TY - JOUR
T1 - Application of the Rheovibron to inorganic glass problems I. The mixed alkali effect loss spectrum
AU - Atake, T.
AU - Angell, C. A.
N1 - Funding Information:
The authors are indebted to the National Science Foundation MRL program for support of this work under Grant No. DMR 76-00889. Thanks are also due to Prof. 0. Day who provided encouragement and advice and also some mixed alkali aluminosilicate fibres on which measurements were attempted (unsuccessfully) before the flexural mode of operation was adopted.
Copyright:
Copyright 2014 Elsevier B.V., All rights reserved.
PY - 1980
Y1 - 1980
N2 - A mechanical spectrometer with four decade frequency range has been used to characterize the isothermal mechanical loss spectrum of a mixed alkali silicate glass. The half width of the mechanical loss spectrum is very much greater than that for electrical relaxation at the same temperature despite the fact that both relaxations are due to alkali ion motion. It is suggested that the difference, which is also present in single alkali glasses is primarily a consequence of the fact that the mechanical relaxation is by nature a secondary relaxation (probably one of a sequence of broad secondary relaxations) while the electrical relaxation is a primary relaxation insofar as it is the process producing the largest of all changes of electrical modulus.
AB - A mechanical spectrometer with four decade frequency range has been used to characterize the isothermal mechanical loss spectrum of a mixed alkali silicate glass. The half width of the mechanical loss spectrum is very much greater than that for electrical relaxation at the same temperature despite the fact that both relaxations are due to alkali ion motion. It is suggested that the difference, which is also present in single alkali glasses is primarily a consequence of the fact that the mechanical relaxation is by nature a secondary relaxation (probably one of a sequence of broad secondary relaxations) while the electrical relaxation is a primary relaxation insofar as it is the process producing the largest of all changes of electrical modulus.
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U2 - 10.1016/0022-3093(80)90458-5
DO - 10.1016/0022-3093(80)90458-5
M3 - Article
AN - SCOPUS:0019018964
SN - 0022-3093
VL - 38-39
SP - 439
EP - 444
JO - Journal of Non-Crystalline Solids
JF - Journal of Non-Crystalline Solids
IS - PART 1
ER -