at various temperatures (295–355 K, 20 K intervals). The surface electrostatic potential (ESP) of the CL-20/HMX cocrystal structure and IPA molecule were studied by the B3LYP method at 6–311++G (d, p) level. The surface energies, polarities, adsorption energy, mass density distribution, radial distribution function (RDF), mean square displacement (MSD) and relative changes of attachment energy were analyzed. The results show that polarities of (1 0 0) and (0 1 1) cocrystal surfaces may be more negative and affected by IPA solvent. The adsorption energy per area indicates that growth of the (1 0–2) face in IPA conditions may be more limited, while the (1 0 0) face tends to grow more freely. MSD and diffusion coefficient (D) analyses demonstrated that IPA molecules gather more easily on the cocrystal surface at lower temperatures, and hence have a larger effect on the growth of cocrystal faces. RDF analysis shows that, with the increasing of temperature, the strength of hydrogen bond interactions between cocrystal and solvent becomes stronger, being highest at 335 K for the (1 0 0) and (0 1 1) interfacial models. Results of relative changes of modified attachment energy show that (1 0 0) and (0 1 1) faces tends to be larger than other faces. Moreover, the predicted morphologies at 295 and 355 K are consistent with experimental values, proving that the CL-20/HMX-IPA interfacial model is a reasonable one for this study.

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Graphical Abstract Construction of 2,4,6,8,10,12-hexanitro-2,4,6,8,10,12-hexaazaisowurtzitane (CL-20) /1,3,5,7-tetranitro-1,3,5,7-tetrazacyclooctane (HMX)-isopropanol (IPA) interfacial model, analysis, and morphology prediction of cocrystal.

     

Theoretical insights into the structures and mechanical properties of HMX/NQ cocrystal explosives and their complexes,and the influence of molecular ratios on their bonding energies

Molecular dynamics (MD) methods were employed to study the binding energies and mechanical properties of selected crystal planes of 1,3,5,7-tetranitro-1,3,5,7-tetrazacyclooctane (HMX)/nitroguanidine (NQ) cocrystals at different molecular molar ratios. The densities and detonation velocities of the cocrystals at different molar ratios were estimated. The intermolecular interaction and bond dissociation energy (BDE) of the N–NO₂ bond in the HMX:NQ (1:1) complex were calculated using the B3LYP, MP2(full) and M06-2X methods with the 6-311++G(d,p) and 6-311++G(2df,2p) basis sets. The results indicated that the HMX/NQ cocrystal prefers cocrystalizing in a 1:1 molar ratio, and the cocrystallization is dominated by the (0 2 0) and (1 0 0) facets. The K, G, and E values of the ratio of 1:1 are smaller than those of the other ratios, and the 1:1 cocrystal has the best ductility. The N–NO₂ bond becomes stronger upon the formation of the intermolecular H-bonding interaction and the sensitivity of HMX decreases in the cocrystal. This sensitivity change in the HMX/NQ cocrystal originates not only from the formation of the intermolecular interaction but also from the increment of the BDE of N–NO₂ bond in comparison with isolated HMX. The HMX/NQ (1:1) cocrystal exhibits good detonation performance. Reduced density gradient (RDG) reveals the nature of cocrystallization. Analysis of the surface electrostatic potential further confirmed that the sensitivity decreases in complex (or cocrystal) in comparison with that in isolated HMX.

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Graphical Abstract Binding energies and mechanical properties of HMX/NQ cocrystals in different molecular molar ratios were studied using molecular dynamics methods. The origin of the sensitivity change in the HMX/NQ cocrystal originates from formation of intermolecular interactions and the bond dissociation energy increment of the N–NO₂ bond

     

Easy methods to study the smart energetic TNT/CL-20 co-crystal

2,4,6,8,10,12-hexanitro-2,4,6,8,10,12-hexaazaisowurtzitane (CL-20) is a high-energy nitramine explosive with high mechanical sensitivity. 2,4,6-trinitrotoluene (TNT) is insensitive but by no means a high performance explosive. To reveal the significant importance and smart-material functionality of the energetic-energetic co-crystals, the stability, mechanical and explosive properties TNT/CL-20 co-crystal, TNT crystal and CL-20 crystal were studied. Non-hydrogen bonded non-covalent interactions govern the structures of energetic-energetic co-crystals. However, it is very difficult to accurately calculate the non-covalent intermolecular interaction energies. In this paper, the local conformation and the intricate non-covalent interactions were effectively mapped and analyzed from the electron density (ρ) and its derivatives. The results show that the two components TNT and CL-20 are connected mainly by nitro–aromatic interactions, and nitro–nitro interactions. The steric interactions in TNT/CL-20 could not be confronted with the attractive interactions. Moreover, the scatter graph of TNT crystal reveals the reason why TNT is brittle. The detailed electrostatic potential analysis predicted that the detonation velocities (D) and impact sensitivity for the compounds both increase in the sequence of CL-20 > TNT/CL-20 co-crystal > TNT. Additionally, TNT/CL-20 co-crystal has better malleability than its pure components. This demonstrates the capacity and the feasibility of realizing explosive smart materials by co-crystallization, even if strong hydrogen bonding schemes are generally lacking in energetic materials.

The quenching characteristics of potassium iridic chloride and their meaning for the origin of chlorophyll fluorescence components

To understand the origins of the different lifetime components of photosystem 2 (PS2) chlorophyll (Chl) fluorescence we have studied their susceptibility to potassium iridic chloride (K₂IrCl₆) which has been shown to bleach antenna pigments of photosynthetic bacteria (Loach et al. 1963). The addition of K₂IrCl₆ to PS2 particles gives rise to a preferential quenching of the variable Chl fluorescence (F_v). At concentrations lower than 20 M, this is brought about mainly by a decrease in the yield, but not in the lifetime, of the slowest component when all the PS2 reaction centres are closed (F_M). The yield of the middle and fast decays are not significantly altered. This type of quenching is not seen with DNB. The iridate-induced quenching of the initial fluorescence level (F₀) is due to a proportional decrease in the yield and lifetime of the three components and correlates with the observed modification in the relative quantum yield of oxygen evolution. In this concentration range a bleaching of Chl a is seen. At higher iridate levels, greater than 20 M, a proportional decrease in the lifetimes and yields of the three kinetic components is seen at F_M. These changes are associated with a carotenoid bleaching. In isolated light harvesting Chl a/b complexes of PS2 (LHC2), iridate addition converts a 4 ns decay into a 200 ps emission and both types of bleaching are observed. By also measuring the rate of PS2 trap closure versus iridate concentration, we have discussed the results in terms of excitation energy transfer.Abbreviations DNB m-dinitrobenzene - F_M maximum Chl fluorescence - F₀ initial fluorescence - F_v variable fluorescence - I pheophytin a primary electron acceptor of PS2 - P₆₈₀ chlorophyll a of photochemical centre - PS2 photosystem 2 - Q_A primary stable electron acceptor of PS2 - Chl chlorophyll - LHC2 light harvesting Chl a/b complex of PS2 - MES 2(N-morpholino) ethanesulfonic acid - DCMU 3-(3-4-dichlorophenyl) 1-1 dimethylurea - PPBQ phenyl-p-benzo-quinone - BBY PS2-enriched membranes prepared as in Berthold et al. (1981) - Q₄₀₀ PS2 electron acceptor with a midpoint potential of 400 mV     

The effect of high-energy-state excitation quenching on maximum and dark level chlorophyll fluorescence yield

The quenching of variable fluorescence yield (q_N) and the quenching of dark level fluorescence yield (q₀) directly atributable to high-energy-state fluorescence quenching (q_E) was studied to distinguish between energy dissipation in the antenna and light harvesting complexes (antenna quenching) and energy dissipation at the reaction centres (reaction centre quenching). A consistent relationship was obtained between q_N and q₀ in barley leaves, the green alga Dunaliella C9AA and in pea thylakoids with 2,3,5,6-tetramethyl-p-phenylene diamine (DAD) as mediator of cyclic electron flow around PS 1. This correlated well with the relationship obtained using m-dinitrobenzene (DNB), a chemical model for antenna quenching, to quench fluorescence in Dunaliella C9AA or pea thylakoids. The results also correlated reasonably well with theoretical predictions by the Butler model for antenna quenching, but did not correlate with the predictions for reaction centre quenching. It is postulated that q_E quenching therefore occures in the antenna and light harvesting complexes, and that the small deviation from the Butler prediction is due to PS 2 heterogeneity.Abbreviations 9-aa 9-aminoacridine - DCMU 3-(3,4-dichlorophenyl)-1,1-dimethylurea - EDTA Ethylenediaminetetra-acetic acid - Hepes 4-(2-hydroxyethyl)-1-piperazineethanesulphonic acid - Mes 2-(N-morpholino) prophanesulfonate - PS 1 photosystem 1 - PS 2 photosystem 2 - Q_A and Q_B primary and secondary stable electron acceptors of photosystem 2 - q_N non-photochemical fluorescence quenching coefficient - q_E high-energy-state fluorescence quenching coefficient - q₀ quenching coefficient for F₀ - F₀ dark level fluorescence yield - F_m maximum fluorescence yield - F_v variable fluorescence yield - F_v/F_m ratio of variable to total fluorescence yield - DAD 2,3,5,6-tetramethyl-p-phenylene diamine - DNB m-dinitrobenzene     

Evidence that the variable chlorophyll fluorescence in Chlamydomonas reinhardtii is not recombination luminescence

Room temperature single photon timing measurements on intact, Chlamydomonas reinhardtii cells at low excitation energies have been analysed using a four exponential kinetic model. Closing the PSII reaction centres produced two major variable lifetime and two minor constant lifetime components. The yield of each component mirrored the changes in lifetime. Such observations indicate the presence of well-connected PSII centres favoring excitation energy transfer. A Chlamydomonas mutant lacking PSII reaction centre proteins exhibited decay components equivalent to those seen at F_M in the wild-type. A titration of in vivo fluorescence, in both the mutant and wild-type algae, using DNB, produced decay components similar to those seen on opening PSII reaction centres. Such observations indicate that the luminescence hypothesis for the origin of the long-lived lifetime component is not the case.Abbreviations DCMU 3-(3,4-dichlorophenyl)-1, 1-dimethyl urea - DNB m,Dinitrobenzene - PSII photosystem II - RCII PSII recation centre - I^- reduced pheophytin - Q_A primary stable electron ecceptor of PSII - Ch1 chlorophyl1 - LHCII light harvesting Ch1a/b protein complex of PSII - F_O initial fluorescence level - F_M maximum fluorescence level - F_V variable fluorescence (F_M-F_O) - ps picosecond - ns nanosecond     

Mechanical properties of aponeurosis and tendon of the cat soleus muscle during whole-muscle isometric contractions

Recent studies have suggested that the mechanical properties of aponeurosis are not similar to the properties of external tendon. In the present study, the lengths of aponeurosis, tendon, and muscle fascicles were recorded individually, using piezoelectric crystals attached to the surface of each structure during isometric contractions in the cat soleus muscle. We used a surgical microscope to observe the surface of the aponeurosis, which revealed a confounding effect on measures of aponeurosis length due to sliding of a thin layer of epimysium over the proximal aponeurosis. After correcting for this artifact, the stiffness computed for aponeurosis was similar to tendon, with both increasing from around 8 F₀/L_c (F₀ is maximum isometric force and L_c is tissue length) at 0.1 F₀ to 30 F₀/L_c at forces greater than 0.4 F₀. At low force levels only (0.1 F₀), aponeurotic stiffness increased somewhat as fascicle length increased. There was a gradient in the thickness of the aponeurosis along its length: its thickness was minimal at the proximal end and maximal at the distal end, where it converged to form the external tendon. This gradient in thickness appeared to match the gradient in tension transmitted along this structure. We conclude that the specific mechanical properties of aponeurosis are similar to those of tendon. © 1995 Wiley-Liss, Inc.     

F0F1 ATP synthase of Streptomycetes: Modulation of activity and oligomycin resistance by protein Ser/Thr kinases

Inverted membrane vesicles of Gram-positive actinobacteria Streptomyces fradiae, S. lividans, and S. avermitilis have been prepared and membrane-bound F₀F₁ ATP synthase has been biochemically characterized. It has been shown that the ATPase activity of membrane-bound F₀F₁ complex is Mg²⁺-dependent and moderately stimulated by high concentrations of Ca²⁺ ions (10–20 mM). The ATPase activity is inhibited by N,N′-dicyclohexylcarbodiimide and oligomycin A, typical F₀F₁ ATPase inhibitors that react with the membrane-bound F₀ complex. The assay of biochemical properties of the F₀F₁ ATPases of Streptomycetes in all cases showed the presence of ATPase populations highly susceptible and insensitive to oligomycin A. The in vitro labeling and inhibitory assay showed that the inverted phospholipid vesicles of S. fradiae contained active membrane-bound Ser/Thr protein kinase(s) phosphorylating the proteins of the F₀F₁ complex. Inhibition of phosphorylation leads to decrease of the ATPase activity and increase of its susceptibility to oligomycin. The in vivo assay confirmed the enhancement of actinobacteria cell sensitivity to oligomycin after inhibition of endogenous phosphorylation. The sequencing of the S. fradiae genes encoding oligomycin-binding A and C subunits of F₀F₁ ATP synthase revealed their close phylogenetic relation to the genes of S. lividans and S. avermitilis.     

Theoretical studies on the crystal structure, thermodynamic properties, detonation performance and thermal stability of cage-tetranitrotetraazabicyclooctane as a novel high energy density compound

The B3LYP/6-31G (d) method of density functional theory (DFT) was used to study molecular geometry, electronic structure, infrared spectrum (IR) and thermodynamic properties. The heat of formation (HOF) and calculated density were estimated to evaluate the detonation properties using Kamlet–Jacobs equations. Thermal stability of 3,5,7,10,12,14,15,16-octanitro- 3,5,7,10,12,14,15,16-octaaza-heptacyclo[7.5.1.1^2,8.0^1,11.0^2,6.0^4,13.0^6,11]hexadecane (cage-tetranitrotetraazabicyclooctane) was investigated by calculating the bond dissociation energy (BDE) at unrestricted B3LYP/6-31G (d) level. The calculated results show that the N–NO₂ bond is a trigger bond during thermolysis initiation process. The crystal structure obtained by molecular mechanics (MM) methods belongs to Pna2₁ space group, with cell parameters a?=?12.840 Å, b?=?9.129 Å, c?=?14.346 Å, Z?=?6 and ρ?=?2.292 g·cm^?3. Both the detonation velocity of 9.96 km·s^?1 and the detonation pressure of 47.47 GPa are better than those of CL-20. According to the quantitative standard of energetics and stability, as a high energy density compound (HEDC), cage-tetranitrotetraazabicyclooctane essentially satisfies this requirement.     

Resolution and Reconstitution of H+-ATPase Complex from Beef Heart Mitochondria

Mitochondrial H⁺-ATPase complex, purified by the lysolecithin extraction procedure, has been resolved into a “membrane” (NaBr-F₀) and a “soluble” fraction by treatment with 3.5 M sodium bromide. The NaBr-F₀ fraction is completely devoid of p, 8, and e subunits of the F, ATPase and largely devoid of α and γ subunits of F₁, where F₀ is used to denote the membrane fraction and F₁, coupling factor 1. This is confirmed by complete loss of ATPase and P₁-ATP exchange activities. The addition of F₁ (400 μg · mg^?1 F₀) results in complete restoration of oligomycin sensitivity without any reduction in the F₁-ATPase activity. Presumably, this is due to release of ATPase inhibitor protein from the F₁-F₀ complex consequent to sodium bromide extraction. Restoration of Pf-ATP exchange and H⁺-pumping activities require coupling factor B in addition to FpATPase. The oligomycin-sensitive ATPase and 32P₁ATP exchange activities in reconstituted Fr F₀ have the same sensitivity to uncouplers and energy transfer inhibitors as in starting submitochondrial particles from the heavy layer of mitochondria and F₁-F₀ complex. The data suggest that the altered properties of NaBr-F₀ observed in other laboratories are probably inherent to their F₁F₀ preparations rather than to sodium bromide treatment itself.

The H⁺-ATPase (F₁-F₀) complex of all known prokaryotic (3, 8, 9, 10, 21, 32, 34) and eukaryotic (11, 26, 30, 33, 35–37) phosphorylating membranes contain two functionally and structurally distinct entities. The hydrophilic component F₁, composed of five unlike subunits, shows ATPase activity that is cold labile as well as uncoupler-and oligomycin-insensitive. The membrane-bound hydrophobic component F₀, having no energy-linked catalytic activity of its own, is indirectly assayed by its ability to regain oligomycin sensitive ATPase and P₁-ATP exchange activities on binding to F¹-ATPase (33). The purest preparations of bovine heart mitochondrial F₀ show seven or eight major components in polyacrylamide gel electrophoresis in the presence of sodium dodecyl sulfate or SDS-PAGE (1, 2, 12, 14), ranging from 6 to 54 ku in molecular weight (12). The precise structure and polypeptide composition of mitochondrial Fo is not known.

The F₀ preparations from bovine heart reported so far have been derived from H⁺-ATPase preparations isolated in the presence of cholate and deoxycholate (11, 33, 36, 37). The ATPase and P₁-ATP exchange activity of the preparations so obtained are low, dependent upon additional phospholipids and coupling factors; they show altered sensitivity to energy transfer inhibitors as compared to submitochondrial particles from the heavy layer of the mitochondria or ETPh (1. 2, 12, 14, 29, 33). Recently, lysolecithin has been successfully employed to extract highly active H⁺-ATPase from beef (17, 19, 28) and pig (24) heart mitochondria. The beef heart H⁺-ATPase preparation has the same ratio of ATPase to PrATP exchange activity and apparently the same sensitivity to energy transfer inhibitors as submitochondrial particles (17). The present communication describes resolution of this F₁-F₀ preparation using sodium bromide (NaBr) and reconstitution of ATPase and Pr ATP exchange activities. The NaBr-F₀ prepared from this preparation shows no dependence on lipids, and the same or increased sensitivity to energy transfer inhibitors when reconstituted with F₁-ATPase. Furthermore, F₁ ATPase activity does not decrease on binding of F₁ to NaBr-F₀, even though the reconstituted ATPase activity is 99% sensitive to oligomy-cin and dicyclohexylcarbodiimide. These properties are in contrast to the properties of F₀ reported by other workers (12, 14).     

Time-resolved chlorophyll fluorescence studies on photosynthetic mutants of Chlamydomonas reinhardtii: origin of the kinetic decay components

The room temperature chlorophyll fluorescence decay kinetics of photosynthetic mutants of Chlamydomonas reinhardtii have been measured as a function of Photosystem 2 (PS2) trap closure, DNB-induced quenching at F_M, and time-resolved emission spectra. The overall decays have been analyzed in terms of three or four kinetic components where necessary. A comparison of the characteristics of the decay components exhibited by the mutants with the wild-type has been carried out to elucidate the precise origins of the different emissions in relation to the observed pigment-protein complexes. It is shown that a) charge recombination in PS2 is not necessary for the presence of long-lived decay components, b) there are two rapid PS1-associated emissions (=30 and 150–200 ps), c) a slow PS1 decay is observed (=1.73 ns) in the absence of PS1 reaction centres, d) the two variable components (=0.25–1.2 and 0.5–2.2 ns) observed in the wild-type arise from LHC2 and e) a rapid (=50–250 ps) decay is associated with the PS2 core antenna (CP3 and CP4). These results show that the intact thylakoid membrane system is too complex to distinguish all of the individual kinetic components.Abbreviations Aexp preexponential factor (Amplitude) - chl chlorophyll - DCMU 3-(3,4-dichlorophenyl)-1,1-dimethyl urea - DNB m, dinitrobenzene - F_M maximum chl fluorescence level - F₀ initial chl fluorescence level - F_v variable chl fluorescence (F_M–F₀) - LHC light harvesting chl a/b protein complex - PS photosystem - Q_A primary stable electron acceptor of PS2     

Single-molecule Analysis of F0F1-ATP Synthase Inhibited by N,N-Dicyclohexylcarbodiimide

N,N-Dicyclohexylcarbodiimide (DCCD) is a classical inhibitor of the F₀F₁-ATP synthase (F₀F₁), which covalently binds to the highly conserved carboxylic acid of the proteolipid subunit (c subunit) in F₀. Although it is well known that DCCD modification of the c subunit blocks proton translocation in F₀ and the coupled ATP hydrolysis activity of F₁, how DCCD inhibits the rotary dynamics of F₀F₁ remains elusive. Here, we carried out single-molecule rotation assays to characterize the DCCD inhibition of Escherichia coli F₀F₁. Upon the injection of DCCD, rotations irreversibly terminated with first order reaction kinetics, suggesting that the incorporation of a single DCCD moiety is sufficient to block the rotary catalysis of the F₀F₁. Individual molecules terminated at different angles relative to the three catalytic angles of F₁, suggesting that DCCD randomly reacts with one of the 10 c subunits. DCCD-inhibited F₀F₁ sometimes showed transient activation; molecules abruptly rotated and stopped after one revolution at the original termination angle, suggesting that hindrance by the DCCD moiety is released due to thermal fluctuation. To explore the mechanical activation of DCCD-inhibited molecules, we perturbed inhibited molecules using magnetic tweezers. The probability of transient activation increased upon a forward forcible rotation. Interestingly, during the termination F₀F₁, showed multiple positional shifts, which implies that F₁ stochastically changes the angular position of its rotor upon a catalytic reaction. This effect could be caused by balancing the angular positions of the F₁ and the F₀ rotors, which are connected via elastic elements.     

Minimizing artifactual elevation of lipid peroxidation products (F2-isoprostanes) in plasma during collection and storage

F₂-isoprostanes (F₂-IsoP’s) are reliable measures of in vivo lipid oxidation, but care is required to prevent artifactual elevation. We examined the effects of blood collection and storage on plasma F₂-IsoP’s. Blood was collected into EDTA/butylated hydroxytoluene/reduced glutathione (EDTA/BHT/GSH) or EDTA, at 4 °C or room temperature. Plasma was stored at −20 or −80 °C for 1 or 6 months before F₂-IsoP’s were assayed by GC–MS. The temperature of blood collection did not affect F₂-IsoP’s. However, storage at −20 °C or collection into EDTA resulted in significant increases in F₂-IsoP’s. Blood collection into EDTA/BHT/GSH and storage at −80 °C minimizes artifactual elevation of plasma F₂-IsoP’s.