ÀÚ¿¬È®»ê, ȤÀº ÆÛÇÁ¸¦ ÅëÇØ ¼¿ ³»ºÎ·Î À¯ÀÔµÈ ¶óµ· ¹×
ÀÚ¼ÕÇÙÁ¾À¸·ÎºÎÅÍ ¸·ÃâµÇ´Â ¾ËÆÄÀÔÀÚ¿Í ZnS °¡ ¹ÝÀÀÇÏ¿© ÆÄ»ýµÇ´Â
¼¶±¤ (ºû) À» ±¤ÀüÁõ ¹è°üÀ» ÅëÇØ ÁõÆø½ÃÄÑ ÃøÁ¤ÇÏ´Â ¹æ¹ýÀ¸·Î
¶óµ· ³óµµ¸¦ ÃøÁ¤ÇÏ´Â ±â°èÀε¥, ¸Å¿ì Àü¹®ÀûÀÎ ¹æ½Ä,
±×¸®°í Àü¹®ÀûÀÎ Àåºñ¶ó ÀϹÝÀεéÀÌ ÈçÈ÷ º¼ ¼ö´Â ¾ø´Â ÀåºñÀ̱⵵ ÇÕ´Ï´Ù.
Pylon AB7 À̶ó´Â ¸íĪÀÇ
LSC °è¿ ÀåºñÀ̸ç,
Á¦Á¶/ÆǸÅóÀÇ ¸µÅ©ÀÔ´Ï´Ù.
https://www.southernscientific.co.uk/products-by-type/radon-monitors/ab6?source=1627
¾Æ·¡´Â WHO ÀÇ ¶óµ· ÇÚµåºÏ¿¡ ¸í½ÃµÇ¾î ÀÖ´Â LSC ÀÇ Á¤ÀÇ¿Í ¿ø¸®¸¦ ÀϺΠ¹ßÃéÇÏ¿´½À´Ï´Ù.
There are several types of commercially available CRMs
using various types of sensors including scintillation cells,
current or pulse ionization chambers, and solid state silicon
detectors. CRMs either collect air for analysis using a small
pump or by allowing air to diffuse into a sensor chamber.
All CRMs have electrical circuitry that provide a summary
report, and often a time-resolved recording, which allows
the calculation of the integrated radon concentration for
specified periods. The different types have their specific
advantages. For example, when using solid-state silicon
detectors, alpha spectrometry is possible allowing
discrimination between radon and thoron [15].
Liquid scintillation counting (LSC) is the most sensitive
and widely used method to measure radon in water. The
popularity of liquid scintillation for radon analysis is due to
several factors including the excellent accuracy and
precision of the method, the low level of detection, the
limited need for sample preparation. The ability to rapidly
measure a large number of samples, and the ability of the
counter to change samples while unattended. The LSC
technique quantifies the activity of radon and decay
products from the rate of photons emitted from the
scintillation fluid [16, 21]. Limitations of the LSC
technique include the initial start-up cost to purchase the
counter and the need to perform the analyses in a
laboratory. a delay of about 3 hours to establish radioactive
equilibrium between radon and its decay products.
Depending on the counting time, a detection limit below 1
BqL-1 can be achieved.
¼¶±¤ ¼¿, Àü·ù ¶Ç´Â ÆÞ½º ÀÌ¿ÂÈÀÇ Ã¨¹ö, ȤÀº °íü ½Ç¸®ÄܵîÀÇ
´Ù¾çÇÑ À¯ÇüÀÇ ¼¾¼¸¦ »ç¿ëÇÏ´Â ÇöÀç »ó¿ëµÇ°í ÀÖ´Â CRM ¿¡´Â ¿©·¯ À¯ÇüÀÌ ÀÖ½À´Ï´Ù.
CRM Àº ÀÛÀº ÆßÇÁ¸¦ »ç¿ëÇÏ¿© °ø±â¸¦ ¼öÁýÇÏ°í ºÐ¼®À» ÇÕ´Ï´Ù.
±×¸®°í ±× °ø±â°¡ ¼¾¼ è¹ö·Î È®»óµÇµµ·Ï ÇÕ´Ï´Ù.
¸ðµç CRM Àº Àü±â ȸ·Î°¡ ÀÖ°í, º¸°í¼¿Í Á¾Á¾
½Ã°£ÀÌ ¿À·¡ °É¸®´Â ±â·ÏµéÀ» ó¸®ÇÏ°í, ±×°ÍÀ» ÀÌ¿ëÇØ
ƯÁ¤ ±â°£¿¡ ÃàôµÈ ¶óµ· ³óµµ¸¦ ÃøÁ¤ÇÕ´Ï´Ù.
´Ù¾çÇÑ À¯Çüµé¿¡ µû¶ó °¢°¢ ƯÀåÁ¢µéÀÌ ÀÖ±¸¿ä.
»ó´ëÀûÀ¸·Î ³·Àº ³óµµÀÇ ¶óµ·À» ÃøÁ¤ÇÒ °æ¿ì¿¡´Â
´ç¿¬È÷ Á¶±Ý ´õ ¸¹Àº ¾çÀÇ °ø±â¸¦ ¸ð¾Æ¾ß ÇÕ´Ï´Ù.
±×¸®°í »ùÇ÷¯ µîÀ» ÅëÇØ ´õ ÀÛÀº ºÎÇÇ·Î ³óÃàÇÏ´Â °úÁ¤ÀÌ
´õ Á¤È®ÇÑ °è»êÀ» À§ÇØ´Â ²À ÇÊ¿äÇÕ´Ï´Ù.
»çÀü ³óÃà °úÁ¤Àº È°¼ºÅº Æ®·¦À» Åë°úÇÏ´Â ¾×ü Áú¼Ò¸¦
°ø±â°¡ Åë°úÇÏ¸é¼ ÀÌ·ç¾îÁý´Ï´Ù.
ÀÌ ¿Âµµ¿¡¼ ¶óµ·Àº ¼®Åº ¾È¿¡¼ º¸°üµÇ°í,
ÀÌ ¼®ÅºÀº è¹ö ³»¿¡¼ °¡¿ µÈ ´ÙÀ½
°á¹ÚµÈ ¶óµ·ÀÇ »óÅ·Π¹æÃâµË´Ï´Ù. ±× ´ÙÀ½ ÀÌ ¹ÐºÀµÈ ¼¶±¤ ¼¿À̳ª
ÀÌ¿ÂÈ Ã¨¹ö¸¦ »ç¿ëÇϴ è¹ö ¾È¿¡¼
µ¥ÀÌÅÍ°¡ ¼öÁýµÇ°í À§¿¡¼ ¼³¸íÇÑ ¹æ¹ýµ¥·Î ³óµµ¸¦ ÃøÁ¤ÇÕ´Ï´Ù.
LSC (Liquid Scintillation Counting) ´Â ¹° ¼Ó ¶óµ· Ä¡¼ö¸¦ ÃøÁ¤Çϱâ À§ÇØ
°¡Àå ³Î¸® »ç¿ëµÇ°í ÀÖ°í °¡Àå ¹Î°¨ÇÑ ¹æ¹ýÀÇ ÃøÁ¤±â ÀÔ´Ï´Ù.
ÀÌ LSC ÀÇ Àαâ´Â, ¶óµ· ºÐ¼®¿¡ ´ëÇÑ ¿ì¼öÇÑ Á¤È®µµ¿Í Á¤¹ÐµµÀÇ ¹æ½Ä,
±×¸®°í ³·Àº ³óµµ¿¡¼¿¡¼µµ ÃøÁ¤ÀÌ °¡´ÉÇÑ Á¡, ±×¸®°í »ùÇà Áغñ¿¡ ÀÖ¾î¼
ÇÊ¿ä¿ä°ÇÀÌ Á¦ÇÑÀûÀ̱⵵ ÇÒ °ÍÀÔ´Ï´Ù.
ÀÌ ±â°è´Â ´Ù¼öÀÇ »ùÇÃÀ» ÃøÁ¤ÇÒ ¼ö ÀÖ´Â ±â´É°ú
¹«ÀÎ »óÅ¿¡¼ »ùÇÃÀ» º¯°æÇÒ ¼ö ÀÖ´Â ±â´Éµµ ÀÖ½À´Ï´Ù.
LSC ±â¹ýÀº, ¼¶±¤ À¯Ã¼¿¡¼ ¹æÃâµÇ´Â ±¤ÀÚÀÇ ºñÀ²·ÎºÎÅÍ ¶óµ·°ú,
¶óµ· ºØ±«ÀÇ »ý¼º¹°ÁúµéÀÇ È°¼ºÀ» Á¤·®ÈÇÕ´Ï´Ù.
LSC ±â¹ý¿¡ ÇÑ°è°¡ ÀÖ´Ù¸é, Ä«¿îÅÍ ±¸ÀÔºñ¿ëÀÇ Ãʱ⠺ñ¿ëÀÌ ºñ½Î°í,
½ÇÇè½Ç¿¡¼ ºÐ¼®À» ¼öÇàÇØ¾ß ÇÏ´Â Àü¹®°¡°¡ °¢°¢ ÇÊ¿äÇÕ´Ï´Ù.
ÀÌ ±â°è´Â 3½Ã°£ ³»¿Ü·Î ¶óµ·°ú ±× ºØ±« »ý¼º¹° »çÀÌÀÇ ±ÕÇüµéÀÌ ÀÌ·ç¾îÁö°í,
Ä«¿îÆà ½Ã°£¿¡ µû¶ó 1BqL-1 ¹Ì¸¸ÀÇ °ËÃâ·®¿¡¼µµ ¶óµ· ³óµµ¸¦ ÃøÁ¤ÇÒ ¼ö ÀÖ½À´Ï´Ù.
(Source: WHO Radon Handbook, ¹ø¿ª: (ÁÖ)¹ÙƼ¿¡)