MHD层流在核聚变反应堆等离子体面组件矩形通道中的传热

K. Takase, M. Z. Hasan
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引用次数: 3

摘要

为了研究横向磁场和表面热流的不均匀性对核聚变反应堆等离子体面组件(pfc)内MHD层流对流换热的影响,对等离子体面组件内MHD层流对流换热进行了数值分析。与前面分析的非mhd层流一样,面向等离子体(PF)侧的角落可能是热点区域;横向磁场的存在并不能在很大程度上缓解这种情况。表面热通量的不均匀性几乎抵消了PF侧Nu的增加。哈特曼数(Ha)为40时,中心Nu由6.9增加到23,而角落Nu由2.2增加到3.2,且热流密度均匀。但随着表面热通量不均匀程度的增加,中心Nu值迅速减小。然而,这种效应随着热通量不均匀性的增加而迅速饱和。在热流不均匀性较大的情况下,Nu随Ha的增加很小。在此条件下,等离子体面向侧中心Nu在Ha= 0时为2.8,Ha=16时为3.02,Ha=400时为3.4。在PF边角处,Nu对应的值分别为2.65、2.88、3.0。热通量高度不均匀时,Ha对入口长度的影响较小。
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Heat transfer in MHD laminar flow through a rectangular channel in the plasma facing components of fusion reactors
Convective heat transfer in MHD laminar flow through a square duct in the plasma facing components (PFCs) of fusion reactors is analyzed numerically to investigate the effects of a transverse magnetic field and the nonuniformity of surface heat flux. As in the case of non-MHD laminar flow, analyzed earlier, the corners of the plasma facing (PF) side are possible hot-spot areas; the presence of a transverse magnetic field does not alleviate this situation to any significant degree. The nonuniformity of surface heat flux nearly cancels this increase of Nu at the PF side. At Hartmann number (Ha) of 40, Nu at the center increases from 6.9 to 23, but at the corner from 2.2 to 3.2 only with uniform heat flux. But, as the extent of nonuniformity of surface heat flux increases, Nu at the center decreases rapidly. This effect, however, saturates rapidly with the increase of the nonuniformity of heat flux. The increase of Nu with Ha is very small for large nonuniformity of the heat flux. Under this condition, Nu at the center of the plasma facing side, is 2.8 at Ha=O, 3.02 at Ha=16 and 3.4 at Ha=400. At the corner of the PF side, the corresponding values of Nu are 2.65, 2.88, and 3.0, respectively. The effect of Ha on entry length is small for highly nonuniform heat flux.
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