¶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

Çѱ¹¼öÀÚ¿øÇÐȸ / v.24, no.1, 1991³â, pp.73-81
ÆÄ Saint-Venant ¹æÁ¤½ÄÀ» ÀÌ¿ëÇÑ ¼öÄ¡ÇØÀÇ Á¤µµºÐ¼®
( An Analysis of Precision of Numerical Solutions by Using the Wave Saint-Versant Equations. )
¿ìÈ¿¼·;±èÇöÁØ; Çѱ¹°Ç¼³±â¼ú¿¬±¸¿ø, ¼öÀÚ¿ø ¿¬±¸½Ç;Çѱ¹°Ç¼³±â¼ú¿¬±¸¿ø, ¼öÀÚ¿ø ¿¬±¸½Ç;
 
ÃÊ ·Ï
°³¼ö·Î¿¡¼­ 1Â÷¿ø ºÎÁ¤·ùÀÇ ¿¬¼Ó¼º°ú ¿îµ¿·® º¸Á¸ ¹ýÄ¢ÀÇ Saint-Venant¹æÁ¤½ÄÀ» ÀÏÁ¤ ¼ö½É, À¯¼Ó, À¯·®ÀÇ ÀüÆÄ¼Óµµ Ç×À¸·Î Ç¥½ÃÇÏ¿´À¸¸ç, ÀÌ·¯ÇÑ °¢ ÀüÆÄ¼Óµµ¿Í ¼ö·Î¼Óµµ´Â ÀÏÁ¤ÇÑ °ü°è°¡ ÀÖÀ½ÀÌ ¹àÇôÁ³´Ù. ÇÑ »ç·Ê¿¬±¸¿¡ ÀÇÇϸé, º» ¿¬±¸¿¡¼­ Á¦½ÃµÈ ÀÌ·¯ÇÑ ÀÏ·ÃÀÇ °ü°èµéÀ» ÀÌ¿ëÇÏ¿© Saint-Venant ¹æÁ¤½ÄÀÇ ¼öÄ¡ÇØÀÇ Á¤µµ¸¦ °¡´ÆÇÒ ¼ö ÀÖ´Ù. ÀÌ·¯ÇÑ ÀÏ·ÃÀÇ °ü°èµéÀÇ ¹°¸®Àû ÇØ¼®°ú Saint-Venant ¹æÁ¤½ÄÀÇ ¼öÄ¡ ÇØ¼®¿¡ ´Ù¾çÇÑ È°¿ë ¹æ¾ÈÀº °è¼Ó ¿¬±¸ÁßÀÌ´Ù.
The Saint-Venant equations of the continuity and momentum principles of one-dimensional, unsteady, open-channel flow are expressed in terms of the phase velocities of constant depth, velocity, and discharge, which results in unique relationships between these phase velocities and channel velocity. A case study shows that these unique relationships developed in this study can be used as an indicator of precision of numerical solutions of the Saint-Venant equations. Further physical interpretation of these relationships and utilization to the numerical analyses of the Saint-Venant equations are to be investigated.
 
Ű¿öµå
 
Çѱ¹¼öÀÚ¿øÇÐȸÁö / v.24, no.1, 1991³â, pp.73-81
Çѱ¹¼öÀÚ¿øÇÐȸ
ISSN : 1738-9488
UCI : G100:I100-KOI(KISTI1.1003/JNL.JAKO199111920093451)
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¿