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Çѱ¹Áö¹Ý°øÇÐȸ / v.23, no.4, 2007³â, pp.185-197
±Ù»çÀûÀÎ ÇØ¼®¹ý°ú À¯ÇÑ¿ä¼ÒÇØ¼®¿¡ ÀÇÇÑ Åͳκر«ÇÏÁß Æò°¡
( Assessment of Tunnel Collapse Load by Closed-Form Analytical Solution and Finite Element Analysis )
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ÇѰèÇØ¼®¹ýÀÎ »ó Çϰè¹ýÀº Á¡Âø¼º, Á¡Âø¼º-¸¶Âû¼º, ¸¶Âû¼ººÐ¸¸ °¡Áö´Â Áö¹Ý¿¡¼­ÀÇ ÁÖ·Î ¾èÀº Åͳο¡ ´ëÇÑ ¾ÈÁ¤¼ö¸¦ ±¸Çϱâ À§ÇØ ¹ßÀüµÇ¾î ¿Ô´Ù. ±×·¯³ª Á¡¼ºÀÌ ¾ø°í ¸¶Âû¼ººÐ¸¸ Á¸ÀçÇÏ´Â Áö¹Ý¿¡¼­ÀÇ ºñ±³Àû ±íÀº Åͳο¡ ´ëÇÑ ÀÌ·¯ÇÑ ÇØ¼®¹ýÀÇ ¿¬ÀåÀº ÇöÀç±îÁö ±× ¿¬±¸°¡ µå¹°°Ô ÁøÇàµÇ¾î¿Ô´Ù. µû¶ó¼­ º» ¿¬±¸´Â ÀÌ·¯ÇÑ »óȲ¿¡¼­ÀÇ Åͳκر«ÇÏÁßÀ» ±¸Çϱâ À§ÇÑ ±Ù»çÀûÀÎ ÇØ¼®¹ýÀ¸·Î ÀÀ·ÂºÒ¿¬¼ÓÀå¿¡ ±Ù°ÅÇÏ´Â Çϰè¹ý°ú µ¿Àû ÆÄ±«¸ÞÄ«´ÏÁò¿¡ ±Ù°ÅÇÏ´Â »ó°è¹ýÀ» °¢°¢ Á¦¾ÈÇÏ¿´´Ù. ÀÌ·¯ÇÑ ÇØ¼®¹ý¿¡ ÀÇÇÑ Åͳκر«ÇÏÁßÀº ¼öÄ¡ÇØ¼®°ú ±âÁ¸ÀÇ °æ°èÇØ¼®¹ý°ú ºñ±³µÇ¾úÀ¸¸ç ƯÈ÷, ÅͳΠ¼öÆòÃà »ó¿¡ À§Ä¡ÇÏ´Â À¯ÇÑÁö¹Ý¿ä¼Òµé¿¡ ´ëÇÑ À¯ÇÑ¿ä¼ÒÇØ¼® °á°ú¿Í Àß ÀÏÄ¡µÊÀ» º¸¿© ÁÖ¾ú´Ù.
Limit analysis of upper and lower bound solutions has been well developed to provide the stability numbers for shallow tunnels in cohesive soil ($c_u$ material), cohesive-frictional soil (c'-$phi$' material) and cohesionless soil ($phi$'material). However, an extension of these methods to relatively deep circular tunnels in the cohesionless soil has been explored rarely to date. For this reason, the closed-form analytical solutions including lower bound solution based on the stress discontinuity concept and upper bound solution based on the kinematically admissible failure mechanism were proposed for assessing tunnel collapse load in this study. Consequently, the tunnel collapse load from those solutions was compared with both the finite element analysis and the previous analytical bound solutions and shown to be in good agreement with the FE results, in particular with the FE soil elements located on the horizontal tunnel axis.
 
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Closed-form analytical solution;Cohesionless soil;Failure mechanism;Finite element analysis;Limit analysis;Stress discontinuity;Tunnel collapse load;
 
Çѱ¹Áö¹Ý°øÇÐȸ³í¹®Áý / v.23, no.4, 2007³â, pp.185-197
Çѱ¹Áö¹Ý°øÇÐȸ
ISSN : 1229-2427
UCI : G100:I100-KOI(KISTI1.1003/JNL.JAKO200718411577311)
¾ð¾î : ¿µ¾î
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