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Architecture & Urban Research Institute

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³í¹®¸í ³­¹æ ¿îÀü ½Ã ºÎ·Â È¿°ú¿¡ ÀÇÇÑ ¼Ò°­´ç ¿Ü±â ħ±â·® ¿µÇâ¿¡ °üÇÑ ½ÇÃø ¹× ÇØ¼®¸ðµ¨ ¿¬±¸ / Experimental and Modeling Study of Buoyancy-Driven Infiltration in a Small Auditorium during Heating Operation
ÀúÀÚ¸í À±Á¾¼®(Jong Seok Yoon) ; ±è¿µÀÏ(Young Il Kim)
¹ßÇà»ç ´ëÇѼ³ºñ°øÇÐȸ
¼ö·Ï»çÇ× ¼³ºñ°øÇÐ³í¹®Áý, Vol.38 No.7 (2026-07)
ÆäÀÌÁö ½ÃÀÛÆäÀÌÁö(393) ÃÑÆäÀÌÁö(11)
ISSN 1229-6422
ÁÖÁ¦ºÐ·ù ȯ°æ¹×¼³ºñ
ÁÖÁ¦¾î ȯ±âȽ¼ö; °­´ç; ºÎ·Â; ³­¹æ; ½Ç³»°ø±âÁú; ȯ±â ; Air change per hour; Auditorium; Buoyancy; Heating; Indoor air quality; Ventilation
¿ä¾à1 ±³À°½Ã¼³ ¼Ò°­´çÀº ´ë±Ô¸ð °­ÀÇ, ÇмúÇà»ç, Ư°­, °ø¿¬, ´Üü ±³À° µî ´Ù¾çÇÑ ¸ñÀûÀ¸·Î ´Ù¼öÀÇ ÀοøÀÌ Àå½Ã°£ ÀÌ¿ëÇÏ´Â ´ÙÁß ½Ã¼³ÀÌ´Ù. ÀÌ·¯ÇÑ °ø°£Àº Àç½ÇÀÚÀÇ È£ÈíÀ¸·Î ÀÎÇØ CO2 ¹× ¿À¿°¹°ÁúÀÌ ºü¸£°Ô Áõ°¡µÇ¹Ç·Î, È¿°úÀûÀΠȯ±â(Ventilation) Àü·«ÀÌ ÇʼöÀûÀÌ´Ù(1,2). ƯÈ÷, Á÷ÆØ½Ä(Direct expansion) °øÁ¶±â¸¦ »ç¿ëÇÏ´Â ¼Ò±Ô¸ð °­´ç¿¡¼­´Â ¿Ü±âµµÀÔ·® Á¶ÀýÀÌ ½Ç³»°ø±âÁú(IAQ)¿¡ °áÁ¤ÀûÀÎ ¿µÇâÀ» ¹ÌÄ£´Ù(3,4). Á÷ÆØ½Ä °øÁ¶±â´Â ³Ã¸Å°¡ °øÁ¶±â¿¡¼­ Á÷Á¢ ¿­±³È¯ÇÏ´Â ¹æ½ÄÀ¸·Î, ±âÁ¸ Áß¾Ó°øÁ¶ ¹æ½Ä¿¡ ºñÇØ ¼³Ä¡°¡ ¿ëÀÌÇÏ°í °³º° Á¦¾î °¡´ÉÇÏ´Ù´Â ÀåÁ¡À» °¡Áø´Ù.
¿Ü±âµµÀÔ ¾øÀÌ ¿ÏÀü Àç¼øÈ¯ ¿îÀü(0% ¿Ü±â)À» ÇÒ °æ¿ì CO2 ³óµµ°¡ ±Þ»ó½ÂÇÏ¿© ½Ç³»°ø±âÁú(IAQ)ÀÌ ¾ÇÈ­µÈ´Ù(1,5). ƯÈ÷, °Ü¿ïö ³­¹æ ¿îÀü ½Ã¿¡´Â ½Ç³»¿Ü ¿ÂµµÂ÷¿¡ ÀÇÇÑ ¿­ºÎ·Â(Buoyancy) È¿°ú·Î ÀÎÇØ °Ç¹° °³±¸ºÎ ÇϺο¡¼­ ¿Ü±â°¡ ħÅõÇϰí, »óºÎ¿¡¼­ ½Ç³» °ø±â°¡ À¯ÃâµÇ´Â ÀÚ¿¬ ħ±â(Natural infiltration)°¡ °­Á¦È¯±â¿Í ÁßøµÇ¾î ½Ç³» ȯ±â¿Í °øÁ¶ ºÎÇÏ¿¡ º¹ÇÕÀûÀÎ ¿µÇâÀ» ¹ÌÄ£´Ù. À̸¦ Á¤·®È­Çϱâ À§Çؼ­´Â ¹®, â, º®ÀÇ Æ´»õ¸¦ ÅëÇÑ À¯ÀÔ ¹× À¯Ãâ Áú·®À¯·®À» ¼Óµµ°è¼ö , Æ´»õ°£°Ý , Æ´»õ±æÀÌ , ¿­ºÎ·Â ¾Ð·ÂÂ÷ , Áß¼º´ë³ôÀÌ ÀÇ ÇÔ¼ö·Î ¸ðµ¨¸µÇϰí, Á¤»ó»óÅ Áú·® ±ÕÇü Á¶°Ç¿¡¼­ À¯ÀÔ·® ¹× À¯Ãâ·®À» »êÃâÇÏ´Â ÀÌ·ÐÀû Á¢±ÙÀÌ ÇÊ¿äÇÏ´Ù(6).
º» ¿¬±¸´Â ÀÌ·¯ÇÑ IAQ Ư¼ºÀ» Á¤·®ÀûÀ¸·Î ºÐ¼®Çϱâ À§ÇØ, °Ü¿ïö Á¶°Ç¿¡¼­ AHU ¿Ü±â´ïÆÛ °³µµÀ²À» 0%(¿ÏÀü Àç¼øÈ¯)¿Í 30%, ³­¹æ(Heating) °¡µ¿ ¿©ºÎ(On/Off)¸¦ Á¶°ÇÀ¸·Î ÇÏ¿© CO2 ³óµµ, ¿Âµµ º¯È­·®À» ÃøÁ¤ÇÏ¿´´Ù. ¶ÇÇÑ, °­´ç¿¡ ¼³Ä¡µÈ 5°³ ¹®ÀÇ Æ´»õ Ä¡¼ö¸¦ °èÃøÇϰí, ASHRAE Handbook Fundamentals Chapter 16(6)ÀÇ ¼Óµµ °è¼ö = 0.65, ÀÌ»ó±âü »óŽÄ, ºÎ·Â½ÄÀ» Àû¿ëÇÏ¿© ¹®°ú º®ÀÇ Æ´»õ¸¦ ÅëÇÑ À¯ÀÔ ¹× À¯Ãâ À¯·®À» °è»êÇÏ¿´´Ù. EES(7)¸¦ Ȱ¿ëÇÏ¿© Áß¼º´ë ³ôÀÌ ¿Í ½Ç³»¿Ü ¾Ð·ÂÂ÷ »êÃâÀ» ÅëÇØ ³­¹æ ½Ã¿Í ºñ³­¹æ ½ÃÀÇ È¯±â·® Â÷À̸¦ °è»êÇÏ°í ½ÇÃø°ª°ú ºñ±³ °ËÁõÇÏ¿´´Ù. À̸¦ ÅëÇØ ¿Ü±âµµÀÔ Á¶°Ç º¯È­¿¡ µû¸¥ IAQ Ư¼º°ú ºÎ·Â ±â¹Ý ħ±â ¿ø¸®¸¦ ±Ô¸íÇϰí, ¼ö¿ä Á¦¾îȯ±â(DCV) ¹× Àç½Ç ±â¹Ý Á¦¾î Àü·«ÀÇ °øÇÐÀû ±Ù°Å¸¦ Á¦½ÃÇϰíÀÚ ÇÑ´Ù.
¿ä¾à2 This study analyzed infiltration characteristics driven by thermal buoyancy during winter heating in a 604 m©ø auditorium. Temperature, humidity, and CO©ü concentration were measured under five conditions: natural ventilation, and outdoor air damper opening ratios of 0% and 30% (both with and without heating). The lowest air change rate was observed during natural ventilation at 0.197 h?©ö. With the outdoor air damper at 0%, the air change rate during heating was 1.127 h?©ö, which was 0.351 h?©ö higher than the non-heating condition (0.776 h?©ö). At a 30% damper opening, the air change rate during heating was 1.351 h?©ö, an increase of 0.254 h?©ö compared to the non-heating condition (1.097 h?©ö). This increase is attributed to the elevated indoor temperature during heating, which creates a density difference between indoor and outdoor air, leading to pressure differences. Consequently, the outdoor pressure becomes higher than the indoor pressure in the lower part of the building envelope, causing infiltration, while the outdoor pressure becomes lower in the upper part, resulting in exfiltration. An analytical model incorporating thermal buoyancy was developed to calculate infiltration through five doors and envelope cracks. The model's results showed excellent agreement with measurements, with errors of 0.14% at 0% opening and 0.26% at 30%. The proposed analytical model can effectively predict infiltration rates during heating operation.
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DOI https://doi.org/10.6110/KJACR.2026.38.7.393