Investigating Influences on the Pb Pseudo‐Isochron Using Three‐Dimensional Mantle Convection Models With a Continental Reservoir

Abstract For mid‐ocean ridge basalts and ocean island basalts, measurements of Pb isotope ratios show broad linear correlations with a certain degree of scatter. In 207Pb/204Pb—206Pb/204Pb space, the best fit line defines a pseudo‐isochron age (τPb) of ∼1.9 Gyr. Previous modeling suggests a relative...

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Main Authors: James Panton, J. Huw Davies, Tim Elliott, Morten Andersen, Don Porcelli, Matthew G. Price
Format: Article
Language:English
Published: Wiley 2022-08-01
Series:Geochemistry, Geophysics, Geosystems
Subjects:
Online Access:https://doi.org/10.1029/2021GC010309
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author James Panton
J. Huw Davies
Tim Elliott
Morten Andersen
Don Porcelli
Matthew G. Price
author_facet James Panton
J. Huw Davies
Tim Elliott
Morten Andersen
Don Porcelli
Matthew G. Price
author_sort James Panton
collection DOAJ
description Abstract For mid‐ocean ridge basalts and ocean island basalts, measurements of Pb isotope ratios show broad linear correlations with a certain degree of scatter. In 207Pb/204Pb—206Pb/204Pb space, the best fit line defines a pseudo‐isochron age (τPb) of ∼1.9 Gyr. Previous modeling suggests a relative change in the behaviors of U and Pb between 2.25 and 2.5 Ga, resulting in net recycling of HIMU (high U/Pb) material in the latter part of Earth's history, to explain the observed τPb. However, simulations in which fractionation is controlled by a single set of partition coefficients throughout the model runs fail to reproduce τPb and the observed scatter in Pb isotope ratios. We build on these models with 3D mantle convection simulations including parameterizations for melting, U recycling from the continents and preferential removal of Pb from subducted oceanic crust. We find that both U recycling after the great oxygenation event and Pb extraction after the onset of plate tectonics, are required in order to fit the observed gradient and scatter of both the 207Pb/204Pb—206Pb/204Pb and 208Pb/204Pb—206Pb/204Pb arrays. Unlike much previous work, our model does not require accumulations of subducted oceanic crust to persist at the core‐mantle boundary for long periods of time in order to match geochemical observations.
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spelling doaj-art-0636248c2e6d4c5d9defbd95f19330fb2025-08-20T02:08:11ZengWileyGeochemistry, Geophysics, Geosystems1525-20272022-08-01238n/an/a10.1029/2021GC010309Investigating Influences on the Pb Pseudo‐Isochron Using Three‐Dimensional Mantle Convection Models With a Continental ReservoirJames Panton0J. Huw Davies1Tim Elliott2Morten Andersen3Don Porcelli4Matthew G. Price5School of Earth and Environmental Sciences Cardiff University Cardiff UKSchool of Earth and Environmental Sciences Cardiff University Cardiff UKSchool of Earth Sciences University of Bristol Bristol UKSchool of Earth and Environmental Sciences Cardiff University Cardiff UKDepartment of Earth Sciences University of Oxford Oxford UKSchool of Earth and Environmental Sciences Cardiff University Cardiff UKAbstract For mid‐ocean ridge basalts and ocean island basalts, measurements of Pb isotope ratios show broad linear correlations with a certain degree of scatter. In 207Pb/204Pb—206Pb/204Pb space, the best fit line defines a pseudo‐isochron age (τPb) of ∼1.9 Gyr. Previous modeling suggests a relative change in the behaviors of U and Pb between 2.25 and 2.5 Ga, resulting in net recycling of HIMU (high U/Pb) material in the latter part of Earth's history, to explain the observed τPb. However, simulations in which fractionation is controlled by a single set of partition coefficients throughout the model runs fail to reproduce τPb and the observed scatter in Pb isotope ratios. We build on these models with 3D mantle convection simulations including parameterizations for melting, U recycling from the continents and preferential removal of Pb from subducted oceanic crust. We find that both U recycling after the great oxygenation event and Pb extraction after the onset of plate tectonics, are required in order to fit the observed gradient and scatter of both the 207Pb/204Pb—206Pb/204Pb and 208Pb/204Pb—206Pb/204Pb arrays. Unlike much previous work, our model does not require accumulations of subducted oceanic crust to persist at the core‐mantle boundary for long periods of time in order to match geochemical observations.https://doi.org/10.1029/2021GC010309mantle convectionmantle modelPb pseudo‐isochronrecycled oceanic crust
spellingShingle James Panton
J. Huw Davies
Tim Elliott
Morten Andersen
Don Porcelli
Matthew G. Price
Investigating Influences on the Pb Pseudo‐Isochron Using Three‐Dimensional Mantle Convection Models With a Continental Reservoir
Geochemistry, Geophysics, Geosystems
mantle convection
mantle model
Pb pseudo‐isochron
recycled oceanic crust
title Investigating Influences on the Pb Pseudo‐Isochron Using Three‐Dimensional Mantle Convection Models With a Continental Reservoir
title_full Investigating Influences on the Pb Pseudo‐Isochron Using Three‐Dimensional Mantle Convection Models With a Continental Reservoir
title_fullStr Investigating Influences on the Pb Pseudo‐Isochron Using Three‐Dimensional Mantle Convection Models With a Continental Reservoir
title_full_unstemmed Investigating Influences on the Pb Pseudo‐Isochron Using Three‐Dimensional Mantle Convection Models With a Continental Reservoir
title_short Investigating Influences on the Pb Pseudo‐Isochron Using Three‐Dimensional Mantle Convection Models With a Continental Reservoir
title_sort investigating influences on the pb pseudo isochron using three dimensional mantle convection models with a continental reservoir
topic mantle convection
mantle model
Pb pseudo‐isochron
recycled oceanic crust
url https://doi.org/10.1029/2021GC010309
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