The mechanism of Zn-phthalocyanine photosensitized lysis of human erythrocytes

The phthalocyanines have recently been suggested as one of most effective possible sensitizers for photodynamic therapy and the blood viral inactivation. The further characterisation of the mechanism of human red blood cell lysis and membrane alterations upon photodynamic treatment in the presence of Zn-phthalocyanine was the aim of this study. It was found that there were (2.7+/-0.4).10(7) dye binding sites per red blood cell with the association constant equal to (1.4+/-0.3).10(4) M(-1). Two types of the photosensitized haemolysis: haemolysis during irradiation ("light" haemolysis) and post-irradiation haemolysis ("dark" haemolysis) were studied. The erythrocyte membrane hyperpolarisation, membrane fluidisation and cell swelling preceded the "light" haemolysis. The modification of the erythrocyte membrane band 3 protein by DIDS (an inhibitor of anion exchange) increased the rate of the "light" haemolysis. The rate of "dark" haemolysis was higher and that of "light" haemolysis was lower in potassium media in comparison to sodium ones. The rates of photohaemolysis depended on the erythrocyte membrane potential: a decrease of membrane potential inhibited both types of haemolysis. The cell shrinkage in the presence of sucrose (up to 15 mM) inhibited the "dark" haemolysis but significantly increased the "light" haemolysis. Oxidation of intracellular oxyHb to metHb by nitrite, which drastically decreases intracellular oxygen concentration, as well as GSH concentration, inhibited the rate of the "light" haemolysis. The results allow for the conclusion that the mechanism of photochemical ("light") haemolysis is not of a colloid-osmotical type, in contrast to the post-irradiation ("dark") haemolysis. The photochemical oxidation or denaturation of band 3 protein plays a significant role in the formation of haemolytic holes. The membrane lipid peroxidation, as well as glutathione oxidation, does not participate in the process of photosensitized haemolysis. From the inhibition of "dark" haemolysis by sucrose the apparent pore radius was estimated to be about 1.1 nm. The pores appear to be transient short-lived ones, the average pore number per cell was 0.02.     

Theoretical analysis of the thermal effects during in vivo tissue electroporation

Tissue electroporation is a technique that facilitates the introduction of molecules into cells by applying a series of short electric pulses to specific areas of the body. These pulses temporarily increase the permeability of the cell membrane to small drugs and macromolecules. The goal of this paper is to provide information on the thermal effects of these electric pulses for consideration when designing electroporation protocols. The parameters investigated include electrode geometry, blood flow, metabolic heat generation, pulse frequency, and heat dissipation through the electrodes. Basic finite-element models were created in order to gain insight and weigh the importance of each parameter. The results suggest that for plate electrodes, the energy from the pulse may be used to adequately estimate the heating in the tissue. However, for needle electrodes, the geometry, i.e. spacing and diameter, and pulse frequency are critical when determining the thermal distribution in the tissue.     

Scaling of Shielded Sliding Discharges for Environmental Applications

Shielded sliding discharges are nanosecond streamer discharges which develop along a dielectric between metal foil electrodes, with one of the foils extended over the entire rear of the dielectric layer. The electrode configuration not only allowed rearranging discharges in parallel due to the decoupling effect of the metal layer, but also to modify the electric field distribution in such a way that components normal to the surface are enhanced, leading to an increased energy density in the discharge plasma. By varying the electrode gap, the applied voltage, and the repetition rate, it is shown that by keeping the average electric field constant, the discharge voltage can be reduced from tens of kV to values on the order of a few kV, but only at the expense of a reduced energy density of the plasma. Varying the repetition rate from 20 to 500 Hz resulted in a slightly reduced energy per pulse, likely caused by residual charges on the dielectric surface. Measurements of the NO conversion to NO₂ and ozone synthesis in dry air showed that the conversion is only dependent on the energy density of the discharge plasma. Although reducing the pulse voltage from the tens of kV range to that of few kV, and possibly even lower, causes a reduction in energy density, this loss can be compensated for by increasing the electrode gap area. This and the possibility to form discharge arrays allows generating large volume discharge reactors for environmental applications, at modest pulsed voltages.     

K-edge angiography utilizing a tungsten plasma X-ray generator in conjunction with gadolinium-based contrast media

The tungsten plasma flash X-ray generator is useful in order to perform high-speed enhanced K-edge angiography using cone beams because K-series characteristic X-rays from the tungsten target are absorbed effectively by gadolinium-based contrast media. In the flash X-ray generator, a 150 nF condenser is charged up to 80 kV by a power supply, and flash X-rays are produced by the discharging. The X-ray tube is a demountable diode, and the turbomolecular pump evacuates air from the tube with a pressure of approximately 1 mPa. Since the electric circuit of the high-voltage pulse generator employs a cable transmission line, the high-voltage pulse generator produces twice the potential of the condenser charging voltage. At a charging voltage of 80 kV, the estimated maximum tube voltage and current were approximately 160 kV and 40 kA, respectively. When the charging voltage was increased, the characteristic X-ray intensities of tungsten K_α lines increased. The K_α lines were clean, and hardly any bremsstrahlung rays were detected. The X-ray pulse widths were approximately 110 ns, and the time-integrated X-ray intensity had a value of approximately 0.35 mGy at 1.0 m from the X-ray source with a charging voltage of 80 kV. Angiography was performed using a film-less computed radiography (CR) system and gadolinium-based contrast media. In angiography of non-living animals, we observed fine blood vessels of approximately 100 μm with high contrasts.     

Clinical evaluation of safety and human tolerance of electrical sensation induced by electric fields with non-invasive electrodes

This paper reports the first clinical safety study of human tolerance of electrical sensation using non-invasive, flexible surface-type electrodes and exponentially decaying electric pulses. The study evaluated the effect of electric fields in the absence of a drug and an anesthetic, and was performed in light of potential applications in the field of erectile dysfunction (ED). Twenty impotent patients who had previously received injection or intraurethral therapies were enrolled in the study. Voltage escalations from 50 to 80 V (in 10-V increments) with a single pulse of 3-ms duration were performed with meander-type electrodes placed on the shaft and part of the glans of the penis. The electric fields-induced sensation was assessed via a pain scale from 0 to 10. All 20 patients, who were free to withdraw from the study at any point, completed the voltage escalation study. No clinical safety concerns were apparent and no skin irritation was observed after electric treatment. Our initial study indicates that the pulses in the tested voltage range were well tolerated by most patients. In previous animal experiments under analogous experimental conditions, the application of 50 V has been found effective for transdermal drug delivery into the penis.     

Effect of high-voltage electric pulses on yeast cells: factors influencing the killing efficiency

The decisive factors determining the killing efficiency of single rectangular electric pulses of 4–28 kV cm⁻¹ amplitude and 1–300 μs duration in Saccharomyces cerevisiae S6/1 are pulse amplitude and duration, cell size and growth phase, post-pulse temperature and medium conductivity. In S. cerevisiae, the minimum pulse duration ensuring substantial killing is about 10 μs, the minimum amplitude being about 2 kV cm⁻¹. The critical pulse-induced transmembrane breakthrough voltage is 0.75 V. A pulse-induced increase in membrane permeability for small species such as inorganic ions suffices to cause cell death. A preset killing rate can be achieved by varying pulse amplitude inversely to pulse duration. Comparison of killing data on S. cerevisiae S6/1 with those on the smaller-celled Kluyveramyces lactis showed the killing pulse amplitude to be roughly proportional to cell size except for low pulse amplitudes, at which smaller cells are much more killing-prone. In exponential S. cerevisiae cells increased pulse amplitude caused a sharp increase in killing while in stationary cells this effect was much lower and occurred only at pulse amplitude above 15–20 kV cm⁻¹. Elevated post-pulse temperature lowered the killing rate whereas lowered temperature promoted it, probably by affecting the pore resealing. Lowering medium conductivity from 66 to 46 μS m⁻¹ by suspension washing reduced the killing rate by 6–20%. Reproducible killing or electroporation therefore requires standardized cell concentration, and number of cell washings.     

Using a micro electroporation chip to determine the optimal physical parameters in the uptake of biomolecules in HeLa cells

In this study, a new micro electroporation (EP) cell chip with three-dimensional (3D) electrodes was fabricated by means of MEMS technology, and tested on cervical cancer (HeLa) cells. Extensive statistical data of the threshold electric field and pulse duration were determined to construct an EP "phase diagram", which delineates the boundaries for 1) effective EP of five different size molecules and 2) electric cell lysis at the single-cell level. In addition, these boundary curves (i.e., electric field versus pulse duration) were fitted successfully with an exponential function with three constants. We found that, when the molecular size increases, the corresponding electroporation boundary becomes closer to the electric cell lysis boundary. Based on more than 2000 single-cell measurements on five different size molecules, the critical size of molecule was found to be approximately 40 kDa. Comparing to the traditional instrument, MEMS-based micro electroporation chip can greatly shorten the experimental time.     

基于SOI基底的高通量细胞电融合芯片

提出了一种以MEMS技术为基础, 可在低电压驱动条件下工作的创新型细胞电融合芯片. 该芯片的设计原理在于通过缩短微电极间的间距, 在低电压条件下获得足够强度的排队和融合电场强度. 原型芯片以SOI硅片为加工材料, 通过刻蚀方式在顶层低阻硅形成微电极和微通道; 在微电极上沉淀2 μm厚的铝膜以降低电阻率, 提高导电性; 通过PECVD方法形成150 nm厚SiO2保障铝膜的抗腐蚀性及芯片生物相容性; 芯片最终采用DIP法进行封装. 在该芯片上进行了低电压(传统电融合设备工作电压的1/20)驱动条件下的基于介电电泳的细胞排队实验及后期的细胞电融合实验, 结果表明, 细胞多以两两结合的方式排列, 与传统的细胞融合电仪器相比较, 降低了多细胞排队概率, 进而减少了传统电融合设备多细胞融合的概率, 为细胞高效率融合奠定了基础. 在加载的低电压短脉冲信号后, 微通道中形成了高压短脉冲电场, 在脉冲作用下, 烟草原生质体细胞在微通道中发生了融合, 融合时间(2 min)远低于传统电融合方法(10~30 min), 融合率远远高于传统的PEG方法(融合率小于1%)和传统电融合方法(利用BTX ECM 2001细胞电融合系统得到, 融合率小于5%).     

丙烯和氧等离子体直接气相合成环氧丙烷

在室温和大气压下,在针板式反应器中,通过脉冲电晕放电等离子体对分子氧和丙烯直接合成环氧丙烷的活化作用,考察了放电电极间距、电晕放电脉冲电压以及电晕放电重复频率参数对丙烯转化率、环氧丙烷产率和其选择性的影响,反应物及各产物通过在线色谱法进行分析.实验结果表明,在室温和大气压下,用脉冲电晕等离子体法可转化丙烯和氧气直接生成环氧丙烷,适当调节上述各参数可提高环氧丙烷的收率.当反应气总流速为200mL/min,极间距为4mm,脉冲放电电压为18kV,放电频率为120Hz时,环氧丙烷的收率、丙烯的转化率及环氧丙烷的选择性分别为5.15%,19.15%和26.89%.     

Efficacy of transgene expression in porcine skin as a function of electrode choice

Gene electrotransfer is a non-viral technique using electroporation for gene transfection. The method is widely used in the preclinical setting and results from the first clinical study in tumours have been published. However, the preclinical studies, which form the basis for the clinical trials, have mainly been performed in rodents and the body of evidence on electrode choice and optimal pulsing conditions is limited.We therefore tested plate and needle electrodes in vivo in porcine skin, which resembles human skin in structure. The luciferase (pCMV-Luc) gene was injected intradermally and subsequently electroporated. Simultaneously, studies with gene electrotransfer to porcine skin using plasmids coding for green fluorescent protein (GFP) and betagalactosidase were performed.Interestingly, we found needle electrodes to be more efficient than plate electrodes (p < 0.001) and electric field calculations showed that penetration of the stratum corneum led to much more homogenous field distribution at the DNA injection site. Furthermore, we have optimised the electric pulse regimens for both plate and needle electrodes using a range of high voltage and low voltage pulse combinations.In conclusion, our data support that needle electrodes should be used in human clinical studies of gene electrotransfer to skin for improved expression.     

Multiple-pulse-mediated electrofusion of intact erythrocyte onto human term placental amnion.

The creation of surface modified human term placental amnion by electrofusing human cells onto its surface has been thought of. A multiple-pulse electrofusion protocol with 10 square pulses of 10-micros pulse length, and electric field of 0.2 kV cm(-1), can make erythrocyte-amnion tissue electrofusion possible. The protocol devised merge the cell-tissue-adherence steps with fusogenic pulse. The finding opens up a new avenue of cell electrofusion onto human tissue with minimal procedural complexities.     

A blue-phase liquid crystal lens array based on dual square ring-patterned electrodes

We propose a blue-phase liquid crystal (BPLC) lens array based on dual square ring-patterned electrodes. A high dielectric constant layer is used to smoothen out the horizontal electric field and reduce the operating voltage. By creating a potential difference between the dual square ring-patterned electrodes, gradient electric fields are generated and lens-like phase profile is obtained. Besides, the focal length of the BPLC lens is adjustable with voltage changes and all simulation results indicate that the BPLC lens array is polarisation-insensitive.     

Very fast electrophoretic separation on commercial instruments using a combination of two capillaries with different internal diameters

A capillary formed by connecting a 9.7 cm‐long separation capillary with id 25 μm with an auxiliary 22.9 cm‐long capillary with id 100 μm (coupled capillary) was tested for electrophoretic separation at high electric field intensities. The coupled capillary was placed in the cassette of a standard electrophoresis apparatus. It was used in the short‐end injection mode for separation of a mixture of dopamine, noradrenaline, and adrenaline in a BGE of 20 mM citric acid/NaOH, pH 3.2. An intensity of 2.7 kV/cm was attained in the separation part of the capillary at a separation voltage of 30 kV, which is 2.9 times more than maximum intensity value attainable in a capillary with the same length with uniform id. At these high electric field intensities, the migration times of the tested neurotransmitters had values of 12.3–13.3 s and the attained separation efficiency was between 2350 and 2760 plates/s. It is thus demonstrated that an effective separation instrument ‐ a coupled capillary ‐ can be used for very rapid separation in combination with standard, commercially available instrumentation.     

Embedded passivated-electrode insulator-based dielectrophoresis (EπDEP)

Here, we introduce a new technique called embedded passivated-electrode insulator-based dielectrophoresis (EπDEP) for preconcentration, separation, or enrichment of bioparticles, including living cells. This new method combines traditional electrode-based DEP and insulator-based DEP with the objective of enhancing the electric field strength and capture efficiency within the microfluidic channel while alleviating direct contact between the electrode and the fluid. The EπDEP chip contains embedded electrodes within the microfluidic channel covered by a thin passivation layer of only 4 μm. The channel was designed with two nonaligned vertical columns of insulated microposts (200 μm diameter, 50 μm spacing) located between the electrodes (600 μm wide, 600 μm horizontal spacing) to generate nonuniform electric field lines to concentrate cells while maintaining steady flow in the channel. The performance of the chip was demonstrated using Gram-negative (Escherichia coli) and Gram-positive (Staphylococcus aureus) bacterial pathogens in aqueous media. Trapping efficiencies of 100 % were obtained for both pathogens at an applied AC voltage of 50 V peak-to-peak and flow rates as high as 10 μl/min.     

The laws of delayed photohaemolysis sensitized by chlorin e6.

The relationships between the rate of post-irradiated photohaemolysis sensitized by chlorin e6 and parameters such as the light fluence (time of irradiation) and sensitizer concentration were studied. On the basis of the single-parametric approach proposed by Valenzeno and Pooler, it was found that the haemolytic rate varies with the square of both the light fluence and the sensitizer concentration. Thus it can be concluded that, in a single erythrocyte lesion, two chlorin e6 molecules participate, each absorbing one photon. The possibility of suppression of post-irradiation haemolysis was also studied using the lipophilic antioxidant, butylated hydroxytoluene (BHT), and scavengers of 1O2, O2.- and HO. radicals. It was found that BHT inhibits, to a considerable extent, the post-irradiation lysis of cells, by about a factor of 2.5 at a BHT concentration of 9 microM. The addition to the medium of NaN3 (a scavenger of 1O2), superoxide dismutase (a scavenger of O2.- radicals), ethanol and D-mannitol (scavengers of HO. radicals), when irradiation was interrupted, did not produce a marked influence on the kinetics of subsequent haemolysis. On the basis of the results obtained, the nature of erythrocyte targets, which are crucial for the photodynamic effect of chlorin e6, is discussed.     

A liquid crystal microlens obtained with a non-uniform electric field

A homogeneously aligned nematic liquid crystal cell with a hole-patterned electrode and with an indium-tin oxide (ITO-) coated counter-electrode has been prepared. A non-uniform electric field can be produced by the asymmetrical electrode structure. The liquid crystal director can be reoriented by applying a voltage across the electrodes, and this produces an axially symmetrical profile of the refractive index. This liquid crystal cell is expected to have a lens effect and so its optical properties have been investigated. The profile of the output light intensity was measured by using a detecting system with an optical fibre. Some relationships between the lens properties, the diameter of the hole and the thickness of the liquid crystal layer have been examined. The liquid crystal cell becomes a convex (converging) lens with a relatively low voltage. A focal length of several millimetres can be obtained by applying voltages of 3-4 V. As the applied voltage increases, the focal length becomes longer, and the cell changes to a concave (diverging) lens when a high voltage is applied (≳ 20 V). These properties are discussed from the viewpoint of the director orientation effects resulting from the non-uniform electric fields in the cell.     

微流控芯片单细胞进样和溶膜

单细胞分析对重大疾病的早期诊断、治疗和药物筛选以及细胞生理、病理过程的研究有重要意义.将毛细管电泳用于单细胞多组分的测定已取得一些成果,但受毛细管的一维结构限制,单细胞进样和溶膜操作较复杂.微流控分析芯片的网络结构和微米级的通道尺寸使简化单细胞分析成为可能.     

A liquid crystal microlens obtained with a non-uniform electric field

Abstract

A homogeneously aligned nematic liquid crystal cell with a hole-patterned electrode and with an indium-tin oxide (ITO-) coated counter-electrode has been prepared. A non-uniform electric field can be produced by the asymmetrical electrode structure. The liquid crystal director can be reoriented by applying a voltage across the electrodes, and this produces an axially symmetrical profile of the refractive index. This liquid crystal cell is expected to have a lens effect and so its optical properties have been investigated. The profile of the output light intensity was measured by using a detecting system with an optical fibre. Some relationships between the lens properties, the diameter of the hole and the thickness of the liquid crystal layer have been examined. The liquid crystal cell becomes a convex (converging) lens with a relatively low voltage. A focal length of several millimetres can be obtained by applying voltages of 3-4 V. As the applied voltage increases, the focal length becomes longer, and the cell changes to a concave (diverging) lens when a high voltage is applied (? 20 V). These properties are discussed from the viewpoint of the director orientation effects resulting from the non-uniform electric fields in the cell.     

Electrotransformation of Saccharomyces cerevisiae protoplast by a plasmid of Escherichia coli

The experiments reported here are aimed at obtaining optimum conditions for gene transformation after electric field pulses. Saccharomyces cerevisiae DBY746 is used as the recipient strain for shuttle plasmid (YRp group). From the relationship between the optimum electric field conditions and the transformation efficiency it is discovered that the maximum transformation efficiency appears at a wide pulse length of 400 μs with an electric field strength of 4 kV/cm, yielding up to 273 transformants/μg DNA. The electroporation unit used in the experiment is a home-made set featuring simplicity, readiness and practicality.