Water in cratonic lithosphere: Calibrating laboratory-determined models of electrical conductivity of mantle minerals using geophysical and petrological observations



[1] Measurements of electrical conductivity of “slightly damp” mantle minerals from different laboratories are inconsistent, requiring geophysicists to make choices between them when interpreting their electrical observations. These choices lead to dramatically different conclusions about the amount of water in the mantle, resulting in conflicting conclusions regarding rheological conditions; this impacts on our understanding of mantle convection, among other processes. To attempt to reconcile these differences, we test the laboratory-derived proton conduction models by choosing the simplest petrological scenario possible – cratonic lithosphere – from two locations in southern Africa where we have the most complete knowledge. We compare and contrast the models with field observations of electrical conductivity and of the amount of water in olivine and show that none of the models for proton conduction in olivine proposed by three laboratories are consistent with the field observations. We derive statistically model parameters of the general proton conduction equation that satisfy the observations. The pre-exponent dry proton conduction term (σ0) and the activation enthalpy (ΔHwet) are derived with tight bounds, and are both within the broader 2σ errors of the different laboratory measurements. The two other terms used by the experimentalists, one to describe proton hopping (exponent ron pre-exponent water contentCw) and the other to describe H2O concentration-dependent activation enthalpy (termαCw1/3 added to the activation energy), are less well defined and further field geophysical and petrological observations are required, especially in regions of higher temperature and higher water content.

1. Introduction

[2] Water within the “solid” Earth has played, and continues to play, a dominant role in shaping our planet [Hirschmann and Kohlstedt, 2012]. Yet, despite the amount of water in the mantle being estimated to be of order of that in the hydrosphere [Bell and Rossman, 1992; Ingrin and Skogby, 2000], we know surprisingly little about its distribution. It is only within the last two to three decades that mineral physicists have established that most nominally anhydrous minerals (NAMs) can absorb water, or rather hydroxyl, to levels of up to some hundreds ppm (see special issue of Reviews of Mineralogy and Geochemistry, 62, 2006 [Keppler and Smyth, 2006]), since the original proposal by Martin and Donnay [1972] and the landmark experiments by Bai and Kohlstedt [1992] (see News and Views comment by Bell [1992]). The presence of water in NAMs has a disproportionately large effect on many crucial physical and chemical properties of mantle minerals [e.g., Thompson, 1992; Hirth and Kohlstedt, 1996; Williams and Hemley, 2001; Peslier, 2010], such as enhancing electrical conductivity [e.g., Karato, 1990], modifying seismic properties [e.g., Jung and Karato, 2001; Karato, 2006], reducing strength [e.g., Karato et al., 1986] and viscosity [e.g., Hirth and Kohlstedt, 1996], facilitating mineral deformation [e.g., Mackwell et al., 1985], lowering the peridotite solidus [e.g., Gaetani and Grove, 1998], and increasing the diffusion rate of other ionic species [e.g., Hier-Majumder et al., 2005]. The presence of hydroxyl point defects in NAMs weakens the Si-O bonds consequently affecting elastic properties, phase equilibria, transport properties and particularly electrical conductivity and viscosity [e.g.,Du Frane and Tyburczy, 2012]. Thus, besides other concerns, geodynamic mantle convection models of our planet are totally reliant on geophysical observations to constrain a largely poorly known, and difficult to know, quantity, but one that critically controls many bulk physical properties. Li et al. [2008] undertook a petrological study of the water content in mantle minerals from xenoliths sourced in lithosphere beneath the Colorado Plateau and southern Basin and Range, and found highest water contents for Colorado Plateau lithosphere and virtually dry olivine beneath San Carlos in the Basin and Range. They interpret their results in terms of implications for viscosity and the recycling of cratonic material. Their paper makes for an excellent tutorial on intricacies of laboratory determination of water content in mantle samples.

[3] As an illustration of the difficulty of remote sensing of water in the mantle using seismology, and pointed out by Karato [2011], different seismic techniques can infer opposing results; the global surface wave study of Meier et al. [2009]suggests that the mantle transition zone (MTZ) beneath eastern Asia is water-poor, whereas the compressional body wave study ofSuetsugu et al. [2006]infers that the MTZ is water-rich in the very same region. This dichotomy is not surprising given that water in NAMs reduces seismic velocity by marginally detectable amounts; 1 wt% water (10,000 ppm) reduces velocity by only ∼1% [Karato, 2006].

[4] The longevity of ancient cratonic lithosphere has been attributed, in part, to internal strength arising from a largely dry composition. Yet petrological evidence is accumulating that, contrary to previously widely held opinion, there is indeed water in NAMs of cratonic lithosphere, at least in its upper part above ∼150 km (coincidently, the approximate depth of the graphite-diamond stability boundary – another important interface for electromagnetic observations).Peslier et al. [2010b] report water contents in olivines of the order of 60–100 ppm in upper mantle lithosphere, with virtually dry olivine in the lower lithosphere, for four regions of the Kaapvaal Craton (the Kimberley region, Jagersfontein, Finch, and Lesotho), based on examination of xenoliths exhumed in kimberlites. This observation is substantiated by a recent study [Baptiste et al., 2012]. Here, we examine whether geophysical observations coupled with laboratory studies support this petrological view, or rather, we take the geophysical observations and the petrological information to test the laboratory-determined parametric descriptions and model parameters.

[5] Deep-probing electromagnetic observations have the potential to image the existence and distribution of water [Karato, 2006], and can significantly contribute to this debate on water in the mantle. Electrical conductivity is a key and unique parameter for detecting water in the mantle, but is somewhat neglected by the geoscientific community. Recent attempts have been made to use laboratory measurements coupled with EM observations to define the water content of the mantle [Khan et al., 2011; Khan and Shankland, 2012]. However, the EM observations must be carefully calibrated by laboratory measurements and, equally as importantly, vice versa.

[6] To perform the latter of these, we compare laboratory measurements of the electrical conductivity of hydrous mantle minerals, particularly olivine, with magnetotelluric observations from two locations in southern Africa where there is xenolith control on composition, water concentration (at one of the locations) and reasonable estimates of probable present-day temperature. We focus on petrological and electromagnetic observations at a depth of 100 km for our study. The choice of this depth is primarily based on optimizing the sensitivity of MT data to absolute resistivity in a moderately resistive mantle beneath a typically conductive crust. By 100 km, the effects of the crustal attenuation are reduced and the true resistivity can usually be resolved [seeJones, 1999, Figure 3]. In Southern Africa, crustal conductivity is nowhere as high as that in Jones [1999, Figure 3], so superior resolution of mantle resistivity is expected (discussed below).

2. Proton Conduction in Hydrous Olivine

[7] Three laboratories, namely those of S.-I. Karato [Wang et al., 2006], T. Yoshino [Yoshino et al., 2009] and B. Poe [Poe et al., 2010], have recently undertaken the very difficult and tedious experiments, and have reported electrical conductivity measurements on hydrous olivine. They and fit their experimental data to an Arrhenius equation of the general form

display math

where k is Boltzmann's constant, T is temperature (in Kelvin), σ0is the pre-exponent dry proton conduction term (in S/m, usually given in terms of its base-10 logarithm),Cw is the water content (in wt ppm H2O), and ΔHwet is the activation enthalpy (in eV). The power term ron the pre-exponent water contentCw is used by the Karato group to describe proton hopping [Karato, 2006], and ranges from 0.50 to 0.75; it is unused (i.e., set to 1) by the Yoshino and Poe groups. The αCw1/3 term is used by the Yoshino and Poe groups to describe H2O concentration-dependent activation enthalpy, with the factor of 1/3 onCw arising from the water activation enthalpy being expected to be proportional to the cubic root of the proton concentration. This term is unused (i.e., α set to 0) by the Karato group and by some other groups who fit models of the form of equation (1) to their data (discussed below). Poe et al. [2010] demonstrate the superiority of fit they obtained by including this α term in “wetter” conditions, i.e., for higher water contents of the order of hundreds to thousands of ppm. The values of the model parameters that the three laboratories report best fit their data are given in Table 1, together with determined errors on each parameter.

Table 1. Parameters for Proton Conduction (Equation (1)) in Hydrous Olivine From Three Different Laboratories and Derived Hereina
Referencelog10 (σ0 [S/m])rΔHwet (eV)αComments
  • a

    Refer to the text for derivations of the “Revised Karato” and “Proposed” parameterizations. The values from Poe et al. [2010, Table 3] have been converted from wt ppm water to wt%. For σ0 this means multiplying by 104then taking the base-10 logarithm. Forα this means multiplying by 21.54 (i.e., (104)1/3). Italic values are implicit. Bold values are used herein.

Wang et al. [2006]3.00 ± 0.40.62 ± 0.150.87 ± 0.050 
Yoshino et al. [2009]1.90 ± 0.4410.92 ± 0.040.16 ± 0.02 
Poe et al. [2010]2.59 ± 0.1611.26 ± 0.041.18 ± 0.04[1 0 0] axis
Poe et al. [2010]3.46 ± 0.0911.50 ± 0.051.43 ± 0.11[0 1 0] axis
Poe et al. [2010]1.02 ± 0.0910.812 ± 0.0160.70 ± 0.015[0 0 1] axis
Fullea et al. [2011]2.35 ± 0.1111.19 ± 0.0351.10 ± 0.055Arithmetic averages of values of Poe et al. [2010]
Revised Karato2.70 ± 0.260.70 ± 0.120.91 ± 0.040 
Proposed herein3.05 ± 0.160.86 ± 0.080.91 ± 0.030.09 ± 0.08 

[8] There is complete agreement between the three laboratories that water significantly enhances the electrical conductivity of hydrous olivine in the mantle by orders of magnitude, but there is strong disagreement about both the strength of the contribution and the mechanism(s) [Huang et al., 2005; Wang et al., 2006; Yoshino et al., 2006; Manthilake et al., 2009; Poe et al., 2010]. Significant debate exists between the groups about their differing results, ranging from experimental procedure to sample handling to data analysis [Karato and Dai, 2009; Yoshino and Katsura, 2009; Yoshino, 2010; Karato, 2011; Karato and Wang, 2012], that are, for the most part, beyond the abilities of the majority of non-specialists to fully appreciate and discriminate between.

[9] Poe et al. [2010] measured electrical conductivity along the three crystallographic axes, and noted electrical anisotropy that increases with increasing water content. Electrical anisotropy, while highly important and a likely indicator of lithospheric fabric and anisotropic flow [Eaton and Jones, 2006], is not considered further herein as the differences in conductivity between the three crystallographic directions are far smaller than the differences between the three laboratories (see Figure 1).

Figure 1.

Proton conduction conductivity in olivine with varying water content (in ppm), from completely dry (0 ppm) to wet (1,000 ppm) at a temperature of 800°C for the three published models of Karato (black line), Yoshino (red line) and Poe (blue lines for along the three crystallographic axes and the average) derived using equation (1) with parameters from Table 1. The revised Karato model (dashed green line) and model proposed herein (solid green line) are also shown (although the latter has only been calibrated in the vicinity of 80 ppm).

[10] Figure 1shows the variation of proton-conduction conductivity with water content, from 0 to 1000 ppm, given byequation (1) with the parameters in Table 1 for a temperature of 800°C. (Note that the Poe measurements [Poe et al., 2010] were made on olivines with higher water contents, from 360 to 2,000 ppm, compared to the Karato [Wang et al., 2006] (predominantly 100–200 ppm) and Yoshino [Yoshino et al., 2009] (all <200 ppm and mostly <100 ppm) ones, and have been extrapolated down to lower water contents using their derived model parameters listed in Table 1.) At low water contents, below 200 ppm, inferred electrical anisotropy is low and the Yoshino and Poe models are in good agreement, but are two orders of magnitude less conductive (more resistive) than the Karato model (Figure 1). As water content increases, anisotropy effects increase in the Poe model, and the Poe conductivities, both individual and average, asymptotically approach the Karato model conductivity, whereas the Yoshino model conductivity remains less conductive than the Karato model conductivity by over 1.5 orders of magnitude (Figure 1). In the following, the “Poe” model refers to the averaged model defined by arithmetically averaging the Poe et al. [2010] parameters listed in Table 1 as used recently by Fullea et al. [2011].

[11] Each of the laboratories derives the errors associated with their model fits to their data, and those errors in the model parameters are listed in Table 1. The possible ranges of permitted conductivities within one sigma from the mean values can be explored by allowing each parameter to maximize or minimize within its one sigma bounds (Figure 2). For the Karato model parameters and defined errors (Figure 2a), the minimum conductivity is given by the lower bound of the pre-exponent conductivityσ0, whereas the maximum conductivity over much of the water content range is given by the lower bound of the activation enthalpy ΔHwet. The maximum range between these minimum and maximum estimates is of order 0.40 log units. For the Yoshino parameters and errors (Figure 2b), the upper and lower conductivity bounds are given by the upper and lower bounds of the pre-exponent conductivityσ0 and the maximum range is also of order half an order of magnitude (0.44 log units). Note that the error in α has little effect on conductivity estimation in the Yoshino model; this is because α is almost negligibly small. For the Poe averaged parameters (Figure 2c), with its more tightly defined errors, the bounds are given by the bounds on the activation enthalpy. Here the maximum range is smaller and of order 0.16 log units.

Figure 2.

Conductivities from the three models at the bound limits for each of the model parameters (see Table 1). (a) Conductivities for the Karato model varying σ0, r and ΔHwet to their respective bounds. Conductivities for the (b) Yoshino and (c) Poe models varying σ0, ΔHwet and α to their respective bounds.

[12] If observations of electrical conductivity are to be used to constrain the amount of water present in the mantle, then there has to be resolution of the differences between these disparate laboratory data sets, especially at the lower water contents inferred for cratonic lithosphere.

2.1. Sensitivity to Amount of Water

[13] Given its high sensitivity, the presence or absence of water is easily determined from the observed electrical conductivity, but sensitivity to the amount of water is given by the gradient of the curve of conductivity against increasing water content. For the Karato water model, σp,K, proton conductivity is given by

display math

and its derivative with respect to water content, Cw, is

display math

For olivine, σ0 = 103.0, r = 0.62, and ΔHwet = 0.90, and thus

display math

and its derivative with respect to changing water content is simply

display math

i.e., the gradient is inversely dependent on the water content (to the power 0.38), and inversely exponentially dependent on temperature. The gradient is only weakly dependent on water content, but is greatly dependent on temperature. For the Yoshino and Poe proton conductivity models, the exponent r on Cw is taken to be unity, and the general form of their model is

display math

The gradient of this formula with respect to water content is

display math

For the low water contents and the temperatures considered here, i.e., Cw of order 100 ppm and T ∼ 800°C, the term Cw1/3/3kTbecomes of order one, and thus the second term in the pre-exponent brackets becomes of orderα. Substituting the values for olivine for the Yoshino and Poe models (Table 1) in equation (7) yields

display math

For the Yoshino model, the α term is small and thus the gradient is only weakly dependent on water content. In contrast, for the Poe model the α term is large which results in a gradient that is strongly dependent on water content.

[14] The changes expected in conductivity when the water content is doubled are shown in Figure 3 for the three water models. Given these gradient considerations, if either the Karato or Yoshino model is correct, then MT studies will be able to detect the presence of water, but will be virtually insensitive to its amount. In contrast, if the Poe model is correct, then, provided there is good temperature control (to better than 100°C, see below), MT data can be used not only to detect the presence of water, but also to define the amount of water in lithospheric mantle.

Figure 3.

Sensitivity of water models to amount of water. Shown are the changes in the logarithm (base10) of conductivity [S/m] when doubling the amount of water for the Karato (black), Yoshino (red) and averaged Poe (blue) water models.

3. Proton Conduction in Hydrous Pyroxenes

[15] Proton conduction observations in hydrous Opx have been reported by Karato's lab [Dai and Karato, 2009] (Table 2), and the model values fitting equation (1) (with α = 0) are used for Opx and Cpx calculations for Karato model calculations and our own. Recent papers from Yang et al. [Yang et al., 2011, 2012; Yang and McCammon, 2012] list model values fitting equation (1) (again with α = 0) for hydrous Opx and Cpx (Table 2), but use lower crustal material with high iron content, thus the pre-exponent term is higher, by an order of magnitude, than that ofDai and Karato [2009].

Table 2. Parameters for Proton Conduction in Hydrous Pyroxenesa
Referencelog10 (σ0 [S/m])rΔHwet (eV)αComments
  • a

    Italic values are implicit. Bold values are used herein.

Dai and Karato [2009]: Opx2.600.620.850Used for Karato model calculations and our own model for both Opx and Cpx
Yang et al. [2012]: Opx3.83 ± 0.100.90 ± 0.040.84 ± 0.010Lower crustal xenolith material with high Fe content
Yang and McCammon [2012]: Cpx3.62 ± 0.171.035 ± 0.080.75 ± 0.100Averages of model parameters from two samples, High ferric content in samples
Yang et al. [2011]: Cpx3.56 ± 0.101.13 ± 0.050.74 ± 0.010Lower crustal xenolith material with high Fe content
Yoshino and Poe model calculations2.3511.191.10Adopted the averaged Ol values of Poe et al. [2010], as used by Fullea et al. [2011]

[16] Following Fullea et al. [2011], for the Yoshino and Poe model calculations we adopt the same values for Opx and Cpx as the Poe averaged olivine values. We note that model values for Ol from Karato's lab are not too dissimilar from their model values for Opx and Gt, hence we assume that Yoshino and Poe's labs would have similar values for Opx and Cpx, were they to measure them, as they do for Ol.

[17] Errors in the model parameters for Cpx are negligible, given the very low Cpx content in the samples we take as representative of the two kimberlite fields.

4. Jagersfontein and Gibeon Xenolith Information

4.1. Composition

[18] For petrological characterization of the lithosphere at 100 km beneath southern Africa, we take as representative xenolith information from two kimberlite fields, namely (1) Jagersfontein in the western Witwatersrand Block of the Kaapvaal Craton, and (2) the Gibeon field in central Namibia on the Rehoboth terrane. The kimberlites in these fields are both classified as Type I, and geochronology on the xenoliths gives Cretaceous eruption ages of some 86 Ma [Smith, 1983] and 71.5–75.1 Ma [Kurszlaukis et al., 1998] for Jagersfontein and Gibeon respectively. The xenolith mineralogy data used here are given in James et al. [2004], and we pick two representative low-temperature, garnet lherzolite xenoliths from each kimberlite field that yield depth estimates close to 100 km, based on theMacGregor [1974] geobarometer. Modal compositions are listed in Table 3, as well as in situ temperature estimates, based on the O'Neill and Wood [1979] geothermometer. The rationale for choosing these geobarometers and geothermometers over the plethora available [see, e.g., Nimis and Grutter, 2010] is given in James et al. [2004].

Table 3. Whole Rock Mg#, Modal Composition, and Petrologically Determined Pressures and Temperatures (at Eruption Age) of Four Xenoliths From the Jagersfontein (FRB Samples) and Gibeon (KGG Samples) Kimberlite Fields (Taken From James et al. [2004]), Plus Locality Averages
SampleMg#Ol (%)Opx (%)Cpx (%)Gt (%)Sp (%)P (kbar)T (°C)Depth (km)
FRB AV93.269.5024.173.401.350.3231.8782102
KGG AV91.7574.511.56.57.5033.35899108.5

4.2. Temperature Estimates

[19] We recognize that the now-outdatedO'Neill and Wood [1979] geothermometer can be in error by, in extreme cases, up to 200°C [Nimis and Grutter, 2010], but the temperature estimates of approximately 800°C beneath Jagersfontein and 900°C beneath Gibeon at a depth of approximately 100 km at the time of eruption of the kimberlites are both reasonable and are unlikely to be in error by more than 50°C. Importantly, the 100°C relative difference between the two is accurate as the same geothermometer was used for all four samples. Recent analyses by Baptiste et al. [2012, Figure 5] of samples from the Kaapvaal craton using different geobarometers and geothermometers fall on a geotherm inferring a temperature at 100 km in the range 760 – 780 ± 60°C, consistent with the above.

[20] Type I kimberlites of the Kaapvaal Craton and neighboring mobile belts erupted in the period 105–70 Ma during and toward the end of a thermal event thought to have begun with the initiation of Type II kimberlitic volcanism at around 150–115 Ma [Kobussen et al., 2009]. Subsequent thermal relaxation since eruption resulted in colder conditions than those indicated by the xenolith samples, accounting for an estimated cooler present-day temperature of around 740°C at 100 km beneath the Witwatersrand Basin in the center of the Kaapvaal Craton [M. Q. W. Jones, 1988]. The present-day geotherm beneath the Rehoboth Terrane is known to be higher than beneath the Kaapvaal Craton [Muller et al., 2009], consistent with the conditions at kimberlite eruption some 80 Myr ago. Therefore, we adjust the xenolith-determined temperatures downward by 50°C to give estimates of present-day temperatures of 740°C and 850°C at 100 km depth beneath Jagersfontein and Gibeon respectively.

[21] A recent estimate for thermal cooling at Gibeon is provided by Schmädicke et al. [2011]of 1,100–1,190°C for Type II eclogitic kimberlites cooling to 965–1,000°C for the later Type I kimberlites, i.e., approximately 160°C of cooling in approximately 60 Myr. This is qualitatively consistent with our estimate of 50°C of exponentially decaying, temperature-dependent conductive cooling over the last 80 Myr since eruption.

[22] The value for Jagersfontein we adopt is warmer than the recently calculated estimate of ∼650–695°C by Fullea et al. [2011, Figure 12] from their modeling of MT and xenolith data, heat flow and elevation using LitMod [Afonso et al., 2008; Fullea et al., 2009]. (LitMod allows for petrological and geophysical modeling of the lithosphere and sub-lithospheric upper mantle using as many observables as possible within an internally consistent thermodynamic-geophysical framework.) In contrast, our adopted value for Gibeon is somewhat cooler than the Rehoboth estimate of ∼890–985°C determined byFullea et al. [2011]. However, these temperature estimates by Fullea et al. [2011] are from the MT data themselves with assumptions about the water model (averaged Poe model used), thus it would be a circular argument to use these thermal estimates in this paper rather than the more conservative values we have adopted based on xenolith observations and thermal relaxation arguments.

[23] Using the compositions defined by the xenoliths and the temperature estimates, we form a modal mineralogical average for each locality from the mineralogy determined in the two individual xenolith samples (Table 3), and use those averages to derive expected values of electrical conductivity for the whole rock.

4.3. Water Content Estimates

[24] Water content estimates in olivine from kimberlitic xenoliths from the hundreds of kimberlites penetrating through Kaapvaal Craton have been derived by a number of experimentalists over the last two decades. Rossman [2006] gives a good review of the various experimental procedures, including a historical perspective, and there are recent comparisons of approaches in Thomas et al. [2009] and Mosenfelder et al. [2011]. We adopt herein the Bell calibration and use wt ppm water throughout (abbreviated to ppm), and convert where reported otherwise (see Appendix A for discussion).

[25] Water content estimates for olivines from the lithospheric mantle of the Kaapvaal Craton have been presented since the paper of Kurosawa et al. [1997, Table 5]. Those authors reported values of 18–70 wt ppm water (average of 50 ± 16 wt ppm H2O) for 7 garnet peridotite xenoliths, predominantly from Lesotho, with geobarometric pressures of 39–66 kbar (Köhler and Brey's [1990] geobarometer), approx. 120–200 km depths. Kurosawa et al. [1997] noted in their analyses an increase in water content with pressure, and a decrease with temperature, which is somewhat puzzling as both P and T increase with depth. Grant et al. [2007, Table 3] analyzed four garnet peridotite xenoliths from the Kaapvaal Craton and reported water contents of 7.5–54 wt ppm OH (Bell calibration), with more tightly defined Opx and Cpx water contents of 180–200 and 350–400 respectively. Geobarometric pressures of 3.7–7.0 GPa give depths of 110–210 km for those samples, with the shallowest sample exhibiting the highest water content in olivine and the deepest sample exhibiting the lowest. There were no pressure-dependent trends observed in the Opx and Cpx data.

[26] Peslier et al. [2010b] present the results of analyzing 18 carefully selected (see below regarding water loss during ascent) xenolith samples from the Kaapvaal Craton, and present them, together with the data of Kurosawa et al. [1997] and Grant et al. [2007], against pressure, temperature, oxygen fugacity and forsterite content [Peslier et al., 2010b, Figure 1]. The Lesotho kimberlitic samples exhibit consistently lower water contents, by 20–30 ppm, than those from the western Kaapvaal Craton kimberlites; Kimberly, Jagersfontein and Finch. In agreement with Grant et al. [2007], Peslier et al. [2010b]find a pressure-dependency [Peslier et al., 2010b, Figure 1a], with highest values of water content in olivine some 60–80 ppm wt H2O (Bell calibration) for pressures 3.3–5.5 GPa, approximately 100–165 km depth. At greater depths the water content decreases systematically to <10 ppm by 200 km, and there is the inference, from very sparse data, that water content also might decrease at shallower depths. This trend is replicated with temperature, as one would expect, with highest values for temperatures of 900–1200°C decreasing systematically with increasing temperature to <10 ppm by 1350°C, i.e., the base of the thermal lithospheric mantle. There is also a trend with iron content, with highest water contents for magnesium numbers (Mg#) of 92.5–94, i.e., depleted rocks, and decreasing with increasing iron to <40 ppm for Mg#<90, i.e., more fertile rocks. Thus, there is a two-part division of the lithosphere beneath the western Kaapvaal craton, with the upper lithosphere being more depleted, colder and wetter, and the lower lithosphere being more fertile, warmer and dry.

[27] These results are verified in a very recent paper by Baptiste et al. [2012] that describes measurements of water contents in olivines and pyroxenes for 14 samples equilibrated at different depths from the Kaapvaal Craton. Consistent with prior work, Baptiste et al. [2012] find water contents in olivine are maximum (150 ppm wt H2O, Bell calibration) for depths of ∼160 km, in contrast to those from depths greater than 180 km that are almost dry. Their single Jagersfontein sample (KBJ59) yielded a geothermometric temperature of 890°C [Brey and Köhler, 1990], which is some 100°C higher than our temperature estimate for 100 km depth and would suggest a somewhat deeper source region. There is no geobarometric depth estimate for that sample, but comparison with the derived geotherm in Baptiste et al. [2012, Figure 5] would suggest that the sample came from ∼115 km depth. The five olivines from sample KBJ59 yielded a range of water contents of 66–202, with an average of 110 ± 55 ppm wt H2O (Bell calibration), which is somewhat higher than the Peslier et al. [2010b] estimates. Their coldest Kimberley sample (FRB1423, 851°C, Brey and Köhler geothermometer) yielded two water content estimates of 63 and 133 ppm, within the range of the Jagersfontein sample.

[28] Taking all of these values together, for a depth of 100 km below Jagersfontein we conclude that an average of 80 ± 20 ppm H2O is reasonable. It is certainly not higher than about 150 ppm, nor lower than about 60 ppm.

[29] The petrological observation by Peslier et al. [2010b] and Baptiste et al. [2012]that the uppermost depleted lithospheric mantle is wetter than the lowermost melt-metasomatized and re-fertilized mantle was a conclusion drawn from modeling the magnetotelluric data on the Kaapvaal Craton together with surface elevation and heat flow byFullea et al. [2011] using the LitMod approach [Afonso et al., 2008; Fullea et al., 2009].

[30] We assume that the water content in the olivine from the Rehoboth Terrane at 100 km is also of the order of 80 ppm, with the pyroxenes two times and three times higher for Opx and Cpx respectively. Off-craton peridotites are, puzzlingly, typically lower in their water contents in olivine, with water in Ol usually <50 ppm, but are the same in pyroxenes, with averages of 163 ppm in Opx and 307 in Cpx [Peslier, 2010]. For our purposes we adopt a value of 80 ppm for Gibeon also, and err on the conservative side.

4.4. Water Loss During Ascent

[31] The issue of potential water loss during kimberlitic magmatic ascent is clearly one that can play a major role in the veracity of our examination, and has been a concern for two decades [Mackwell and Kohlstedt, 1990]. Petrological evidence exists, namely the differential water content seen from rims to cores of the mantle grains, that yields strong support for potentially significant water loss in olivine in alkali basalts during ascent [Demouchy et al., 2006]; Demouchy et al. [2006] consider up to two thirds of the water in olivine may be lost. For kimberlitic xenolithic olivines, the amount of water lost from olivine appears to depend on the host magma, and, generally, the H+ diffusion profiles are far less pronounced than for alkali basalts. This difference is ascribed to kimberlitic magmas being more volatile rich, at lower temperatures (1000–1200°C, compared to ∼1200–1300°C) and with far higher ascent rates (up to 37 m/s, compared to 6 m/s) than alkali basalts [Peslier et al., 2008]. Peslier [2010], in her review on water in the Earth's mantle, gives only two localities for which one can be fairly certain that water loss did not occur in olivine from alkali basalts during ascent, namely Kilbourne Hole (New Mexico, USA) and Ichinomegata (Japan); Kilbourne Hole has low values of water in olivine, 3–54 ppm [Grant et al., 2007]. In contrast, many olivines in xenoliths from kimberlitic magmas exhibit flat hydrogen profiles and can reasonably be assumed to be representative of the water content in olivine at source [Peslier, 2010]. Consistent with the prior results of Grant et al. [2007], Peslier et al. [2008] found no hydrogen profile variation across olivine grains from the Kaapvaal craton, with the exception of one anomalous sample.

[32] In the case of the water content values used in this paper, taken from Peslier et al. [2010b, p. 78], those authors stated that “Diffusion modelling of the H profiles across the olivine of these samples (Supplementary Information) reveals that the cores of the olivine preserved their original water content and that only the edges were affected by H loss. Consequently, the water contents presented here are believed to reflect accurately the mantle values.” We therefore assume that the water contents reported by Peslier et al. [2010b], and recently by Baptiste et al. [2012], for the Jagersfontein xenoliths of around 80 ppm, are representative to within ±20 ppm. It is highly unlikely that the actual water content is more than two times greater, i.e., >160 ppm, as could be argued for olivines from alkali basalts.

[33] We cannot though exclude the possibility that, despite the observations of flat hydrogen profiles in the olivine grains from kimberlitic xenoliths, the water contents in olivines have all been systematically underestimated. That alternative, unlikely though it is, is explored in the Discussion and Conclusions.

[34] Hydrogen diffusion profiles of pyroxenes and garnet indicate that they do not appear to lose any water during ascent, but why there is this difference between water loss in olivine compared to the other minerals is the subject of speculation [see Peslier, 2010, and references therein].

4.5. Water Partitioning

[35] We have two regions where we can define the observed electrical resistivity and where we know modal mineralogy and can estimate present-day temperature reasonably well. For Jagersfontein, we also have an estimate of the water content in olivine, but for our calculations we need to assume the water partitioning in the pyroxenes. Water partitioning in NAMs was discussed byAubaud et al. [2004, 2007], Hauri et al. [2006], and Li et al. [2008], among many others, and the inconsistency between various studies is beyond the scope of this paper. We require only an approximate rule for our calculations.

[36] Typically there is up to twice as much water in Cpx as Opx [Li et al., 2008; Peslier, 2010], but, given the small amounts of Cpx in our samples (<5%), the effect of water variation in Cpx on bulk conductivity is negligible. Global cratonic averages give water contents in cratonic peroditic xenoliths of 58 ppm in Olivine, 157 ppm in Opx, and 276 ppm in Cpx [Peslier, 2010] – a ratio of 1:2.7:4.7 – with whole rock water content of 58 ppm (same as olivine). Averages for water in South African cratonic pyroxenes are 244 ± 107 ppm for Opx and 397 ± 61 ppm for Cpx, with a whole rock average of 124 ± 62 ppm [Xia et al., 2010]. If the whole rock sample is reasonably representative of the olivine water content this supports an approximately 1:2:3 partitioning, which is close to the partitioning seen at Monastery kimberlite in Lesotho by Bell et al. [2004] of 1:1.6 (±0.2):3.0 (±0.5).

[37] We recognize in global compilations that whereas the partitioning between Opx and Cpx is reasonably supported by observation [Peslier, 2010, Figure 2a], there is less support for a partitioning relationship between Ol and Opx [Peslier, 2010, Figure 2d], and indeed one could argue from global extant data that Ol water content varies independently of Opx water content. However, the error introduced by adopting an incorrect partitioning relationship is minor compared to all of the other variables and unknowns, and we thus assume for our calculations that there is twice as much water in Opx as in Ol, and three times as much in Cpx. To the best of our knowledge there are no laboratory measurements at lithospheric-mantle temperatures and pressures that constrain the equilibrium partitioning of water between Ol, Opx and Cpx. Therefore, recourse to the observed relative water concentrations in xenolith samples, as has been done here, is the only possible approach for estimating water partitioning between the three major mantle minerals.

5. Petrologically Defined Electrical Conductivity of Mantle Rocks

5.1. Electrical Conductivity of Mantle Minerals

[38] For electrical conductivity the equations of state for dry mantle minerals are reviewed in detail in Jones et al. [2009a], and, for small polaron conduction, are given as

display math

based on the work of Hirsch et al. [1993] for Ol, Xu and Shankland [1999] for Opx, Xu et al. [2000] for Cpx, and Romano et al. [2006] for Gt (but with a correction applied, see Jones et al. [2009a]), where mineral XFe is the iron number (related to the magnesium number Mg# by XFe= 1 − Mg#/100; can be different for each mineral), k is Boltzmann's constant, and T is temperature in Kelvin. Note that the conductivities of the pyroxenes are not iron-dependent – this is because either the measurements have not been made or the laboratories are inconsistent in their results (see discussion inJones et al. [2009a]), so we have little choice but to assume iron dependency is negligible. Also, spinel is ignored as the evidence from mantle xenoliths is that its occurrence is well below 1% at the depth of interest in this paper (100 km).

[39] Fullea et al. [2011] revised the above equations taking into account newer laboratory studies and also the measurements of the effects of water in the minerals. The revised equations are of the general form

display math


display math

The first term in equation (10) describes small polaron conduction, and includes a dependency on mineral iron number XFe. The second term describes the contribution of Mg vacancies at high temperatures (and lacks XFedependency). The third term describes proton conduction in the water-present case, as described in the general case byequation (1).

[40] At the conditions of interest in this study, the temperatures are sufficiently low that conduction from Mg vacancies is negligible (it only becomes important at temperatures beyond 1200°C).

5.2. Variation of Olivine Conductivity With Temperature

[41] The small polaron conductivity models of olivine at cratonic lithosphere temperatures, for a representative magnesium number for cratonic lithosphere (Mg# = 92.5) and typical pressure at 100 km depth (3.25 GPa), from Jones et al. [2009a] (equation (9)) and Fullea et al. [2011] (equations (10) and (11) with the parameters from Table 4) are shown in Figure 4, together with the SEO3 defined conductivity of Constable [2006] at both QFM and IW oxygen buffering conditions.

Table 4. Parameters for Conductivity Equations of Fullea et al. [2011]a
 Small Polaron ConductionMg VacanciesProton Conduction
Karato ModelYoshino/Poe Model
log σ0,spabcdefΔVlog σ0iΔHiΔHwet (eV)log σ0rΔHwet (eV)log σ0α
  • a

    Values in italics are assumed as no measurements exist.

Ol2.4–3.01.6420.246−4.853.2590.684.732.310.87 ± 0.053.0 ± 0.40.62 ±
Gt(2.67–3.39) + log10(1–0.044P)2.6−15.3380.4−194.6202.6−7520.540.9620.0500.72520.2900.6310.1920.3510.1
Figure 4.

Variation of conductivity with temperature for olivine at a pressure of 3.25 GPa (∼100 km depth) with an Mg# of 92.5 and a water content of 100 ppm. Small polaron conductivity from the Fullea et al. [2011] (green solid line) and Jones et al. [2009a] (blue solid line) models plus the SEO3 model of Constable [2006] for both QFM (black solid line) and IW (red solid line) oxygen fugacity buffering. Proton conductivity from the Karato (dashed black line), Yoshino (dashed red line) and Poe (dashed blue line) models.

[42] Also shown in Figure 4 are the conductivity estimates for proton conduction for 100 ppm water from the three models, Karato (Figure 4, dashed black line), Yoshino (Figure 4, dashed red line) and Poe (Figure 4, dashed blue line). Comparing Figure 1 with Figure 4, proton conduction dominates over small polaron conduction for even small amount of water; <45 ppm for the Poe AV model and far less for the other two models. Thus, the differences between the polaron models and the errors introduced by adopting a particular polaron conductivity model, and also ignoring iron effects on pyroxene conductivity, are irrelevant at the water contents of interest in this study given the dominance of proton conduction.

[43] Note that for the water contents of interest, the proton conduction term has a relatively small gradient with temperature, regardless of model chosen, of approx. 0.37–0.42 log units for a 100°C change. Thus, a 50°C error in our present-day temperature estimates for either Jagersfontein (740°C) or Gibeon (850°C) will result in an error of 0.2 log units in our estimate of conductivity. This is the same order as the experimental errors of our resistivity estimates (0.20 log units for Jagersfontein and 0.09 log units for Gibeon, see below).

[44] The complete conductivity calculations in temperature-water content (T-Cw) space for the three proton conduction models are shown in Figure 5. For all of them, at low water contents temperature is virtually immaterial. This changes at high water contents, where there is a strong gradient with both temperature and water content for the Poe model, but for the Karato and Yoshino models conductivity becomes insensitive to actual water content, as discussed above.

Figure 5.

Electrical conductivity from proton conduction with temperature and water content using equation (1) with the parameters listed in Table 1 for (a) the Karato [Wang et al., 2006], (b) the Yoshino [Yoshino et al., 2009], (c) the averaged Poe [Poe et al., 2010; Fullea et al., 2011], and (d) this paper's model parameters. Also shown are the expected temperatures and water contents for Jagersfontein (Jag, 740°C, 80 ppm, yellow square) and Gibeon (Gib, 750°C, 80 ppm, purple square), and the resistivities at 100 km depth below Jagersfontein (−3.41 ± 0.2 log units, solid yellow line with one sigma errors shown as dashed yellow lines) and Gibeon (−2.78 ± 0.09 log units, solid purple line with one sigma errors shown as dashed purple lines).

5.3. Whole Rock Conductivity Calculation

[45] The parameters used for equations (10) and (11) for the four minerals are listed in Table 4. In implementing the generalized form for proton conduction, σp, in equation (11) for the different conduction models derived by the three laboratories, the following formulations were used (with parameters specified in Table 3): (1) For the Karato model, a constant value of ΔHwet (i.e., α assumed to be zero) and f(Cw) = σ0Cwr. (2) For the Yoshino and Poe models, ΔHwet = ΔH0αCw(1/3) and f(Cw) = σ0Cw (i.e., r assumed to be one).

[46] Following the Jones et al. [2009a] approach, we calculate whole rock conductivity for the four samples and two averages using the (P,T) conditions and modal compositions from Table 3, the formulae in equations (10) and (11), and aggregate the individual minerals using second-order, multiphase Hashin-Shtrikman extremal bounds [Berryman, 1995], taking into account possible interfacial effects [Salje, 2007]. Simple mixing laws, such as arithmetic or geometric relations, Archie's Law, and Voigt and Reuss estimates, give first-order variational bounds, whereas Hashin-Shtrikman represents a member of the class of second-order variational bounds. There exist third-order variational bounds [Beran, 1965; Beran and Molyneux, 1966] that have been applied in seismology [X F Xu, 2011] but not yet in electromagnetism. An additional term was added to the Hashin-Shtrikman equations ofBerryman [1995] by Salje [2007]to explain observations that were found to lie outside the Hashin-Shtrikman bounds. The term considers interfacial effects that are shown to scale withf(1-f), where f is the volume proportion of the individual phase. For intermediate cases, where both volume and interfacial effects are important, the volume proportion f in the averaging scheme is replaced by f(1 − S) + Sf2, where S ranges from 0 (no interfacial effects) to 1 (only interfacial effects).

[47] Extremal bounds are more important for electrical conductivity than for bulk moduli, as the influence of the highest conductivity phase, even if only a minor component (1%), can be dramatic if the minor phase is sufficiently well interconnected. However, olivine (Ol) and pyroxene (Opx, Cpx) minerals when dry have conductivities that are within an order of magnitude of each other at any given (P,T) conditions, and, for the mineral assemblages considered herein, Ol and Opx make up the bulk of the whole rock, over 95% in most cases, so the extremal bounds are not wide. We derive estimates using the geometric means of the upper and lower Hashin-Shtrikman bounds with and without interfacial effects; the individual values are so close to each other that the geometric and arithmetic means are virtually the same.

[48] Our average petrologically based estimates for log10(conductivity) at 100 km depth beneath Jagersfontein and Gibeon, under water-absent, dry conditions, i.e., small polaron conduction only, are −5.30 and −4.39 log units respectively (Table 5).

Table 5. Hashin-Shrikman Estimates of Log10(Conductivity [S/m]) at 100 km Depth Beneath Jagersfontein (FRB Samples) and Gibeon (KGG Samples), Assuming Dry Conditions (No Water)a
SampleT (°C)HS (S = 0)HS+ (S = 0)HS (S = 1)HS+ (S = 1)HS GAV
  • a

    The parameter S, varying between 0 and 1, accounts for the potential variation in the strength of interfacial processes on conductivity. HS GAV refers to the geometric average of the Hashin-Shtrikman estimates. Temperatures used are estimated present-day temperatures and are approximately 50°C less than temperatures at the time of kimberlite eruption (Table 3). Bold values represent the averages that are used in this paper.

FRB AV740−5.30−4.96−5.29−5.28−5.21
KGG AV850−4.51−3.99−4.53−4.41−4.36

[49] Given the observations of water in the lithosphere, we must derive the expected conductivities under “slightly damp,” conditions. None of the data in Peslier et al. [2010b]are from xenoliths sourced as shallow as 100 km nor as cold as 740°C, so we have to extrapolate from their results at higher temperatures (900°C) beneath Kimberley that show evidence for around 80 ppm water in the olivine. Given the lack of any depth-dependence shown for the upper lithosphere inPeslier et al. [2010b], we assume a value of 80 ± 10 ppm later in the text, but calculate at this point conductivity for water content from 0–200 ppm in olivine.

[50] The conductivity calculations for wet conditions for olivine for the Karato, Yoshino and Poe (average) models that include the effects of proton conduction using equations (10) and (11) for temperatures of 740°C and 850°C, i.e., our Jagersfontein and Gibeon estimated ambient temperatures at 100 km, are shown as the dashed lines in Figure 6.

Figure 6.

(a) Variation of conductivity at Jagersfontein parameters at 100 km depth of T = 740°C, P = 3.2 GPa, for olivine water concentration varying from 0 – 200 ppm for the Karato (black lines), Yoshino (red lines) and Poe (blue lines) models (equation (10)) for olivine alone (Mg# = 93.2) (dashed lines) and for the Jagersfontein composition assemblage (Mg# = 93.2, except for Gt where Mg# = 75.0) (solid lines). Note that the abscissa annotates olivine water concentration, and that for the composition assemblage calculations, water concentrations for Opx, Cpx and Gt are taken as 2 × Ol, 3 × Ol and zero respectively, as discussed in the text. The observation datum (green point) is for a water content in Ol of 80 ± 20 ppm (from xenoliths) and a log(conductivity) of −3.41 ± 0.41 (from mapping of MT observations, with 2σ error bounds). The dashed green line represent the revised Karato water model for olivine, with log(σ0) = 2.70 (±0.26), r = 0.70 (±0.12), and ΔHwet = 0.91 (±0.04). The solid green line represents the revised water model for olivine that best fits equation (1) with 1og10(σ0) = 3.05 (±0.16), r = 0.86 (±0.08), ΔHwet = 0.91 (±0.04), and α = 0.09 (±0.07), valid for water content in damp lithosphere of around 60–100 ppm. The dotted lines are ±1σ. (b) Variation of conductivity at Gibeon parameters at 100 km depth of T = 850°C, P = 3.335 GPa, for water varying from 0 – 200 ppm. The observation datum (green point) is for a water content in Ol of 80 ± 20 ppm (assumed to be the same as for Jagersfontein in the absence of xenolith water content measurements at Gibeon) and a log(conductivity) of −2.78 ± 0.18 (from mapping of MT observations, with 2σ error bounds). Curves as for Figure 6a. The dotted lines are ±1σ.

[51] Olivine is not the only mantle mineral, even though it comprises >70% (Table 3) of the rock mass, so consideration must be given to the contribution to proton conduction from the other mantle minerals, pyroxenes and garnet, of which Opx dominates. Water in pyroxenes is higher than in olivine, with averages of 200 ppm in Opx and 300 ppm in Cpx, and virtually zero in garnet, in the Kaapvaal peridotite xenolith samples reported in Peslier [2010, supplementary material]. A recent abstract lists a narrow range for both Opx and Cpx of 119–251 ppm and 149–398 ppm respectively [Peslier et al., 2010a], bracketing the average given above, with the intriguing suggestion of an increase in water content in pyroxenes from Liqhobong (Lesotho), through Finsch Mine, Jagersfontein, to Kimberley xenoliths. In contrast, far lower values are reported for xenoliths from the Letseng kimberlite in Lesotho [Sundvall and Stalder, 2011], from 20 ppm. As discussed above, we assume a water partitioning of 1:2:3 between the Ol, Opx and Cpx.

[52] Computing the resistivities for the composition given in Table 3 for water contents of x ppm in Ol, 2x ppm in Opx, 3x ppm in Cpx, and 0 ppm in Gt (values observed are 0–15 ppm at 4 Gpa in Peslier [2010], but given the very low volumes of these minerals we set the water contents to zero), where x varies from 0 to 200 and the increase in water in pyroxenes is assumed to be linearly related to the increase in water in olivine, yields the solid lines shown in Figure 6a for the conductivity beneath Jagersfontein with varying water content. Holding the water contents of the pyroxenes fixed at the averages of 200 ppm and 300 ppm for Opx and Cpx respectively and varying Ol only from 0 to 200 ppm introduces very little change in our conductivity estimates over assuming a 1:2:3 water partitioning, especially at the water contents of interest, around 80 ppm.

[53] The water content of minerals from xenoliths beneath Gibeon is unknown, but it is reasonable to assume that it will be of the same order, if not somewhat less. Undertaking the computations for Gibeon parameters (Table 3) yields the solid lines in Figure 6b for the Karato, Yoshino and Poe models.

6. Field Observations of Electrical Resistivity at 100 km Beneath Jagersfontein and Gibeon

[54] A regional-scale magnetotelluric survey of Southern Africa took place during 2003–2008 called SAMTEX (Southern African MT Experiment) [Jones et al., 2009b], following on from the teleseismic SASE (Southern African Seismic Experiment) [James et al., 2001] project. Two-dimensional resistivity models have been published from three of the main profiles, a SW-NE profile across the Kaapvaal Craton [Evans et al., 2011], a crossing NW-SE profile from the Kaapvaal Craton onto the Rehoboth Terrane [Muller et al., 2009], and a N-S profile across the Zimbabwe Craton in northeastern Botswana [Miensopust et al., 2011]. In addition, maps of approximate resistivity at depths of 100 km and 200 km from the whole SAMTEX database have been published [Jones et al., 2009b].

[55] The log10(conductivities) at 100 km beneath Jagersfontein and Gibeon are estimated by averaging the approximate resistivities in the 100 km depth image of Jones et al. [2009b]. The means and one-sigma (1σ) bounds within 100 km radius of the two kimberlite fields are −3.41 ± 0.20 and −2.78 ± 0.09 log units respectively. These values are substantiated below by undertaking modeling of the sites closest to the two kimberlite fields, and from comparing them with an existing regional two-dimensional model.

[56] For Jagersfontein, the closest site to the kimberlite field is kim015, and the MT data at this location (Figure 7a) are clearly one-dimensional (1D), with minor static shifts [A. G. Jones, 1988], over the whole period range except for the very longest periods. For Gibeon, the closest site is gib012, and the data (Figure 7b) are 1D at high frequencies, but become 2D at longer periods, with geoelectrical strike close to geographic coordinates.

Figure 7.

(a) Magnetotelluric data observed at site kim015 within 20 km of the Jagersfontein kimberlite field. The open symbols are the original estimates of the MT impedance tensor off-diagonal elements (XY and YX, where the YX phases have been rotated from the 3rd into the 1st quadrant), which are a merge of broadband (Phoenix Geophysics MTU-V5) and long period (LIMS) data. The solid symbols are the data after replacing estimates that lie more than 2σ away from their Rho+ [Parker and Booker, 1996] estimates. (b) Magnetotelluric data (Phoenix Geophysics MTU-V5 only) observed at site gib012 located within the Gibeon kimberlite field. (Symbols same as in Figure 7a.)

[57] One-dimensional (1D) models of the Berdichevsky-averaged MT data (i.e.,Zav = ZxyZyx) from kim015 and gib012, were derived using the Occam approach [Constable et al., 1987] (Figure 8). Minimum possible χ2 misfits are given by the D+ solutions of Parker [1980], and for the kim015 and gib012 Zav data are 85.0 and 87.7 respectively, which, for 52 and 84 complex data, are minimum RMS misfits of 0.90 and 0.72. Two models are shown for each site, one that exhibits the initiation of oscillatory behavior seen when Occam models are pushed too close toward the D+ minimum misfit limit, and a second that is some 7–9% higher misfit that does not show the strong oscillations. Both models at each site are very similar at 100 km depth and are in agreement with the electrical resistivity at 100 km depth being around 2,000 Ωm (i.e., log10(conductivity) of −3.30 log units) for Jagersfontein and around 450 Ωm (log10(conductivity) of −2.65 log units) for Gibeon.

Figure 8.

Best fitting Occam [Constable et al., 1987] 1-D models to the averaged data from kim015 (Figure 7a) and gib012 (Figure 7b) for minimum RMS misfit (dashed lines) and approx. 10% higher misfit (solid lines).

[58] Two-dimensional (2D) modeling of the SAMTEX profile that traverses SE-NW across Jagersfontein from the Kaapvaal Craton onto the Rehoboth Terrane [Muller et al., 2009] yields conductivity estimates that overlap in error with the above values, but that are somewhat lower. For both Jagersfontein and the Gibeon field, log10(resistivity) averages of the 2D model at 100 km depth were computed over a 200 km wide zone centered on the perpendicular projection of the kimberlite occurrences onto the 2D profile (∼20 km and ∼160 km projection distances for Jagersfontein and Gibeon respectively). Average resistivities observed at 100 km depth are 5,800 Ωm (log10(conductivity) of −3.76 ± 0.43 (1σ) log units) and 840 Ωm (log10(conductivity) of −2.92 ± 0.22 log units) for Jagersfontein and Gibeon respectively. Given the relatively large projection distance in the case of the Gibeon field, some uncertainty exists in assuming both a perpendicular projection onto the profile and little geological heterogeneity over the projection distance. To address the former uncertainty, and to some extent the latter, the Gibeon field was projected onto the profile parallel to the observed geoelectric strike direction (projection azimuth 25° E of N, versus 40° E of N for the perpendicular projection), yielding an average resistivity at 100 km depth of 660 Ωm (log10(conductivity) of −2.82 ± 0.19 log units) and, arguably, a more geologically justifiable measurement.

[59] In summary, the approximate depth mapping and the formal 1D and 2D modeling yield estimates of log10(conductivity) below Jagersfontein of −3.41 ± 0.20, −3.30 and −3.76 ± 0.43 log units, and for Gibeon of −2.78 ± 0.09, −2.65 and −2.82 ± 0.19 log units respectively. All three approaches are consistent and within errors of each other. For the purposes of the comparison with laboratory studies, we take the approximate depth mapping estimates.

7. Comparison of Field Observations With Laboratory Models

[60] Our derived Cw-log10(σ) points for Jagersfontein and Gibeon are plotted in Figure 5 (yellow square for Jag and purple square for Gib, contours are for proton conduction only) and Figure 6 (green points, total rock conductivity), and, in both cases, the Karato model is too conducting, by an order of magnitude, and the Yoshino and Poe models are not conducting enough, again by an order of magnitude, for a water content of 80 ppm and the temperature estimates we have assumed. Note in Figure 6that the whole rock calculations (solid lines) are within one quarter of a decade or less, i.e., the error of the resistivity measurement, of the resistivity of the olivine-only calculations (dashed lines). Considerations of the appropriate water model for the pyroxenes and garnet, and of iron content and composition, are all secondary compared to the olivine proton conduction model. Hence we focus on improving the parameters of the olivine proton conduction model.

[61] For Jagersfontein, using the mean parameters for olivine listed in Table 1 the Karato water model is certainly far too conductive; for log10(conductivity) of −3.41 one only needs 8 ppm water, an unrealistically low number. The Yoshino and Poe models though are too resistive for the reported water contents; a log10(conductivity) of −3.41 requires 250 ppm of water in the olivine for the Poe model and 350 ppm for the Yoshino model, both of which are more than a factor of three higher than the reported water content. Similarly for Gibeon with a log10(conductivity) of −2.78, the Karato model would predict a water content in olivine of 10 ppm, the Poe model 320 ppm, and the Yoshino model 550 ppm, all of which are unrealistic.

[62] Figure 5shows the trade-offs between temperature and water content for the three models, withFigure 5a for the Karato model and parameters, Figure 5b for the Yoshino/Poe model and Yoshino parameters, and Figure 5c for the Yoshino/Poe model and averaged Poe parameters, plus a fourth model we develop below that combines the Karato and Yoshino/Poe models (Figure 5d). Even assuming that both our temperature and water content estimates are seriously in error, there is no reasonable combination of temperature and water content for any of the three laboratory models that are an acceptable fit to the two resistivity data points.

7.1. Monte-Carlo Model Fitting

[63] The three parameters for the Karato olivine water model, log10(σ0), r, and ΔHwet, have rather large standard deviations in Wang et al. [2006] (Table 1), so one can test if realizations taken randomly from the statistical distributions of the parameters fit the resistivity observations from Jagersfontein and Gibeon. Undertaking a Monte-Carlo stochastic modeling exercise by generating 1,000,000 realizations for the five parameters randomly sampled from Gaussian distributions with means and standard deviations of

display math

yields best fit models listed in Table 6 fitting to within one tenth, one quarter and one half of the standard deviations of log10(conductivity) of −3.41 ± 0.20 and −2.78 ± 0.09 respectively for Jagersfontein and Gibeon. Note that the few found within σ/10 are all close to the one sigma bounds of the experimental data of Wang et al. [2006], and the summed difference from the Wang et al. parameters is 2σ. Adopting the field observation refined values of log10(σ0) = 2.70, r = 0.70, and ΔHwet = 0.91 for olivine and the existing values for the other minerals yields the dashed green curves in Figure 6.

Table 6. Karato Model Parameters for Olivine Conductivity Fitted to Jagersfontein and Gibeon Observed Resistivities to Within σ/10 (2,450–2,700 Ω m and 590–620 Ω m Respectively), σ/4 (2,000–3,250 Ω m and 550–670 Ω m Respectively) and σ/2 (1,600–4,100 Ω m and 500–750 Ω m Respectively) Bounds for Cw = 80 ppm (±10) Water at Temperatures t of 740°C and 850°C (Both ± 25°C) Respectively From 1,000,000 Realizations by Monte Carlo Random Selection From Six Gaussian Distributed Parameters log(σ0), r, ΔHwet, Cw, tJag and tGiba
 % Accept.log10 (σ0 [S/m])rΔHwet (eV)Jagersfontein log10 (σ [S/m])Gibeon log10 (σ [S/m])
Wang et al. [2006] parameters and SAMTEX observations3.0 ± 0.40.62 ± 0.150.87 ± 0.05−3.41 ± 0.20−2.78 ± 0.09
Within σ/10
Jagersfontein1.12.63 ± 0.290.73 ± 0.130.90 ± 0.05−3.41 ± 0.01
Gibeon0.752.72 ± 0.280.71 ± 0.120.89 ± 0.05−2.78 ± 0.005
Jagersfontein and Gibeon0.032.70 ± 0.260.70 ± 0.120.91 ± 0.04−3.41 ± 0.01−2.78 ± 0.005
Within σ/4
Jagersfontein2.82.63 ± 0.290.73 ± 0.130.90 ± 0.04−3.41 ± 0.03
Gibeon1.92.71 ± 0.280.71 ± 0.120.89 ± 0.05−2.78 ± 0.01
Jagersfontein and Gibeon0.22.71 ± 0.280.71 ± 0.130.90 ± 0.04−3.40 ± 0.03−2.78 ± 0.01
Within σ/2
Jagersfontein5.72.63 ± 0.290.73 ± 0.130.90 ± 0.05−3.40 ± 0.06
Gibeon3.82.71 ± 0.280.70 ± 0.120.90 ± 0.05−2.78 ± 0.03
Jagersfontein and Gibeon0.82.71 ± 0.280.71 ± 0.130.90 ± 0.04−3.38 ± 0.05−2.78 ± 0.03

[64] Our strategy of “calibrating” the proton conduction model parameters log10(σ0), r, and ΔHwetfor olivine-only against observed whole rock data is justifiable as the error bounds on the observed conductivity data are significantly greater than the differences between the “olivine only” and “assemblage” models inFigure 6. The observed data available (two points each of three data) are also too few to allow the proton conduction model parameters to be determined or calibrated independently for the pyroxenes and garnet as well – this could be potentially introduced in the future when more observed data points are available.

[65] Undertaking this stochastic exercise for the Yoshino model and parameters log10(σ0), ΔHwet, and α yields for σ/10 only 11 acceptable models of the one million tested, with the parameters given in Table 7. These mean model parameters lie though 4.5σaway from the laboratory-derived values, and are thus highly unlikely to be explainable by laboratory random error. Similarly for the Poe model (Table 8); the averages of the 14 models of the one million tested that fit the Jagersfontein and Gibeon data to within σ/10 lie 17σaway from the laboratory-determined values.

Table 7. Yoshino Model Parameters for Olivine Conductivity Fitted to Jagersfontein and Gibeon Observed Resistivities to Within σ/10 (2,450 – 2,700 Ω m and 590 – 620 Ω m Respectively), σ/4 (2,000 – 3,250 Ω m and 550 – 670 Ω m Respectively) and σ/2 (1,600 – 4,100 Ω m and 500 – 750 Ω m Respectively) Bounds for Cw = 80 ppm (±10) Water at Temperatures t of 740°C and 850°C (Both ±25°C) Respectively From 1,000,000 Realizations by Monte Carlo Random Selection From Six Gaussian Distributed Parameters log(σ0), ΔHwet, α, Cw, tJag and tGiba
 % Accept.log10 (σ0 [S/m])ΔHwet (eV)αJagersfontein log10 (σ [S/m])Gibeon log10 (σ [S/m])
Yoshino et al. parameters and SAMTEX observations1.9 ± 0.440.92 ± 0.040.16 ± 0.02−3.41 ± 0.20−2.78 ± 0.09
Within σ/10
Jagersfontein0.22.84 ± 0.190.85 ± 0.040.16 ± 0.02−3.41 ± 0.01
Gibeon0.023.07 ± 0.180.85 ± 0.040.16 ± 0.02−2.78 ± 0.005
Jagersfontein and Gibeon0.0013.13 ± 0.180.87 ± 0.030.17 ± 0.02−3.40 ± 0.01−2.78 ± 0.005
Within σ/4
Jagersfontein0.42.84 ± 0.200.85 ± 0.040.16 ± 0.02−3.41 ± 0.03
Gibeon0.053.06 ± 0.180.85 ± 0.040.16 ± 0.02−2.78 ± 0.01
Jagersfontein and Gibeon0.0073.05 ± 0.200.86 ± 0.040.16 ± 0.02−3.40 ± 0.03−2.78 ± 0.01
Within σ/2
Jagersfontein0.92.84 ± 0.210.85 ± 0.040.16 ± 0.02−3.43 ± 0.06
Gibeon0.13.05 ± 0.180.84 ± 0.040.16 ± 0.02−2.78 ± 0.03
Jagersfontein and Gibeon0.033.04 ± 0.200.86 ± 0.040.16 ± 0.02−3.38 ± 0.06−2.79 ± 0.03
Table 8. Poe Model Parameters for Olivine Conductivity Fitted to Jagersfontein and Gibeon Observed Resistivities to Within σ/10 (2,450–2,700 Ω m and 590–620 Ω m Respectively), σ/4 (2,000–3,250 Ω m and 550–670 Ω m Respectively) and σ/2 (1,600–4,100 Ω m and 500–750 Ω m Respectively) Bounds for Cw = 80 ppm (±10) Water at Temperatures t of 740°C and 850°C (Both ±25°C) Respectively From 1,000,000 Realizations by Monte Carlo Random Selection From Six Gaussian Distributed Parameters log(σ0), ΔHwet, α, Cw, tJag and tGiba
 % Accept.log10 (σ0 [S/m])ΔHwet (eV)αJagersfontein log10 (σ [S/m])Gibeon log10 (σ [S/m])
  • a

    Each of the three runs was independent. Bold values are those of Poe et al. [2010].

Poe et al. averaged parameters and SAMTEX observations2.35 ± 0.111.19 ± 0.0351.10 ± 0.055−3.41 ± 0.20−2.78 ± 0.09
Within σ/10
Jagersfontein0.23.25 ± 0.210.93 ± 0.041.10 ± 0.02−3.41 ± 0.01
Gibeon0.033.43 ± 0.190.93 ± 0.041.10 ± 0.02−2.78 ± 0.005
Jagersfontein and Gibeon0.0013.38 ± 0.190.92 ± 0.031.10 ± 0.02−3.41 ± 0.01−2.78 ± 0.005
Within σ/4
Jagersfontein0.53.24 ± 0.210.93 ± 0.041.10 ± 0.02−3.41 ± 0.03
Gibeon0.093.42 ± 0.190.93 ± 0.041.10 ± 0.02−2.78 ± 0.01
Jagersfontein and Gibeon0.023.41 ± 0.180.93 ± 0.041.10 ± 0.02−3.40 ± 0.03−2.78 ± 0.01
Within σ/2
Jagersfontein1.13.24 ± 0.210.93 ± 0.041.10 ± 0.02−3.43 ± 0.06
Gibeon0.23.42 ± 0.190.93 ± 0.041.10 ± 0.02−2.78 ± 0.03
Jagersfontein and Gibeon0.073.40 ± 0.190.93 ± 0.041.10 ± 0.02−3.39 ± 0.06−2.79 ± 0.03

[66] The Karato, Yoshino and Poe model parameters are in reasonably close agreement in the estimates of the pre-exponent term, log10(σ0), and the activation energy term, ΔHwet, with means and standard deviations of 3.07 ± 0.20 and 0.90 ± 0.03 respectively (Table 9). Disagreement lies in the value of the exponent on the water content, r, from 0.70 (Karato) to 1.0 (Yoshino and Poe), and on the additional activation energy term, αC1/3, with α from 0.0 (Karato) to 0.17 (Yoshino) to 1.1 (Poe). We have three knowns, namely olivine water content of 80 ppm and log10(conductivity) of −3.41 for Jagersfontein, and log10(conductivity) of −2.78 for Gibeon, one assumed datum, olivine water content of 80 ppm for Gibeon, and two derived data, the ambient temperature at 100 km beneath Jagersfontein and Gibeon. We thus have six knowns and four unknowns, two of which (log(σ0) and ΔHwet) are tightly bounded and, we assume, Gaussian distributed, and the other two (r and α) are poorly bounded and for which we must assume uniform distributions in the ranges 0.7–1.0 and 0.0–1.1 respectively.

Table 9. Parameters Fitted to Jagersfontein and Gibeon Observed Resistivities to Within σ/10 (2,450–2,700 Ω m and 590–620 Ω m Respectively), σ/4 (2,000–3,250 Ω m and 550–670 Ω m Respectively) and σ/2 (1,600–4,100 Ω m and 500–750 Ω m Respectively) Bounds for Cw = 80 ppm (±5) Water at Temperatures t of 740°C and 850°C (Both ±10°C) Respectively From 10,000,000 Realizations by Monte Carlo Random Selection From Five Gaussian Distributed Parameters log(σ0), ΔHwet, Cw, tJag and tGib and Two Uniformly Distributed Parameters, r and αa
 %log10 (σ0 [S/m])rΔHwet (eV)αJagersfontein log10 (σ [S/m])Gibeon log10 (σ [S/m])
  • a

    Each of the three runs was independent. Bold values are those adopted for the distributions.

Karato model best fitting parameters2.70 ± 0.260.70 ± 0.120.91 ± 0.040.0 (implicit)−3.41 ± 0.20−2.78 ± 0.09
Yoshino model best fitting parameters3.13 ± 0.181.0 (implicit)0.87 ± 0.030.17 ± 0.02  
Poe AV model best fitting parameters3.38 ± 0.191.0 (implicit)0.92 ±0.031.10 ±0.02  
Parameters adopted for distributions3.07 ± 0.20 (Gaussian)0.701.0 (uniform)0.90 ± 0.03 (Gaussian)0.01.1 (uniform)  
Within σ/10
Jagersfontein1.012.91 ± 0.160.92 ± 0.070.88 ± 0.030.18 ± 0.15−3.41 ± 0.01
Gibeon0.932.96 ± 0.170.90 ± 0.070.86 ± 0.040.26 ± 0.19−2.78 ± 0.005
Jagersfontein and Gibeon0.000663.05 ± 0.160.86 ± 0.080.91 ± 0.030.09 ± 0.08−3.40 ± 0.01−2.78 ± 0.005
Within σ/4
Jagersfontein2.542.91 ± 0.160.92 ± 0.070.88 ± 0.030.18 ± 0.15−3.41 ± 0.03
Gibeon2.322.96 ± 0.170.90 ± 0.070.86 ± 0.040.26 ± 0.19−2.78 ± 0.01
Jagersfontein and Gibeon0.00943.03 ± 0.170.86 ± 0.080.90 ± 0.030.13 ± 0.12−3.38 ± 0.02−2.79 ± 0.01
Within σ/2
Jagersfontein5.142.91 ± 0.170.91 ± 0.070.88 ± 0.030.19 ± 0.15−3.40 ± 0.06
Gibeon4.652.96 ± 0.170.90 ± 0.070.86 ± 0.040.26 ± 0.19−2.78 ± 0.03
Jagersfontein and Gibeon0.193.01 ± 0.160.88 ± 0.080.89 ± 0.030.16 ± 0.13−3.33 ± 0.02−2.80 ± 0.02

[67] Undertaking the same Monte Carlo exercise, but with tighter bounds on water content (±5 ppm) and temperature (±10°C), for 10 million random realizations taken from the parameter distributions yields the statistics of the acceptable solutions given in Table 9 of log10(σ0) = 3.05 ± 0.16, r = 0.86 ± 0.08, ΔHwet = 0.91 ± 0.03, and α = 0.09 ± 0.07 for olivine proton conduction for the 66 models found that fit both the Jagersfontein and Gibeon MT data to within σ/10 of their statistical limits. Conductivities from these model parameters are shown as the solid green curves in Figure 6, and for temperature and water content variation in Figure 5d.

8. Discussion

[68] Both the petrological and electromagnetic observations infer the existence of water in the upper lithosphere, with kimberlitic xenoliths yielding values around 60–100 ppm in olivine and higher in the pyroxenes (200 ppm and 300 ppm for Opx and Cpx respectively). Of the three water models defined by laboratory measurements, that of Karato is too conductive, and those of Yoshino and Poe are too resistive, all by an order of magnitude or more. Searching stochastically for model parameters acceptable to the observations (Jagersfontein and Gibeon resistivities, water contents and temperatures) yields narrowly defined values for log10(σ0), r, ΔHwet, and α. The determined values define a combination of the Karato and Yoshino/Poe models, with log10(σ0) of 3.05, which is close to the Karato value (3.0), r of 0.86, which lies between the Karato value (0.62) and unity (i.e., not considered) of Yoshino and Poe, ΔHwet of 0.91, which is at the Yoshino value (0.92) and within error of the Karato estimate (0.87), and αof 0.09 lying between the Karato value (0.0, i.e., not considered) and the Yoshino value (0.16). It must, however, be borne in mind that the field-observed calibrations have been undertaken at “barely damp” water contents, of order 60–100 ppm, andα becomes important at the higher water contents studied by Poe.

[69] In this analysis we assume that our temperature estimates are reasonable. As shown in Figures 4 and 5, temperature errors of order 50°C introduce 0.2 log unit error in estimates of proton conductivity. To explain the observations with the laboratory data, the temperature estimates would have to be underestimated by 200°C, which is unreasonable and inconsistent with all other observables [see Fullea et al., 2011].

[70] We further assume that the water contents reported for the Kaapvaal Craton [Peslier et al., 2010b; Baptiste et al., 2012] are reasonably accurate and are unbiased by water loss. We cannot though exclude the possibility, however faint, that despite the flat hydrogen profiles in almost all olivines recovered from kimberlitic xenoliths there has been water loss during escape in a manner that yields universally flat diffusion profiles. The Karato model and model parameters cannot be fit to our data for water contents beyond some 10 ppm, so are unaffected by such an argument. The Yoshino model and model parameters infer some 350 ppm water in olivine to fit the Jagersfontein resistivity, and some 550 ppm to fit the Gibeon resistivity, both of which are certainly unrealistically high. The averaged Poe model parameters requires 250 ppm and 320 ppm respectively, which is a factor of 3× greater than Peslier et al.'s [2010b] estimate for Jagersfontein and 4× greater than our assumed water content for Gibeon. Even admitting underestimation of water contents in olivines, such factors are, we believe, also too high.

[71] Last, we cannot exclude the alternate possibility that indeed either the Poe or Yoshino model parameters are correct, but there exists another exotic conducting phase, currently unknown, that increases conductivity by an order of magnitude yielding the observations shown in Figures 5 and 6. We can reasonable exclude enhanced polaron conduction; our temperature estimates would have to be in error by over 200°C, which is highly unlikely as it would require significant heating since kimberlite eruption 80 Myr ago and is inconsistent with the study of Fullea et al. [2011], among others. Carbon, at depths above the graphite-diamond stability field (approx. 150 km beneath cratons), has long been proposed to enhance mantle electrical conductivity [Duba and Shankland, 1982], but given its very high conductivity (>106 S/m) it would have to be present at extremely low fractions and that would question interconnectivity [Watson et al., 2010]. Spratt et al. [2009] discuss possible candidates for enhancing conductivity above that expected for dry minerals, and exclude almost all of them. They appeal to the speculative results of ten Grotenhuis et al. [2004] regarding grain boundary conduction in fine grained olivine to explain their observations of reduced resistivity within the Wopmay Orogen compared to the bounding cratons. Given typical grain sizes observed in xenolith samples (1 cm), this explanation can also be excluded. Finally, interstitial iron sulfides precipitated from metasomatic fluids can reduce resistivity [Ducea and Park, 2000], but again high volumes are required (>1%) to ensure interconnectivity [Watson et al., 2010] and such sulfides are not seen in xenolith material.

[72] In conclusion, given the extant data we prefer to adopt the view that the simplest explanation is likely correct, and that the reduced resistivity values we observe in the lithospheric mantle beneath Jagersfontein and Gibeon are best explained in terms of conductivity enhancement by proton conduction from hydrogen diffusion. The difficulty arises that none of the proton conduction models for olivine from the three active laboratories fit the geophysical and petrological observations. However, parameters can be found that fit the basic proton conduction equation (equation (1)) that are within error of the three labs in their estimates of the pre-exponent term and the activation energy term, but are different in the additional terms used by the labs, namely the power termron the pre-exponent water contentCw used by the Karato group to describe proton hopping, and the αCw1/3 term used by the Yoshino and Poe groups to describe H2O concentration-dependent activation enthalpy.

9. Conclusions

[73] Geodynamic models of the mantle require accurate and precise knowledge of water content and its distribution, and models without such careful consideration are misleading and are not useful exercises. The effects on viscosity of varying water content are illustrated in Li et al. [2008], who propose that cratonic material may be recycled into the mantle. Further verification of that model requires mapping of water content of the world's cratonic lithospheres.

[74] Electrical conductivity is a key and unique physical property that can yield valuable information relevant to remote sensing of water in the mantle that is difficult, if not impossible, to determine using any other approach. The water effect on enhancing conductivity is orders of magnitude, compared to minor variation in seismic velocity (∼1% reduction for 1 wt% water [Karato, 2006]) of the same order as effects from possible compositional variation (to which conductivity is essentially insensitive, see Jones et al. [2009a]). The difficulty that seismology has in inferring water content is exemplified by the comparison discussed in Karato [2011]of water content estimates in the mantle transition zone (MTZ) beneath eastern Asia, with one technique suggesting the MTZ is water-poor, and another suggesting it is water-rich (see Introduction). For the cratonic lithosphere, the difference between dry and “slightly damp” (i.e., water contents of order 100 ppm) are impossible to detect using seismology, whereas careful, well-designed EM methods can easily detect the one or more orders of magnitude increase in conductivity (Figure 1).

[75] The laboratory studies on wet mantle minerals discussed herein by Karato's, Yoshino's and Poe's groups are providing important and critical information, and their work is needed. However, the disparity in the observations and the contention between the labs is, unfortunately, resulting in low appreciation and acceptance by the geoscience community of the key role electrical conductivity observations can play in constraining water content in the mantle. The three labs have to reconcile their differences, and simultaneously we need to have more geophysical-petrological controls to calibrate the lab results. This latter point is highlighted byFigure 5 that shows the derived conductivity for the three models, plus the model defined herein, for possible lithospheric temperatures and water contents. The T-Cw model space is large, and herein we are only sampling it at two locations, namely those of Jagersfontein and Gibeon.

[76] Based on T-Cw data from two localities, i.e., 6 data, we fit a four parameter Arrhenius model of proton conduction of the general form given in equation (1)using Monte-Carlo stochastic modeling. We assume that the two better-determined parameters, log10(σ0) and ΔHwet, are Gaussian distributed in rather narrow ranges defined by the laboratory experiments, whereas the more difficult to determine parameters, r and α, are uniformly distributed with broader ranges, also defined by the experiments. Of the ten million realizations generated from the four distributions, the 66 that fit the two conductivity observations to within σ/10 have values of log10(σ0) = 3.05 ± 0.16, r = 0.86 ± 0.08, ΔHwet = 0.91 ± 0.03, and α = 0.09 ± 0.07. This model must be tested through application to other areas where we have sufficient petrological and geophysical knowledge.

Appendix A

[77] A note for the non-specialists (like us!), one must be careful when comparing various determined estimates of water content by different experimentalists depending on the calibration used. The three main ones are the Paterson calibration [Paterson, 1982], the Libowitzky and Rossman calibration [Libowitzky and Rossman, 1997], and the Bell calibration [Bell et al., 2003] (which was developed to accommodate crystal anisotropy although we do not consider anisotropic effects), yield values that are factors of up to 3 different (with Bell being the highest).

[78] Also, water concentration is reported by different authors from different communities with different units. Geochemists and petrologists mostly use weight percent (wt%) and parts per million by weight (ppm wt = 10,000 × wt%). On the other hand, in the mineral physics community H/106Si and ppm H/Si are more popular. For an olivine with a mantle composition (Fo90), 1 ppm H2O wt = 16.35 H/106Si (read 16.35 atoms of H per 106 atoms of silicon). It can also be presented as 1 ppm H2O wt = 16.35 at ppm H/Si (atomic ppm of H per atom of silicon). Those units are commonly used in studies quantifying water by Fourier transform infrared spectroscopy. When analyses are obtained by SIMS (secondary ion mass spectrometry), the detection of the chemical composition for the calibration is often presented using ratio of counts number (cts) as, for example, 16O1H/30Si (cts) or 1H/30Si (cts). One should always keep in mind that the conversion factor to go from ppm H2O wt to H/106Si or vice versa is density-dependent, then mineral-dependent (see, e.g.,Bolfan-Casanova et al. [2000, Table 1] for the calculation method). The conversion factor provided here is only for an olivine with Fo90, for a pure forsterite (Fo100), it will be 1 ppm H2O wt = 15.65 at ppm H/Si. Those values cannot be used for pyroxenes or garnet. However, pressure is expected to have little effect on those conversion coefficients.


[79] The SAMTEX data were acquired through funding provided by the Continental Dynamics program of the U.S. National Science Foundation (grant EAR0455242 to RLE), the South African Department of Science and Technology (grant to South African Council for Geoscience), and Science Foundation Ireland (grant 05/RGP/GEO001 to AGJ) plus financial and/or logistical support provided by all members of the SAMTEX consortium listed in the acknowledgments of Jones et al. [2009b]. Many people strove hard to acquire the SAMTEX data set, and all are very gratefully thanked (see authors and those acknowledged in Jones et al. [2009b]). JF was initially supported by an IRCSET grant to AGJ for the TopoMed project (TopoMed: Plate reorganization in the western Mediterranean: Lithospheric causes and topographic consequences) within the European Science Foundation's TOPO-EUROPE EUROCORES (http://www.esf.org/activities/eurocores/running-programmes/topo-europe.html), and subsequently by an SFI PI grant (10/IN.1/I3022) to AGJ for IRETHERM (www.iretherm.ie). The Editor and Reviewer are gratefully thanked for their positive and constructive reviews of the original version of this manuscript, and Sylvie Demouchy for her instruction (particularly regarding the water concentration units in Appendix A), advice and comments on water in the mantle. Their comments and perspectives caused us to include more material that is, we hope, insightful.