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Vesiculation of rhyolite magma in the IDDP-1 borehole at Krafla, Iceland

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Vesiculation of rhyolite magma in the IDDP-1 borehole at Krafla, Iceland. / Trewick, Laura; Tuffen, Hugh; Owen, Jacqueline et al.
Geophysical Research Abstracts. Vol. 18 European Geosciences Union, 2016. EGU2016-10002-1.

Research output: Contribution in Book/Report/Proceedings - With ISBN/ISSNConference contribution/Paperpeer-review

Harvard

Trewick, L, Tuffen, H, Owen, J, Kennedy, BM, Eichelberger, J & Zierenberg, R 2016, Vesiculation of rhyolite magma in the IDDP-1 borehole at Krafla, Iceland. in Geophysical Research Abstracts. vol. 18, EGU2016-10002-1, European Geosciences Union. <http://meetingorganizer.copernicus.org/EGU2016/EGU2016-10002-1.pdf>

APA

Trewick, L., Tuffen, H., Owen, J., Kennedy, B. M., Eichelberger, J., & Zierenberg, R. (2016). Vesiculation of rhyolite magma in the IDDP-1 borehole at Krafla, Iceland. In Geophysical Research Abstracts (Vol. 18). Article EGU2016-10002-1 European Geosciences Union. http://meetingorganizer.copernicus.org/EGU2016/EGU2016-10002-1.pdf

Vancouver

Trewick L, Tuffen H, Owen J, Kennedy BM, Eichelberger J, Zierenberg R. Vesiculation of rhyolite magma in the IDDP-1 borehole at Krafla, Iceland. In Geophysical Research Abstracts. Vol. 18. European Geosciences Union. 2016. EGU2016-10002-1

Author

Trewick, Laura ; Tuffen, Hugh ; Owen, Jacqueline et al. / Vesiculation of rhyolite magma in the IDDP-1 borehole at Krafla, Iceland. Geophysical Research Abstracts. Vol. 18 European Geosciences Union, 2016.

Bibtex

@inproceedings{7ebecd0bed8843798dcf5d185ac8d4b7,
title = "Vesiculation of rhyolite magma in the IDDP-1 borehole at Krafla, Iceland",
abstract = "In 2009 the IDDP-1 borehole at Krafla, Iceland unexpectedly intersected rhyolitic magma at 2.1 km depth [1,2], providing unprecedented opportunities to investigate silicic melt formation and storage, and potential for powerful geothermal energy production. A key objective is to constrain the nature of the rhyolitic melt and its response to drilling. As no intact core was extracted, evidence is fragmental - from glassy rhyolitic clasts retrieved from the cuttings. These exhibit a range of glass colours, vesicularities and phenocryst contents [1,2]. Here we use benchtop infra-red spectroscopy and petrological microscopy to characterise the H2O concentrations and bubble number densities within diverse glassy clasts, complemented by 1 Atm bubble growth experiments with a heated stage to investigate vesicle growth. Juvenile glassy clasts were divided into three categories (brown>banded>very dark glass). H2O concentrations within clasts showed some spatial variability, with enrichment towards bubble-rich areas that may be resorption-related but could not be adequately characterised with a benchtop source. However, mean values ranged from 1.41-1.68 wt %, with no statistically significant difference between clast types. This is broadly consistent with previous studies [1,2]. Bubble growth rates in all clast types were determined during isothermal dwells at 600, 650 and 700 C, for which bubbles grew at 0.03-0.09, 0.11-0.31, and 0.46-0.82 m s-1 respectively. The highest growth rates were measured for the most water-rich clast analysed - a banded clast with mean H2O of 1.68 wt %, and initially-larger bubbles also grew more rapidly. Measured bubble number densities (BNDs) range from 10[11.7] m-3 in banded clasts to 10[13.1] m-3 in very dark clasts, corresponding to decompression rates of 0.1-1 MPa/s [3], although experimentation on IDDP-1 magma is needed to properly calibrate BNDs as a decompression rate meter. Nonetheless, such decompression rates suggest nucleation occurred over tens-hundreds of seconds, as pressure dropped from magmastatic towards lower borehole values. The duration of vesicle growth was roughly estimated from measured bubble sizes, which range from 5 m in very dark clasts to 30 m in banded clasts, and extrapolated bubble growth rates at magmatic temperature (900 C) and appropriate pressure. Results suggest only brief pre-quenching growth occurred, over seconds. We therefore propose that magma adjacent to the drill head experienced decompression prior to interception, leading to a brief period of bubble nucleation and a briefer period of growth prior to fragmentation and quenching. The high bubble strain, low bubble number density and largest bubble sizes in banded clasts all point towards slower decompression and more protracted viscous flow in this part of the rhyolitic magma. However, better temporal constraints are required on the extraction of distinct clast types to determine how magma response evolved through time, and better piece together this enigmatic magmatic jigsaw.",
author = "Laura Trewick and Hugh Tuffen and Jacqueline Owen and Kennedy, {Ben M.} and John Eichelberger and Robert Zierenberg",
year = "2016",
month = apr,
day = "15",
language = "English",
volume = "18",
booktitle = "Geophysical Research Abstracts",
publisher = "European Geosciences Union",

}

RIS

TY - GEN

T1 - Vesiculation of rhyolite magma in the IDDP-1 borehole at Krafla, Iceland

AU - Trewick, Laura

AU - Tuffen, Hugh

AU - Owen, Jacqueline

AU - Kennedy, Ben M.

AU - Eichelberger, John

AU - Zierenberg, Robert

PY - 2016/4/15

Y1 - 2016/4/15

N2 - In 2009 the IDDP-1 borehole at Krafla, Iceland unexpectedly intersected rhyolitic magma at 2.1 km depth [1,2], providing unprecedented opportunities to investigate silicic melt formation and storage, and potential for powerful geothermal energy production. A key objective is to constrain the nature of the rhyolitic melt and its response to drilling. As no intact core was extracted, evidence is fragmental - from glassy rhyolitic clasts retrieved from the cuttings. These exhibit a range of glass colours, vesicularities and phenocryst contents [1,2]. Here we use benchtop infra-red spectroscopy and petrological microscopy to characterise the H2O concentrations and bubble number densities within diverse glassy clasts, complemented by 1 Atm bubble growth experiments with a heated stage to investigate vesicle growth. Juvenile glassy clasts were divided into three categories (brown>banded>very dark glass). H2O concentrations within clasts showed some spatial variability, with enrichment towards bubble-rich areas that may be resorption-related but could not be adequately characterised with a benchtop source. However, mean values ranged from 1.41-1.68 wt %, with no statistically significant difference between clast types. This is broadly consistent with previous studies [1,2]. Bubble growth rates in all clast types were determined during isothermal dwells at 600, 650 and 700 C, for which bubbles grew at 0.03-0.09, 0.11-0.31, and 0.46-0.82 m s-1 respectively. The highest growth rates were measured for the most water-rich clast analysed - a banded clast with mean H2O of 1.68 wt %, and initially-larger bubbles also grew more rapidly. Measured bubble number densities (BNDs) range from 10[11.7] m-3 in banded clasts to 10[13.1] m-3 in very dark clasts, corresponding to decompression rates of 0.1-1 MPa/s [3], although experimentation on IDDP-1 magma is needed to properly calibrate BNDs as a decompression rate meter. Nonetheless, such decompression rates suggest nucleation occurred over tens-hundreds of seconds, as pressure dropped from magmastatic towards lower borehole values. The duration of vesicle growth was roughly estimated from measured bubble sizes, which range from 5 m in very dark clasts to 30 m in banded clasts, and extrapolated bubble growth rates at magmatic temperature (900 C) and appropriate pressure. Results suggest only brief pre-quenching growth occurred, over seconds. We therefore propose that magma adjacent to the drill head experienced decompression prior to interception, leading to a brief period of bubble nucleation and a briefer period of growth prior to fragmentation and quenching. The high bubble strain, low bubble number density and largest bubble sizes in banded clasts all point towards slower decompression and more protracted viscous flow in this part of the rhyolitic magma. However, better temporal constraints are required on the extraction of distinct clast types to determine how magma response evolved through time, and better piece together this enigmatic magmatic jigsaw.

AB - In 2009 the IDDP-1 borehole at Krafla, Iceland unexpectedly intersected rhyolitic magma at 2.1 km depth [1,2], providing unprecedented opportunities to investigate silicic melt formation and storage, and potential for powerful geothermal energy production. A key objective is to constrain the nature of the rhyolitic melt and its response to drilling. As no intact core was extracted, evidence is fragmental - from glassy rhyolitic clasts retrieved from the cuttings. These exhibit a range of glass colours, vesicularities and phenocryst contents [1,2]. Here we use benchtop infra-red spectroscopy and petrological microscopy to characterise the H2O concentrations and bubble number densities within diverse glassy clasts, complemented by 1 Atm bubble growth experiments with a heated stage to investigate vesicle growth. Juvenile glassy clasts were divided into three categories (brown>banded>very dark glass). H2O concentrations within clasts showed some spatial variability, with enrichment towards bubble-rich areas that may be resorption-related but could not be adequately characterised with a benchtop source. However, mean values ranged from 1.41-1.68 wt %, with no statistically significant difference between clast types. This is broadly consistent with previous studies [1,2]. Bubble growth rates in all clast types were determined during isothermal dwells at 600, 650 and 700 C, for which bubbles grew at 0.03-0.09, 0.11-0.31, and 0.46-0.82 m s-1 respectively. The highest growth rates were measured for the most water-rich clast analysed - a banded clast with mean H2O of 1.68 wt %, and initially-larger bubbles also grew more rapidly. Measured bubble number densities (BNDs) range from 10[11.7] m-3 in banded clasts to 10[13.1] m-3 in very dark clasts, corresponding to decompression rates of 0.1-1 MPa/s [3], although experimentation on IDDP-1 magma is needed to properly calibrate BNDs as a decompression rate meter. Nonetheless, such decompression rates suggest nucleation occurred over tens-hundreds of seconds, as pressure dropped from magmastatic towards lower borehole values. The duration of vesicle growth was roughly estimated from measured bubble sizes, which range from 5 m in very dark clasts to 30 m in banded clasts, and extrapolated bubble growth rates at magmatic temperature (900 C) and appropriate pressure. Results suggest only brief pre-quenching growth occurred, over seconds. We therefore propose that magma adjacent to the drill head experienced decompression prior to interception, leading to a brief period of bubble nucleation and a briefer period of growth prior to fragmentation and quenching. The high bubble strain, low bubble number density and largest bubble sizes in banded clasts all point towards slower decompression and more protracted viscous flow in this part of the rhyolitic magma. However, better temporal constraints are required on the extraction of distinct clast types to determine how magma response evolved through time, and better piece together this enigmatic magmatic jigsaw.

M3 - Conference contribution/Paper

VL - 18

BT - Geophysical Research Abstracts

PB - European Geosciences Union

ER -