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Measuring Pressure In Warm Dense Tungsten Plasma Created In Plasma Filled Rod-Pinch Diodes

机译:在等离子体填充杆夹钉二极管中产生的温致密钨等离子体中的测量压力

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Pressure (or equivalently, energy density) measurements are crucial for determining, or testing models of, the equation of state (EOS) in warm, dense plasma. The plasma-filled rod pinch diode (PFRP)1 on the Gamble II generator creates tungsten plasma with parameters in the warm, dense regime: T ~ 30 eV, ρ ~ 0.7 g/cm3, Z ~ 18 and P ~ 16 Mb.2 The plasma is created by an intense ~ MeV electron beam that forms at the tip of a 1-mm diameter tungsten rod tapered over 15 mm to a sharp point. The beam develops after an injected plasma conducts the generator current like a short circuit for 50 ns while the current increases to 600 kA, then the PFRP impedance increases and an ~ MeV, 500 kA electron beam rapidly deposits energy at the end of the tapered rod. The energetic electrons that heat the tungsten-rod plasma also produce hard x-ray emission. The time-dependent axial and radial shapes of the x-ray distribution are diagnosed using an array of PIN diodes behind rolled edges. The x-ray distributions are assumed to match the mass distribution, an assumption to be tested using Monte-Carlo calculations. Using this assumption, the axial and radial x-ray distributions are converted to mass distributions, since the dimensions of the solid rod tip are known. The evolution of the mass distributions is determined by the internal pressure (and to a lesser extent by the external magnetic pressure). The radial distributions can be represented by Gaussian functions, and a self-similar equation of motion determines the pressure. The pressure calculated this way is many times greater than the kinetic pressure (1+Z)nkT. This could be the result of ionion repulsion in this unconventional plasma, in which the number of electrons in a Debye sphere is of order unity. Independent measurements of ionization (Z) and temperature imply the coulomb coupling factor is also much greater than one, supporting the importance of ion-ion coupling causing high internal pressure.
机译:压力(或等效地,能量密度)测量对于确定或测试型号的型号(EOS)的模型至关重要,该模型(EOS)中的温暖致密等离子体的等式。等离子体填充杆PINCH二极管(PFRP) 1 在赌博II发电机上,在温暖的,致密的状态下使用参数产生钨等离子体:T〜30eV,ρ〜0.7g / cm 3 ,z〜18和p〜16 mb。 2 等离子体由强烈的〜MEV电子束产生,该束形成在1mm直径钨杆的尖端上,锥形超过15mm到尖锐点。在喷射等离子体在电流增加到600ka的情况下,光束在喷射等离子体如短路上传导发生器电流,然后将PFRP阻抗增加和〜MEV,500ka电子束在锥形杆的末端迅速沉积能量。 。加热钨杆等离子体的能量电子也产生硬X射线发射。使用滚动边缘后面的销钉阵列诊断诊断X射线分布的时间依赖性轴向和径向形状。假设X射线分布匹配质量分布,使用Monte-Carlo计算进行测试的假设。使用这种假设,轴向和径向X射线分布被转换为质量分布,因为固体杆尖端的尺寸是已知的。质量分布的演变由内部压力(通过外部磁力较小)确定。径向分布可以由高斯函数表示,并且自类似的运动方程决定了压力。这种方式计算的压力比动力学压力(1 + Z)NKT大量大量大。这可能是这种非传统等离子体中电离的结果,其中德拜斯球中的电子的数量是统一的。离子化(Z)和温度的独立测量意味着库仑耦合因子也大于1,支持离子离子偶联的重要性,导致高内部压力。

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