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1
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33947442893
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-
For early reviews, see, W. Kauzmann, Chem. Rev. 43, 219 (1948)
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(1948)
Chem. Rev.
, vol.43
, pp. 219
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-
Kauzmann, W.1
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4
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-
0028416385
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-
An excellent review containing numerous references is I. M. Hodge, J. Non-Cryst. Solids 169, 211 (1994).
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(1994)
J. Non-Cryst. Solids
, vol.169
, pp. 211
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-
Hodge, I.M.1
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5
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-
85036213920
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-
A good overview is given by the articles in Thermochim. Acta 304/305, (1997)
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A good overview is given by the articles in Thermochim. Acta 304/305, (1997).
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-
-
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6
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0000808497
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See, e.g., H. Fujimori, H. Fujita, and M. Oguni, Bull. Chem. Soc. Jpn. 68, 447 (1995).
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(1995)
Bull. Chem. Soc. Jpn.
, vol.68
, pp. 447
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-
Fujimori, H.1
Fujita, H.2
Oguni, M.3
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9
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0000147918
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Inorganic glass-formers have also been studied. For a recent example, see R. Brüning and M. Sutton, Phys. Rev. B 49, 3124 (1994).
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(1994)
Phys. Rev. B
, vol.49
, pp. 3124
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-
Brüning, R.1
Sutton, M.2
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10
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1242268843
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-
For inorganic glasses the (optical) density has often been determined using the index of refraction; see, e.g., P. B. Macedo and A. Napolitano, J. Res. Natl. Bur. Stand., Sect. A 71A, 231 (1967).
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(1967)
J. Res. Natl. Bur. Stand., Sect. A
, vol.71A
, pp. 231
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Macedo, P.B.1
Napolitano, A.2
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12
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0030172718
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See, e.g., C. Meingast, M. Haluska, and H. Kuzmany, J. Non-Cryst. Solids 201, 167 (1996).
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(1996)
J. Non-Cryst. Solids
, vol.201
, pp. 167
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-
Meingast, C.1
Haluska, M.2
Kuzmany, H.3
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15
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85036360279
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L. D. Landau and E. M. Lifshitz, Statistical Physics, Vol. 5 of Course of Theoretical Physics (Pergamon, Oxford, 1980)
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L. D. Landau and E. M. Lifshitz, Statistical Physics, Vol. 5 of Course of Theoretical Physics (Pergamon, Oxford, 1980).
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-
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18
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85036371046
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If time-reversal symmetry holds, one has (Formula presented) Thus the order of terms appearing in Eq. (2) may be interchanged
-
If time-reversal symmetry holds, one has (Formula presented) Thus the order of terms appearing in Eq. (2) may be interchanged.
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-
-
-
20
-
-
85036342472
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-
Here the equilibrium state is to be understood as the metastable melt and of course not the crystalline phase which in most cases will constitute the true equilibrium state close to (Formula presented)
-
Here the equilibrium state is to be understood as the metastable melt and of course not the crystalline phase which in most cases will constitute the true equilibrium state close to (Formula presented)
-
-
-
-
21
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-
0021459132
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or Ref. 2
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In fact, this expression is equivalent to the Vogel-Fulcher or WLF equation. It involves the fact that the thermal susceptibility is inversely proportional to temperature; see G. W. Scherer, J. Am. Ceram. Soc. 67, 504 (1984) or Ref. 2.
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(1984)
J. Am. Ceram. Soc.
, vol.67
, pp. 504
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Scherer, G.W.1
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22
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85036355427
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L. D. Landau and E. M. Lifshitz, Theory of Elasiticity, Vol. 7 of Course of Theoretical Physics (Pergamon, Oxford, 1986)
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L. D. Landau and E. M. Lifshitz, Theory of Elasiticity, Vol. 7 of Course of Theoretical Physics (Pergamon, Oxford, 1986).
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-
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23
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0001087913
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For materials with (Formula presented) see, e.g., R. Lakes, Adv. Mater. 5, 293 (1993).
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(1993)
Adv. Mater.
, vol.5
, pp. 293
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Lakes, R.1
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24
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85036413766
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polymeric glasses, ν is rarely smaller than 0.3; see, e.g., W. D. Callister, Jr., Materials Science and Engineering—An Introduction (Wiley, New York, 1997)
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In polymeric glasses, ν is rarely smaller than 0.3; see, e.g., W. D. Callister, Jr., Materials Science and Engineering—An Introduction (Wiley, New York, 1997).
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-
-
-
25
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-
85036376306
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Other expressions may be used instead, but for the relatively small dielectric constants of interest here, this should make no significant difference
-
Other expressions may be used instead, but for the relatively small dielectric constants of interest here, this should make no significant difference.
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-
-
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27
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85036167860
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T. Bretz, diploma thesis, Fachhochschule Wiesbaden, 1996
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T. Bretz, diploma thesis, Fachhochschule Wiesbaden, 1996.
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-
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28
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85036182052
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Taking typical values for K (≈ 1 GPa) and α (Formula presented) a temperature change of 1 K alters the pressure on the rigid capacitor plates by about 1 bar
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Taking typical values for K (≈ 1 GPa) and α (Formula presented) a temperature change of 1 K alters the pressure on the rigid capacitor plates by about 1 bar.
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-
-
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29
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0000802484
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J. A. Forrest, C. Svanberg, K. Révész, M. Rohdal, L. M. Torell, and B. Kasemo, Phys. Rev. E 58, R1226 (1998).
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(1998)
Phys. Rev. E
, vol.58
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Forrest, J.A.1
Svanberg, C.2
Révész, K.3
Rohdal, M.4
Torell, L.M.5
Kasemo, B.6
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33
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0001328636
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An approximate linearity of response up to oscillation amplitudes of 1–1.5 K was also observed in thermomodulated DSC experiments, J. E. K. Schawe and S. Theobald, J. Non-Cryst. Solids 235-237, 496 (1998)
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(1998)
J. Non-Cryst. Solids
, vol.235-237
, pp. 496
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Schawe, J.E.K.1
Theobald, S.2
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35
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85036149374
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Since in the vicinity of (Formula presented) the slope of (Formula presented) is negative, outside of the dispersive range the experimentally determined phase lags are close to 180°
-
Since in the vicinity of (Formula presented) the slope of (Formula presented) is negative, outside of the dispersive range the experimentally determined phase lags are close to 180°.
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-
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36
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0003774488
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edited by J. Brandrup and E. H. Immergut, Wiley, New York
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Polymer Handbook, 2nd ed., edited by J. Brandrup and E. H. Immergut (Wiley, New York, 1975).
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(1975)
Polymer Handbook, 2nd ed.
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-
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37
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0001300435
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-
The alternative set of parameters with (Formula presented)given in this reference yields somewhat less satisfactory agreement with our data shown in Fig. 99
-
I. M. Hodge, Macromolecules 20, 2897 (1987). The alternative set of parameters with (Formula presented)given in this reference yields somewhat less satisfactory agreement with our data shown in Fig. 99.
-
(1987)
Macromolecules
, vol.20
, pp. 2897
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Hodge, I.M.1
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38
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0017104476
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For previous comparisons of dilatometric and calorimetric responses, see, e.g., C. T. Moynihan , Ann. (N.Y.) Acad. Sci. 279, 15 (1976)
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(1976)
Ann. (N.Y.) Acad. Sci.
, vol.279
, pp. 15
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Moynihan, C.T.1
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39
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0001578078
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S. Takahara, M. Ishikawa, O. Yamamuro, and T. Matsuo, J. Phys. Chem. B 103, 792 (1999)
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(1999)
J. Phys. Chem. B
, vol.103
, pp. 792
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Takahara, S.1
Ishikawa, M.2
Yamamuro, O.3
Matsuo, T.4
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44
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0001757063
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performed a similar comparison for PS using modulated calorimetry
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A. Hensel and C. Schick, J. Non-Cryst. Solids 235-237, 510 (1998) performed a similar comparison for PS using modulated calorimetry.
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(1998)
J. Non-Cryst. Solids
, vol.235-237
, pp. 510
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Hensel, A.1
Schick, C.2
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47
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33751124528
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R. Böhmer, K. L. Ngai, C. A. Angell, and D. J. Plazek, J. Chem. Phys. 99, 4201 (1993).
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(1993)
J. Chem. Phys.
, vol.99
, pp. 4201
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Böhmer, R.1
Ngai, K.L.2
Angell, C.A.3
Plazek, D.J.4
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49
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0001374509
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K. U. Schug, H. E. King, Jr., and R. Böhmer, J. Chem. Phys. 109, 1472 (1998).
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(1998)
J. Chem. Phys.
, vol.109
, pp. 1472
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Schug, K.U.1
King, H.E.2
Böhmer, R.3
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50
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0001079241
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K. Ito, J. L. Green, K. Xu, and C. A. Angell, J. Phys. Chem. 103, 3991 (1999).
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(1999)
J. Phys. Chem.
, vol.103
, pp. 3991
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Ito, K.1
Green, J.L.2
Xu, K.3
Angell, C.A.4
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52
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0015728769
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From their Table 2 we find for the loss-peak amplitude (Formula presented) normalized by the dispersion step (Formula presented) that (Formula presented) for (Formula presented)
-
C. T. Moynihan, L. P. Boesch, and N. L. Laberge, Phys. Chem. Glasses 14, 122 (1973). From their Table 2 we find for the loss-peak amplitude (Formula presented) normalized by the dispersion step (Formula presented) that (Formula presented) for (Formula presented)
-
(1973)
Phys. Chem. Glasses
, vol.14
, pp. 122
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-
Moynihan, C.T.1
Boesch, L.P.2
Laberge, N.L.3
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