scholarly journals A Two-stage Thermal Evolution Model of Magmas in Continental Crust

1999 ◽  
Vol 40 (2) ◽  
pp. 241-254 ◽  
Author(s):  
T. Koyaguchi ◽  
K. Kaneko
2020 ◽  
Vol 125 ◽  
pp. 103681
Author(s):  
Florent Cheval-Garabédian ◽  
Michel Faure ◽  
Eric Marcoux ◽  
Jérome Gouin ◽  
Maxime Picault

Icarus ◽  
2013 ◽  
Vol 226 (1) ◽  
pp. 212-228 ◽  
Author(s):  
S. Henke ◽  
H.-P. Gail ◽  
M. Trieloff ◽  
W.H. Schwarz

2010 ◽  
Vol 119 (6) ◽  
pp. 1215-1227 ◽  
Author(s):  
Hiroki SENSHU ◽  
Shigenori MARUYAMA ◽  
Shuji RINO

2020 ◽  
Vol 643 ◽  
pp. A44
Author(s):  
Rob J. Spaargaren ◽  
Maxim D. Ballmer ◽  
Dan J. Bower ◽  
Caroline Dorn ◽  
Paul J. Tackley

Aims. The secondary atmospheres of terrestrial planets form and evolve as a consequence of interaction with the interior over geological time. We aim to quantify the influence of planetary bulk composition on the interior–atmosphere evolution for Earth-sized terrestrial planets to aid in the interpretation of future observations of terrestrial exoplanet atmospheres. Methods. We used a geochemical model to determine the major-element composition of planetary interiors (MgO, FeO, and SiO2) following the crystallization of a magma ocean after planet formation, predicting a compositional profile of the interior as an initial condition for our long-term thermal evolution model. Our 1D evolution model predicts the pressure–temperature structure of the interior, which we used to evaluate near-surface melt production and subsequent volatile outgassing. Volatiles are exchanged between the interior and atmosphere according to mass conservation. Results. Based on stellar compositions reported in the Hypatia catalog, we predict that about half of rocky exoplanets have a mantle that convects as a single layer (whole-mantle convection), and the other half exhibit double-layered convection due to the presence of a mid-mantle compositional boundary. Double-layered convection is more likely for planets with high bulk planetary Fe-content and low Mg/Si-ratio. We find that planets with low Mg/Si-ratio tend to cool slowly because their mantle viscosity is high. Accordingly, low-Mg/Si planets also tend to lose volatiles swiftly through extensive melting. Moreover, the dynamic regime of the lithosphere (plate tectonics vs. stagnant lid) has a first-order influence on the thermal evolution and volatile cycling. These results suggest that the composition of terrestrial exoplanetary atmospheres can provide information on the dynamic regime of the lithosphere and the thermo-chemical evolution of the interior.


2019 ◽  
Vol 628 ◽  
pp. A77
Author(s):  
Hans-Peter Gail ◽  
Mario Trieloff

Context. The cooling history of individual meteorites can be reconstructed if closure temperatures and closure ages of different radioisotopic chronometers are available for a couple of meteorites. If a close similarity in chemical and isotopic composition suggests a common origin from the same parent body, some basic properties of this body can be derived. Aims. The radius of the L chondrite parent body, its formation time, and its evolution history are determined by fitting theoretical models to empirical data of radioisotopic chronometers for L chondrites. Methods. A simplified evolution model for the L chondrite parent body was constructed considering sintering of the initially porous material, temperature dependent heat conductivity, and an insulating regolith layer. Such models were fitted to thermochronological data of five meteorites for which precise data for the Hf-W and U-Pb-Pb thermochronometers have been published. Results. A set of parameters for the L chondrite parent body is found that yields excellent agreement (within error bounds) between a thermal evolution model and thermochonological data of five examined L chondrites. Empirical cooling rate data also agree with the model results within error bounds such that there is no conflict between cooling rate data and the onion-shell model. Two models are found to be compatible with the presently available empirical data: one model with a radius of 115 km and a formation time of 1.89 Ma after CAI formation, and another model with 160 km radius and formation time of 1.835 Ma. The central temperature of the smaller body remains well below the Ni,Fe-FeS eutectic melting temperature and is consistent with the apparent non-existence of primitive achondrites related to the L chondrites. For the bigger model, incipient melting in the central core region is predicted, which opens the possibility that primitive achondrites related to L chondrites could be found.


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