¼ÒÃÄË¡¿Í¡¡ÊªÍýõºº³Ø²ñ
Âè127²ó(Ê¿À®24ǯÅÙ½©µ¨)³Ø½Ñ¹Ö±é²ñ


Å纬¸©Àи«¥¼¥ª¥é¥¤¥È¹Û¾²¤Ë¤ª¤±¤ëAMTÄ´ºº

¹Ö±éÍ×»Ý(ÏÂʸ)
Àи«¹Û¾²¡ÊÅ纬¸©ÂçÅĻԸ޽½Ìԡˤϡ¤Âè»°µªÃæ¿·À¤¤Î¥°¥ê¡¼¥ó¡¦¥¿¥ÕÃÏ°è¤ËæõÂÛ¤¹¤ë¹õ¹Û·¿¹Û¾²¤Ç¤¢¤ë¡¥¤«¤Ä¤Æ¤Ï±ô¡¤°¡±ô¡¤Æ¼¤Ê¤É¤ò»º½Ð¤¹¤ë¹Û»³¤Ç¤¢¤Ã¤¿¤¬¡¤¸½ºß¤ÏήÌæ´ä¼Á¶Å³¥´äÃæ¤Î¥¼¥ª¥é¥¤¥È¤¬¼ç¤ËºÎ·¡¤µ¤ì¤Æ¤¤¤ë¡¥¥¼¥ª¥é¥¤¥È¤ÎÉʼÁ¤ò·×¤ë¥Ñ¥é¥á¡¼¥¿¤Î°ì¤Ä¤Ë±ö´ðÃÖ´¹ÍÆÎ̤¬¤¢¤ë¤¬¡¤ÈæÄñ¹³¤È¤ÎÍ­°Õ¤Ê´ØÏ¢À­¤òÌÀ¤é¤«¤Ë¤Ê¤ì¤Ð¡¤»î¿í¤Ë¤è¤é¤º¤ËÅŵ¤Ãµºº¤äÅż§Ãµºº¤Ë¤è¤ëõ¹Û¤¬²Äǽ¤Ë¤Ê¤ë¡¥Ëܸ¦µæ¤Ç¤Ï¡¤Àи«¹Û¾²¥¨¥ê¥¢¤òËÌËÌÀ¾-ÆîÆîÅì¤Ë²£ÃǤ¹¤ë¬Àþ¡ÊŤµÌó700m¡Ë¤ÇAMTˡõºº¤ò¼Â»Ü¤·¤¿¡¥2¼¡¸µÈæÄñ¹³¹½Â¤¤ò¿äÄꤷ¤¿¤È¤³¤í¡¤ÃϼÁ¹½Â¤¤ÎÆÃħ¤È°ìÃפ·¤Æ¤ª¤ê¡¤­¡¹õ¹Û¹Û¾²¤äÀйѹ۾²¡¤ÌÖ¾õ¹ÛÀ÷¹ÛÂΤÎʬÉÛ¤¹¤ëÎΰè¤Ç¤Ï¿ôOhm-mÄøÅÙ¤ÎÄãÈæÄñ¹³Ãͤò¼¨¤¹¤³¤È¡¤­¢Î®Ìæ´ä¼Á¶Å³¥´ä¤ÎÈæÄñ¹³¤ÏÌó10¦¸m¤À¤¬¡¤Ç®¿åÊѼÁ¤Î±Æ¶Á¤¬Â礭¤ÊÎΰè¤Ç¤ÏÌó20¦¸mÄøÅ٤Ȥ鷺¤«¤Ë°ã¤¤¤¬¸«¤é¤ì¡¤¤½¤ÎÎΰ褬¥¼¥ª¥é¥¤¥È¹Û¾²¤Î³«È¯Îΰè¤È¤è¤¯°ìÃפ¹¤ë¤³¤È¡¤¤Ê¤É¤ÎÃ諤¬ÆÀ¤é¤ì¤¿¡¥

¹Ö±éÍ×»Ý(±Ñʸ)
The Iwami mine is known as the kuroko-type deposit in the "green tuff region" of the Southwest Japan, where the zinc-lead-copper ore had been produced during the period of 1966 to 1984. Presently, the development of zeolite deposit has been conducted. To investigate the relationship between the resistivity structure and the distribution and its grade of zeolite deposit, electromagnetic studies have been carried out in the Iwami mine area. In this study, an audio-frequency MT investigation was conducted in the kuroko and zeolite deposits. The estimated resistivity distributions by two-dimensional inversion show good correlation with the geological features obtained by the drillings. The location of extremely conductive zone (around a few Ohm-m) is consistent with the kuroko deposit and the border of rhyolitic rocks, indicating the existence of zinc-lead-copper ore and gypsum deposit. The resistivity of rhyolitic tuff layer is about 10 Ohm-m, however, slightly resistive (about 20 Ohm-m) around the border of kuroko deposit, where is overlapping to the zeolite mining zone. The hydrothermal alteration might cause the resistivity change in the rhyolitic tuff layer.