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| | A rare microwave type Ⅳ burst was observed with Phoenix ⅠCorona-Radiospectrometer at Yunnan Observatory(1.42GHz、2.84GHz and 4.00GHz) from 08h31m to 09h41m UT on December 16,1988.The type Ⅳ burst was extended from the metric wave to the microwave bands. The burst long duration,high intensity and complex morphology.Five main peaks appeared from beginning to the end. A short period oscillation of 1.2 minutes and a long period oscillation of 12.5 minutes were observed.... | | 1988年12月16日世界时08h31min至09h41min,云南天文台PhoenixI日冕射电频谱仪(1.42GHz,2.84GHz,4.00GHz)收到一个罕见的微波Ⅳ型大爆发,爆发从米波Ⅳ型一直延伸到微波Ⅳ型,持续时间长,爆发强度大,爆发型别复杂。前后出现了五个主峰段,呈现出1.2min和1.25min的短周期和长周期振荡。在其中的两个频段上叠加有丰富的Spike辐射,根据爆发源区的扭斜磁场位形,我们采用磁俘获模型,计算了源区的有效温度,源区磁场随高度的变化,并算出了峰值频率在8.89GHz,其结果表明爆发是高能电子被磁场俘获,做回旋同步辐射所致 | | 文摘来源 | | There are very close relations between the radio moving type Ⅳbursts and coronal mass ejections.On the basis of the studies of radio moving type Ⅳ burst and of the physical condition of open magnetic field of CMEs,the physical conditions on the generation and ejection of CMEs are studied in this paper.When the magnetic flux is sudden injected and a large number of magnetic energy is released,the plasma in closed magnetic field of CMEs is accelerated.For this reason,the accelerated en... | | 射电Ⅳ型运动爆发同日冕物质抛射(CMEs)关系极为密切。本文基于对Ⅳ型运动爆发的研究以及CMEs开放场的物理条件,探讨了CMEs形成及抛射的物理条件。由于磁通量突然喷发,能量大量释放,在CME闭合场中的等离子体被加速,导致高能质子和高能电子被大磁环捕获。随着磁环内的热压P和磁压Pm的升高,当β>βT时磁环将炸裂,从而产生CMEs。抛射出的未离化的等离子体团将产生等离子体基波与谐波辐射。随着等离子体的不断离化,高能相对论电子绕开放磁场线作螺旋飞行,这时等离体辐射降到次要地位,回旋同步加速辐射上升到主导地位,这就是射电Ⅳ型运动爆发。如果离化的早,则在微波波段也能看到Ⅳ型运动爆发。这就是微波Ⅳ型爆发,也是微波Ⅳ型爆发罕见的原因。射电运动Ⅳ型爆发源就是日冕抛射的物质。 | | 文摘来源 | |   |
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