|
|
|
Çѱ¹Áö¹Ý°øÇÐȸ / v.21, no.8, 2005³â, pp.27-35
|
¾×»óÈ ÇØ¼®À» À§ÇÑ °£´ÜÇÑ ±¸¼º¸ðµ¨
( A Simple Constitutive Model for Soil Liquefaction Analysis ) |
| ¹Ú¼º½Ä;±è¿µ¼ö;;±è´ë¸¸; ºê¸®Æ¼½Ã ÄÝ·Òºñ¾Æ´ëÇб³ Åä¸ñ°øÇаú;°æºÏ´ëÇб³ °ø°ú´ëÇÐ Åä¸ñ°øÇаú;ºê¸®Æ¼½Ã ÄÝ·Òºñ¾Æ´ëÇб³ Åä¸ñ°øÇаú;°æºÏ´ëÇб³ °ø°ú´ëÇÐ Åä¸ñ°øÇаú;
|
|
|
 |
|
| |
| ÃÊ ·Ï |
| ¾×»óÈ¿¡ µû¸¥ Áö¹ÝÀÇ °úµµÇÑ º¯ÇüÀ¸·Î ÀÎÇÑ ÇÇÇØ°¡ ÀÚÁÖ ¹ß»ýµÇ°í ÀÖ´Ù. ±×¿¡ µû¸¥ Áö¹ÝÀÇ ¿òÁ÷ÀÓÀ» ¿¹ÃøÇϱâ À§Çؼ´Â À¯È¿ÀÀ·Â °³³ä¿¡ ±âÃÊÇÑ ¼öÄ¡ÇØ¼® ±â¹ýÀÌ ¿ä±¸µÇ¾î Áø´Ù. º» ¿¬±¸¿¡¼´Â ÁöÁø ¹× À¯»çÇÑ ¹Ýº¹ ÇÏÁß¿¡ µû¸¥ ¼ö¾ÐÀÇ »ó½ÂÀ» ¿¹ÃøÇÒ ¼ö ÀÖ´Â ¿¬¼º(fully coupled) À¯È¿ÀÀ·Â ±¸¼º¸ðµ¨ÀÎ UBCSAND¸¦ Á¦¾ÈÇÏ¿´´Ù. Á¦¾ÈµÈ ¸ðµ¨Àº °£´ÜÇÑ ¿ÏÀüź¼Ò¼º¸ðµ¨ÀÎ Mohr-CoulombÀ» º¯ÇüÇÑ ÇüÅ·Π¸¶Âû°¢(friction angle)°ú ÆØÃ¢°¢(dilation angle)À» Á¡ÁøÀûÀ¸·Î Áõ°¡½ÃÅ´À¸·Î½á, ±âÁ¸ÀÇ ÆÄ±«»óų»¿¡¼µµ ¿¬¼ÓÀûÀÎ ¼Ò¼ºº¯Çü ¹ß»ýÀ» Ç¥ÇöÇÒ ¼ö ÀÖ´Ù. Ç׺¹ÇÔ¼ö´Â Àü´ÜÀÀ·Â°ú Æò±ÕÀÀ·ÂÀÇ ºñÀÎ $(sigma'_1-sigma'_3)/(sigma'_1-sigma'_3)$·Î ³ªÅ¸³»¸ç, ÀÀ·ÂµµÀÇ ¿øÁ¡¿¡¼ ½ÃÀÛÇÏ´Â ¹«ÇѰ³ÀÇ ¹æ»ç¼±À» ÀǹÌÇÑ´Ù. µû¶ó¼, Mohr-CoulombÀÇ ÆÄ±«¸é°ú °°Àº ÇüÅÂÀÇ ¹«¼öÇÑ Ç׺¹¸éÀ» °¡Áø´Ù. ¼Ò¼º °æÈ¹ýÄ¢Àº µî¹æ°æÈ(isotropic hardening)¿Í À̵¿°æÈ(kinematic hardening)¸¦ È¥ÇÕÇÑ ÇüŸ¦ ÀÌ·ç°í ÀÖ´Ù. ÀçÇÏ(loading) ¹× ÀçÀçÇÏ(reloading)½Ã¿¡´Â ¿¬¼ÓÀûÀÎ ¼Ò¼º º¯ÇüÀÌ ÀϾ³ª, Á¦ÇÏ(unloading)½Ã¿¡´Â ź¼ºº¯ÇüÀ» °¡Á¤ÇÏ¿´´Ù. Á¦¾ÈµÈ ¸ðµ¨Àº ´À½¼ÇÑ Fraser River ¸ð·¡¸¦ ÀÌ¿ëÇÑ Á÷Á¢´Ü¼øÀü´Ü½ÃÇè(Direct simple shear test)°á°ú¿Í ºñ±³ÇÏ¿© °ËÁõÇÏ¿´´Ù. |
|
| Several damages due to large displacement caused by liquefaction have been reported increasingly. Numerical procedures based on effective stress analysis are therefore necessary to predict liquefaction-induced deformation. In this paper, the fully coupled effective stress model called UBCSAND is proposed to simulate pore pressure rise due to earthquake or repeated loadings. The proposed model is a modification of the simple perfect elasto-plactic Mohr-Coulomb model, and can simulate a continuous yielding by mobilizing friction and dilation angles below failure state. Yield function is defined as the ratio of shear stress to mean normal stress. It is radial lines on stress space and has the same shape of Mohr-Columob failure envelope. Plastic hardening is based on an isotropic and kinematic hardening rule. The proposed model always causes plastic deformation during loading and reloading but it predicts elastic unloading. It is verified by capturing direct simple shear tests on loose Fraser River sand. |
| |
| Ű¿öµå |
| Constitutive model;Liquefaction;Mohr-Coulomb;UBCSAND; |
| |
|
|
 |
|
Çѱ¹Áö¹Ý°øÇÐȸ³í¹®Áý / v.21, no.8, 2005³â, pp.27-35
Çѱ¹Áö¹Ý°øÇÐȸ
ISSN : 1229-2427
UCI : G100:I100-KOI(KISTI1.1003/JNL.JAKO200507523322238)
¾ð¾î : Çѱ¹¾î |
|
| ³í¹® Á¦°ø : KISTI Çѱ¹°úÇбâ¼úÁ¤º¸¿¬±¸¿ø |
|
|
|
|
|
|