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图9-6 跃进山拼贴带及邻域三维岩石圈电性结构示意图
沿5条MT剖面已展示工区不同断面岩石圈电性结构(上节)。为更清楚、完整地表示工区不同地块体岩石圈电性结构特征,利用上述5条剖面资料和工区4个盆地分布,以及原来完成的HRMT剖面资料(刘国兴等,2006),MSGGT部分资料(杨宝俊等,1999),综合绘制工区三维电性结构图9-6。图9-6中Ⅰ-Ⅰ直线是对完达山地体和佳木斯地块拼贴带的简化,由图9-4可知,构成Ⅰ-Ⅰ线的L、W、B、S四点不在同一条直线上。Ⅱ-Ⅱ线与Ⅰ-Ⅰ线相似。另外表征各块体岩石圈电性结构特征的粗线(图例中地电结构特征线)是各块体特征的简化,所画的位置代表块内。四个盆地中仅勃利盆地位于佳木斯地块范围内,其余三个盆地的范围都跨不同地块。Ⅰ-Ⅰ与Ⅱ-Ⅱ两条简化线夹角已由图9-5上实际的约20°加以扩大,目的是能够表示清楚各块体独立特征。
由图9-6所表示的电性结构特征:①佳木斯地块、完达山地体和兴凯地块具有不同的电性结构特征。佳木斯地块以高阻块体为主;兴凯地块也存在高阻块体,但存在范围不大,自东而西逐渐加深加厚,到绥芬河市西一带(测点34、35/DB3)已达到深25~30km。完达山地体的岩石圈电性结构因该地块成因复杂性而形成电性的复杂特征。由完达山地体的东南面(Ⅱ线所在面)标绘的高阻埋深变化与西北面(Ⅰ线所在面)标绘的高阻块分布与埋深变化以及HR上宝清至饶河段高阻块分布可分析得到,完达山地体的南部在50km深以内具有较多的高阻块带,向北方向逐渐变少。②工作区的4个盆地分别位于不同地块体内,三江盆地位跨佳木斯地块和完达山地体,勃利盆地位于佳木斯地块内,鸡西盆地位跨佳木斯地块和完达山地体,虎林盆地位跨完达山地体和兴凯地块。根据工区岩石圈地电法结构图件(图9-6)和盆地地理位置可知,勃利盆地基底为高阻体;三江盆地西部,基底电性结构大致为两层,上部是厚20~30km的高阻带,下部是几十欧姆米的低阻区带,东部仅在深至10km之内存在零星高阻小块,其余为几十欧姆米的低阻区带;鸡西盆地的基底,上部存在零散高阻块体(深至25km之内),下部是巨厚几十欧姆米的低阻带;虎林盆地在兴凯地块范围内部分,基底基本是低阻特征(几十欧姆米),而位于完达山地体范围部分,基底内部多有高阻块体。③由Ⅰ线和Ⅱ线围起的完达山地体,其西南部分呈一“牛角”形状范围把佳木斯地块和兴凯地块分开,这是迄今为止所得到的三个地块体交会处最完整的图像。用一、二条剖面得不出空间位置,位场资料反演不到岩石圈尺度上的接触关系,本次用6条MT剖面和MSGGT研究结果,综合分析得到的图像具有相当大的可信性。同时自EN向WS方向,基底内零散分布的高阻块体增多,而北部仅存在稀少的高阻小块。佳木斯地块内,自南而北方向,高阻带分布逐渐减少,表明这一稳定地块的“高阻核”向北减薄。由MSGGT结果,在牡丹江市东的佳木斯地块范围内,电性呈现不到20km厚的浅部高阻带。表明佳木斯这一稳定地块的“高阻核”向南也在减薄。
几个地块岩石圈三维电性结构特征表明,佳木斯地块是稳定的,也基本均匀;兴凯地块也比较稳定,虽然均匀程度不大,但变化不剧烈;而完达山地体在岩石圈尺度下,上中部地壳分布的高阻块范围小而且零碎,之下是巨厚低阻层带,说明完达山地体均匀程度差,稳定性小。完达山地体中的高阻块带可能是西向俯冲的岩石圈岩片,以各种形态存在的低阻带可能是新生代喷发玄武岩所致。本文提供的5条MT剖面与完达山地体有关的部分,其岩石圈电性结构特征与HRMT剖面的宝清-饶河特征基本是一致的,所以由HRMT剖面所建立的地质解释模型也适用于本研究工区。只是在文献中地质解释模型指出的“直立低阻带”,在本文中电性结构中并不占多数。
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