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±¤È¸Àý ÃøÁ¤¿¡ À־ Mie theory ÀÇ Àû¿ëÀº ¾Æ·¡ÀÇ ¹üÁÖ³»ÀÇ ±¸ÇüÀÔÀÚ¿¡ ÀûÇÕÇÏ´Ù.:

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2 micronÀÌÇϰ¡ 90%ÀÎ °æ¿ì¿¡ Àû¿ë.
Åõ¸í ÀÔÀÚ 200 micronÀÌÇϰ¡ 90%ÀÎ °æ¿ì¿¡ Àû¿ë.

Mie ÀÌ·ÐÀÇ Àû¿ë½Ã ºñ±¸ÇüÀÔÀÚ, È¥ÇÕ¼ººÐ¿¡´Â ÀûÇÕÇÏÁö ¾Ê°í, ¹Ýµå½Ã ÀÔÀÚÀÇ ±¼ÀýÀ²À» ¾Ë¾Æ¾ß ÇÑ´Ù.

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 ±¤È¸Àý ÃøÁ¤±â HELOS ¹× MYTOS
ÃøÁ¤¹üÀ§: R1 ~ R4 ÀÔµµ 350 micron ÀÌÇÏ
±¼Àý»ó°ü °è¼ö±ºÀÇ ¹üÀ§ n - i*k: ±¼Àý»ó¼ö
0.01 <= n <= 3.0
Èí¼ö°è¼ö
0.0 <= k <= 5.0
Æò°¡: HRLD evaluation mode high resolution, high speed

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The basis for applying the Mie theory is the publication by G. Mie[2] in 1908³â G. Mie¿¡ ÀÇÇÏ¿© ¾Ë·ÁÁø MieÀÌ·ÐÀº Maxwell¹æÁ¤½ÄÀÇ Á¤È®ÇÑ ÇØ¹ýÀ̸ç, ±¸ÇüÀÔÀÚÀÇ ÀÜÀ򮀱¤ÇÐÀ¸·Î ±¸¼ºµÇ°í ÀÖ°í,¾Æ·¡¿Í °°Àº MieÀÌ·Ð[3].À¸·Î ¾Ë·ÁÁ® ÀÖ´Ù.

ÀÌ MieÀÌ·ÐÀÇ Àû¿ëÀ» À§Çؼ­´Â ±¼Àý»ó°ü°è¼ö±º, m, À» ¹Ýµå½Ã ¾Ë¾Æ¾ß Çϸç, ´ÙÀ½°ú °°ÀÌ Á¤ÀǵȴÙ.

m = n - i * k

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n         ¹Ý»ç, ±¼Àý·Î Ç¥½ÃµÇ´Â ±¼ÀýÀ²
k         Èí¼ö·Î Ç¥½ÃµÇ´Â Èí¼ö°è¼ö
i         ±¼Àý»ó°ü°è¼ö±ºÀÇ mÀÇ ÀÜ»ó °è¼ö.



[2] G. Mie, Ann. Phys. 25 (1908), 377

[3] H.C. van de Hulst, "Light Scattering by Small Particles", Wiley New York (1957)

WINDOX 5 ¼ÒÇÁÆ®¿þ¾î
MIE Module

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