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Chemická termodynamika II

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D 1.<br />

Empirické a semiempirické rovnice pro bezrozměrnoudodatkovou<br />

Gibbsovu energii u<br />

binárních systémů a některé další veličiny<br />

O. Ideální směs<br />

1. Striktně regulární roztok<br />

Q = O, In71 = ln 72 = In7f =ln7r = O,<br />

Ql = Qu = Q11l = H E = O,<br />

1 1 1<br />

Cll = , GIlI = - - -<br />

XtX2 x~ xi<br />

Q = XIX2 b, In71 = bx;, 1111'2 = bxi<br />

ln 7f" = b, ln 7r = b, QI=b(X2- XI),<br />

QlI -2b, Q11l = O, E ( Ob)<br />

= H j(RT) = -XIX2 T 8T<br />

2. Margulesova tříkonstantovárovnice<br />

Q = XIX2[x IB +X2A - xlx'lD] ,<br />

ln 71 = x;[A +2xt{B - A - D) +3xiD],<br />

ln 72 = xi[B +2X2(A - B - D) +3xiD],<br />

ln If" = A, 1117r = B,<br />

Qtl = 2[A(XI -2x'l) + B(x'l - 2xd +D(6xtX2 - 1)],<br />

= .-6(B - A) + 12D(x'l - xd,<br />

Q1ll<br />

HE<br />

RT<br />

ln 7'('<br />

=<br />

-XIX2 [Xl (T~~)<br />

3. Van Laarova dvoukonstantová rovnice<br />

+Xz (T~~) -XtX2 (T~~)]<br />

Xt X 2AB<br />

Q = Xt x2B j[XI +x2(BjA)] = -A B'<br />

Xl +X2<br />

XtA)2 ( X2B)2<br />

-ln <strong>II</strong> (<br />

= Aj 1 + xzB ln 72 = B j 1 + xlA<br />

= fl, lIlie: = B ,<br />

247

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