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19 Orientation of long axis for each phase derived from FOAMS analysis for M490. 90° correspond to the vertical axis of sample cylinder and 0° is perpendicular sample cylinder axis ,
, *l-1,4)+result(2*l,4))/2; %frequency average Sf = 1*10^(-6), f=, issue.2
, % phi1-phi2 %if some functions are missing, please contact D.Freitas Sphi=(sqrt(SphiTC1^2+SphiTC2^2))*pi()/180;% std on phi (1s) while phi<0 %important step to keep the phase shift phi=abs
, *P^2+25.019*P+3225.5+temperature*(-0.11749); %calculated from Li and Li, 2007.
/(temperature^2))/0.14069; % heat capacity, 1991. ,
,
, -alpha*(temperature-298.15)+P/K)^(-1/3); %calculation of size variations Sd = sqrt(((1-alpha*(temperature-298.15)+P/K)^(-1/3))^2*Sd0^2
M525 -166b (4 GPa) experimental procedure with temperature history with time and power/temperature calibration. Microphotographs of recovered sample are provided perpendicular (left) and parallel (right) to sample cylinder axis ,
Phase shift (first raw), amplitude ratio (third raw) and inferred diffusivities (second and fourth raw respectively), are represented as function of temperature and frequency ,
Phase shift (first raw), amplitude ratio (third raw) and inferred diffusivities (second and fourth raw respectively), are represented as function of temperature and frequency ,