Microwave Hall mobility measurements on heavy beef heart mitochondria

The observed initial microwave Hall mobility values at 1·21 tesla of heavy beef heart mitochondria is at least six times greater than that observed for bovine serum albumin at similar resistivity values. The respiratory inhibitor cyanide significantly reduces the initial Hall mobility values for HBHM and for a preparation of HBHM cytochrome oxidase.The four enzymic complexes of the respiratory chain were partially or completely separated. Of these complexes cytochrome oxidase exhibits the largest microwave Hall mobility.The maximum hydration content of loosely bound water for freezedried preparations of cytochrome oxidase is 5% by weight; 60% of this hydration content is driven off by microwave power. Since the effective ac resistivity of the samples of cytochrome oxidase did not appreciably vary with changes in hydration content, the true resistivity of cytochrome oxidase has a value of the order 5×10³ ohm cm and possibly much lower.The electron transport pathway (as measured by Hall signal) of cytochrome oxidase is irreversibly damaged by prolonged exposure to microwave irradiation at 9·2 GHz. This is accompanied by the complete loss of capacity to oxidise ferrocytochromec. Such changes do not occur with HBHM or with the other respiratory complexes.There appears to be a direct relationship between observed Hall signals and the capacity of cytochrome oxidase to oxidize ferrocytochromec. There is a background signal which is not directly related to electron transport but which is dependent on the conformation of the cytochrome oxidase.The observed electronic parameters of cytochrome oxidase do not depend appreciably on its redox state.Acid denaturation of cytochrome oxidase drastically reduces the Hall signal, to include almost complete removal of the background signal. It also more than doubles ac resistivity.An electron tunnelling model is outlined.     

Untersuchung der Beziehung zwischen Pigmentzusammensetzung und CO2-Gaswechsel bei der Blaualge Anacystis nidulans

Summary Changes in culture conditions caused strong changes in the pigment composition in the blue-green alga Anacystis nidulans. Under normal illumination (white light; 0.6·10³ erg/cm²·sec) the relation between the amounts of chlorophyll a and phycocyanin was 1:6.6. In a high light intensity (20.8·10³ erg/cm²·sec) the phycocyanin content was reduced and the relations thus changed to 1:1.9. Growing the algae in red light of high intensity (20·10³ erg/cm²·sec) increased the phycocyanin content; the chlorophyll a: phycocyanin relation was then 1:12.1.The action spectrum of apparent photosynthesis showed a minimum at 473 nm in all three cultures. The maximum of photosynthesis in low light cultures fell in the absorption region of phycocyanin at 621 nm. The action spectrum of the red light culture showed a reduced rate of photosynthesis in the same region. The strong light culture had an action spectrum similar to that of the red light culture with a maximum at 651 nm. The differing action spectrum of the low light culture may be a result of interruption in the energy transfer from phycocyanin to chlorophyll a within pigment system II.The transients of CO₂ exchange are independent of the pigment composition. Two different types of transients were found depending on the wavelength of the incident light. In red light of 550–650 nm a higher stationary rate was reached after a maximum of photosynthesis at the beginning of the illumination period. In blue and far red light a lower rate was found after the first maximum. Following a illumination period in blue or far red light a CO₂ evolution in the dark was observed. On the other hand, this CO₂ evolution was not found after illumination with red light. These effects are possiblt caused by a decarboxylation reaction (photorespiration) which occurs only in blue and far red light.     

Aminocarboxylate complexes of vanadium(III): Electronic structure investigation by high-frequency and -field electron paramagnetic resonance spectroscopy

Aminocarboxylate complexes of vanadium(III) are of interest as models for biologically and medicinally relevant forms of this interesting and somewhat neglected ion. The V(III) ion is paramagnetic, but not readily suited to conventional EPR, due to its integer-spin ground state (S = 1) and associated large zero-field splitting (zfs). High-frequency and -field EPR (HFEPR), however, has the ability to study such systems effectively. Three complexes, all previously structurally characterized: Na[V(trdta)] · 3H₂O, Na[V(edta)(H₂O)] · 3H₂O, and [V(nta)(H₂O)₃] · 4H₂O (where trdta stands for trimethylenediamine-N,N,N′,N′-tetraacetate and nta stands for nitrilotriacetate) were studied by HFEPR. All the investigated complexes produced HFEPR responses both in the solid state, and in aqueous solution, but those of [V(nta)(H₂O)₃] · 4H₂O were poorly interpretable. Analysis of multi-frequency HFEPR spectra yielded a set of spin Hamiltonian parameters (including axial and rhombic zfs parameters: D and E, respectively) for these first two complexes as solids: Na[V(trdta)] · 3H₂O: D = 5.60 cm⁻¹, E = 0.85 cm⁻¹, g = 1.95; Na[V(edta)(H₂O)] · 3H₂O: D = 1.4 cm⁻¹, E = 0.14 cm⁻¹, g = 1.97. Spectra in frozen solution yielded similar parameters and showed multiple species in the case of the trdta complex, which are the consequence of the flexibility of this ligand. The EPR spectra obtained in frozen aqueous solution are the first, to our knowledge, of V(III) in solution in general and show the applicability of HFEPR to these systems. In combination with very insightful previous studies of the electronic absorption of these complexes which provided ligand-field parameters, it has been possible to describe the electronic structure of V(III) in [V(trdta)]⁻ and [V(edta)(H₂O)]⁻; the quality of data for [V(nta)(H₂O)₃] does not permit analysis. Qualitatively, six-coordinate V(III) complexes with O,N donor atoms show no electronic absorption band in the NIR region, and exhibit relatively large magnitude zfs (D ? 5 cm⁻¹), while analogous seven-coordinate complexes do have a NIR absorption band and show relatively small magnitude zfs (D < 2 cm⁻¹).     

Inhibition of photosynthetic electron transport by DDT and DDE

The effect of DDT and DDE (a metabolite of DDT) on chloroplast electron transport was investigated. Photosynthetic electron transport in isolated spinach and barley chloroplasts as well as chloroplasts isolated from macroscopic green algae,Cdium fragile andChaetomorpha aerea, was inhibited by both compounds. Photoreduction and photophosphorylation measured in the presence of ferricyanide showed 50% inhibition at 2×10^–5 M DDT and DDE. P/2e ratios were 1·2–1·5, and remained constant in the presence of both inhibitors. The addition of uncouplers such as ammonium ion and carbonyl cyanide,m-chlorophenylhydrazone did not overcome the inhibition of the chlorinated hydrocarbons. Inhibition of phenazine methosulfate-catalyzed cyclic photophosphorylation by DDT and DDE was observed at low light intensities but was not seen at 2·5×10⁵ erg cm^–2sec^–1 and above. In the presence of DDT, a slow rise in measuring beam fluorescence was observed. The actinic beam fluorescence was slightly less than that in the control. Inhibition by DDT and DDE appears to be similar to that of DCMU. Brief sonication of the chloroplasts increases the sensitivity to DDT. The lack of penetration of DDT to terrestrial plant chloroplasts may be the reason why these are protected from this insecticide.     

A laser-T-jump study of the adsorption of dipolar molecules to planar lipid membranes

The adsorption of the herbicide 2,4-dichlorophenoxyacetic acid (2,4-D) as well as of other dipolar molecules to the interface of artificial lipid membranes gives rise to a change of the dipole potential between the membrane interior and water. As a consequence of the adsorption of the neutral species, the conductance of planar membranes, observed in the presence of the macrocyclic ion carriers nonactin or valinomycin, may change by many orders of magnitude. Using this effect in combination with a laser-T-jump technique, the kinetics of the adsorption process were measured and were interpreted on the basis of a Langmuir-isotherm. A partition coefficient (at small concentrations) of _HA =4.7·10^–4 cm, a rate constant of desorption k _HA100 s^-1 and a maximum surface density N _D=7.7·10¹³/cm² were found. The concentration at half saturation is K _HA=2.7·10^-4 M.Using these values the membrane conductance induced by the ion carrier nonactin and the shape of the current-voltage relationship as a function of the ligand concentration in water was analyzed. A maxiumum dipole potential of V _D ^max =-239 m V and a contribution of b=3.1·10^-15V cm² per single adsorbed 2,4-D molecule was found. 74% of the dipole potential acts on the inner membrane barrier separating the two interfacial adsorption planes of nonactin. The remainder (26%) favours interfacial complex formation between nonactin and K⁺ from the aqueous phase. The data hold for membranes formed from dioleoyllecithin in n-decane.     

Two stable electron-conformational states of photoactivated reaction center and their observation in primary donor recovery kinetics

We investigated the peculiarity of primary donor recovery kinetics in the reaction centers from the purple bacteriaRb. Sphaeroides at low levels of their cw photoactivation. A pronounced biphasity of the relaxation kinetics was found for the total light activating intensity <5×10¹² quanta·cm^-2·s^-1. The effect was attributed to strong dependence of an electron transfer rate constant for the reactionP ⁺Q _infA ^pup- Q_B P ⁺Q_AQ _infB ^sup- upon the RC conformational state controlled by the light. We showed the existence of two different electron-conformational states for the photoexcited RC. The first reveals itself at low intensity of cw photoactivation while the second becomes actual under the intensity >5×10¹² quanta · cm^-2 · s^-1.     

Differences in the response of several cell types to inhibition of surface receptor mobility by local concanavalina binding

Concanavalin A (conA) modulates the lateral mobility of cell surface receptors differently on different cell types. This was demonstrated by using fluorescence photobleaching recovery (FPR) to measure the inhibition of the lateral mobility of conA receptors by localized binding of conA on lymphocytes, fibroblasts, and macrophages. On mouse spleen lymphocytes, binding of conA platelets above a threshold coverage (about 12% of the upper cell-surface area) reduced the diffusion coefficient of mobile TMR-SconA-receptor complexes from 3.0×10^?10 cm²/sec to 0.6× 10^?10 cm²/sec (a 5-fold decrease), and the fraction of mobile receptors was concomitantly reduced from 0.4 to 0.11. Below the threshold occupancy, no effect on either parameter was detected. On 3T3 cells, a qualitatively similar threshold phenomenon was observed: coverage of over 9% of the upper cell surface by conA platelets induced a 3-fold reduction in the diffusion coefficient of TMR-SconA-receptor complexes from 5×10^?10 cm²/sec to 1.7× 10^?10 cm²/sec. However, no effect on the mobile fraction (about 0.4) was observed. In contrast, neither the diffusion coefficient nor the mobile fraction of TMR-SconA-receptor complexes on mouse peritoneal macrophages (both resident and thioglycolate-stimulated) or on the mouse macrophage cell line P388D₁ were affected by the binding of conA platelets in amounts covering over 50% of the upper cell surface (approx. 4.6× 10^?10 cm²/sec and 0.5 for the diffusion coefficient and mobile fraction, respectively). These differences are correlated to the different cytoskeletal functions of the various cell types studied, and are discussed regarding the mechanism of the conA-induced modulation.     

Die Wirkung monochromatischen Lichts auf die extracelluläre Glykolsäure-Ausscheidung und die Lichtatmung bei der Blaualge Anacystis nidulans

Summary The algae were grown under normal air conditions in a low light intensity (400 lux) and measured in the normal CO₂-concentration (0.03 Vol. %). After an illumination period we observed a CO₂ gush which is dependent on the temperature and wavelength used during the measurements. At +20°C a CO₂ gush occurs only in the blue and far red regions. At +35°C, on the other hand, a CO₂ outburst appears over the whole spectrum. The magnitude of the CO₂ gush varies with the wavelength used during the light period. On this basis we have measured an action spectrum of photorespiration which is identical with the action spectrum of photosynthetic CO₂ uptake.Only at a low temperature (+20°C) and illumination with red light (550 to 651 nm; 10^-s einsteins/cm²·sec) did we find a light induced release of glycolate; in blue (432 and 473 nm; 10^-s einsteins/cm²·sec) and far red light (681 and 703 nm; 10^-8 einsteins/cm²·sec) no glycolate excretion occurred. But after addition of -hydroxy-2-pyridylmethane sulfonate (10^-3M) glycolate was excreted during illumination with all used wavelengths. The magnitude of glycolate production was nearly the same in all cases. No glycolate excretion occurred at +35°C in the whole region of the spectrum. Here, too, the addition of -HPMS forced release of glycolate in all wavelengths, indicating that glycolate biosynthesis was occurring.The results are discussed with reference to the physiological behaviour of the algae and activation of photorespiration in blue light. The obtained action spectrum of photorespiration is explained on the basis of a close relationship to photosynthesis.     

Plasmodesmatal frequency and radial translocation rates in ray cells of poplar (Populus x canadensis Moench ‘robusta’)

The minimum radial translocation rate of sugars has been determined from the starchaccumulation rate for the wood rays of Populus x canadensis Moench robusta, and related to ultrastructural peculiarities of the cell walls to be passed. The minimum radial flux or flow of sugars through the tangential walls, the pit fields, and per plasmodesma was 80.7 pmol · cm^-2 · s^-1, 400 to 800 pmol · cm^-2 · s^-1, and 1.0 to 1.7 · 10^-7 pmol · plasmodesma^-1 · s^-1, respectively. These values exclude a transmembrane flux mechanism and indicate that the radial translocation in this tissue must proceed via plasmodesmata. In the isolation cells of the ray center we found 39 plasmodesmata per m² of pit field, 8.0 per m² of tangential wall, and 1.98% of the wall occupied by plasmodesmata. Cells of the ray margins show plasmodesmata on only 1.16% of their tangential wall area and thus appear to be slightly inferior for radial translocation. As judged from both the observed plasmodesmatal frequencies and the translocation rates, the ray parenchyma cells are comparable to cells specialized in short-distance translocation.Abbreviations CCR contact-cell row - IC isolation cell - ICR isolation-cell row     

Scandinavian limnochronology of sediments and heavy metals

Sediment and peat accumulation rates as well as heavy metal fluxes are examined in Scandinavian lakes, marine coasts and peatlands. Modern accumulation rates are determined using Pb-210 and other chronological tools. Mean deposition rates in the past 150 ± 20 yrs are 3–95, 40–190 and 1–5 mg·cm^–2·yr^–1 for lakes, marine coasts and peatlands respectively. The Pb-210 fluxes at the investigated sites are quite variable. The lowest values are found for peatlands 0.04–0.20 pCi·cm^–2·yr^–1 while coastal marine environments showed 0.35–0.70 pCi·cm^–2·yr^–1. A wide range of variation of Pb-210 fluxes is obtained for the studied lake sediments 0.01–0.51 pCi·cm^–2·yr^–1.The chronological records of Pb, Zn, Cu, Cd and Hg show that heavy metal fluxes are much higher in coastal marine areas. Inland lakes and ombrotrophic peat-bogs indicate that Pb is introduced exclusively through the atmosphere and decrease exponentially from South to North Scandinavia. However, the other heavy metals are transported to freshwater systems by different hydrologic and atmospheric processes. Zn and Fe exhibit some correlation with lake-drainage area.     

Mitochondrial chemiluminescence elicited by acetaldehyde

Acetaldehyde-dependent chemiluminescence has been found to be a sensitive technique for the study of superoxide and hydrogen peroxide formation in beef heart mitochondria. The system responds to ATP and antimycin A with increased emission intensities and to ADP and rotenone with decreased intensities, indicating that the chemiluminescence reflects the energy status of the mitochondrion. These effects are based on the ability of acetaldehyde to react with superoxide and hydrogen peroxide to form metastable intermediates which decay spontaneously with the emission of light. Additionally, these intermediates can react with cyanide to give alternative products which can also decay with the emission of light, the cyanide-evokable chemiluminescence. The interaction of acetaldehyde with mitochondria is complex because acetaldehyde can serve as a hydrogen source for NADH and as an inhibitor (at high concentration) of electron transport, and appears to be a reducing agent for a heat-stable site that autoxidatively generates HOOH from O₂ ^–·. Inasmuch as acetaldehyde is a metabolite of ethanol, this broad spectrum of reactivity may play a role in the hepatic and cardiac toxicity that is associated with alcoholism. The heat-stable site that generates HOOH from O₂ ^–· has been studied further and appears to contain vicinal dithiol which is primarily responsible for the cyanide-evokable chemiluminescence.The work reported in this paper was carried out by Erin E. Boh in partial fulfillment of the requirements for the Doctor of Philosophy degree.     

On the evaluation of photoreceptor properties by micro-fluorimetric measurements of fluorochrome diffusion

By use of the microfluorimetric technique it is possible to study the diffusion of the fluorochrome di-dansylcystine (DDC) within isolated frog rod outer segments (ros) which are immobilysed in agarose gel. For this purpose, by a short hypotonic shock a leak is applied to one end of the ros. By this open end the DDC enters the rod and migrates through the whole outer segment. Following the propagation of the fluorescence boundary with time the cytoplasmatic diffusion constant can be determined if a Chromatographic model is used to allow for the considerable binding of DDC to the inner membrane surface. With a binding constant K=5·10^–4 cm the cytoplasmatic diffusion constant was found to be D= 1.3·10^–6cm²/s whereas D _g =2·10^–6cm²/s and D _r =3.5·10^–6cm²/s were found in agarose gel or ringer solution, respectively. Using the mobility reduction factor given by D/D _r 0.4 to calculate the cytoplasmatic conductivity an inner resistance per length of 1.7 M / could be calculated for a frog rod which is in good agreement with corresponding data obtained from electrophysiological measurements.     

Synthesis, crystal structure and magnetic properties of a 1D mixed-metal-mixed-ligand Ni(II)/Fe(II) coordination polymer built on the nitroprusside anion

A new complex [Ni(L)Fe(CN)₅NO] · 2H₂O (L = 4,6,6-trimethyl-1,9-diamino-3,7-di-aza-nona-3-ene) has been obtained and characterized by means of X-ray crystallographic analysis and magnetochemistry. The Fe(CN)₅NO²⁻ anion links to the Ni(L)²⁺ cation through two bridging cyanide groups in a bent fashion. The intrachain Ni?Ni and interchain Ni?Ni distances are equal to 9.81(8) and 7.75(1) Å, respectively. The magnetic behaviour of the complex indicates the zero field splitting parameter D higher than 3 cm⁻¹ and the average exchange parameter (intra- and interchain) corresponding to direct Ni-Ni magnetic interaction in the crystal lattice equals ∼−0.2 cm⁻¹.     

Volume flows and pressure changes during an action potential in cells ofChara australis

Summary Methods have been used for monitoring either volume flows or pressure changes, simultaneously with membrane potentials, in giant algal cells ofChara australis during an action potential. The volume flows were measured from the movement of a mercury bead in a capillary tube recorded by a photo-transducer. The pressure changes were measured by monitoring the deflection of a thin wedge, resting transversely across a cell, and using the same photo-transducer, the deflection of the wedge being directly related to the cell's turgor pressure. The average maximum rate of volume flow per unit area during an action potential was 0.88±0.11 nliter·sec^–1·cm^–2 in the direction of an outflow from the cell (total volume outflow being about 3 nliter·cm^–2 per action potential). Similarly, the maximum rate of change of pressure was 19.6±3.8×10^–3 atm·sec^–1 (peak change being 19.3±2.9×10^–3 atm equivalent to 14.7±2.2 mm Hg). The volume flow and pressure changes followed the vacuolar potential quite closely, the peak rate of volume flow lagging behind the peak of the action potential by 0.17±0.08 sec and the peak rate of pressure change leading it by 0.09±0.07 sec.     

Aldosterone regulates paracellular pathway resistance in rabbit distal colon

Summary Regulation of the paracellular pathway in rabbit distal colon by the hormone aldosterone was investigated in vitro in Ussing chambers by means of transepithelial and microelectrode techniques. To evaluate the cellular and paracellular resistances an equivalent circuit analysis was used. For the analysis the apical membrane resistance was altered using the antibiotic nystatin. Under control conditions two groups of epithelia were found, each clearly dependent on the light: dark regime. Low-transporting epithelia (LT) were observed in the morning and high-transporting epithelia (HT) in the afternoon. Na⁺ transport was about 3-fold higher in HT than in LT epithelia. Incubating epithelia of both groups with 0.1 mol·1^-1 aldosterone on the serosal side nearly doubled in LT epithelia the short circuit current and transepithelial voltage but the transepithelial resistance was not influenced. Maximal values were reached after 4–5 h of aldosterone treatment. In HT epithelia due to the effect of aldosterone all three transepithelial parameters remained constant over time. Evaluation of the paracellular resistance revealed a significant increase after aldosterone stimulation in both epithelial groups. This increase suggests that tight junctions might have been regulated by aldosterone. The hormonal effect on electrolyte transport was also dependent on the physiological state of the rabbit colon. Since net Na⁺ absorption in distal colon is, in addition to transcellular absorption capacity, also dependent on the permeability of the paracellular pathway, the regulation of tight junctions by aldosterone may be a potent mechanism for improving Na⁺ absorption during hormone-stimulated ion transport.Abbreviations V _t transepithelial potential difference (mV) - R _t transepithelial resistance (·cm²) - G _t transepithelial conductance (mS·cm^-2) - I_sc calculated short circuit current (A·cm^-2) - V _a apical membrane potential difference (mV) - V _bl basolateral membrane potential difference (mV) - voltage divider ratio - R _a apical membrane resistance (·cm²) - R _bl basolateral membrane resistance (·cm²) - R _c cellular resistance ( of apical and basolateral resistance) (·cm²) - R _p resistance of the paracellular pathway (·cm²) - G _a apical membrane conductance (mS·cm^-2) - G _bl basolateral membrane conductance (mS·cm^-2) - G _p paracellular conductance (mS·cm^-2) - G _t transepithelial conductance (mS·cm^-2) - HT _contr high transporting control epithelia - LT _contr low transporting control epithelia - HT _aldo aldosterone incubated high transporting epithelia - LT _aldo aldosterone incubated low transporting epithelia     

Electric field-induced lateral mobility of photosystem I in the photosynthetic membrane: A study by electrophotoluminescence

Electrophoretic movement of photosystem I (PS I) along the photosynthetic membrane of hypotonically swollen thylakoid vesicles was studied by analyzing the electric field-stimulated delayed luminescence (electrophotoluminescence) emitted from PS I. The electrophoretic mobility was inferred from the differences in electrophotoluminescence (EPL) of the photosynthetic vesicles in presence and absence of trains of low amplitude (<80 V/cm) prepulses of 1 ms duration at 4 ms spacing. The average apparent electric mobility, determined from the time course of EPL increase on one hemisphere or its decrease on the other one, as function of prepulse length and intensity was of the order of 3 · 10^-5 cm²V^-1s^-1. The assymetric distribution of the PS I reached a steady state when the diffusional, electrostatic, and elastic forces balanced the electrophoretic driving force. A lateral diffusion coefficient of ~5 · 10^-9 cm²s^-1 was found for the PS I complex from the diffusional relaxation after cessation of the electric field pulse train. Experimental conditions such as concentration, temperature, and viscosity of the aqueous solution were not critical for the effect. Between 23 and 150 electron charges per moving particle were estimated from the measured electrophoretic mobility.     

Mobility and electric charge of screening pigment granules in the superposition eye ofEphestia kuehniella Z.

Summary The mobility and the electric charge of screening pigment granules of the mealmoth superposition eye were determined electrophoretically in buffer solutions. In potassium phosphate buffer the mobility of the negatively charged granules is linearly dependent on the pH in the range from 4.8 to 7.7 (Fig. 2), and in veronal buffer from pH= 2.3 to pH=7.5 (Fig. 3). At pH=6.6 the values of the effective charge per granule vary between 9.4·10^–17 C and 2.0·10^–16 C, those of the real charge between 2.4·10^–14 C and 5.6·10^–14 C (Table 1, Appendix). For equal electric fields, the mobility of the granules decreases with increasing ionic strength, and it remains the same for > 0.075 mol/1 (Fig. 4).     

Phototropic fluence-response relations for Avena coleoptiles on a clinostat

Phototropism of Avena sativa L. has been characterized using a clinostat to negate the gravitropic response. The kinetics for development of curvature was measured following induction by a single pulse of blue light (BL), five pulses of BL at 20-min intervals, and this same pulsed-light regime following a 2-h red light (RL) pre-irradiation. A final curvature of about 14° is expressed within 180 min following the single pulse; a final curvature of about 62° in about 240 min following five pulses without pre-irradiation; and a curvature of over 125° in 360 min following five pulses after the RL pre-irradiation. For seedlings not pre-irradiated, the final curvature to five pulses of BL at a total fluence of 9.4 pmol·cm^-2 increases with time of darkness between pulses up to 15 min; with seedlings pre-irradiated with RL, curvature increased more slowly with time of darkness between pulses to a maximum at 35 min. The final curvature induced by a constant fluence of 9.4 pmol·cm^-2 increases linearly with time between the first pulse and last pulse of a five-pulse sequence. The curvature induced by a single BL pulse with a 5-min RL co-irradiation increases with fluence to a maximum of about 60° at about 10 pmol·cm^-2, and then decreases to 0° at about 200 pmol·cm^-2. Curvature induced by five BL pulses following a 2-h RL pre-irradiation increased with fluence from a threshold of about 0.05 pmol·cm^-2 to a maximum of 90° at about 10 pmol·cm^-2, and then gradually decreased with fluence to 50° at 1 000 pmol·cm^-2. Based on these data, it is concluded that the initial photoproduct formed by a BL pulse has a limited lifetime, that there is a kinetic limitation downstream of the photoreceptor pigment for phototropism, and that the additivive effect of pulsed BL is distinct from the potentiating effect of RL on phototropism. Thus, any degree of curvature from 0° to over 90° may be induced by a fluence in the ascending arm of what is traditionally called the first positive phototropic response.Abbreviations BL blue light - RL red light     

Photobleaching recovery studies of membrane events accompanying lectin stimulation of rabbit lymphocytes.

Fluorescence photobleaching recovery methods reveal marked changes in lateral mobilities of rabbit lymphocyte membrane components during the course of stimulation with succinyl concanavalin A (S Con A). The diffusion constant of S Con A receptors on T lymphocytes falls from 1.6×10^?10 cm²/sec to 6.5×10^?11 cm²/sec within 4 hr after stimulation, remains constant for 14 hr, and returns to its former value. The mobility of B cell receptors similarly falls from 1.4×10^?10 cm²/sec to 5.5×10^?11 cm²/sec but regains its unstimulated value much more slowly. In contrast, a fluorescent phospholipid analog shows constant mobilities of 1.9×10^?8 cm²/sec and 1.5×10^?8 cm²/sec in T and B cells, respectively, throughout the experiment.     

Studies on the transition of the cristal membrane from the orthodox to the aggregated configuration. II: Determinants of the orthodox-aggregated transition in adrenal cortex mitochondria

Bovine adrenal cortex mitochondria when isolated in a medium 0·25 M in sucrose contaminated (with calcium) have tubular cristae which are periodically expanded to spherical vesicles and contracted to flattened connecting sections. This scalloped tubular form of the cristae corresponds to the nonenergized orthodox configuration—a configuration in which the matrix space is maximally expanded. When adrenal cortex mitochondria are isolated in media in which the free calcium content is relatively low, e.g., a medium 0·25 M in sucrose and 0·1 mM in EDTA, the cristae assume the aggregated configuration—a nonenergized configuration in which the matrix space is maximally contracted. The composition of the isolation medium determined the configuration. Procedures have been described for isolating bovine adrenal cortex mitochondria (a) predominantly in the orthodox configuration, (b) predominantly in the aggregated configuration, or (c) in a mixed (11) population of configurations. The concentration of Ca²⁺ bound to the mitochondrion was found to be a determinant of the nonenergized configuration. When the level of bound Ca⁺⁺ was 20–25 moles/mg protein, the cristae of the mitochondria were entirely in the orthodox configuration. Addition of Ca²⁺ could induce the transition of cristae from the aggregated to the orthodox configuration whereas addition of Mg²⁺ could induce the transition of cristae from the orthodox to the aggregated configuration. The configurational transition could be followed by any of several methods—a change in 90° light scattering, a change in O.D._{520 m}, a change in pH, or examination by electron microscopy. The orthodox to aggregated transition is energy-independent since it proceeds even in presence of inhibitors both of electron transfer and of ATP hydrolysis. The binding of Ca²⁺ is independent of the binding of Mg²⁺; this independent binding is consistent with the opposite effects induced by Ca²⁺ and Mg²⁺, respectively. Whereas Ca²⁺ induces a proton release, a decrease in 90° light scattering and a decrease in O.D._{520 m} (when the cristae are initially in the aggregated configuration), Mg²⁺ induces equal and opposite changes (when the cristae are initially in the orthodox configuration).