Abstract
Volcanic materials can experience up to eleven orders of magnitude of cooling rate (qc) starting from 10–5 K s−1. The glassy component of volcanic material is routinely measured via differential scanning calorimeter (DSC) to obtain qc through the determination of the glass fictive temperature (Tf). Conventional DSC (C-DSC), which has been employed for decades, can only access a relatively small range of qc (from ~ 10–2 to ~ 1 K s−1). Therefore, extrapolations up to six orders of magnitude of C-DSC data are necessary to derive qc of glasses quenched both at extremely low and high qc. Here, we test the reliability of such extrapolations by combining C-DSC with the recently introduced flash calorimetry (F-DSC). F-DSC enables to extend the qc exploration up to 104 K s−1. We use three synthetic glasses as analogs of volcanic melts. We first apply a normalization procedure of heat flow data for both C-DSC and F-DSC to derive Tf as a function of experimental qc, following the “unified area-matching” approach. The obtained Tf–qc relationship shows that Arrhenius models, widely adopted in previous studies, are only valid for qc determination within the calibration range. In contrast, a non-Arrhenius model better captures qc values, especially when a significant extrapolation is required. We, therefore, present a practical “how-to” protocol for estimating qc using DSC.
Highlights
IntroductionThe estimation of the cooling rate (qc) embedded in volcanic glasses is pivotal for the reconstruction of their petrogenesis
Motivation and aimsThe estimation of the cooling rate embedded in volcanic glasses is pivotal for the reconstruction of their petrogenesis (Wilding et al 1995, 1996a, b, 2000, 2004; Gottsmann and Dingwell 2001a, b, 2002; Gottsmann et al 2004; PotuzakCommunicated by Mark S Ghiorso.Here we present a combined conventional and flash differential scanning calorimetry (C-differential scanning calorimeter (DSC) and F-DSC) calibration by subjecting for the first time silicate melts of interest for volcanic processes to qc ranging between 0.08 and 30,000 K s−1
The non-Arr η Μοdel requires a priori knowledge of the viscosity–temperature relation, whereas, in non-Arr Conventional DSC (C-DSC) and non-Arr C-DSC + F-DSC Models, this relationship is internally calibrated based on DSC measurements
Summary
The estimation of the cooling rate (qc) embedded in volcanic glasses is pivotal for the reconstruction of their petrogenesis We present a combined conventional and flash differential scanning calorimetry (C-DSC and F-DSC) calibration by subjecting for the first time silicate melts of interest for volcanic processes to qc ranging between 0.08 and 30,000 K s−1. We significantly exceed the interval of qc previously investigated in geospeedometry studies (~ 1 0–2 to ~ 1 K s−1) and explore the validity of previous extrapolations from the relatively slow experimental qc to the realm (> 10 K s−1) of the submarine and explosive volcanism (e.g., Potuzak et al 2008; Nickols et al 2009). We provide a practical “howto” guide to calculating the cooling rate of volcanic glasses.
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