Figure 10.
![Measurements at ${P_{{\rm{eff}}}} = [ {5,\,\,15} ]$ MPa under a pore pressure ${P_{\rm{P}}} = 1.2$ MPa, showing the frequency dependence of Young's modulus E, Young's attenuation $Q_{\rm{E}}^{ - 1}$, and inferred elastic moduli in the fully glycerine-saturated sandstone sample at temperatures of (a)–(d) ${23^{\rm{o}}}\,{\rm{C}}$, (e)–(h) ${10^{\rm{o}}}\,{\rm{C}}$ and (i)–(l) ${3^{\rm{o}}}\,{\rm{C}}$. Solid curves in graphs (a), (e), and (i) represent a parametric fit to the experimental measurements based on the Kramers–Kronig relationship. Note that each symbol of open circle (ο) from Pair 1# and cross (×) from Pair 2# represents the mean measurement of three experiments, with corresponding error bars illustrated.](https://oup.silverchair-cdn.com/oup/backfile/Content_public/Journal/gji/240/2/10.1093_gji_ggae442/2/ggae442fig10.jpeg?Expires=1750224313&Signature=FsY-z6rFJTrOeraF0wBG7OMf2evPtd73Uq5DvuVb9FRIOWzBb52No~JkK1EBs-0EcDp1Cb8Oxzw6mL4bXmfkYq7YmvxwBHVYanMCoJ9KnJsx-3IxAMKyVsdlJkKww9EI3YjsjOKUpfWEfdnUdL92axElJz2iI5m-RgZZlqR86F~hnFsLnNfTRpx-fAwWI7kcCOtM2KMdO2RmEzgJG6Wm2pE89HUTcO4LxgTg83sKhdFsCfBfPwW7uWZ~IgFtGH5aeiaSWqBiFtQ3FJhkfhnHEmu0PH7pIJ0baSUyo8YfrRe0nZahJWP1OW2ZTaaRcicuytvyUdq9~l2-cKr98wlBdQ__&Key-Pair-Id=APKAIE5G5CRDK6RD3PGA)
Measurements at |${P_{{\rm{eff}}}} = [ {5,\,\,15} ]$| MPa under a pore pressure |${P_{\rm{P}}} = 1.2$| MPa, showing the frequency dependence of Young's modulus E, Young's attenuation |$Q_{\rm{E}}^{ - 1}$|, and inferred elastic moduli in the fully glycerine-saturated sandstone sample at temperatures of (a)–(d) |${23^{\rm{o}}}\,{\rm{C}}$|, (e)–(h) |${10^{\rm{o}}}\,{\rm{C}}$| and (i)–(l) |${3^{\rm{o}}}\,{\rm{C}}$|. Solid curves in graphs (a), (e), and (i) represent a parametric fit to the experimental measurements based on the Kramers–Kronig relationship. Note that each symbol of open circle (ο) from Pair 1# and cross (×) from Pair 2# represents the mean measurement of three experiments, with corresponding error bars illustrated.
