¶óÆæÆ®¦¢Ä«Æä¦¢ºí·Î±×¦¢´õº¸±â
¾ÆÄ«µ¥¹Ì Ȩ ¸í»çƯ°­ ´ëÇבּ¸½Ç޹æ Á¶°æ½Ç¹« µ¿¿µ»ó°­ÀÇ Çѱ¹ÀÇ ÀüÅëÁ¤¿ø ÇÐȸº° ³í¹®
ÇÐȸº° ³í¹®

Çѱ¹°Ç¼³°ü¸®ÇÐȸ
Çѱ¹°ÇÃà½Ã°øÇÐȸ
Çѱ¹µµ·ÎÇÐȸ
Çѱ¹»ý¹°È¯°æÁ¶ÀýÇÐȸ
Çѱ¹»ýÅÂÇÐȸ
Çѱ¹¼öÀÚ¿øÇÐȸ
Çѱ¹½Ä¹°ÇÐȸ
Çѱ¹½Ç³»µðÀÚÀÎÇÐȸ
Çѱ¹ÀÚ¿ø½Ä¹°ÇÐȸ
Çѱ¹ÀܵðÇÐȸ
Çѱ¹Á¶°æÇÐȸ
Çѱ¹Áö¹Ý°øÇÐȸ
Çѱ¹ÇÏõȣ¼öÇÐȸ
Çѱ¹È¯°æ»ý¹°ÇÐȸ
Çѱ¹È¯°æ»ýÅÂÇÐȸ

Çѱ¹Áö¹Ý°øÇÐȸ / v.27, no.5, 2011³â, pp.85-92
Áö¹Ý-¸»¶Ò ½Ã½ºÅÛ¿¡ ´ëÇÑ 3Â÷¿ø µ¿Àû ¼öÄ¡ ¸ðµ¨¸µ ±â¹ý °³¹ß
( Development of 3D Dynamic Numerical Simulation Method on a Soil-Pile System )
±è¼ºÈ¯;³ª¼±È«;ÇÑÁøÅÂ;±è¼º·Ä;¼±Ã¢±¹;±è¸í¸ð; ¼­¿ï´ëÇб³ °Ç¼³È¯°æ°øÇкÎ;(ÁÖ) °ÇÈ­, ±â¼ú¿¬±¸¼Ò;¼­¿ï´ëÇб³ °Ç¼³È¯°æ°øÇкÎ;µ¿¾Æ´ëÇб³ °ø°ú´ëÇÐ Åä¸ñ°øÇаú;Çѱ¹ÁöÁúÀÚ¿ø¿¬±¸¿ø ÁöÁø¿¬±¸¼¾ÅÍ;¼­¿ï´ëÇб³ °Ç¼³È¯°æ°øÇкÎ;
 
ÃÊ ·Ï
¸»¶ÒÀÇ µ¿Àû °Åµ¿Àº Áö¹Ý-¸»¶ÒÀÇ µ¿Àû»óÈ£ÀÛ¿ë, Áö¹ÝÀÇ ºñ¼±Çü¼º, Áö¹Ý-¸»¶Ò ½Ã½ºÅÛÀÇ °øÁø Çö»ó µî ¸¹Àº ¿ä¼Ò°¡ »óÈ£ ÀÛ¿ëÀ» ÇϹǷΠ¸Å¿ì º¹ÀâÇÏ´Ù. ±×·¯¹Ç·Î, ¸»¶ÒÀÇ µ¿Àû °Åµ¿À» ¼öÄ¡ÇØ¼®À¸·Î Á¤È®È÷ ¸ð»çÇÏ·Á¸é ¸¹Àº ³ë·Â°ú ½Ã°£ÀÌ ÇÊ¿äÇÏ´Ù. º» ¿¬±¸¿¡¼­´Â ±âÁ¸ÀÇ ¹ü¿ë ¼öÄ¡ÇØ¼® ÇÁ·Î±×·¥ÀÎ FLAC 3D¸¦ Ȱ¿ëÇϸ鼭µµ ÇØ¼®½Ã°£À» Å©°Ô °¨¼Ò ½Ãų ¼ö ÀÖ´Â »õ·Î¿î ¸ðµ¨¸µ ±â¹ýÀ» °³¹ßÇÏ¿´´Ù. º» ±â¹ýÀº Àüü ÇØ¼® ¿µ¿ªÀ» ±Ù¿ª Áö¹Ý°ú ¿ø¿ª Áö¹ÝÀ¸·Î ³ª´©°í Áö¹Ý-¸»¶Ò µ¿Àû»óÈ£ÀÛ¿ë¿¡ ¿µÇâÀ» ¹ÞÁö ¾Ê´Â ¿ø¿ª Áö¹ÝÀ» ¿ä¼Ò¸ÁÀ¸·Î ¸ðµ¨¸µÇÏ´Â ´ë½Å ¿ø¿ª Áö¹ÝÀÇ Áö¹Ý ¿îµ¿ ½Ã°£ÀÌ·ÂÀ» ±Ù¿ª Áö¹ÝÀÇ °æ°è Á¶°Ç¿¡ ÀÔ·Â ÇÏÁßÀ¸·Î Àû¿ëÇÏ´Â ±â¹ýÀÌ´Ù. ÀÌ ¼öÄ¡ ¸ðµ¨¸µ¿¡¼­ ÁöÁøÆÄÀÇ °­µµ°¡ Ŭ ¶§ ÀϾ´Â Áö¹ÝÀÇ ºñ¼±Çü °Åµ¿À» ¸ð»çÇϱâ À§ÇÏ¿© ÀÌ·Â °¨¼è ¸ðµ¨À» ÀÌ¿ëÇÏ¿© Á¢¼± ź¼º °è¼ö¸¦ Àü´Ü º¯Çü·üÀÇ ÇÔ¼ö °ªÀ¸·Î ÀÔ·ÂÇÏ¿´À¸¸ç, Áö¹Ý°ú ¸»¶Ò »çÀÌÀÇ ºÐ¸® Çö»óÀ» ¸ð»çÇϱâ À§ÇÏ¿© Áö¹Ý-¸»¶Ò °æ°è ¿ä¼Ò¸¦ µµÀÔÇÏ¿´´Ù. ÀÌ ¹æ¹ýÀº ±âÁ¸ÀÇ ¹æ¹ý°ú ºñ±³ÇÏ¿© ÇØ¼® °á°úÀÇ Á¤È®¼ºÀ» À¯ÁöÇϸ鼭 ÇØ¼® ½Ã°£À» 1/3·Î °¨¼Ò½ÃÄ×´Ù. Á¦¾ÈµÈ ¼öÄ¡ÇØ¼® ¹æ¹ýÀ¸·Î ¿¹ÃøÇÑ 1g Áøµ¿´ë ¸ðÇü ½ÇÇèÀÇ ¿øÇü °Åµ¿Àº ¿øÇüÀ¸·Î ȯ»êÇÑ ¸ðÇü ½ÇÇè °á°ú¿Í À¯»çÇÏ°Ô ³ªÅ¸³µ´Ù.
The dynamic behavior of piles becomes very complex due to soil-pile dynamic interaction, soil non-linearity, resonance phenomena of soil-pile system and so on. Therefore, the proper numerical simulation of the pile behavior needs much effort and calculation time. In this research, a new modeling method, which can be applied to the conventional finite difference analysis program FLAC 3D, was developed to reduce the calculation time. The soil domain in this method is divided into a near-field region and a far-field region, which is not influenced by the soil-pile dynamic interaction. Then, the ground motion of the far-field is applied to the boundaries of the near-field instead of modeling the far-field region as finite meshes. In addition, the soil non-linearity behavior is modeled by using the hysteretic damping model, which determines the soil tangent modulus as a function of shear strain and the interface element was applied to simulate the separation and slip between the soil and pile. The proposed method reduced the calculation time by as much as one third compared with a usual modeling method and maintained the accuracy of the calculated results. The calculated results by the proposed method showed a good agreement with the prototype pile behavior, which was obtained by applying a similitude law to the 1-g shaking table test results.
 
Ű¿öµå
1 g shaking table tests;Dynamic soil-pile interaction;Finite difference method;Numerical simulation;
 
Çѱ¹Áö¹Ý°øÇÐȸ³í¹®Áý / v.27, no.5, 2011³â, pp.85-92
Çѱ¹Áö¹Ý°øÇÐȸ
ISSN : 1229-2427
UCI : G100:I100-KOI(KISTI1.1003/JNL.JAKO201121559391886)
¾ð¾î : Çѱ¹¾î
³í¹® Á¦°ø : KISTI Çѱ¹°úÇбâ¼úÁ¤º¸¿¬±¸¿ø
¸ñ·Ïº¸±â
ȸ»ç¼Ò°³ ±¤°í¾È³» ÀÌ¿ë¾à°ü °³ÀÎÁ¤º¸Ãë±Þ¹æÄ§ Ã¥ÀÓÀÇ ÇѰè¿Í ¹ýÀû°íÁö À̸ÞÀÏÁÖ¼Ò ¹«´Ü¼öÁý °ÅºÎ °í°´¼¾ÅÍ
   

ÇÏÀ§¹è³ÊÀ̵¿