Friedhelm
von Blanckenburg
*a,
Marcus
Oelze
a,
Dietmar G.
Schmid
b,
Kirsten
van Zuilen
f,
Hans-Peter
Gschwind
b,
Alan J.
Slade
c,
Sylvie
Stitah
d,
Daniel
Kaufmann
e and
Piet
Swart
b
aGFZ German Research Center for Geosciences, Potsdam, Germany. E-mail: fvb@gfz-potsdam.de
bNIBR/DMPK, Novartis Pharma AG, Basel, Switzerland
cNIBR/Translational Medicine, Novartis Corporation, East Hanover, USA
dClinical Science and Innovation, Novartis Pharma AG, Basel, Switzerland
eChemical and Analytical Development, Novartis Pharma AG, Basel, Switzerland
fInstitute of Geological Sciences, University of Berne, Switzerland
First published on 24th June 2014
We present precise iron stable isotope ratios measured by multicollector-ICP mass spectrometry (MC-ICP-MS) of human red blood cells (erythrocytes) and blood plasma from 12 healthy male adults taken during a clinical study. The accurate determination of stable isotope ratios in plasma first required substantial method development work, as minor iron amounts in plasma had to be separated from a large organic matrix prior to mass-spectrometric analysis to avoid spectroscopic interferences and shifts in the mass spectrometer's mass-bias. The 56Fe/54Fe ratio in erythrocytes, expressed as permil difference from the “IRMM-014” iron reference standard (δ56/54Fe), ranges from −3.1‰ to −2.2‰, a range typical for male Caucasian adults. The individual subject erythrocyte iron isotope composition can be regarded as uniform over the 21 days investigated, as variations (±0.059 to ±0.15‰) are mostly within the analytical precision of reference materials. In plasma, δ56/54Fe values measured in two different laboratories range from −3.0‰ to −2.0‰, and are on average 0.24‰ higher than those in erythrocytes. However, this difference is barely resolvable within one standard deviation of the differences (0.22‰). Taking into account the possible contamination due to hemolysis (iron concentrations are only 0.4 to 2 ppm in plasma compared to approx. 480 ppm in erythrocytes), we model the pure plasma δ56/54Fe to be on average 0.4‰ higher than that in erythrocytes. Hence, the plasma iron isotope signature lies between that of the liver and that of erythrocytes. This difference can be explained by redox processes involved during cycling of iron between transferrin and ferritin.
These observations raise mechanistic questions about the observed tissue dependent iron isotope fractionation. Mass-dependent stable isotope fractionation may occur during transport of ions or molecules, or during formation or breaking of chemical bonds. Nevertheless, isotope fractionation will only become detectable if the atomic species, differing in their isotope ratios, are separated in physically distinct compartments. Following these considerations it has been suggested that the uptake of dissolved iron via the intestinal mucosa is the most likely site of fractionation. In the case of intestinal iron absorption, the transfer from the luminal side to the blood plasma is incomplete; on average only 1 mg of dietary supply of approx. 10 to 15 mg of ingested iron is absorbed.1,7 In addition, the uptake of elemental iron requires the reduction of dietary Fe(III) to Fe(II) that is transported by a divalent metal transporter (DMT-1) via an intestinal ferric reductase (Dcytb).8 The redox processes involve an equilibrium isotope fractionation shifting the 56Fe/54Fe ratio by approx. 3‰ to low values in the ferrous iron as shown by experimental determination9 and ab initio calculation of isotope fractionation factors.10 Within the intestinal mucosa, a similar, oxidative process via the ferroxidase hephaestin is required to convert the absorbed Fe(II) back to Fe(III) for further distribution via transferrin.8
In this regard, the protein transferrin, bearing two iron binding sites, and contained mostly in blood plasma, is a key player.11 After intestinal uptake, freshly absorbed iron is loaded onto transferrin and transported within the blood plasma to various organs and tissues. Although only about 0.1% of total body iron (3 mg) is bound to transferrin, the daily turnover is significant, where 20 to 25 mg are transported through the blood plasma each day.7a Most iron is transported into the red bone marrow for synthesis of hemoglobin and erythrocytes. As noted previously, the internal distribution of iron within the human body is subject to further isotopic fractionation.1,5 One possible explanation for the different isotopic compositions of these iron storage compartments is isotope fractionation during transport or during iron loading and unloading from transferrin. The same holds for iron release from transferrin. Upon binding to the transferrin receptor, the transferrin–receptor complex is internalized via endocytosis. Should isotope fractionation during transferrin loading and release be zero, then the iron composition of erythrocytes should resemble that of plasma. However, transferrin also transports a substantial amount of iron from other storage compartments like the liver. Thus, another potential process entailing fractionation is during iron storage and release from various tissue depots. Iron is stored as a stable ferrihydrate complex in ferritin where Fe(II) is oxidized to Fe(III) by ferroxidase in the ferritin complex.12 It has been shown in humans that the liver contains iron of which the 56Fe/54Fe ratio is higher than that of erythrocytes.1,5 If during release from the liver this heavy iron is not fractionated towards the erythrocytes' ratio, then transferrin should contain iron comprising a mixture of that delivered during hemoglobin synthesis with that delivered from the liver. Hence, the transferrin's isotope composition should lie between that of the liver and that of erythrocytes. To date, only one study has reported the iron composition of human blood plasma and found it to be enriched in 56Fe over 54Fe relative to blood, and hence being of composition closer to liver iron.13
In this study we test these hypotheses by presenting precise iron stable isotope ratios measured in human erythrocytes and plasma samples. Blood was sampled over a period of 21 days from 12 healthy male adults. The study was performed within the context of a ferrokinetics and uptake study of iron following administration of oral doses of the compound SBR759, labeled with the stable isotope 58Fe. The results of the iron uptake study are presented in a companion paper.14 A challenge for such an investigation is the determination of accurate, stable iron isotope ratios in plasma. Plasma iron concentrations are approx. 0.4 to 2 ppm compared to that of erythrocytes which can be greater than 400 ppm. Hence, a large organic matrix has to be separated prior to mass-spectrometric analysis to avoid spectroscopic interferences and shifts in the mass-bias introduced during measurements by impurities contained in the samples.15 Presenting suitable analytical protocols is therefore the first aim of this study.
Plasma was obtained from heparinized blood by centrifugation at 2000 × g, at 4 °C for 10 min. Plasma was recovered into pre-weighed tubes (Monovettes for metal analysis, Sarstedt) and stored at ≤−20 °C. Plasma samples which displayed visible signs of hemolysis were excluded from data analysis. Plasma was prepared from blood at 0 h (pre-dose), 6, 12, 16, 22 and 26 h post first dose.
After sample collection, erythrocyte and plasma samples were frozen immediately and stored at ≤−20 °C until and after analysis in the analytical laboratories. Samples were shipped to analytical laboratories under dry ice to keep them frozen.
To test whether the insoluble residues were free of iron, a standard addition experiment was conducted on a plasma test sample. This sample was split into two aliquots before freeze-drying. The first aliquot was then split into 6 sub-splits. To each of these a known amount of CertiPUR® iron standard was added in increasing volumes. To the first aliquot, the additions were made before freeze-drying. To the second aliquot, the additions were made after dissolution and separation of the insoluble residue by centrifugation. The iron amounts found in both experiments were roughly identical within analytical error, which ranged from 1 to 7%. Hence no iron from the original plasma or from the additions was lost into the precipitate. Given that this step did not result in loss of iron, all plasma concentration measurements were performed on a 300 μL aliquot taken from the 6 M hydrochloric acid solution.
For samples containing high initial amounts of transition metals or organic matrices, iron separated by anion exchange chromatography may not be entirely matrix-free and requires further purification. Therefore, all samples were neutralised with ammonia and subjected to a precipitation step.15 For plasma samples which in general contain much less iron when compared to blood, a normal precipitation step15,16 could not be applied. Instead, plasma samples were co-precipitated after chromatographic separation by adding 1 mL of a 1000 ppm aluminum solution into 0.3 M HNO3, which was first pre-cleaned by anion exchange chromatography to remove traces of iron. The co-precipitation was achieved by adding NH4OH to the samples. To achieve maximum iron yields, the solutions were allowed to equilibrate for 1 hour before centrifugation. The supernatants were removed and the precipitates were washed 2-times with Milli-Q H2O, followed again by centrifugation and finally re-dissolved in 1 mL of 6 M hydrochloric acid. To remove the aluminum, a second anion exchange chromatography was necessary, which followed the same procedure as the first one at the beginning of the iron separation scheme. The eluents were then dried and dissolved in 5 mL of 0.3 M HNO3.
Whereas argides can be resolved from each corresponding iron isotope due to the high mass resolving power of the MC-ICP-MS, potential isobaric interferences of 54Cr+ and 58Ni+ on 54Fe+ and 58Fe+, respectively, were minimised by removal of chromium and nickel using anion exchange chromatography. The purity of the fractions after anion exchange chromatography was monitored by ICP-OES. To correct for minor residual interferences, the isotopes 52Cr and 60Ni were measured in parallel with 54Fe, 56Fe, 57Fe and 58Fe. The interference correction for 54Cr on 54Fe and 58Ni on 58Fe was performed according to ref 15. Briefly, the amount of 54Cr was calculated from the intensity of 52Cr measured simultaneously and from the average natural 54Cr/52Cr ratio. The amount of interfering 58Ni was calculated from the average natural 60Ni/58Ni ratio. An instrumental mass discrimination factor was applied to 52Cr and 58Ni intensities, respectively, which was determined from the measured 57Fe/56Fe ratio by applying the exponential mass bias law.
Instrumental mass discrimination induced by the incomplete removal of the sample matrix or non-reproducible mass-spectrometric run conditions potentially introduced a substantial bias into the resulting isotope ratio measurements. As iron concentrations in blood plasma are low, and a large organic matrix is present, these measurements are particularly prone to such bias. For this reason the measurement of 18 separated plasma iron samples was repeated on a similar instrument (Thermo Neptune Plus Multicollector ICP-MS) based at the GeoForschungsZentrum Potsdam. For these measurements, ESI Apex-Q desolvating apparatus using a low flow (aspiration rate of 100 μL min−1) PFA self-aspirating nebuliser was used. The ESI Apex-Q apparatus consists of a heated cyclonic glass spray chamber coupled with a Peltier element-cooled glass spiral condenser. The mass spectrometer's interface was equipped with Thermo “Jet” cones. This instrumental setup, which differs considerably from that used at the University of Hannover, would detect a potential matrix-induced mass bias in the form of non-reproducible isotope ratios.
A similar equation is used for δ57Fe and δ58Fe when 56Fe is replaced by 57Fe or 58Fe, respectively.
Another test for the presence of isobaric interferences is the use of three isotope plots, where offsets from the predicted mass-dependent fractionation curve indicate the presence of isobaric interferences. The delta/delta graphs of normalised iron isotope ratios (δ57Fe/54Fe versus δ56Fe/54Fe and δ58Fe/54Fe versus δ56Fe/54Fe) of the “JM” and “HanFe” iron standards are depicted in Fig. S1a–d (ESI†) and of baseline blood and plasma samples in Fig. S1e–h (ESI†). All standard and sample results plot onto the mass-dependent isotope fractionation line, which indicates measurements that were free of spectral interferences. Blood and plasma samples post first dose containing absorbed [58Fe]SBR759-related iron might contain a relatively higher fraction of 57Fe (i.e. “impurity” in the 58Fe label), as compared to its natural abundance. The isotopic composition of [58Fe]SBR759 relative to the international “IRMM-014” reference material was determined to be 5.706% 54Fe, 89.552% 56Fe, 2.077% 57Fe, and 2.665% 58Fe,14 which compares to 5.845% 54Fe, 91.754% 56Fe, 2.12% 57Fe, and 0.281% 58Fe for the reference material “IRMM-014”.19 Hence in this study δ57Fe and δ58Fe for post first dose samples are not used.
For plasma samples, we observed higher 52Cr levels than for either blood samples or the standard materials. We tested whether this increase was due to unresolved 40Ar12C interferences on mass 52. In that case the 54Fe intensities would be over-corrected for 54Cr. We plotted the δ57Fe/56Fe ratio against δ56Fe/54Fe of plasma baseline samples (Fig. 1). The 57Fe/56Fe ratio is not subject to a Cr interference correction. The fact that all data plot on the mass-dependent fractionation curve, regardless of whether they have been corrected for Cr interferences, shows that Cr corrections did not introduce a bias resulting from excessive 54Fe corrections.
![]() | ||
Fig. 1 δ 57Fe/56Fe versus δ56Fe/54Fe diagram as test for excessive 54Cr interference due to the presence of an 40Ar12C interference on the monitor isotope 52Cr in plasma baseline samples (taken before administration of SBR759 to ensure the absence of a 57Fe contribution from the spike). The 57Fe/56Fe ratio is not subject to a Cr interference correction. Open symbols: δ56Fe not corrected for “Cr” interference; closed symbols: δ56Fe ratios corrected for interferences. The error ellipse denotes the correlated 2·standard deviation as derived from “JM” standard measurements (Table S1, ESI†). The fact that all data plots on the mass-dependent fractionation curve shows that Cr corrections did not introduce a bias resulting from excessive 54Fe corrections. |
Subject | Blood samples | Plasma samples | Difference plasma – blood | |||||||||||
---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
0–490 hours | 0–26 hours | 0–26 hours | 0–26 hours | |||||||||||
Fe conc. [ppm] | 2·SD [ppm] | δ 56/54Fe [‰] | 2·SD [‰] | δ 56/54Fe [‰] | 2·SD [‰] | Fe conc. [ppm] | 2·SD [ppm] | δ 56/54Fe [‰] | 2·SD [‰] | δ 56/54Fe [‰] | 2·SD [‰] | δ 56/54Fe [‰] | ||
Hannover | Potsdam | Hann | Pots | |||||||||||
5101 | 433 | 32 | −2.214 | 0.059 | −2.194 | 0.032 | 1.01 | 0.63 | −2.31 | 0.45 | −1.95 | — | −0.12 | 0.25 |
5102 | 428 | 22 | −2.490 | 0.075 | −2.470 | 0.019 | 0.59 | 0.25 | −2.21 | 0.20 | −2.33 | 0.13 | 0.26 | 0.15 |
5103 | 452 | 38 | −2.627 | 0.079 | −2.609 | 0.027 | 1.21 | 1.19 | −2.30 | 0.23 | −2.40 | — | 0.31 | 0.21 |
5104 | 471 | 19 | −2.801 | 0.090 | −2.785 | 0.095 | 0.70 | 0.48 | −2.77 | 0.15 | — | — | 0.01 | — |
5105 | 491 | 26 | −2.708 | 0.115 | −2.730 | 0.102 | 0.77 | 0.97 | −2.45 | 0.17 | — | — | 0.28 | — |
5106 | 460 | 17 | −2.676 | 0.059 | −2.686 | 0.028 | 0.66 | 0.36 | −2.56 | 0.10 | — | — | 0.13 | — |
5107 | 466 | 25 | −2.626 | 0.109 | −2.648 | 0.069 | 0.92 | 0.64 | −2.38 | 0.49 | −2.58 | — | 0.26 | 0.06 |
5108 | 443 | 26 | −2.640 | 0.151 | −2.690 | 0.048 | 0.66 | 0.31 | −2.29 | 0.23 | −2.61 | 0.11 | 0.40 | 0.08 |
5109 | 442 | 28 | −3.061 | 0.081 | −3.070 | 0.088 | 0.71 | 0.59 | −2.73 | 0.29 | −2.95 | — | 0.34 | 0.12 |
5110 | 495 | 28 | −2.642 | 0.112 | −2.634 | 0.112 | 1.02 | 0.48 | −2.53 | 0.25 | — | — | 0.10 | — |
5111 | 497 | 25 | −2.904 | 0.067 | −2.910 | 0.090 | 0.71 | 0.30 | −2.58 | 0.18 | −2.88 | 0.17 | 0.33 | 0.03 |
5112 | 495 | 28 | −2.561 | 0.075 | −2.573 | 0.069 | 0.71 | 0.35 | −2.07 | 0.09 | — | — | 0.51 | — |
Mean | 464 | −2.663 | −2.667 | 0.81 | −2.43 | −2.53 | 0.23 | 0.13 | ||||||
Min | 428 | 17 | −3.061 | 0.059 | −3.070 | 0.019 | 0.59 | 0.25 | −2.77 | 0.09 | −2.95 | 0.11 | −0.12 | 0.03 |
Max | 497 | 38 | −2.214 | 0.151 | −2.194 | 0.112 | 1.21 | 1.19 | −2.07 | 0.49 | −1.95 | 0.17 | 0.51 | 0.25 |
δ 56Fe in erythrocytes ranges from approx. −3.1 to −2.2‰ (Fig. 2), a range typical for male Caucasian adults.3 The 2·SD value of erythrocyte samples taken at different intervals from an individual subject varied between ±0.06 and ±0.15‰ (2·SD), which is in most cases indistinguishable from the analytical precision of laboratory standards (Table 1). Hence, erythrocyte Fe isotopic compositions can be regarded as uniform over the 21 days investigated (Fig. 2). In plasma samples, δ56Fe values ranged from approx. −3.0 to −2.0‰ (Fig. 3). The 2·SD value of all plasma samples from an individual subject was mostly around ±0.2‰, but varied between ±0.09 and ±0.49‰ (2·SD, Table 1). We quantified the attainable reproducibility for plasma measurements from our inter-laboratory comparison, which provides the strongest possible quantification of the most likely source of uncertainty, i.e. mass-spectrometric bias from uncorrectable matrix effects. For our 16 duplicate measurements δ56Fe is on average 0.26‰ and δ57Fe 0.37‰ lower at GFZ Potsdam than at the University of Hannover (Table S3, ESI†). This systematic bias resulted from the entirely different run conditions and places a lower limit on the reproducibility that is attainable for such complex matrix. Such an effect might arise, for example, from excess amounts of organic carbon that were still present in the Fe separates during MC-ICP-MS analysis. Calculating the 2·SD value from the sixteen duplicates, we obtain for δ56Fe 0.28‰ and for δ57Fe 0.39‰. We use this reproducibility in the interpretation of the data. The plasma samples taken at 26 hours of subjects 5101 and 5102, respectively, yielded δ56Fe values that deviated more than 25% from that of all other plasma samples of these subjects (Table S3, ESI†). We have no explanation for this deviation, and used instead the repeat measurement performed at GFZ Potsdam that agreed well with the other samples from these subjects. Overall, the iron isotopic composition in plasma was more variable than in erythrocytes. We attribute this variability to the lower reproducibility of these measurements.
![]() | ||
Fig. 3 δ 56Fe in plasma of the 12 subjects against sampling time. The symbols denote individual subjects and are the same as in Fig. 2. Error bars show 2 standard deviations. |
δ 56Fe in plasma samples is higher than that in erythrocytes in 11 out of 12 samples by 0.01 to 0.51‰ (Fig. 4). Only the subject 5101 features a δ56Fe value in its plasma sample that is lower than that in erythrocytes by 0.21‰. The average difference in δ56Fe between plasma iron and erythrocyte iron is 0.23‰ (Table 1). This difference is only marginally in excess of the 2·SD value resulting from our inter-laboratory comparison. We therefore cannot conclude with certainty that the difference is real. We note that after administration of [58Fe]SBR759, 57Fe in plasma samples is elevated over baseline as the 58Fe spike added also contains elevated levels of 57Fe (see Table S4, ESI†). 56Fe however is unaffected, and plots of 56Fe/54Fe vs.58Fe/54Fe do not yield correlations as would be expected if contamination of 56Fe by [58Fe]SBR759 would occur. However, plasma samples might have been affected by hemolysis. We proceed to discuss this question in comparison to literature data in the next section.
![]() | ||
Fig. 4
δ
56Fe in plasma against erythrocytes. Most data plot within 0.5‰ within the 1![]() ![]() |
As spectrophotometric measurements of hemoglobin levels in our plasma samples were not done, we evaluate this possibility based on literature data. Our measured plasma iron concentrations are within known values that range between 0.75 and 1.75 ppm for males4b,22 suggesting that iron in plasma was not contaminated by erythrocyte iron. We can evaluate the contribution of iron to plasma from hemoglobin further from hemoglobin levels quantified in plasma by spectrophotometry.23 The hemoglobin levels in plasma reported in that study range between 0.002 and 0.019 (mean 0.007) w/V%. Using the iron concentration of hemoglobin (0.35 weight%) typical iron contamination levels between 0.07 and 0.66 ppm with a mean of 0.24 ppm can be calculated. Since our samples have been taken and centrifuged with great care, we adopt the mean minimum hemoglobin iron contamination level of 0.24 ppm and assume that all iron in excess of this value is truly plasma iron. This assumption means that iron concentrations of uncontaminated plasma are between 0.5 and 1.5 ppm.
To calculate the plasma iron isotope composition despite the possibility of contamination by erythrocyte hemolysis, we plotted the difference in δ56Fe between erythrocytes and plasma against the inverse concentration of iron in plasma (Fig. 5). In such a diagram, mixtures yield a linear relationship and the end member compositions can be inferred. The figure shows that the isotope difference between Fe in erythrocytes and Fe in plasma increases with a decrease in the concentration. As δ56Feerythrocytes is constant for each subject this means that δ56Feplasma increases with a decrease in the concentration. This trend is more pronounced for samples taken from Hours 22 to 26 (open colored symbols) than those taken from Hours 0 to 16 (closed colored symbols). We explain this trend with the decreasing effect of hemolysis introduced during sampling, as the inserted plastic cannula remained in place throughout. Hence the samples taken last approach the true δ56Feplasma most closely.
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Fig. 5 δ 56Feerythrocytes – δ56Feplasmaversus 1/Fe concentration in plasma. The colored symbols are from this study (subjects as in Fig. 2), where closed symbols show data for samples taken from 0 to 16 hours and open symbols for samples taken from 22 to 26 hours. The grey symbols show data from ref. 13. The lines and tick marks show three mixing models that serve to predict how data would be aligned if plasma iron were contaminated by erythrocyte-sourced iron. In each model the iron concentration in erythrocytes was set to 480 ppm, while the iron concentration in plasma was set to 0.4 ppm. The true isotope difference Δ56Fe erythrocytes – plasma was set to −0.4‰, −1.5‰, and −2.5‰ in the three models. The weight% tick marks on the model curve indicate the weight fraction of total erythrocyte sample mixed with total plasma by hemolysis (from 0 to 0.5 and 100 weight%). |
A linear regression analysis through all our data (Fig. 5) yields a slope of −0.2 with R2 of 0.2. We used this slope to model where δ56Feerythrocytes – δ56Feplasma would plot if plasma was contaminated by variable amounts of erythrocytes during centrifugation (Fig. 5). In this calculation, we assumed the “pure”, but unknown plasma iron isotope composition with three independent models, as shown by the lines and tick marks in Fig. 5 – in each model the iron concentration in erythrocytes was set to 480 ppm, while the iron concentration in uncontaminated plasma was set to 0.4 ppm. For our data the isotope difference Δ56Feerythrocytes–plasma obtained to satisfy a slope of −0.2 is −0.4‰. We conclude that this value is the average difference between erythrocyte Fe isotope composition and uncontaminated plasma isotope composition in our samples.
We can compare this relationship to the one obtained in ref. 13 Fe in these serum samples13 were on average 1‰ heavier than erythrocytes in females and 0.6‰ heavier in males, respectively. We note however that while our mean Fe concentrations in plasma (0.8 ppm) were similar to the serum data from ref. 4b (0.9 ppm), Fe concentrations in serum samples of Albarède et al.13 were higher with a mean concentration of 1.4 ppm. If the samples in that study were still affected by hemolysis, modeled slopes demand that their δ56Fe in the serum differs by −1.5‰ from erythrocytes in males, and by −2.5‰ in females, respectively, (see Δ56Fe erythrocytes–plasma models −1.5‰ and −2.5‰ in Fig. 5). We regard such strong isotope fractionation as unlikely. If these experiments were not affected by hemolysis, the possibility remains that isotope ratios are subject to an unidentified analytical mass bias. Given the difficult matrix that plasma or serum represents, and the challenge we have encountered in developing a suitable analytical protocol, this explanation cannot be fully excluded.
Using our new plasma data presented here, we proceed with the conclusion that δ56Fe in plasma is at least 0.4‰ higher than that in erythrocytes.
Where does the isotope fractionation between plasma Fe and erythrocyte Fe occur? The liver, spleen, and red bone marrow contain iron that can be up to 1‰ heavier than erythrocytes.1,5 Transferrin is the molecule transporting iron contained in plasma into and from these compartments. In this regard, it is important that this study recruited healthy male subjects who were iron replete i.e. nonanemic and are expected to have a normal erythrocyte turnover rate. At the end of their ∼120 day lifespan, heme iron from erythrocytes in blood, and myoglobin from the damaged muscle tissue are recycled after being phagocytosed by circulating macrophages or the reticuloendothelial system (RES) of the spleen24 and released back into the plasma bound to transferrin. This recycling rate is approximately 2 mg per day from erythrocytes and another 2 mg from the muscle tissue,25 potentially dominating the isotope composition of the iron contained in plasma. As heavy liver iron is stored in the ferritin molecule, release of iron from ferritin could play a key role in tissue fractionation since tissues enriched in heavier iron isotopes are generally high in ferritin content. In general, two chemical reaction types, binding to organic molecules and redox processes, lead to different degrees of isotope fractionation. Fe(III) – chelate fractionation is +0.2‰ at equilibrium.26 This fractionation factor is too small to explain the large difference between plasma and liver iron or erythrocyte iron. Reduction from ferric to ferrous iron through activity of a reductase is a more likely explanation.6,11 Iron binding to ferritin involves oxidation of iron via a ferroxidase.27 As noted in the Introduction, these redox processes can be accompanied by equilibrium isotope fractionation amounting to up to 3‰ in δ56Fe,9,10 potentially favouring heavy iron isotopes in ferritin. If transferrin iron remains in the ferric state, whereas heme iron carried by erythrocytes is in the ferrous state,1 then plasma iron isotope composition will be intermediate between that of erythrocyte and ferritin iron, as the liver will release preferentially heavy iron isotopes, which are then mixed with light iron isotopes from quantitative erythrocyte recycling. Hence, redox processes play the decisive role in iron isotope fractionation between compartments of the human body, regardless of whether the pathways are direct or indirect.1,13
Footnote |
† Electronic supplementary information (ESI) available: Supplement 1: Fe isotope delta–delta graphs of reference materials and samples. Supplement 2: compilation of internal laboratory reference iron standards. Supplement 3: measured Fe concentration and isotope data on blood. Supplement 4: measured Fe concentration and isotope data on blood plasma. Supplement 5: SBR759 measured iron isotope composition. See DOI: 10.1039/c4mt00124a |
This journal is © The Royal Society of Chemistry 2014 |