In this work, five Mg-silicate glasses with compositions between MgSiO3\documentclass[12pt]{minimal}
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\begin{document}$$_4$$\end{document} were synthesized by aerodynamic levitation combined with laser melting. Low-temperature heat capacity (Cp\documentclass[12pt]{minimal}
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\begin{document}$$C_p$$\end{document}) was measured (by relaxation calorimetry in the range 2–310 K) for all of them, with the resulting vibrational entropies at T = 298.15 K: sample MG50 with composition Mg0.996\documentclass[12pt]{minimal}
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\begin{document}$$_{0.996}$$\end{document}SiO2.996\documentclass[12pt]{minimal}
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\begin{document}$$_{2.996}$$\end{document} and entropy 72.88 J mol-1\documentclass[12pt]{minimal}
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\begin{document}$$^{-1}$$\end{document}; MG54 Mg1.174\documentclass[12pt]{minimal}
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\begin{document}$$_{1.174}$$\end{document}SiO3.174\documentclass[12pt]{minimal}
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\begin{document}$$_{3.174}$$\end{document} 78.54; MG58 Mg1.364\documentclass[12pt]{minimal}
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\begin{document}$$_{1.364}$$\end{document}SiO3.364\documentclass[12pt]{minimal}
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\begin{document}$$_{3.364}$$\end{document} 85.05; MG62 Mg1.611\documentclass[12pt]{minimal}
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\begin{document}$$_{1.611}$$\end{document}SiO3.611\documentclass[12pt]{minimal}
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\begin{document}$$_{3.611}$$\end{document} 91.40; and MG67 Mg1.907\documentclass[12pt]{minimal}
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\begin{document}$$_{1.907}$$\end{document}SiO3.907\documentclass[12pt]{minimal}
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\begin{document}$$_{3.907}$$\end{document} 102.75. Heat capacity of the glasses is higher than that of the corresponding crystal mixtures below 200 K but plunges below the Cp,crystal\documentclass[12pt]{minimal}
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\begin{document}$$_{p,\mathrm{crystal}}$$\end{document} at higher temperatures. High-temperature Cp\documentclass[12pt]{minimal}
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\begin{document}$$C_p$$\end{document} was measured (by differential scanning calorimetry in the range 300–970 K) for MG50 and MG67 up to ≈\documentclass[12pt]{minimal}
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\begin{document}$$\approx $$\end{document} 1000 K. Using our Cp\documentclass[12pt]{minimal}
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\begin{document}$$C_p$$\end{document} data, selected data for entropies of fusion, Cp\documentclass[12pt]{minimal}
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\begin{document}$$C_p$$\end{document} of crystals, and fictive temperatures, the configurational entropy (Sconf\documentclass[12pt]{minimal}
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\begin{document}$$S_\mathrm{conf}$$\end{document}) at glass transition temperature (Tg\documentclass[12pt]{minimal}
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\begin{document}$$T_\mathrm{g}$$\end{document}) were calculated. For the near-forsterite glass MG67, the Sconf\documentclass[12pt]{minimal}
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\begin{document}$$S_\mathrm{conf}$$\end{document} is 1.9 J mol-1\documentclass[12pt]{minimal}
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\begin{document}$$T_\mathrm{g}$$\end{document} = 1040 K. As this small value is a difference of several large numbers, its uncertainty is relatively high; we consider a conservative estimate of 15 J mol-1\documentclass[12pt]{minimal}
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\begin{document}$$^{-1}$$\end{document}. Using the expression logη=A+B/[TSconf(T)]\documentclass[12pt]{minimal}
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\begin{document}$$\log \eta = A + B/[T S_\mathrm{conf}(T)]$$\end{document}, the available experimental viscosities (η\documentclass[12pt]{minimal}
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\begin{document}$$\eta $$\end{document}) and the temperature-dependent configurational entropy from our work, we refined the parameters A=-2.34\documentclass[12pt]{minimal}
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\begin{document}$$A = -2.34$$\end{document} and B=76,500\documentclass[12pt]{minimal}
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\begin{document}$$B = 76,500$$\end{document} for this equation, with Sconf(T)=1.90+(83.7ln(T/1040))\documentclass[12pt]{minimal}
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\begin{document}$$S_\mathrm{conf} (T) = 1.90+(83.7 \ln (T/1040))$$\end{document}. The configurational entropy for the enstatitic MG50 glass is 16.8 J mol-1\documentclass[12pt]{minimal}
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\begin{document}$$^{-1}$$\end{document} K-1\documentclass[12pt]{minimal}
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\begin{document}$$^{-1}$$\end{document} at Tg\documentclass[12pt]{minimal}
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\begin{document}$$T_\mathrm{g}$$\end{document} = 1063 K. The presented data can be combined with enthalpies of formation and thermophysical properties of Mg-silicate glasses for models that could elucidate geological and geophysical observations in the crust and mantle of the Earth.