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Çѱ¹¼öÀÚ¿øÇÐȸ / v.21, no.4, 1988³â, pp.399-406
¸¸°î¼ö·Î¿¡¼­ÀÇ Ice Jam°ú È帧Ư¼º
( Characteristics of Ice Jam and flow in channel Bends )
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¸¸°î¼ö·Î¿¡¼­ÀÇ È帧, ice jamÀÇ Çü¼º ¹× ºÐÆ÷Ư¼ºÀ» ±Ô¸íÇϱâ À§ÇÏ¿© ±âº»ÀÌ·ÐÀ» ºÐ¼®Çϰí, ½ÇÇè¼ö·Î·Î´Â ¿¬¼Ó ¸¸°î¼ö·Î¿Í ´ÜÀÏ ¸¸°î¼ö·Î¸¦ »ç¿ëÇÏ¿´´Ù. ¿¬¼Ó ¸¸°î¼ö·Î´Â 13°³ÀÇ Á߽ɰ¢ $90^{circ}$¸¸°îºÎ°¡ ¿¬°áµÈ ¼ö·ÎÀ̸ç ÇÏÆø¿¡ ´ëÇÑ ¼ö½ÉÀÇ ºñ°¡ 2ÀÌ¸ç ´ÜÀÏ ¸¸°î¼ö·Î´Â Á߽ɰ¢ $180^{circ}$À̸ç ÇÏÆø¿¡ ´ëÇÑ ¼ö½ÉÀÇ ºñ°¡ 4·Î ºñ±³Àû ¼ö½ÉÀÌ ¾èÀº ¼ö·ÎÀÌ´Ù. ½ÇÇè¿¡ »ç¿ëµÈ ¾óÀ½Àç·á´Â Æú¸®¿¡Ä¥·»°ú Æú¸®ÇÁ·ÎÇÊ·» ±¸½½(bead)¿Í Á¶°¢(block)ÀÌ´Ù. ¿¬¼Ó ¸¸°î¼ö·Î¿¡¼­´Â Àú¸éÀ¯¼ÓÀÌ Ç¥¸éÀ¯¼Óº¸´Ù Å©¸ç ice jamÀÇ Çü¼ºÀ¸·Î ÀÌ·¯ÇÑ Çö»óÀº ´õ¿í Å©°Ô ³ªÅ¸³µ´Ù. JamÀÇ µÎ²²´Â ÀϹÝÀûÀ¸·Î ³»ÃøÀÌ ¿ÜÃøº¸´Ù µÎ²¨¿üÀ¸¸ç ÃÖ´ë À¯¼Ó¼±Àº ice jamÀÇ ¹ß»ýÀ¸·Î ÀÎÇÏ¿© ´õ¿í ³»ÃøÀ¸·Î ÆíÀ̵Ǿú´Ù. Ⱦ¹æÇâ jamÀÇ µÎ²²´Â ÇÏÆø¿¡ ´ëÇÑ ¾óÀ½ Á¶°¢ÀÇ ±æÀÌ ºñ°¡ Áõ°¡ÇÔ¿¡ µû¶ó ±ÔÄ¢ÀûÀ¸·Î ºÐÆ÷ µÇ¾ú´Ù. ´ÜÀÏ ¸¸°î¼ö·Î¿¡¼­ÀÇ jam hed´Â ¾óÀ½ÀÇ ¿î¼Û·®ÀÌ ÀÏÁ¤ÇÑ °æ¿ì ¿ÜÃøÀÌ ³»Ãø º¸´Ù »¡¸® ÁøÇàµÇ¾úÀ¸¸ç ±× ¼Óµµ´Â ºñ±³Àû ÀÏÁ¤ÇÏ¿´´Ù. Froude ¼ö°¡ Áõ°¡µÇ¹Ç·Î jam µÎ²²´Â Ⱦ´Ü¸é¿¡ °ÉÃÄ ºÒ±ÕÀÏÇÏ°Ô µÇ¸ç, ³»Ãø°ú jam ³¡ºÎºÐÀÌ µÎ²®°Ô µÈ´Ù. Two-Layer modelÀº ¼ö½ÉÀÌ ¾èÀº ¸¸°îºÎ¿¡¼­ Àû¿ë°¡´ÉÇϸç, 2Â÷ È帧ÀÇ ºÐÆ÷´Â »óÇÏ 2°³ÀÇ cellÀÌ Á¸ÀçÇÔÀ» ¾Ë ¼ö ÀÖ¾ú´Ù.
Presented in this paper is a brief summary of the basic theory and observation from a laboratory investigation aimed at determining flow characteristics and ice jam topography in a sinuous channel, and in a single-bend channel. The sinuous channel comprised thirteen $90^{circ}$ bends and was of comparatively small saspect ratio. The single-bend channel was a $180^{circ}$ bend, which was an order of magnitude large in width as well as aspect ratios than the sinuous channel. The simulated ices were polyethylene and polypropylene beads and block. The streamwise velocities near the bottom were larger than that of surface in sinuous channel and forming ice jam in sinuous channel, this phenoumena were found strongly. Jams were generally thicker along the inner bank of bends. The path of maximum-streamwise velocity was displaced towards approachs side of the inner bank of bends. Radial variation of jam thickness was to be regular by increasing size of ice fragments. The rate of jam head progression around outer bank of the single bend was faster than that of inner bank and its velocity was roughly steady. With increasing Froude number, jm thickness became less uniformly distributed; being generally thicker along the inner bank and near the jam's toe. Two-layer model might be adaptable for the computing the streamwise velocity in shallow river bends. Two cells of secondary flow cound be expected in ice covered-river bends.
 
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Çѱ¹¼öÀÚ¿øÇÐȸÁö / v.21, no.4, 1988³â, pp.399-406
Çѱ¹¼öÀÚ¿øÇÐȸ
ISSN : 1738-9488
UCI : G100:I100-KOI(KISTI1.1003/JNL.JAKO198811920092559)
¾ð¾î : Çѱ¹¾î
³í¹® Á¦°ø : KISTI Çѱ¹°úÇбâ¼úÁ¤º¸¿¬±¸¿ø
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