Glass transition: Difference between revisions

Revision as of 14:16, 19 June 2007

In the laboratory the glass transition is not a sharp transition; its properties change smoothly across $T_{g}$ .

$T_{g}$ increases with a decrease in the observation time, $\tau _{\rm {obs}}$ .
$\Delta H=0$
$\Delta V=0$

See Ref 1.

$\tau _{\rm {obs}}$

@@ Line 1: / Line 1: @@
+In the laboratory the '''glass transition''' is not a sharp transition; its properties change smoothly across <math>T_g</math>.
+*<math>T_g</math> ''increases'' with a decrease in the observation time, <math>\tau_{\rm obs}</math>.
+*<math>\Delta H =0</math>
+*<math>\Delta V =0</math>
 ==Ideal glass transition temperature==
 See Ref 1.
+==Observation time==
+<math>\tau_{\rm obs}</math>
+==Intrinsic average structural relaxation time==
 ==See also==
 *[[Kauzmann's paradox]]