不同声强超声对孕鼠子宫收缩及胎鼠神经损伤的影响及机制

目的:探讨不同声强超声对孕鼠子宫收缩及胎鼠神经损伤的影响及机制。方法:将32只孕鼠随机分为A(0)组、B(2)组、C(4)组、D(8)组,每组各8只,分别接受声强为0 W cm~(-2)、2 W cm~(-2)、4 W cm~(-2)和8 W cm~(-2)的超声辐照20 min。记录孕鼠子宫收缩及子宫平滑肌ATP酶的活力,检测胎鼠大脑皮层与海马神经元凋亡及胆碱能神经系统相关酶的活力。结果:超声增加孕鼠子宫收缩频率、收缩幅度、收缩张力和子宫活动度(P均0.05),降低孕鼠子宫平滑肌中钠钾ATP酶、钙ATP酶和钙镁ATP酶的活性(P均0.05)。超声降低胎鼠大脑皮层和海马中Bcl~(-2)水平(P0.05),增加Bax和Caspase-3水平(P均0.05)。以及促进乙酰胆碱酯酶活力,降低乙酰胆碱和乙酰胆碱转移酶水平(P均0.05)。且4 W cm~(-2)和8 W cm~(-2)的超声比2 W cm~(-2)超声对这些指标的作用更强。结论:4 W cm~(-2)和8 W cm~(-2)超声可能通过降低ATP酶的活性促进孕鼠子宫平滑肌收缩,并可引起胎鼠大脑皮层和海马神经元损伤,机制可能与胆碱能神经元系统失衡有关,2 W cm~(-2)声强的超声对胎鼠神经元损伤甚小。     

An experimental study of the use of ultrasound to facilitate the loading of trehalose into platelets

Trehalose is widely used as a freeze-drying protectant in biomaterial preservation. For this purpose, trehalose has to be loaded into the cells but this is difficult and many methods have been tried. The application of ultrasound can temporarily permeabilize cell membranes, which offers a non-chemical, non-viral, and non-invasive method of cellular drug delivery. Ultrasound is employed here to enhance the loading of trehalose into human platelets. Two frequencies were used, 25 kHz and 800 kHz. The estimated intensity of ultrasound in the sample was varied from 0 to 1.5 W/cm². The trehalose concentration in the platelets was 11.27 ± 2.53 mmol/L when Wolkers et al.’s method was used without ultrasound. The application of 0.8 W/cm², 800 kHz ultrasound for 1 h increased the concentration of trehalose loaded by 54%. The application of 0.8 W/cm², 25 kHz ultrasound for 30 min increased the trehalose concentration that was loaded by 172%. The number and mean volume of the platelets following ultrasonic radiation in these two cases remained normal as compared with fresh untreated platelets. Morphological examination of the radiated platelets showed slight changes. Although further work is needed, ultrasound has been shown to be efficient for the loading of trehalose into platelets.     

Location and sequence of muscle onset in deep abdominal muscles measured by different modes of ultrasound imaging

Various modes of ultrasound (US) imaging have been introduced as an alternative to electromyography for determining muscle onset. The purpose of this study was to compare the agreement between US motion-mode (US_m-mode) and US strain rate (US_SR) derived from tissue velocity imaging in determining latency time, location and sequence of muscle onset in abdominal muscles using the same data set (contractions). Twenty-four subjects performed four rapid arm flexions in response to a light signal while US recordings were made from the abdominal muscles on the contralateral side. The examined muscles were transversus abdominis (TrA), superficial and deep obliquus internus abdominis (OI_deep and OI_sup), and obliquus externus abdominis (OE). The results showed that the two methods detected the first muscle onset on average within 0.1 ms (95% CI; ±1.4 ms) of each other. US_SR detected the second muscle onset on average 27 ms after US_m-mode. While US_SR and US_m-mode can be used interchangeably to detect the first muscle onset, the location of both first onset and subsequent muscle onsets can be reliably detected by US_SR only. Furthermore, this study indicates that OI may be functionally subdivided into a superficial and deep region, with onset in OI_deep occurring on average 53 ms before OI_sup. First onset was detected more frequently in OI than in TrA (65% versus 25% of detected onsets, 10% were equal).     

Size constraints of telemeters in rats

This study was designed to determine themaximum-size subcutaneous telemeter that would enable long-term andmultichannel data collection in a 170-g rat for 90 days. Inphase 1, rats with implants weighing 5 (2.5 cm³), 15 (7.5 cm³), 25 (12.5 cm³), 35 (17.5 cm³), or 45 (22.5 cm³) g were compared withsham-operated (SOC) and nonoperated (NOC) control animals. Severe skinlesions, seromas, and lower growth rates were observed in rats havingimplants 35 g. Thus, in phase 2,rats implanted with 23.5 g (17.5 cm³; 11-g active telemeter and12.5-g implant) were compared with rats implanted with 11 g (6 cm³; telemeter only) and with theSOC and NOC groups. No differences were found among implanted groups inmean arterial pressure (MAP), heart rate (HR), subcutaneoustemperature, or spontaneous activity under standard housing conditions.All groups were more active and had a higher MAP during the dark thanthe light phase of the daily cycle. During 2 h of cold exposure(3°C), both telemetered groups exhibited similar changes in HR,MAP, temperature, and activity levels. Adrenal glands were larger inthe 23.5-g group (51 ± 1.6 mg) than in the SOC (46 ± 1.0 mg)and the NOC groups (41 ± 2.0 mg). No other significant differenceswere found in organ, muscle, or bone weights. These data verify thefeasibility of using 23.5-g (17.5 cm³) subcutaneous telemeters forchronic recordings in young adult rats.

     

Enhanced Gene Transduction into Skeletal Muscle of Mice In Vivo with Pluronic Block Copolymers and Ultrasound Exposure

The pluronic block copolymers are able to enhance the ultrasound-induced gene delivery in vitro. In the present study, the effects of pluronics on the efficiency of gene transfer into skeletal muscle in vivo under sonoporation were investigated. Plasmid DNA encoding green fluorescent protein (GFP) in combination with three different pluronics, F127, L61, and P85, was injected into the tibialis anterior (TA) muscle of mice with and without adjunct ultrasound (1 MHz, 3 W/cm² 1 min, 20% duty cycle). Mice were killed 1 week after injection. The TA muscles were removed and snap frozen immediately in isopentane cooled by liquid nitrogen and sections of 7 μm thick were cut. Transfection efficiency was assessed by counting the number of GFP-positive fibers under fluorescence microscopy, and tissue damage by hematoxylin and eosin staining. The results suggested that all three pluronics significantly enhanced transgene expression in skeletal muscle (P < 0.01), especially the P85 showed significantly higher efficiency than the other two pluronics (P < 0.05). Ultrasound synergistically enhanced the gene delivery efficiency with P85 (P < 0.01), but was unable to do so with F127 and L61 groups. In short, P85 displays significantly synergistic effect with ultrasound for enhancing plasmid DNA transduction in skeletal muscle of mice in vivo.     

Effect of low power ultrasonic radiation on anaerobic biodegradability of sewage sludge

The effect of low power ultrasonic radiation on anaerobic biodegradability of sewage sludge was investigated. For this purpose, soluble substances and variation of microbial system of sewage sludge subjected to low power ultrasonic radiation were tested. The well known hydromechanical shear forces and heating effect of low frequency ultrasound plays a major role in the sludge pre treatment process. More, the increase of soluble substance may partly result from the destruction of microbial cell by excess ultrasonic pretreatment, which will inhibit the anaerobic process. By orthogonal tests, the optimal parameters were found to be an exposure time of 15 min, ultrasonic intensity of 0.35 W/cm² and ultrasonic power density of 0.25 W/ml. Under the optimal condition, anaerobic biodegradability of sewage sludge (R_(vss/ss) %) was increased by 67.6%. Consequently, it can be concluded that low power ultrasonic pretreatment is a valid method for improving anaerobic biodegradability of sewage sludge.     

Speeding the Recovery from Ultraslow Inactivation of Voltage-Gated Na+ Channels by Metal Ion Binding to the Selectivity Filter: A Foot-on-the-Door?

Slow inactivated states in voltage-gated ion channels can be modulated by binding molecules both to the outside and to the inside of the pore. Thus, external K⁺ inhibits C-type inactivation in Shaker K⁺ channels by a “foot-in-the-door” mechanism. Here, we explore the modulation of a very long-lived inactivated state, ultraslow inactivation (I_US), by ligand binding to the outer vestibule in voltage-gated Na⁺ channels. Blocking the outer vestibule by a mutant μ-conotoxin GIIIA substantially accelerated recovery from I_US. A similar effect was observed if Cd²⁺ was bound to a cysteine engineered to the selectivity filter (K1237C). In K1237C channels, exposed to 30 μM Cd²⁺, the time constant of recovery from I_US was decreased from 145.0 ± 10.2 s to 32.5 ± 3.3 s (P < 0.001). Recovery from I_US was only accelerated if Cd²⁺ was added to the bath solution during recovery (V = −120 mV) from I_US, but not when the channels were selectively exposed to Cd²⁺ during the development of I_US (−20 mV). These data could be explained by a kinetic model in which Cd²⁺ binds with high affinity to a slow inactivated state (I_S), which is transiently occupied during recovery from I_US. A total of 50 μM Cd²⁺ produced an ∼8 mV hyperpolarizing shift of the steady-state inactivation curve of I_S, supporting this kinetic model. Binding of lidocaine to the internal vestibule significantly reduced the number of channels entering I_US, suggesting that I_US is associated with a conformational change of the internal vestibule of the channel. We propose a molecular model in which slow inactivation (I_S) occurs by a closure of the outer vestibule, whereas I_US arises from a constriction of the internal vestibule produced by a widening of the selectivity filter region. Binding of Cd²⁺ to C1237 promotes the closure of the selectivity filter region, thereby hastening recovery from I_US. Thus, Cd²⁺ ions may act like a foot-on-the-door, kicking the I_S gate to close.     

Construction of protein-modified TiO2 nanoparticles for use with ultrasound irradiation in a novel cell injuring method

Recently, our group discovered an alternative titanium dioxide (TiO₂) activation method that uses ultrasound irradiation (US/TiO₂) instead of ultraviolet irradiation. The pre-S1/S2 protein from hepatitis B virus, which recognizes liver cells, was immobilized to the surface of TiO₂ nanoparticles using an amino-coupling method. The ability of the protein-modified TiO₂ nanoparticles to recognize liver cells was confirmed by surface plasmon resonance analysis and immuno-staining analyses. After uptake of TiO₂ nanoparticles by HepG2 cancer cells, the cells were injured using this US/TiO₂ method; significant cell injury was observed at an ultrasound irradiation intensity of 0.4 W/cm². Together with these results, this strategy could be applied to new cell injuring systems that use ultrasound irradiation in place of photodynamic therapy in the near future.     

Adsorption characteristics of sulfur powder by bamboo charcoal to restrain sulfur allergies

Exposures to particulate matter with a diameter of 2.5 μm or less (PM2.5) may influence the risk of birth defects and make you allergic, which causes serious harm to human health. Bamboo charcoal can adsorb harmful substances,that was of benefitto people’s health. In order to figure out the optimal adsorbtion condition and the intrinsic change of bamboo charcoal, five chemicals were adsorbed by bamboo charcoal and were analyzed by FT-IR. The optimal blast time was 80 min of Na₂SO₃, 100 min of Na₂S₂O₈, 20 min of Na₂SO₄, 120 min of Fe₂(SO₄)₃ and 60 min or 100 min of S. FT-IR spectra showed that bamboo charcoal had five characteristic peaks of SS stretch, H₂O stretch, OH stretch, CO stretch or CC stretch, and NO₂ stretch at 3850 cm⁻¹, 3740 cm⁻¹, 3430 cm⁻¹, 1630 cm⁻¹ and 1530 cm⁻¹, respectively. For Na₂SO₃, the peaks at 3850 cm⁻¹, 3740 cm⁻¹, 3430 cm⁻¹, 1630 cm⁻¹ and 1530 cm⁻¹ achieved the maximum at 20 min. For Na₂S₂O₈, the peaks at 3850 cm⁻¹, 3740 cm⁻¹, 3430 cm⁻¹ and 1530 cm⁻¹ achieved the maximum at 40 min. For Na₂SO₄, the peaks at 3850 cm⁻¹, 3740 cm⁻¹ and 1530 cm⁻¹ achieved the maximum at 40 min. For Fe₂(SO₄)₃, the peaks at 3850 cm⁻¹, 3740 cm⁻¹, 1630 cm⁻¹ and 1530 cm⁻¹ achieved the maximum at 120 min. For S, the peaks at 3850 cm⁻¹ and 3740 cm⁻¹ achieved the maximum at 40 min, the peaks at 1630 cm⁻¹ and 1530 cm⁻¹ achieved the maximum at 40 min. It proved that bamboo charcoal could remove sulfur powder from air to restrain sulfur allergies.     

Characteristics of activated carbon remove sulfur particles against smog

Sulfur particles, which could cause diseases, were the main powder of smog. And activated carbon had the very adsorption characteristics. Therefore, five sulfur particles were adsorbed by activated carbon and were analyzed by FT-IR. The optimal adsorption time were 120 min of Na₂SO₃, 120 min of Na₂S₂O₈, 120 min of Na₂SO₄, 120 min of Fe₂(SO₄)₃ and 120 min of S. FT-IR spectra showed that activated carbon had the eight characteristic absorption of SS stretch, H₂O stretch, OH stretch, CH stretch, conjugated CO stretch or CC stretch, CH₂ bend, CO stretch and acetylenic CH bend vibrations at 3850 cm^–1, 3740 cm^–1, 3430 cm^–1, 2920 cm^–1, 1630 cm^–1, 1390 cm^–1, 1110 cm^–1 and 600 cm^–1, respectively. For Na₂SO₃, the peaks at 2920 cm^–1, 1630 cm^–1, 1390 cm^–1 and 1110 cm^–1 achieved the maximum at 20 min. For Na₂S₂O₈, the peaks at 3850 cm^–1, 3740 cm^–1 and 2920 cm^–1 achieved the maximum at 60 min. The peaks at 1390 cm^–1, 1110 cm^–1 and 600 cm^–1 achieved the maximum at 40 min. For Na₂SO₄, the peaks at 3430 cm^–1, 2920 cm^–1, 1630 cm^–1, 1390 cm^–1, 1110 cm^–1 and 600 cm^–1 achieved the maximum at 60 min. For Fe₂(SO₄)₃, the peaks at 1390 cm^–1, 1110 cm^–1 and 600 cm^–1 achieved the maximum at 20 min. For S, the peaks at 1630 cm^–1, 1390 cm^–1 and 600 cm^–1 achieved the maximum at 120 min. It provided that activated carbon could remove sulfur particles from smog air to restrain many anaphylactic diseases.     

Kinetic models and process parameters for ultrasound-assisted extraction of water-soluble components and polysaccharides from a medicinal fungus

This study was on the kinetics and process parameters for ultrasound-assisted extraction (UAE) of water-soluble components and polysaccharides (PS) from the dry mycelium of a medicinal fungus, Cordyceps sinensis Cs-HK1. Four process variables (factors) were evaluated at different levels, ultrasound intensity (2.44–44.1 W/cm²), temperature (40–70 °C), solid particle size (156.5–750 μm), and solid-to-liquid ratio (1/30–1/70 g/mL). The experimental data of yields versus time in most cases were fitted closely to two empirical kinetic models for solid–liquid extraction, parabolic diffusion equation (y = y_o + y₁t^1/2) and power law (y = βtⁿ) with high correlation coefficients (R²) of 0.95–0.99 for total extract yield, and 0.90–0.96 for PS yield. The PS yield was increased more significantly than the total extract yield with the ultrasound intensity. Reducing the particle size and increasing the extraction temperature led to a higher yield and extraction rate; increasing the solid-to-liquid ratio (or decreasing the liquid volume) increased the PS yield and extraction rate but had little influence on the total extract. Significant correlations were found between extraction rate (dy/dt) and ultrasound power density (P/V), and between extract yield (y) and energy density (Pt/V). The kinetic and process parameters are useful for rational design and efficient operation of UAE processes.     

Adsorption characteristics of sulfur solution by acticarbon against drinking-water toxicosis

Sulfur and ammonia nitrogen are rich nutrient pollutants, after entering water can cause algal blooms, cause eutrophication of water body, the spread of them will not only pollute the environment, destroy the ecological balance, but also harm human health through food chain channels, especially drinking-water toxicosis. Acticarbon can adsorb harmful substances, it was beneficial for people’s health. In order to figure out the optimal adsorption condition and the intrinsic change of acticarbon, five chemicals were adsorbed by acticarbon and analyzed by FT-IR. The optimal adsorption condition of Fe₂(SO₄)₃, Na₂SO₄, Na₂S₂O₈, S and Na₂SO₃ was 9 g/1000 g at 80 min, 21 g/1000 g at 20 min, 15g/1000 g at 20 min, 21 g/1000 g at 60 min and 21 g/1000 g at 100 min, respectively. FT-IR spectra showed that acticarbon had eight characteristic peaks, such as S-S stretch, H₂O stretch, OH stretch, CH stretch, CO or CC stretch, CH₂ bend, CH were at 3850 cm⁻¹, 3740 cm⁻¹, 3435 cm⁻¹, 2925 cm⁻¹, 1630 cm⁻¹, 1390 cm⁻¹, 1115 cm⁻¹, 600 cm⁻¹, respectively. For FT-IR spectra of Fe₂(SO₄)₃, the peaks at 3850 cm⁻¹, 3740 cm⁻¹, 2925 cm⁻¹ achieved the maximum with 9 g/1000 g at 20 min. For Na₂SO₄, the peaks at 2925 cm⁻¹, 1630 cm⁻¹, 1390 cm⁻¹, 1115 cm⁻¹, 600 cm⁻¹ achieved the maximum with 21 g/1000 g at 120 min. For ones of Na₂S₂O₈, the peaks at 3850 cm⁻¹, 3740 cm⁻¹, 1390 cm⁻¹, 1115 cm⁻¹, 600 cm⁻¹, achieved the maximum with 2 g/1000 g at 80 min. For ones of S, the peaks at 3850 cm⁻¹, 3740 cm⁻¹, 2925 cm⁻¹ achieved the maximum with 19 g/1000 g at 100 min, the peaks at 1390 cm⁻¹, 1115 cm⁻¹, 600 cm⁻¹ achieved the maximum with 19 g/1000 g at 20 min. For FT-IR spectra of Na₂SO₃, the peaks at 1630 cm⁻¹, 1390 cm⁻¹, 1115 cm⁻¹, 600 cm⁻¹ achieved the maximum with 2 g/1000 g at 100 min. It provided that acticarbon could adsorb and desulphurize from sulfur solution against drinking-water toxicosis.     

Polyphenolic Antioxidants Efficiently Protect Urease from Inactivation by Ultrasonic Cavitation

Inactivation of urease (25 nM) in aqueous solutions (pH 5.0–6.0) treated with low-frequency ultrasound (LFUS; 27 kHz, 60 W/cm², 36–56°C) or high-frequency ultrasound (HFUS; 2.64 MHz, 1 W/cm², 36 or 56°C) has been characterized quantitatively, using first-order rate constants: k _in, total inactivation; k _in ^*, thermal inactivation; and k _in(us), ultrasonic inactivation. Within the range from 1 nM to 10 M, propyl gallate (PG) decreases by approximately threefold the rate of LFUS-induced inactivation of urease (56°C), whereas resorcinol poly-2-disulfide stops this process at 1 nM or higher concentrations. PG completely inhibits HFUS-induced inactivation of urease at 1 nM (36°C) or 10 nM (56°C). At 0.2–1.0 M, human serum albumin (HSA) increases the resistance of urease treated with HFUS to temperature- and cavitation-induced inactivation. Complexes of gallic acid polydisulfide (GAPDS) with HSA (GAPDS–HSA), formed by conjugation of 1.0 nM GAPDS with 0.33 nM HSA, prevent HFUS-induced urease inactivation (56°C).     

Sub-0.6 eV Inverted Metamorphic GaInAs Cells Grown on Inp and GaAs Substrates for Thermophotovoltaics and Laser Power Conversion

Inverted metamorphic Ga_0.3In_0.7As photovoltaic converters with sub-0.60 eV bandgaps grown on InP and GaAs are presented. Threading dislocation densities are 1.3 ± 0.6 × 10⁶ and 8.9 ± 1.7 × 10⁶ cm⁻² on InP and GaAs, respectively. The devices generate open-circuit voltages of 0.386 and 0.383 V, respectively, under irradiance producing a short-circuit current density of ≈10 A cm⁻², yielding bandgap-voltage offsets of 0.20 and 0.21 V. Power and broadband reflectance measurements are used  to estimate thermophotovoltaic (TPV) efficiency. The InP-based cell is estimated to yield 1.09 W cm⁻² at 1100 °C versus 0.92 W cm⁻² for the GaAs-based cell, with efficiencies of 16.8 versus 9.2%. The efficiencies of both devices are limited by sub-bandgap absorption, with power weighted sub-bandgap reflectances of 81% and 58%, respectively, the majority of which is assumed to occur in the graded buffers. The 1100 °C TPV efficiencies are estimated to increase to 24.0% and 20.7% in structures with the graded buffer removed, if previously demonstrated reflectance is achieved. These devices also have application to laser power conversion in the 2.0–2.3 µm atmospheric window. Peak laser power converter efficiencies of 36.8% and 32.5% are estimated under 2.0 µm irradiances of 1.86 and 2.81 W cm⁻², respectively.     

Low-amplitude ultrasound enhances hydrodynamic-based gene delivery to rat kidney

The synergistic combination of hydrodynamic-based gene delivery and ultrasound was investigated to achieve improved gene transfer to the kidney. Plasmids encoding firefly luciferase and Erythropoietin (EPO) gene were delivered into the left kidney of rats by single or combinative application of renal vein hydrodynamic injection and ultrasound treatment with or without the addition of ultrasound contrast agents (UCA). Ultrasound exposure was found to enhance the efficiency of hydrodynamic-based gene delivery for both luciferase and EPO expression. An ultrasound exposure intensity of 2 W/cm² at 10% duty cycle for 15 min, produced a maximal gene expression 4.5 times higher than hydrodynamic delivery alone. Duration, location, and tissue-specificity of gene expression were not changed by ultrasound exposure. Application of UCA reduced the intensity and exposure duration of ultrasound treatment needed for optimal expression. Appropriate application of ultrasound and UCA did not alter histological structure or impair physiological function of the treated kidney.     

Desulphurization characteristics of bamboo charcoal from sulfur solution

Sulfur powder and sulfur dioxide (SO₂) often floated in air, produced acid rain and algal blooms, and could cause diseases. Bamboo charcoal could have adsorption and filtration properties. In order to figure out the optimal adsorption condition and the intrinsic change of the bamboo charcoal, five chemicals were adsorbed by bamboo charcoal and were analyzed by FT-IR. Fe₂(SO₄)₃’s, Na₂SO₄’s, Na₂S₂O₈’s, S’s, and Na₂SO₃’s optimal adsorption condition was the concentration of 19 g/1000 g and stir time of 20 min, 21 g/1000 g and stir time of 60 min, 7 g/1000 g and stir time of 120 min, 11 g/1000 g and stir time of 120 min, 21 g/1000 g and stir time of 60 min, respectively. FT-IR spectra showed that for FT-IR spectra of Fe₂(SO₄)₃, the transmissivity of the peaks at 3435 cm⁻¹ and 2925 cm⁻¹ achieved the maximum for 60 min and the concentration was 19 g/1000 g, the transmissivity of the peaks at 1630 cm⁻¹, 1060 cm⁻¹ and 660 cm⁻¹ achieved the maximum for 60 min and the concentration was 7 g/1000 g. For FT-IR spectra of Na₂SO₄, the transmissivity of the peaks at 1630 cm⁻¹, 1060 cm⁻¹ and 660 cm⁻¹ achieved the maximum for 20 min and the concentration was 13 g/1000 g. For FT-IR spectra of Na₂S₂O₈, the transmissivity of the peaks at 3435 cm⁻¹, 2925 cm⁻¹, 1630 cm⁻¹ and 1060 cm⁻¹ achieved the maximum for 120 min and the concentration was 19 g/1000 g. For FT-IR spectra of S, the transmissivity of the peaks at 3435 cm⁻¹, 2925 cm⁻¹, 1630 cm⁻¹ and 1060 cm⁻¹ achieved the maximum for 20 min and the concentration was 11 g/1000 g, 17 g/1000 g and 21 g/1000 g. For FT-IR spectra of Na₂SO₃, the transmissivity of the peaks at 3435 cm⁻¹ achieved the maximum for 120 min and the concentration was 5 g/1000 g, the transmissivity of the peaks at 2925 cm⁻¹, 1630 cm⁻¹ and 1060 cm⁻¹ achieved the maximum for 120 min and the concentration was 11 g/1000 g. In these states, the number of the transmissivity of the maximum peaks is the largest.     

Repellency and toxicity of a CO2-derived cedarwood oil on hard tick species (Ixodidae)

The repellency and toxicity of a CO₂-derived cedarwood oil (CWO) was evaluated against actively questing unfed nymphs of four species of hard ticks: Amblyomma americanum (L.), Dermacentor variabilis (Say), Ixodes scapularis Say, and Rhipicephalus sanguineus (Latreille). Using a vertical climb bioassay for repellency, nymphs of these species avoided a CWO-treated filter paper in proportional responses to treatment concentrations. At 60 min of exposure, I. scapularis nymphs were most sensitive with 50% repellency concentration (RC₅₀) of 19.8 µg cm^?2, compared with RC₅₀ of 30.8, 83.8 and 89.6 µg cm^?2 for R. sanguineus, D. variabilis and A. americanum, respectively. Bioassays determined the lethal concentration for 50% (LC₅₀) and 90% (LC₉₀) mortality of nymphs exposed to CWO in treated vials after 24- and 48-h exposure. After 24 h exposure, the LC₅₀ values were 1.25, 3.45 and 1.42 µg cm^?2 and LC₉₀ values were 2.39, 7.59 and 4.14 µg cm^?2 for D. variabilis, I. scapularis and R. sanguineus, respectively, but had minimal effect on A. americanum. After 48 h exposure, the LC₅₀ values were 4.14, 0.78, 0.79 and 0.52 µg cm^?2, and LC₉₀ values were 8.06, 1.48, 1.54 and 1.22 µg cm^?2 for A. americanum, D. variabilis, I. scapularis and R. sanguineus, respectively. The repellency of CWO on tick species decreased with time. The repellency and toxicity bioassays demonstrated concentration-dependent responses of tick nymphs to the oil, indicating the potential of the CO₂-derived cedarwood oil be developed as an eco-friendly repellent and/or acaricide.

     

The effect of irradiance on long-term skeletal growth and net photosynthesis in Galaxea fascicularis under four light conditions

The relation between irradiance, skeletal growth and net photosynthesis was studied for the scleractinian coral Galaxea fascicularis to provide experimental evidence for mediation of light-enhanced calcification through photosynthesis. The hypothesis was tested that skeletal growth and photosynthesis are linearly correlated.A long-term experiment was performed in a closed-circuit aquarium system, in which four series of nine nubbins (single polyp clones of a coral colony) of Galaxea fascicularis were exposed to four light treatments (10L:14D): 144 W T8 fluorescent lighting providing an irradiance of 68 µE/m²/s and 70, 250 and 400 W Metal Halide lighting providing an irradiance of 38 µE/m²/s, 166 µE/m²/s and 410 µE/m²/s, respectively. Growth of these nubbins was measured as buoyant weight at different time intervals in a 294 day experiment. A light-saturation curve for photosynthesis was measured in a respirometric flow cell using a 54 week Galaxea fascicularis colony grown at 60 µE/m²/s.No saturation of net photosynthesis of Galaxea fascicularis was found at the irradiances tested. The specific growth rate (µ, in day^- 1) of the coral nubbins increased with irradiance. Whereas irradiance varied 11-fold (38 to 410 µE/m²/s), buoyant weight (increase after 294 days) increased 5.7 times (2243 to 12374 mg), specific growth rate (1-294 days) increased 1.6 times (0.0103 to 0.0161 day^- 1), while net photosynthetic rate increased 8.9 times (0.009 µmol O₂/min/cm² to 0.077 µmol O₂/min/cm²). The increase of specific growth rate with irradiance was less than expected based on the increase in net photosynthetic rate with irradiance. This discrepancy between potential energy produced in photosynthesis and energy used for skeletal growth indicates that skeletal growth is not limited by photosynthetic potential at high irradiance levels.     

Optimization of intravascular shear stress assessment in vivo

The advent of microelectromechanical systems (MEMS) sensors has enabled real-time wall shear stress (WSS) measurements with high spatial and temporal resolution in a 3-D bifurcation model. To optimize intravascular shear stress assessment, we evaluated the feasibility of catheter/coaxial wire-based MEMS sensors in the abdominal aorta of the New Zealand white (NZW) rabbits. Theoretical and computational fluid dynamics (CFD) analyses were performed. Fluoroscope and angiogram provided the geometry of aorta, and the Doppler ultrasound system provided the pulsatile flow velocity for the boundary conditions. The physical parameters governing the shear stress assessment in NZW rabbits included (1) the position and distance from which the MEMS sensors were mounted to the terminal end of coaxial wire or the entrance length, (L_e), (2) diameter ratios of aorta to the coaxial wire (D_aorta /D_{coaxial wire}=1.5–9.5), and (3) the range of Reynolds numbers (116–1550). At an aortic diameter of 2.4 mm and a maximum Reynolds number of 212 (a mean Reynolds number of 64.2), the time-averaged shear stress (τ_ave) was computed to be 10.06 dyn cm^?2 with a systolic peak at 33.18 dyn cm^?2. In the presence of a coaxial wire (D_aorta /D_{coaxial wire}=6 and L_e=1.18 cm), the τ_ave value increased to 15.54 dyn cm^?2 with a systolic peak at 51.25 dyn cm^?2. Real-time intravascular shear stress assessment by the MEMS sensor revealed an τ_ave value of 11.92 dyn cm^?2 with a systolic peak at 47.04 dyn cm^?2. The difference between CFD and experimental τ_ave was 18.5%. These findings provided important insights into packaging the MEMS sensors to optimize in vivo shear stress assessment.     

Quantum mechanical analysis of excitation energy transfer couplings in photosystem II

We evaluated excitation energy transfer (EET) coupling (J) between all pairs of chlorophylls (Chls) and pheophytins (Pheos) in the protein environment of photosystem II based on the time-dependent density functional theory with a quantum mechanical/molecular mechanics approach. In the reaction center, the EET coupling between Chls P_D1 and P_D2 is weaker (|J(P_D1/P_D2)| = 79 cm^?1), irrespective of a short edge-to-edge distance of 3.6 Å (Mg-to-Mg distance of 8.1 Å), than the couplings between P_D1 and the accessory Chl_D1 (|J(P_D1/Chl_D2)| = 104 cm^?1) and between P_D2 and Chl_D2 (|J(P_D2/Chl_D1)| = 101 cm^?1), suggesting that P_D1 and P_D2 are two monomeric Chls rather than a “special pair”. There exist strongly coupled Chl pairs (|J| > ～100 cm^?1) in the CP47 and CP43 core antennas, which may be candidates for the red-shifted Chls observed in spectroscopic studies. In CP47 and CP43, Chls ligated to CP47-His26 and CP43-His56, which are located in the middle layer of the thylakoid membrane, play a role in the “hub” that mediates the EET from the lumenal to stromal layers. In the stromal layer, Chls ligated to CP47-His466, CP43-His441, and CP43-His444 mediate the EET from CP47 to Chl_D2/Pheo_D2 and from CP43 to Chl_D1/Pheo_D1 in the reaction center. Thus, the excitation energy from both CP47 and CP43 can always be utilized for the charge-separation reaction in the reaction center.