Identifikasi Struktur Bawah Permukaan Tuff ring Dengan Menggunakan Metode Geolistrik Konfigurasi Dipol-Dipol

Gregorio Arikalang, Ferdy Ferdy, Guntur Pasau, G. Tamuntuan
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Abstract

Tuff ring Geoelectric Resistivity Dipole-dipole The research has been done to identify the subsurface structure of the tuff ring in plantation area Mahawu using geoelectric method of dipole-dipole configuration.It has been divided into two lines measuring with the length of 480 m for each lines, one space 10 m between the electrodes and the line 2 has 240 m length with spaces 5 m between electrodes. The data was obtained and processed using software RES2DINV to get an image of the structure below the tuff ring into two dimensions. The results of data processing shown an image of resistivitas beneath the surface on the line 1. In general, it can be seen that the resistivitas beneath the surface line 1 is dominated by resistivitas more than 300 Ωm (purple colour image). Especially in meter 250-260 and meter 280-290, there are two zones with resistivitas value that is relatively small at less than 50 m. While on the line two, the resistivitas value is less than 60 Ωm (blue and green coloured zone ) that form patterns extend from the maximum depth to the surface, visible form a funnel/the cust from a depth of about 40 m (under electrodes to 18 or in meters to 90) To the surface (under electrodes 25 – 33 or in meters 125 -165) is directed to the northwest-southeast with the angle of inclination of about 40°42°and the resistivitas pattern elongated funnelshaped by contrast it also limited by the high resistivitas (> 300 Ωm) which is a structure with high density and less conductive. Which is interpreted as a former eruption channel preatomagmatic.
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使用校准二极管配置找出土夫环的地下结构
利用偶极-偶极组态地电方法,对马哈坞人工区凝灰岩环的地下结构进行了识别研究。它被分成两条线,每条线长480米,电极之间间隔10米,2号线长240米,电极之间间隔5米。利用RES2DINV软件获取数据并进行处理,得到凝灰岩环下结构的二维图像。数据处理的结果显示了1号线表面下的电阻率图像。一般情况下,可以看到地表1线以下的电阻率以300以上的电阻率为主Ωm(紫色图像)。特别是在250 ~ 260米和280 ~ 290米,在50m以下有两个电阻率值相对较小的区域。而在第二线上,电阻率值小于60 Ωm(蓝绿带),形成的图案从最大深度延伸到表面,可见形成漏斗/从深度约40米(电极下至18米或在米至90米)到表面(电极下25 - 33米或在米125 -165米)被引导到西北-东南,倾角约为40°42°,电阻率模式拉长漏斗形相比之下,它也受到高电阻率(> 300 Ωm)的限制,这是一个高密度和低导电性的结构。这被解释为一个前喷发通道。
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审稿时长
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