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托卡马克等离子体中的电子回旋波电流驱动 总被引:7,自引:1,他引:6
通过将波迹方程与相对论情况下的完全Fokker-Planck方程联合进行求解,研究了寻常波基频电子回旋波从托卡马克等离子体中平面弱场侧发射时的电流驱动。数值结果表明:随着等离子体电子密度、温度的提高, 功率沉积和电流分布的位置将向等离子体的边缘方向偏移,并且产生的总的驱动电流随之减小;入射波极向发射角和环向发射角度的改变对功率沉积、电流分布及其大小产生明显的影响。 相似文献
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在给定的等离子体总电流和中心电流密度条件下,数值求解平衡方程,求出不同拉长比和三角形变因子的托卡马克等离子体温度、密度、磁场分布,然后通过求解波迹方程和Fokker-Planck方程,分别计算这些位形下的电子回旋波波迹和电流驱动.结果表明:电子回旋波X模从顶部发射时,随着拉长比的增大,波迹会向弱场侧偏移.电子回旋波X模从弱场侧发射时,电子回旋波在等离子体中传播沉积的功率份额随着拉长比的增大而增加,驱动电流位置随着三角形变因子的增大向等离子体中心移动.驱动电流位置随环向和极向发射角的减小向中心移动,对应的电流密度峰值也变大. 相似文献
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在考虑到捕获电子效应的情况下,对求解二维Fokker-Planck方程的编程进行了反弹平均的修改,使用了交替方向隐式法来求解方程。分析和计算了在不同扩散系数和不同共振区间的情况下,捕获电子效应对驱动电流的影响。结果显示:随着逆纵横比的增加驱动电流密度有明显的下降,在磁轴附近捕获电子效应对电流驱动影响很小;提高波功率并不能很好的改善捕获电子效应对电流驱动的影响;右移共振区间提高共振电子的速度,也不能很好的改善捕获电子效应对电流驱动的影响。所得结果与理论分析基本一致。 相似文献
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在考虑到捕获电子效应的情况下,对求解二维Fokker-Planck方程的编程进行了反弹平均的修改,使用了交替方向隐式法来求解方程。分析和计算了在不同扩散系数和不同共振区间的情况下,捕获电子效应对驱动电流的影响。结果显示:随着逆纵横比的增加驱动电流密度有明显的下降,在磁轴附近捕获电子效应对电流驱动影响很小;提高波功率并不能很好的改善捕获电子效应对电流驱动的影响;右移共振区间提高共振电子的速度,也不能很好的改善捕获电子效应对电流驱动的影响。所得结果与理论分析基本一致。 相似文献
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在给定等离子体密度分布下,从电子、离子的能量方程出发,根据不同运行模式下等离子体的热传导率不同,分别求出了中心负剪切模式,常规剪切H模式和L模式下的等离子体温度分布,然后通过求解波迹方程与相对论情况下的Fokker-Planck方程,分别计算了这些模式下的电子回旋波电流驱动和波功率沉积.得到在中心负剪切下,驱动电流最大,驱动效率最高,功率沉积和电流分布区间跨度大;在常规剪切H模式下,驱动电流较小,分布区间跨度比较窄,驱动效率相对较低;在常规剪切L模式,驱动电流效率最低,分布区间跨度也非常集中.
关键词:
托卡马克
电子回旋波电流驱动
中心负剪切
常规剪切 相似文献
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本文探索波驱动等离子体电流的一种新机制,称之为随机驱动效应。在相干波与磁化等离子体相互作用的系统中,当波的强度超过某个阈值时,速度空间中的一些共振区将互相重迭。共振区的重迭可导致粒子的随机运动,引起速度空间中的扩散现象。如果在电子平行于磁场方向的速度分布中,这种重迭区是不对称的,这样,就可驱动纵向等离子体电流。
关键词: 相似文献
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利用不同加热机制产生的超热电子所导致的相干渡越辐射(CTR)在谐波分量强度比上的不同,给出了区分飞秒激光等离子体相互作用产生超热电子过程中的主要与次要加热机制的一种可能方法.得到了加热周期不同的加热机制所产生超热电子的比例与CTR谐波分量的二倍频和一倍频的强度比之间的具体关系式.如果在实验上测到此谐波分量强度比,就可以推出不同加热机制在加热过程中所起作用的大致比例关系.另外,CTR谐波分量的强度比还与超热电子的温度、实验上所使用靶的厚度有一定依赖关系,对此作了较为详细的讨论.
关键词:
相干渡越辐射
超热电子
加热机制 相似文献
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W. Potzel J. Moser Ulrike Potzel F. J. Litterst G. M. Kalvius J. Gal M. Boge J. Chappert J. Spirlet 《Hyperfine Interactions》1987,34(1-4):391-405
Due to the wider radial extent of 5f electrons when compared to their 4f counterparts, intermetallics of the light actinides show a broad spectrum of magnetic properties ranging from the localized magnetism of the lanthanides to the itinerant magnetism often found in transition metal compounds. One parameter which strongly influences the magnetic character of the compound is the actinide-actinide separation which can experimentally be varied by the application of high pressure. The question of 5f electron delocalization will be reviewed with respect to Moesshauer high pressure data on NpCo2si2, NpAl2, NpOs2 and new results will be presented of NpAs. The connection of hyperfine parameters with results of X-ray diffraction studies will be discussed.Work supported by the Bundesministerium für Forschung und Technologie, Federal Republic of Germany 相似文献
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O. Hartmann E. Karlsson R. Wäppling J. Chappert A. Yaouanc L. Asch G. M. Kalvius 《Hyperfine Interactions》1984,18(1-4):491-496
Transverse fieldSR measurements in the paramagnetic region on polycrystalline samples of CeAl2, NdAl2, PrAl2, GdAl2, ErAl2, HoAl2, DyAl2 and TmAl2 are reported. We have observed increased damping rate and frequency shifts of the muon precession signal asT
c is approached from above. The shifts are linear in applied magnetic field, while the damping rates are more complicated functions of magnetic field strength and temperature.We interpret the damping as being partly due to inhomogeneous broadening proportional to the magnetic susceptibility, and partly due to apparent slowing down of RE spin fluctuations. These slow fluctuations are ascribed to the existence of correlations between the RE spins also at temperatures well aboveT
c. The variations of shifts and damping rates within the series of REAl2 compounds will be discussed. 相似文献
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A. G. Leonov D. I. Chekhov A. N. Starostin 《Journal of Experimental and Theoretical Physics》1997,84(4):703-715
An experimental investigation and numerical simulation of resonant laser breakdown are performed. As a result, quantitative
agreement between the experimental data on the parameters of a dense resonant plasma (the electron density and the electron
temperature) and the results of calculations in the range of detunings of the laser radiation from resonance Δλ>2–2.5 nm, in which the spatial instability of the intense resonant laser beam and the absorption of radiation are minimal,
is obtained for the first time. It is shown that the previously proposed mechanism of resonant breakdown associated with laser-induced
associative ionization introduces only a small correction to the final extent of ionization of the resonant plasma and scarcely
alters its temperature. The influence of quantum stimulated inverse bremsstrahlung processes, which are usually described
as collisions of the second kind in the resonance case, on the energy gain by electrons is analyzed for the first time in
reference to specific experimental findings. The numerical calculations show that at detunings of the order of the Rabi frequency,
the mechanism by which electrons gain energy through the resonant system does not reduce to collisions of the second kind
and can significantly increase the density of the resonant plasma. However, in this range of detunings the laser beam is still
strongly perturbed by instability processes, precluding a proper comparison of the theory with experiment. At large Δλ the classical and quantum cases differ from one another only slightly, and the values of N
e calculated for both mechanisms lie within the measurement error.
Zh. éksp. Teor. Fiz. 111, 1274–1296 (April 1997) 相似文献
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L. Rebohle T. Gebel J. von Borany W. Skorupa M. Helm D. Pacifici G. Franzò F. Priolo 《Applied physics. B, Lasers and optics》2002,74(1):53-56
Si-based light emitters will be a key element of future optoelectronics. One of the most promising approaches is Ge implantation
into thin SiO2 films on crystalline Si. This system exhibits a strong violet electroluminescence with a power efficiency up to 0.5% [18],
but the mechanism of electrical excitation is not yet fully understood. In this paper the electrical excitation of the luminescence
centers is investigated by means of electrical and electroluminescence transient measurements. It is found that the most probable
way to excite luminescence centers is the impact excitation by hot electrons. Whereas the injection is explained by trap-assisted
tunneling of electrons from the substrate into the oxide, the electrons will be transported via traps or in the SiO2 conduction band. Furthermore, the electroluminescence rise and decay time is estimated to be of the order of 100 μs.
Received: 26 September 2001 / Published online: 29 November 2001 相似文献