State Transitions in the Green Alga Scenedesmus Obliquus Probed by Time-Resolved Chlorophyll Fluorescence Spectroscopy and Global Data Analysis

Decay-associated fluorescence spectra of the green alga Scenedesmus obliquus have been measured by single-photon timing with picosecond resolution in various states of light adaptation. The data have been analyzed by applying a global data analysis procedure. The amplitudes of the decay-associated spectra allow a determination of the relative antenna sizes of the photosystems. We arrive at the following conclusions: (a) The fluorescence kinetics of algal cells with open PS II centers (F₀ level) have to be described by a sum of three exponential components. These decay components are attributed to photosystem (PS) I (τ ≈ 85 ps, λ_max^em ≈ 695-700 nm), open PS II α-centers (τ ≈ 300 ps, λ_max^em = 685 nm), and open PS II β-centers (τ ≈ 600 ps, λ_max^em = 685 nm). A fourth component of very low amplitude (τ ≈ 2.2-2.3 ns, λ_max^em = 685 nm) derives from dead chlorophyll. (b) At the F_max level of fluorescence there are also three decay components. They originate from PS I with properties identical to those at the F₀ level, from closed PS II α-centers (τ ≈ 2.2 ns, λ_max^em = 685 nm) and from closed PS β-centers (τ ≈ 1.2 ns, λ_max^em = 685 nm). (c) The major effect of light-induced state transitions on the fluorescence kinetics involves a change in the relative antenna size of α- and β-units brought about by the reversible migration of light-harvesting complexes between α-centers and β-centers. (d) A transition to state II does not measurably increase the direct absorption cross-section (antenna size) of PS I. Our data can be rationalized in terms of a model of the antenna organization that relates the effects of state transitions and light-harvesting complex phosphorylation with the concepts of PS II α,β-heterogeneity. We discuss why our results are in disagreement with those of a recent lifetime study of Chlorella by M. Hodges and I. Moya (1986, Biochim. Biophys. Acta., 849:193-202).     

Primary Events, Energy Transfer, and Reactions in Photosynthetic Units: Lifetime of the Excited State In Vivo: I. Chlorophyll a in Algae, at Room and at Liquid Nitrogen Temperatures; Rate Constants of Radiationless Deactivation and Trapping

Using a mode-locked laser (λ, 632.8 nm), fluorescence decay of chlorophyll (Chl) a in the green alga Chlorella pyrenoidosa, the red alga Porphyridium cruentum, and the blue-green alga Anacystis nidulans was measured by the phase-shift method under conditions when photosynthesis was not operative (3-(3,4-dichlorophenyl)-1,1-dimethylurea [DCMU] poisoning, or cooling to 77°K). In the presence of 10^-5 M DCMU, the lifetime of Chl a fluorescence (τ) at room temperature is about 1.7 nsec in Chlorella, 1.0 nsec in Porphyridium, and 0.7 nsec in Anacystis. At 77°K, τ is 1.4 nsec (for fluorescence at about 685 nm, F-685) and 2.3 nsec (for F-730) in Chlorella, 0.9 nsec (F-685) and 1.2 nsec (F-730) in Porphyridium, and 0.8 nsec (F-685 and F-730) in Anacystis. From the above measurement, and the assumption that τ₀ (the intrinsic fluorescence lifetime) for Chl a in all three algae is 15.2 nsec, we have calculated the rate constants of radiationless transition (that includes energy transfer to weakly fluorescent system I) processes competing with fluorescence at room temperature to be about 5 × 10⁸ sec^-1 in Chlorella, 9 × 10⁸ sec^-1 in Porphyridium, and 13 × 10⁸ sec^-1 in Anacystis. At 77°K, this rate constant for Chl a that fluoresces at 685 nm remains, in the first approximation, the same as at room temperature. From the τ data, the rate constant for the trapping of excitation energy is calculated to be about 1.2 × 10⁹ sec^-1 for Chlorella, 2 × 10⁹ sec^-1 for Porphyridium, and 2 × 10⁹ sec^-1 for Anacystis. The efficiency of trapping is calculated to be about 66% (Chlorella), 68% (Porphyridium), and 60% (Anacystis). (It is recognized that variations in the above values are to be expected if algae grown under different conditions are used for experimentation.) The maximum quantum yield of Chl a fluorescence for system II (λ, 632.8 nm), calculated from τ measurements, is about 10% in Chlorella, 6-7% in Porhyridium, and 5% in Anacystis under conditions when photosynthesis is not operative; the values at 77°K appear to be very close to those with DCMU added at room temperature. ø for F-730 at 77°K, however, is somewhat higher than for F-685. The predicted quantum yields of fluorescence for Chl a in intact cells (both systems I and II) at low intensities of 632.8 nm light are about 2-3, 1-2, and 1% for Chlorella, Porphyridium, and Anacystis, respectively.     

Primary Events, Energy Transfer, and Reactions in Photosynthetic Events: Lifetime of the Excited State In Vivo: II. Bacteriochlorophyll in Photosynthetic Bacteria at Room Temperature

Lifetime of the excited state (τ) of bacteriochlorophyll (BChl) in photosynthetic bacteria, measured with a mode-locked argon laser (oscillating at 488 nm; mode locked at 56 MHz) as light source, ranged from 0.3 to 2.5 nsec. These τ values are reported with a precision of ±0.1 nsec. The value of τ at high exciting light intensity (I) was two to three times that at low intensity. For young cultures of green bacterium Chloropseudomonas ethylicum, τ ranged from 0.5 (low I) to 1.0 nsec (high I); for those of the purple bacterium Rhodospirillum rubrum, from 0.4 (low I) to 1.0 nsec (high I); and for those of the BChl b-containing Rhodopseudomonas viridis, from 1.0 (low I) to 2.5 nsec (high I). These data provide information regarding the efficiencies of the photochemical process in these bacteria. Quantum yield (ø) of BChl fluorescence, calculated from ø = τ/τ₀ (where τ₀ is the intrinsic lifetime of fluorescence), ranges from 2-6% at low intensities to 6-14% at high intensities.     

Comparative Study of Action of Cell Wall Proteinases from Various Strains of Streptococcus cremoris on Bovine αs1-, β-, and κ-Casein

Partially purified cell wall proteinases of eight strains of Streptococcus cremoris were compared in their action on bovine α_s1-, β-, and κ-casein, as visualized by starch gel electrophoresis, sodium dodecyl sulfate-polyacrylamide gel electrophoresis, and thin-layer chromatography. Characteristic degradation profiles could be distinguished, from which the occurrence of two proteinases, represented by strain HP and strain AM₁, was concluded. The action of the HP-type proteinase P₁ (also detectable in strains Wg₂, C₁₃, and TR) was established by electrophoretic methods to be directed preferentially towards β-casein. The AM₁-type proteinase P_III (also detectable in strain SK₁₁) was also able to degrade β-casein, but at the same time split α_s1- and κ-casein more extensively than did P_I. Strain FD₂₇ exhibited mainly P_I activity but also detectable P_III degradation characteristics. The cell wall proteinase preparation of strain E₈ showed low P_I as well as low P_III activity. All proteinase preparations produced from κ-casein positively charged degradation products with electrophoretic mobilities similar to those of degradation products released by the action of the milk-clotting enzyme chymosin. The differences between P_I and P_III in mode of action, as detected by gel electrophoresis and thin-layer chromatography, were reflected by the courses of the initial degradation of methyl-¹⁴C-labeled β-casein and by the effect of α_s1- plus κ-casein on these degradations. The results are discussed in the light of previous comparative studies of cell wall proteinases in strains of S. cremoris and with respect to the growth of this organism in milk.     

Somatostatin receptor subtype 4 modulates L-type calcium channels via Gβγ and PKC signaling in rat retinal ganglion cells

Somatostatin subtype-4 receptors (sst₄) inhibit L-type calcium channel currents (I_Ca) in retinal ganglion cells (RGCs). Here we identify the signaling pathways involved in sst₄ stimulation leading to suppression of I_Ca in RGCs. Whole cell patch clamp recordings were made on isolated immunopanned RGCs using barium as a charge carrier to isolate I_Ca. Application of the selective sst₄ agonist, L-803 (10 nM), reduced I_Ca by 41.2%. Pretreatment of cells with pertussis toxin (Gi/o inhibitor) did not prevent the action of L-803, which reduced I_Ca by 34.7%. To determine the involvement of Gβγ subunits after sst₄ activation, depolarizing pre-pulse facilitation paradigms were used to remove voltage-dependent inhibition of calcium channels. Pre-pulse facilitation did not reverse the inhibitory effects of L-803 on I_Ca (8.4 vs. 8.8% reductions, ctrl vs. L-803); however, pharmacologic inhibition of Gβγ reduced I_Ca suppression by L-803 (23.0%, P < 0.05). Inhibition of PKC (GF109203X; GFX) showed a concentration-dependent effect in preventing the action of L-803 on I_Ca (1 μM GFX, 34.3%; 5 μM GFX, 14.6%, P < 0.05). When both PKC and Gβγ were inhibited, the effects of L-803 on I_Ca were blocked (1.8%, P < 0.05). These results suggest that sst₄ stimulation modulates RGC calcium channels via Gβγ and PKC activation. Since reducing intracellular Ca²⁺ is known to be neuroprotective in RGCs, modulating these sst₄ signaling pathways may provide insights to the discovery of unique therapeutic targets to reduce intracellular Ca²⁺ levels in RGCs.     

Elastic-Mathematical Theory of Cells and Mitochondria in Swelling Process: II. Effect of Temperature upon Modulus of Elasticity of Membranous Material of Egg Cells of Sea Urchin, Strongylocentrotus purpuratus, and of Oyster, Crassostrea virginica

The elastic behavior of the cell wall as a function of the temperature has been studied with particular attention being given to the swelling of egg cells of Strongylocentrotus purpuratus and Crassostrea virginica in different sea water concentrations at different temperatures. It was found that the modulus of elasticity is a nonlinear function of temperature. At about 12-13°C the modulus of elasticity (E) is constant, independent of the stress (σ) and strain (ε_ν) which exist at the cell wall; the membranous material follows Hooke's law, and E ≈ 3 × 10⁷ dyn/cm² for S. purpuratus and C. virginica. When the temperature is higher or lower than 12-13°C, the modulus of elasticity increases, and the membranous material does not follow Hooke's law, but is almost directly proportional to the stresses existing at the cell wall. On increasing the stress, the function E_σ = E(σ) approaches saturation. The corresponding stress-strain diagrams, σ = σ(ε_ν), and the graphs, E_σ = E(σ) and E_σ = E(t) are given. The cyto-elastic phenomena at the membrane are discussed.     

In Vitro Laser Ablation of Natural Marine Biofilms

We studied the efficiency of pulsed low-power laser irradiation of 532 nm from an Nd:YAG (neodymium-doped yttrium-aluminum-garnet) laser to remove marine biofilm developed on titanium and glass coupons. Natural biofilms with thicknesses of 79.4 ± 27.8 μm (titanium) and 107.4 ± 28.5 μm (glass) were completely disrupted by 30 s of laser irradiation (fluence, 0.1 J/cm²). Laser irradiation significantly reduced the number of diatoms and bacteria in the biofilm (paired t test; P < 0.05). The removal was better on titanium than on glass coupons.     

Kinetic diversity of single-channel burst openings underlying persistent Na(+) current in entorhinal cortex neurons

The kinetic diversity of burst openings responsible for the persistent Na⁺ current (I_NaP) in entorhinal cortex neurons was examined by separately analyzing single bursts. Although remarkable kinetic variability was observed among bursts in terms of intraburst opening probability and mean open and closed times, the values of time constants describing intraburst open times (τ_o(b)s) and closed times (τ_c(b)s) were distributed around well-defined peaks. At −40 mV, τ_o(b) peaks were found at ~0.34 (τ_o(b)1) and 0.77 (τ_o(b)2) ms, and major τ_c(b) peaks were found at ~0.24 (τ_c(b)1) and 0.54 (τ_c(b)2) ms. In ~80% of the bursts two preferential gating modes were found that consisted of a combination of either τ_o(b)1 and τ_c(b)2 (“intraburst mode 1”), or τ_o(b)2 and τ_c(b)1 (“intraburst mode 2”). Individual channels could switch between different gating modalities, but normally tended to maintain a specific gating mode for long periods. Mean burst duration also displayed considerable variability. At least three time constants were found to describe burst duration, and the frequencies at which each of the corresponding “bursting states” occurred varied in different channels. Short-lasting bursting states were preferentially associated with intraburst mode 1, whereas very-long-lasting bursts tended to gate according to mode 2 only or other modes that included considerably longer mean open times. These results show that I_NaP channels can generate multiple intraburst open and closed states and bursting states, but these different kinetic states tend to combine in definite ways to produce a limited number of prevalent, well-defined gating modalities. Modulation of distinct gating modalities in individual Na⁺ channels may be a powerful form of plasticity to influence neuronal excitability and function.     

Early Picosecond Events in the Photocycle of Bacteriorhodopsin

The primary processes of the photochemical cycle of light-adapted bacteriorhodopsin (BR) were studied by various experimental techniques with a time resolution of 5 × 10^-13 s. The following results were obtained. (a) After optical excitation the first excited singlet state S₁ of bacteriorhodopsin is observed via its fluorescence and absorption properties. The population of the excited singlet state decays with a lifetime τ₁ of ~0.7 ps (430 ± 50 fs) (52). (b) With the same time constant the first ground-state intermediate J builds up. Its absorption spectrum is red-shifted relative to the spectrum of BR by ~30 nm. (c) The second photoproduct K, which appears with a time constant of τ₂ = 5 ps shows a red-shift of 20 nm, relative to the peak of BR. Its absorption remains constant for the observation time of 300 ps. (d) Upon suspending bacteriorhodopsin in D₂O and deuterating the retinal Schiff base at its nitrogen (lysine 216), the same photoproducts J and K are observed. The relaxation time constants τ₁ and τ₂ remain unchanged upon deuteration within the experimental accuracy of 20%.     

Binding of NFκB Appears to Twist the Ankyrin Repeat Domain of IκBα

Total internal reflection fluorescence-based single-molecule Förster resonance energy transfer (FRET) measurements were previously carried out on the ankyrin repeat domain (ARD) of IκBα, the temporally regulated inhibitor of canonical NFκB signaling. Under native conditions, most of the IκBα molecules showed stable, high FRET signals consistent with distances between the fluorophores estimated from the crystal structures of the NFκB(RelA/p50)-IκBα complex. Similar high FRET efficiencies were found when the IκBα molecules were either free or in complex with NFκB(RelA/p50), and were interpreted as being consistent with the crystallographically observed ARD structure. An exception to this was observed when the donor and acceptor fluorophores were attached in AR3 (residue 166) and AR6 (residue 262). Surprisingly, the FRET efficiency was lower for the bound IκBα molecules (0.67) than for the free IκBα molecules (0.74), apparently indicating that binding of NFκB(RelA/p50) stretches the ARD of IκBα. Here, we conducted confocal-based single-molecule FRET studies to investigate this phenomenon in greater detail. The results not only recapitulated the apparent stretching of the ARD but also showed that the effect was more pronounced when the N-terminal domains (NTDs) of both RelA and p50 were present, even though the interface between NFκB(RelA/p50) and IκBα encompasses only the dimerization domains. We also performed mass spectrometry-detected amide hydrogen/deuterium exchange (HDXMS) experiments on IκBα as well as IκBα bound to dimerization-domain-only constructs or full-length NFκB(RelA/p50). Although we expected the stretched IκBα to have regions with increased exchange, instead the HDXMS experiments showed decreases in exchange in AR3 and AR6 that were more pronounced when the NFκB NTDs were present. Simulations of the interaction recapitulated the increased distance between residues 166 and 262, and also provide a plausible mechanism for a twisting of the IκBα ARD induced by interactions of the IκBα proline-glutamate-serine-threonine-rich sequence with positively charged residues in the RelA NTD.     

Regulation of Cardiac Inward Rectifier Potassium Current (IK1) by Synapse-associated Protein-97

Synapse-associated protein-97 (SAP97) is a membrane-associated guanylate kinase scaffolding protein expressed in cardiomyocytes. SAP97 has been shown to associate and modulate voltage-gated potassium (Kv) channel function. In contrast to Kv channels, little information is available on interactions involving SAP97 and inward rectifier potassium (Kir2.x) channels that underlie the classical inward rectifier current, I_K1. To investigate the functional effects of silencing SAP97 on I_K1 in adult rat ventricular myocytes, SAP97 was silenced using an adenoviral short hairpin RNA vector. Western blot analysis showed that SAP97 was silenced by ∼85% on day 3 post-infection. Immunostaining showed that Kir2.1 and Kir2.2 co-localize with SAP97. Co-immunoprecipitation (co-IP) results demonstrated that Kir2.x channels associate with SAP97. Voltage clamp experiments showed that silencing SAP97 reduced I_K1 whole cell density by ∼55%. I_K1 density at −100 mV was −1.45 ± 0.15 pA/picofarads (n = 6) in SAP97-silenced cells as compared with −3.03 ± 0.37 pA/picofarads (n = 5) in control cells. Unitary conductance properties of I_K1 were unaffected by SAP97 silencing. The major mechanism for the reduction of I_K1 density appears to be a decrease in Kir2.x channel abundance. Furthermore, SAP97 silencing impaired I_K1 regulation by β₁-adrenergic receptor (β1-AR) stimulation. In control, isoproterenol reduced I_K1 amplitude by ∼75%, an effect that was blunted following SAP97 silencing. Our co-IP data show that β1-AR associates with SAP97 and Kir2.1 and also that Kir2.1 co-IPs with protein kinase A and β1-AR. SAP97 immunolocalizes with protein kinase A and β1-AR in the cardiac myocytes. Our results suggest that in cardiac myocytes SAP97 regulates surface expression of channels underlying I_K1, as well as assembles a signaling complex involved in β1-AR regulation of I_K1.     

ON THE VARIABILITY OF CRITICAL ILLUMINATION FOR FLICKER FUSION AND INTENSITY DISCRIMINATION

From the data of experiments with bees in which threshold response is employed as a means of recognizing visual discrimination between stripes of equal width alternately illuminated by intensities I ₁ and I ₂, it is shown that the detectable increment of intensity ΔI, where ΔI = I ₂ - I ₁, is directly proportional to σ_I2 (I ₁ being fixed). From tests of visual acuity, where I ₁ = 0 and the width of the stripes is varied, σ_I2 = kI ₂ + const.; here I ₂ = ΔI, and ΔI/I ₂ = 1. When the visual excitability of the bee is changed by dark adaptation, λI ≡ kΔI (= k'' σ_ΔI) = k'''' I + const. For the measurements of critical illumination at threshold response to flicker, σ_I2 (= σ_ΔI) = k I ₂ = k'' ΔI + const. The data for critical illumination producing threshold response to flicker in the sun-fish Lepomis show for the rods σ_I2 = K I ₂ for the cones σ_I2 = K''(I ₂ + const.). The data thus indicate that in all these experiments essentially the same visual function is being examined, and that the recognition of the production of a difference in effect by alternately illuminated stripes takes place in such a way that d (ΔI)/d (σ_I2) = const., and that ΔI is directly proportional to I (or "I ₂," depending on the nature of the experiment). It is pointed out that the curve for each of the cases considered can be gotten equally well if mean I or σ_I is plotted as a function of the independent variable involved in the experiment. Certain consequences of these and related facts are important for the treatment of the general problem of intensity discrimination.     

Bacteriorhodopsin wildtype and variant aspartate-96 → aspargine as reversible holographic media

Air dried films of purple membranes (PM) from Halobacterium halobium containing the photochromic protein bacteriorhodopsin (BR) were prepared and the BR-photocycle of this material analyzed. The absorption maxima of the initial state B (λ_max = 570 nm) and the photochemical intermediate M (λ_max = 412 nm), which is the longest living intermediate in suspension (τ ≈ 10 ms), were spectrally well separated. Light-induced population gratings between B and M were used for reversible holographic recording in these dry PM films. The resolution (>5,000 lines/mm) of PM films was comparable to the corresponding values of conventional photochromic recording materials. The longterm stability toward photochemical degradation of PM films is excellent (> 100.000 recording cycles). The spectral bandwidth (400-680 nm) of such films covers nearly the whole visible spectrum. Both the photochemical transition from B → M with wavelengths in the green-red range and from M → B with blue light were utilized for holographic recording. The latter possibility (M → B) seems to be advantageous for several applications because the holographic grating is only formed during reconstruction. Higher reading intensities lead to higher population of the M-state and result in an increase of the fringe contrast instead of decreasing it. New possibilities for the further development of holographic media based on bacteriorhodopsin are raised by the availability of PM variants with modified optical properties. By the use of the variant BR-326, which differs from the wildtype PM by a single amino acid exchange (aspartate-96 → asparagine), the sensitivity of PM films is increased by ~50% from 12 cm²/J to 19 cm²/J for recording with 568 nm. The sensitivity for recording with 413 nm (33 cm²/J) is not influenced by the amino acid exchange. The observed diffraction efficiency η of PM films with BR-326 is twice that of BR-wildtype (BR-WT) films and is in the range of conventional organic photochromics (≈ 1%). In dried films of both BR-WT and BR-326 the M-decay was shown to be at least biexponential.     

Phosphoinositide-3-kinase/akt - dependent signaling is required for maintenance of [Ca2+]i,ICa, and Ca2+ transients in HL-1 cardiomyocytes

The phosphoinositide 3-kinases (PI3K/Akt) dependent signaling pathway plays an important role in cardiac function, specifically cardiac contractility. We have reported that sepsis decreases myocardial Akt activation, which correlates with cardiac dysfunction in sepsis. We also reported that preventing sepsis induced changes in myocardial Akt activation ameliorates cardiovascular dysfunction. In this study we investigated the role of PI3K/Akt on cardiomyocyte function by examining the role of PI3K/Akt-dependent signaling on [Ca²⁺]_i, Ca²⁺ transients and membrane Ca²⁺ current, I_Ca, in cultured murine HL-1 cardiomyocytes. {"type":"entrez-nucleotide","attrs":{"text":"LY294002","term_id":"1257998346","term_text":"LY294002"}}LY294002 (1–20 μM), a specific PI3K inhibitor, dramatically decreased HL-1 [Ca²⁺]_i, Ca²⁺ transients and I_Ca. We also examined the effect of PI3K isoform specific inhibitors, i.e. α (PI3-kinase α inhibitor 2; 2–8 nM); β (TGX-221; 100 nM) and γ (AS-252424; 100 nM), to determine the contribution of specific isoforms to HL-1 [Ca²⁺]_i regulation. Pharmacologic inhibition of each of the individual PI3K isoforms significantly decreased [Ca²⁺]_i, and inhibited Ca²⁺ transients. Triciribine (1–20 μM), which inhibits AKT downstream of the PI3K pathway, also inhibited [Ca²⁺]_i, and Ca²⁺ transients and I_Ca. We conclude that the PI3K/Akt pathway is required for normal maintenance of [Ca²⁺]_i in HL-1 cardiomyocytes. Thus, myocardial PI3K/Akt-PKB signaling sustains [Ca²⁺]_i required for excitation-contraction coupling in cardiomyoctyes.     

Elastic-Mathematical Theory of Cells and Mitochondria in Swelling Process: The Membranous Stresses and Modulus of Elasticity of the Egg Cell of Sea Urchin, Strongylocentrotus purpuratus

To the revolution-ellipsoidal and spherical membranous shell (cell mitochondrion) are introduced the equations for the calculation of both the modulus of elasticity (Young's modulus) and the stresses, which exist at the membrane. The existing pressure difference between the inner and outer surface of the membrane is calculated in the dilution of seawater media in the osmotic steady state. The experimental results are obtained by using egg cells of the sea urchin, Strongylocentrotus purpuratus. Up to the specific volume of the egg cell (V_E ≈ 35·10^-8 cm³) Boyle-van't Hoff's law is valid (defined as the subelastic range) beyond that the elastic stresses exist (elastic range). For the maximum value of the stresses existing at the cell wall one obtains σ ≈ 5.5·10⁶ dyne/cm² and for the modulus of elasticity E = 1.0·10⁷ dyne/cm², which is constant when the value of relative strain ε_ν > 15%. The breaking limit by an approximate calculation is σ_U ≈ 11·10⁶ dyne/cm². The membrane is assumed to be convoluted and its hypothetical degree of folding was calculated [unk]_a = 34%. The results are compared with the values existing in the literature and other types of cells are found to have values of elasticity in the same range as values of the membrane of S. purpuratus. Both compression and cell elastometer methods are criticized and in certain cases results of these methods are considered to belong to the subelastic domain.     

Sodium and Calcium Inward Currents in Freshly Dissociated Smooth Myocytes of Rat Uterus

Freshly dissociated myocytes from nonpregnant, pregnant, and postpartum rat uteri have been studied with the tight-seal patch-clamp method. The inward current contains both I_Na and I_Ca that are vastly different from those in tissue-cultured material. I_Na is abolished by Na⁺-free medium and by 1 μM tetrodotoxin. It first appears at ∼−40 mV, reaches maximum at 0 mV, and reverses at 84 mV. It activates with a voltage-dependent τ of 0.2 ms at 20 mV, and inactivates as a single exponential with a τ of 0.4 ms. Na⁺ conductance is half activated at −21.5 mV, and half inactivated at −59 mV. I_Na reactivates with a τ of 20 ms. I_Ca is abolished by Ca²⁺-free medium, Co²⁺ (5 mM), or nisoldipine (2 μM), and enhanced in 30 mM Ca²⁺, Ba²⁺, or BAY-K 8644. It first appears at ∼−30 mV and reaches maximum at +10 mV. It activates with a voltage-dependent τ of 1.5 ms at 20 mV, and inactivates in two exponential phases, with τ''s of 33 and 133 ms. Ca²⁺ conductance is half activated at −7.4 mV, and half inactivated at −34 mV. I_Ca reactivates with τ''s of 27 and 374 ms. I_Na and I_Ca are seen in myocytes from nonpregnant estrus uteri and throughout pregnancy, exhibiting complex changes. The ratio of densities of peak I_Na/I_Ca changes from 0.5 in the nonpregnant state to 1.6 at term. The enhanced role of I_Na, with faster kinetics, allows more frequent repetitive spike discharges to facilitate simultaneous excitation of the parturient uterus. In postpartum, both currents decrease markedly, with I_Na vanishing from most myocytes. Estrogen-enhanced genomic influences may account for the emergence of I_Na, and increased densities of I_Na and I_Ca as pregnancy progresses. Other influences may regulate varied channel expression at different stages of pregnancy.     

Random Coil to Globular Thermal Response of a Protein (H3.1) with Three Knowledge-Based Coarse-Grained Potentials

The effect of temperature on the conformation of a histone (H3.1) is studied by a coarse-grained Monte Carlo simulation based on three knowledge-based contact potentials (MJ, BT, BFKV). Despite unique energy and mobility profiles of its residues, the histone H3.1 undergoes a systematic (possibly continuous) structural transition from a random coil to a globular conformation on reducing the temperature. The range over which such a systematic response in variation of the radius of gyration (R_g) with the temperature (T) occurs, however, depends on the potential, i.e. ΔT_MJ ≈ 0.013–0.020, ΔT_BT ≈ 0.018–0.026, and ΔT_BFKV ≈ 0.006–0.013 (in reduced unit). Unlike MJ and BT potentials, results from the BFKV potential show an anomaly where the magnitude of R_g decreases on raising the temperature in a range ΔT_A ≈ 0.015–0.018 before reaching its steady-state random coil configuration. Scaling of the structure factor, S(q) ∝ q^−1/ν, with the wave vector, q = 2π/λ, and the wavelength, λ, reveals a systematic change in the effective dimension (D_e∼1/ν) of the histone with all potentials (MJ, BT, BFKV): D_e∼3 in the globular structure with D_e∼2 for the random coil. Reproducibility of the general yet unique (monotonic) structural transition of the protein H3.1 with the temperature (in contrast to non-monotonic structural response of a similar but different protein H2AX) with three interaction sets shows that the knowledge-based contact potential is viable tool to investigate structural response of proteins. Caution should be exercise with the quantitative comparisons due to differences in transition regimes with these interactions.     

Cooperative polymerization of photosynthetic pigments in formamide-water solution

The aggregation of bacteriochlorophyll a and bacteriopheophytin a into large oligomers with maximum optical absorption at 860 nm was studied in a 3:1 (vol/vol) formamide/water solution, using optical absorption spectroscopy and electron microscopy. The aggregation is cooperative and proceeds according to two equilibrium constants. Initially, two pigment molecules form a “seed” that absorbs at ≈860 nm. The equilibrium constant, K_a, governing this reaction equals 1.3 × 10³ M^-1 in the case of bacteriochlorophyll a (due to experimental limitations, K_a for bacteriopheophytin a could not be determined). The addition of monomers to aggregates consisting of two or more units is governed by an equilibrium constant, K_b, equal to 2.2 × 10⁶ M^-1 for bacteriochlorophyll a and ≈ 10⁹ M^-1 for bacteriopheophytin a. The enthalpy and entropy changes that drive the bacteriochlorophyll oligomer formation are -9.25 and ≈0.0 kcal/mol, respectively. Above a threshold concentration, the amount of oligomers remains constant but their length continues to increase. Each oligomer appears to consist of dimers that are associated by hydrophobic interactions among their alcohol residues, forming long strands. Single strands presumably coil into helices that are seen as cylinders. The bacteriochlorophyll a oligomers form cylinders with a constant diameter of 150 Å and an average length of 2,000 Å (at 1.5 × 10^-5 M bacteriochlorophyll a). These cylinders contain 200-250 bacteriochlorophyll a dimers. The bacteriopheophytin oligomers coil into wider cylinders (≈400 Å in diameter) which contain ≈600-700 bacteriopheophytin a dimers. In both cases, the separation between the dimers is ≈20 Å. At such distances, the dipolar interactions among adjacent dimers are negligible and do not affect the optical absorption of each individual pair. Therefore, the optical absorption of these pairs can be a tool for investigating the absorption pattern of photosynthetic pigments in vivo.