为了提高积云模式对雷暴云内电过程的模拟能力,将Mansell提出的放电参数化方案在起始击穿阈值和闪电通道感应电荷的分配过程上进行改进,耦合了已有的三维强风暴动力—电耦合模式中。对STEPS(Severe Thunderstorm Electrification and Pr...为了提高积云模式对雷暴云内电过程的模拟能力,将Mansell提出的放电参数化方案在起始击穿阈值和闪电通道感应电荷的分配过程上进行改进,耦合了已有的三维强风暴动力—电耦合模式中。对STEPS(Severe Thunderstorm Electrification and Precipitation Study)试验中一次雷暴个例以及对中纬度地区理想雷暴个例的模拟表明,引入了新放电参数化方案的模式模拟出闪电在发展特性和几何结构上和观测结果有较好的一致性。模拟结果还表明:闪电的类型与极性取决于背景电荷结构以及闪电的起始位置,只有底部存在正电荷堆时才会产生负地闪,且负地闪的起始点均具有较高的负电势。闪电通道上感应电荷的沉降会改变通道附近水成物粒子上携带的电荷,这对雷暴云内复杂电荷结构的形成有重要作用。经统计,模拟的地闪和云闪通道的分形维数平均值分别为1.47和1.69。对起始击穿阈值的敏感性试验表明,随着起始击穿阈值的增大,首次闪电时间会向后推迟,当采用逃逸击穿时首次闪电产生的时间最早;闪电数量随起始击穿阈值的增大而减少;当使用固定击穿阈值(100,150和200 k V)时得到的云地闪比均小于使用逃逸击穿时得到的云地闪比,使用逃逸击穿时得到的云地闪比与观测结果最为接近。展开更多
Intracloud (IC) lightning flashes have been simulated in fine resolution (12.5 m) by using a bidirectional stochastic lightning parameterization scheme within 2-dimensional domain. The simu-lated results show that the...Intracloud (IC) lightning flashes have been simulated in fine resolution (12.5 m) by using a bidirectional stochastic lightning parameterization scheme within 2-dimensional domain. The simu-lated results show that the IC flashes have a bilevel channel structure and the altitudes of the hori-zontal channels are at the same heights of potential wells, which are supported by the previous VHF source observations and balloon soundings of electric field profile in the thundercloud. Further con-clusions are: (1) After an IC flash is initiated near the boundary between positve and nagetive charge zone, the negative (or positive) leader tends to propagate into the positive (or negative) charge zone. Both types of positive and negative IC flashes have been reproduced and their polarity depends on the up and down disposition of the positive and negative charge regions. (2) The extension range of leaders is correlative with the cloud charge distribution. The leader is possible to extend through the inverted charge region all over where it is extending, but keeps away from the isolated charge area of the same polarity. (3) The channel structures also depend on the electric potential distributions in the thundercloud. Before propagating into the central area of potential wells, the leader tends to extend along the direction with the maximum of potential gradient. Once extending away from the center of potential wells, the leader tends to extend along the direction with the slowest potential change. (4) The IC flash channels have the fractal feature with fractal dimension 1.45 before leaders pass through the central area of charge regions. The exponent decreases rapidly once leaders extend into the low-density charge regions. (5) The induced charges of opposite polarity are deposited in the leader channels within preexisting positive and negative charge regions during IC flash discharges. This causes a new and complicated charge distribution in the thundercloud, and the potential extremum drops from 200 to 20 Mv when the IC flash terminates.展开更多
文摘为了提高积云模式对雷暴云内电过程的模拟能力,将Mansell提出的放电参数化方案在起始击穿阈值和闪电通道感应电荷的分配过程上进行改进,耦合了已有的三维强风暴动力—电耦合模式中。对STEPS(Severe Thunderstorm Electrification and Precipitation Study)试验中一次雷暴个例以及对中纬度地区理想雷暴个例的模拟表明,引入了新放电参数化方案的模式模拟出闪电在发展特性和几何结构上和观测结果有较好的一致性。模拟结果还表明:闪电的类型与极性取决于背景电荷结构以及闪电的起始位置,只有底部存在正电荷堆时才会产生负地闪,且负地闪的起始点均具有较高的负电势。闪电通道上感应电荷的沉降会改变通道附近水成物粒子上携带的电荷,这对雷暴云内复杂电荷结构的形成有重要作用。经统计,模拟的地闪和云闪通道的分形维数平均值分别为1.47和1.69。对起始击穿阈值的敏感性试验表明,随着起始击穿阈值的增大,首次闪电时间会向后推迟,当采用逃逸击穿时首次闪电产生的时间最早;闪电数量随起始击穿阈值的增大而减少;当使用固定击穿阈值(100,150和200 k V)时得到的云地闪比均小于使用逃逸击穿时得到的云地闪比,使用逃逸击穿时得到的云地闪比与观测结果最为接近。
基金supported by the National Natural Science Foundation of China(Grant Nos.40205002 and 40475004).
文摘Intracloud (IC) lightning flashes have been simulated in fine resolution (12.5 m) by using a bidirectional stochastic lightning parameterization scheme within 2-dimensional domain. The simu-lated results show that the IC flashes have a bilevel channel structure and the altitudes of the hori-zontal channels are at the same heights of potential wells, which are supported by the previous VHF source observations and balloon soundings of electric field profile in the thundercloud. Further con-clusions are: (1) After an IC flash is initiated near the boundary between positve and nagetive charge zone, the negative (or positive) leader tends to propagate into the positive (or negative) charge zone. Both types of positive and negative IC flashes have been reproduced and their polarity depends on the up and down disposition of the positive and negative charge regions. (2) The extension range of leaders is correlative with the cloud charge distribution. The leader is possible to extend through the inverted charge region all over where it is extending, but keeps away from the isolated charge area of the same polarity. (3) The channel structures also depend on the electric potential distributions in the thundercloud. Before propagating into the central area of potential wells, the leader tends to extend along the direction with the maximum of potential gradient. Once extending away from the center of potential wells, the leader tends to extend along the direction with the slowest potential change. (4) The IC flash channels have the fractal feature with fractal dimension 1.45 before leaders pass through the central area of charge regions. The exponent decreases rapidly once leaders extend into the low-density charge regions. (5) The induced charges of opposite polarity are deposited in the leader channels within preexisting positive and negative charge regions during IC flash discharges. This causes a new and complicated charge distribution in the thundercloud, and the potential extremum drops from 200 to 20 Mv when the IC flash terminates.
