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±¤È¸Àý ÃøÁ¤¿¡ ÀÖ¾î¼ Mie theory ÀÇ Àû¿ëÀº ¾Æ·¡ÀÇ ¹üÁÖ³»ÀÇ ±¸ÇüÀÔÀÚ¿¡ ÀûÇÕÇÏ´Ù.:
ºÒÅõ¸í ÀÔÀÚ |
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.
sensors: |
HELOS family | MYTOS family |
| measuring ranges: | all measuring ranges | all particle sizes |
| range of relative complex refractive index | refraction coefficient 0.1 <= n <= 5.0 |
absorption coefficient 0.0; 1E-5<= k <= 8.0 |
| evaluation: | MIEE | Mie Extended Evaluation Mode |
The basis for applying the Mie theory is the publication by G. Mie[2] in 1908, in which an exact solution of Maxwell's equations was formulated for scattering of electromagnetic waves by spherical particles. This solution is known as the Mie theory. A detailed description is presented in [3].
For the application of Mie theory, the complex refractive index, n of the particles and the refractive index nm of the (non-absorbing) fluid must be known.
The complex refractive indes ist defined by: |
n = np - i * kp |
The relative complex refractive index is defined by: |
m =n/nm |
where |
|
np |
the refractive index of the particle, describes reflection and refraction, |
nm |
the refractive index of the fluid, |
kp |
the absorption coefficien of the particle, describes the absorption, |
i |
the imaginary unity. |
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WINDOX 5 |
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| Server Administration |
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| Data Visualisation Program |
| QT Module |
| Mie Module |
| Revalidation Module |
| KSIGMA Module |
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QX2 |
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| Process Add-on |
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