Department of Information Engineering, Second University of Naples, via Roma 29, Aversa, Italy.
J Membr Biol. 2010 Jul;236(1):55-60. doi: 10.1007/s00232-010-9273-2. Epub 2010 Jul 7.
Intense nanosecond pulsed electric fields (nsPEFs) have been shown to induce, on intracellular structures, interesting effects dependent on electrical exposure conditions (pulse length and amplitude, repetition frequency and number of pulses), which are known in the literature as "bioelectrical effects" (Schoenbach et al., IEEE Trans Plasma Sci 30:293-300, 2002). In particular, pulses with a shorter width than the plasma membrane charging time constant (about 100 ns for mammalian cells) can penetrate the cell and trigger effects such as permeabilization of intracellular membranes, release of Ca(2+) and apoptosis induction. Moreover, the observed effects have led to exploration of medical applications, like the treatment of melanoma tumors (Nuccitelli et al., Biochem Biophys Res Commun 343:351-360, 2006). Pulsed electric fields allowing such effects usually range from several tens to a few hundred nanoseconds in duration and from a few to several tens of megavolts per meter in amplitude (Schoenbach et al., IEEE Trans Diel Elec Insul 14:1088-1109, 2007); however, the biological effects of subnanosecond pulses have been also investigated (Schoenbach et al., IEEE Trans Plasma Sci 36:414-422, 2008). The use of such a large variety of pulse parameters suggests that highly flexible pulse-generating systems, able to deliver wide ranges of pulse durations and amplitudes, are strongly required in order to explore effects and applications related to different exposure conditions. The Blumlein pulse-forming network is an often-employed circuit topology for the generation of high-voltage electric pulses with fixed pulse duration. An innovative modification to the Blumlein circuit has been recently devised which allows generation of pulses with variable amplitude, duration and polarity. Two different modified Blumlein pulse-generating systems are presented in this article, the first based on a coaxial cable configuration, matching microscopic slides as a pulse-delivery system, and the other based on microstrip transmission lines and designed to match cuvettes for the exposure of cell suspensions.
纳秒级强脉冲电场(nsPEFs)已被证明可在细胞内结构上诱导出依赖于电暴露条件(脉冲长度和幅度、重复频率和脉冲数)的有趣效应,这些效应在文献中被称为“生物电效应”(Schoenbach 等人,IEEE Trans Plasma Sci 30:293-300, 2002)。特别是,宽度小于细胞膜充电时间常数(对于哺乳动物细胞约为 100 ns)的脉冲可以穿透细胞并引发细胞内膜的通透性、Ca(2+)释放和凋亡诱导等效应。此外,观察到的效应促使人们探索医学应用,例如治疗黑色素瘤肿瘤(Nuccitelli 等人,Biochem Biophys Res Commun 343:351-360, 2006)。允许产生这种效应的脉冲电场通常持续时间从几十纳秒到几百纳秒,幅度从几十到几十兆伏/米(Schoenbach 等人,IEEE Trans Diel Elec Insul 14:1088-1109, 2007);然而,亚纳秒脉冲的生物效应也已被研究(Schoenbach 等人,IEEE Trans Plasma Sci 36:414-422, 2008)。使用如此广泛的脉冲参数表明,强烈需要能够提供广泛脉冲持续时间和幅度范围的高度灵活的脉冲产生系统,以便探索与不同暴露条件相关的效应和应用。Blumlein 脉冲形成网络是一种常用于产生具有固定脉冲持续时间的高压电脉冲的电路拓扑。最近设计了对 Blumlein 电路的创新修改,该修改允许产生具有可变幅度、持续时间和极性的脉冲。本文介绍了两种不同的改进型 Blumlein 脉冲产生系统,第一种基于同轴电缆配置,将显微镜载玻片作为脉冲传输系统,另一种基于微带传输线,旨在匹配用于细胞悬浮液暴露的培养皿。