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½ºÅ×Æijë Stefano   14-08-04 15:31
(1) °íºÐÀÚÀÇ Á¡µµ´Â °íÀ¯Á¡µµ¸¦ ÀÌ¿ëÇÏ¿© ±¸Çϴµ¥ °íºÐÀÚ¸¦ ¿ëÁ¦¿¡ ³ì¿© Á¡µµ¸¦ ÃøÁ¤ÇßÀ» ¶§ ¹«ÇÑÈñ¼®³óµµ¿¡¼­ÀÇ Á¡µµ°¡ ¹Ù·Î °íÀ¯Á¡µµ(Intrinsic Viscosity)ÀÔ´Ï´Ù.  ¼ö·®Æò±Õ, Áú·®Æò±Õ, µîÀ» Æ÷ÇÔÇÏ¿© Á¡µµÆò±Õ ºÐÀÚ·®Àº ÀÌ°÷
http://nsdl.niscair.res.in/jspui/bitstream/123456789/406/2/Molecular%20weights%20of%20polymers.pdf ¿¡ Àß ¼³¸íµÇ¾î ÀÖ½À´Ï´Ù.  ¼ö½Ä ¹øÈ£¸¸ °íÃļ­ ÀοëÇÏ¸é º» ´ä±ÛÀÇ ½Ä(5, ¿ø¹®ÀÇ ¼ö½Ä (28))¸¦ ÀÌ¿ëÇÏ¿© °è»êÇÏ¸é µË´Ï´Ù. 
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(Quote/)
General Expression for Viscosity Average Molecular Weight:
 
At infinite dilution (c ¡æ o), the polymer molecules in solution contribute to viscosity discretely without mutual interference. Solubilization of a polymer sample is preceded by a large amount of swelling if left undisturbed and the swelling degree is higher in a better solvent. Similarly, the intrinsic viscosity is also higher in a good solvent than in a poor solvent. What all these would mean is that in a better solvent, as the polymer chain molecules go into solution, a unit mass of the same expands more to give a higher hydrodynamic volume.

Let there be a heterogeneous (polydisperse) polymer in dilute solution of concentration c considered to behave ideally in that the individual molecules contribute to viscosity enhancement independently of one another. In that event, if ( ¥çsp ) i be the specific viscosity contribution due to the species of size i , then one may express the overall specific viscosity ¥çsp as
            ¥çsp = ¥Ò (¥çsp )i ------------------------------(1)
Considering Mi and ci as the molecular weight and concentration of the species of size i and in view of the ideal specific viscosity component ( ¥çsp )i = KMi^ a * ci , it is further possible to write. 

            ¥çsp = K ¥Ò (Mi^a * ci)------------------------(2) 
and so,
          ( ¥çsp / c ) = [¥ç] = ( K ¥Ò Mi^a * ci ) / c -----(3)
where, c = ¥Ò ci stands for overall concentration taking all polymer species into consideration. Further taking c = ¥Ò ci = ¥Ò Ni Mi , and considering the (Mark Houwink) equation (21), one may have :

            [¥ç] = K ¥Ò Ni Mi^(1 + a)/¥Ò Ni Mi = K M¥í^a -------------------(4)

such that,
            M¥í = {¥Ò Ni Mi^(1 + a)/¥Ò Ni Mi }^(1/a) -----------------------(5)
 
Clearly, one may see that for the limiting case when a = 1 , M¥í = Mw
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(/Unquote)

ÀοëÇÑ ºÎºÐÀ» °£´ÜÈ÷ ¿ä¾àÇÏ¸é  i ¼ººÐÀÇ ºñÁ¡µµ (Specificic Viscosity)´Â  ( ¥çsp)i = K Mi^ a ¿Í °°ÀÌ ³ªÅ¸³¾ ¼ö Àִµ¥ À̸¦ °¢ i¼ººÐÀÇ ³óµµºÐÀ²  ci ´ëÇØ °¡ÁßÆò±ÕÇÏ¿© ±¸ÇÑ °ªÀÌ µË´Ï´Ù.  K¿Í  alpha(a)´Â °íÀ¯Á¡µµ¸¦ ±¸Çϴµ¥ »ç¿ëÇÏ´Â ¿ëÁ¦¿¡ µû¸¥ »ó¼öÀÔ´Ï´Ù. 

(1)~(5) ¼ö½Äµé Àº (5)½ÄÀÌ ¾ò¾îÁö´Â °úÁ¤À» À¯µµÇÑ °ÍÀ̹ǷΠ°á±¹ (5)½Ä ¸¸À» ÀÌ¿ëÇϸé Á¡µµÆò±Õ ºÐÀÚ·®À» ±¸ÇÒ ¼ö ÀÖ½À´Ï´Ù.
   

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