Javascript must be enabled to continue!
An overview of the geochemistry and petrology of the mantle-sourced Fagradalsfjall eruption, Iceland
View through CrossRef
<p>The recent eruption of the Fagradalsfjall complex in the Reykjanes Peninsula of Iceland represents incompletely mixed basaltic magma directly erupted from a sub-crustal storage region. The eruption comprises olivine tholeiite lava with whole rock MgO between 8.7 and 10.1 wt%. The macrocryst cargo comprises olivine up to Fo<sub>90</sub>, plagioclase up to An<sub>89</sub>, and Cr-rich clinopyroxene up to Mg# 89. Gabbro and anorthosite xenoliths are rare. Olivine-plagioclase-augite-melt (OPAM) barometry of the groundmass glass from tephra collected from 28<sup>th</sup> April to 6<sup>th</sup> May yield high equilibration pressures and suggest that this eruption is originally sourced from a deep (0.48&#177;0.06 GPa) storage zone at the crust-mantle boundary.</p><p>&#160;</p><p>Over the course of the eruption, Fagradalsfjall lavas have changed significantly in source signature. The first erupted lavas (mid-March) were more depleted (K<sub>2</sub>O/TiO<sub>2</sub> &#173;= 0.14, La/Sm = 2.1, <sup>87</sup>Sr/<sup>86</sup>Sr = 0.703108, <sup>143</sup>Nd/<sup>144</sup>Nd = 0.513017, <sup>206</sup>Pb/<sup>204</sup>Pb = 18.730) and similar in composition to basalts previously erupted on the Reykjanes Peninsula. As the eruption continued, the lavas became increasingly enriched and were most enriched in early May (K<sub>2</sub>O/TiO<sub>2</sub> = 0.27, La/Sm = 3.1, <sup>87</sup>Sr/<sup>86</sup>Sr = 0.703183, <sup>143</sup>Nd/<sup>144</sup>Nd = 0.512949, <sup>206</sup>Pb/<sup>204</sup>Pb = 18.839), having unusual compositions for Reykjanes Peninsula lavas and similar only to enriched Reykjanes melt inclusions. From early May until the end of the eruption (18<sup>th</sup> September), the lava K<sub>2</sub>O/TiO<sub>2</sub> and La/Sm compositions displayed a sinuous wobble through time at lower amplitude than observed in the early part of the eruption. The enriched lavas produced later in the eruption are more enriched than lavas from Stapafell, a Reykjanes eruption thought to represent the enriched endmember on the Reykjanes. The full range of compositional variation observed in the eruption is large &#8211; about 2.5 times the combined variation of all other historic Reykjanes lavas.</p><p>&#160;</p><p>The major, trace, and radiogenic isotope compositions indicate that binary mixing controls the erupted basalt compositions. The mixing endmembers appear to be depleted Reykjanes melts, and enriched melts with compositions similar to enriched Reykjanes melt inclusions or Snaefellsnes alkali basalts. The physical mechanism of mixing and the structure of the crust-mantle boundary magmatic system is a task for future study.</p><p>&#160;</p><p>In contrast to the geochemical variations described above, the oxygen isotope composition (&#948;<sup>18</sup>O) of the groundmass glass (5.1&#177;0.1&#8240;) has little variation and is lower than MORB (~5.5&#8240;). Olivine phenocrysts &#948;<sup>18</sup>O &#160;values range from typical mantle peridotite values (5.1&#8240;) to lower values (4.6&#8240;), with the lower values in close equilibrium with the host melt. Given the crust-mantle boundary source of the eruption, these low &#948;<sup>18</sup>O values are unlikely to represent crustal contamination, and are more likely to represent an intrinsically low &#948;<sup>18</sup>O mantle beneath the Reykjanes Peninsula.</p>
Title: An overview of the geochemistry and petrology of the mantle-sourced Fagradalsfjall eruption, Iceland
Description:
<p>The recent eruption of the Fagradalsfjall complex in the Reykjanes Peninsula of Iceland represents incompletely mixed basaltic magma directly erupted from a sub-crustal storage region.
The eruption comprises olivine tholeiite lava with whole rock MgO between 8.
7 and 10.
1 wt%.
The macrocryst cargo comprises olivine up to Fo<sub>90</sub>, plagioclase up to An<sub>89</sub>, and Cr-rich clinopyroxene up to Mg# 89.
Gabbro and anorthosite xenoliths are rare.
Olivine-plagioclase-augite-melt (OPAM) barometry of the groundmass glass from tephra collected from 28<sup>th</sup> April to 6<sup>th</sup> May yield high equilibration pressures and suggest that this eruption is originally sourced from a deep (0.
48&#177;0.
06 GPa) storage zone at the crust-mantle boundary.
</p><p>&#160;</p><p>Over the course of the eruption, Fagradalsfjall lavas have changed significantly in source signature.
The first erupted lavas (mid-March) were more depleted (K<sub>2</sub>O/TiO<sub>2</sub> &#173;= 0.
14, La/Sm = 2.
1, <sup>87</sup>Sr/<sup>86</sup>Sr = 0.
703108, <sup>143</sup>Nd/<sup>144</sup>Nd = 0.
513017, <sup>206</sup>Pb/<sup>204</sup>Pb = 18.
730) and similar in composition to basalts previously erupted on the Reykjanes Peninsula.
As the eruption continued, the lavas became increasingly enriched and were most enriched in early May (K<sub>2</sub>O/TiO<sub>2</sub> = 0.
27, La/Sm = 3.
1, <sup>87</sup>Sr/<sup>86</sup>Sr = 0.
703183, <sup>143</sup>Nd/<sup>144</sup>Nd = 0.
512949, <sup>206</sup>Pb/<sup>204</sup>Pb = 18.
839), having unusual compositions for Reykjanes Peninsula lavas and similar only to enriched Reykjanes melt inclusions.
From early May until the end of the eruption (18<sup>th</sup> September), the lava K<sub>2</sub>O/TiO<sub>2</sub> and La/Sm compositions displayed a sinuous wobble through time at lower amplitude than observed in the early part of the eruption.
The enriched lavas produced later in the eruption are more enriched than lavas from Stapafell, a Reykjanes eruption thought to represent the enriched endmember on the Reykjanes.
The full range of compositional variation observed in the eruption is large &#8211; about 2.
5 times the combined variation of all other historic Reykjanes lavas.
</p><p>&#160;</p><p>The major, trace, and radiogenic isotope compositions indicate that binary mixing controls the erupted basalt compositions.
The mixing endmembers appear to be depleted Reykjanes melts, and enriched melts with compositions similar to enriched Reykjanes melt inclusions or Snaefellsnes alkali basalts.
The physical mechanism of mixing and the structure of the crust-mantle boundary magmatic system is a task for future study.
</p><p>&#160;</p><p>In contrast to the geochemical variations described above, the oxygen isotope composition (&#948;<sup>18</sup>O) of the groundmass glass (5.
1&#177;0.
1&#8240;) has little variation and is lower than MORB (~5.
5&#8240;).
Olivine phenocrysts &#948;<sup>18</sup>O &#160;values range from typical mantle peridotite values (5.
1&#8240;) to lower values (4.
6&#8240;), with the lower values in close equilibrium with the host melt.
Given the crust-mantle boundary source of the eruption, these low &#948;<sup>18</sup>O values are unlikely to represent crustal contamination, and are more likely to represent an intrinsically low &#948;<sup>18</sup>O mantle beneath the Reykjanes Peninsula.
</p>.
Related Results
The 2021-23 Fagradalsfjall fires: geochemical and petrological insights
The 2021-23 Fagradalsfjall fires: geochemical and petrological insights
After 7000 years of quiescence, three eruptions occurred in 2021, 2022 and 2023 AD in the Fagradalsfjall volcanic system, in Reykjanes peninsula in southwest Iceland. Looking at th...
Feedbacks between a non-Newtonian upper mantle, mantle viscosity structure and mantle dynamics
Feedbacks between a non-Newtonian upper mantle, mantle viscosity structure and mantle dynamics
SUMMARY
Previous studies have shown that a low viscosity upper mantle can impact the wavelength of mantle flow and the balance of plate driving to resisting force...
Kinematics and flow patterns in deep mantle and upper mantle subduction models: Influence of the mantle depth and slab to mantle viscosity ratio
Kinematics and flow patterns in deep mantle and upper mantle subduction models: Influence of the mantle depth and slab to mantle viscosity ratio
Three‐dimensional fluid dynamic laboratory simulations are presented that investigate the subduction process in two mantle models, an upper mantle model and a deep mantle model, an...
Numerical modelling of mantle exhumation in inverted rift systems
Numerical modelling of mantle exhumation in inverted rift systems
The tectonic exhumation of mantle material is a well-known phenomenon and may occur during both rifting and subsequent (large-scale) basin inversion. However, the processes leading...
Imaging of the Mantle Transition Zone with SS Precursors in the Iceland-Mid-Atlantic Ridge Region
Imaging of the Mantle Transition Zone with SS Precursors in the Iceland-Mid-Atlantic Ridge Region
The nature of Iceland hotspot, located on the Mid-Atlantic Ridge, has been subject of contentious debate. Earlier seismic tomographic studies have suggested the presence of a deep ...
A study of the mantle flow field and lithospheric deformation beneath the Kuril-Kamchatka subduction zone using seismic anisotropy
A study of the mantle flow field and lithospheric deformation beneath the Kuril-Kamchatka subduction zone using seismic anisotropy
We investigate the flow field and deformation in the mantle wedge and subslab mantle beneath the Kuril-Kamchatka subduction zone using seismological data from a recently deployed s...
Heterogeneous lithospheric mantle
Heterogeneous lithospheric mantle
<p>The lithosphere is a thermal boundary layer atop mantle convection and a chemical boundary layer formed by mantle differentiation and melt extraction. The two boun...
On the measurement of Sdiff splitting caused by lowermost mantle anisotropy
On the measurement of Sdiff splitting caused by lowermost mantle anisotropy
Seismic anisotropy has been detected at many depths of the Earth,
including its upper layers, the lowermost mantle, and the inner core.
While upper mantle seismic anisotropy is rel...

