Stable carbon isotope fractionation data between H(2)CO(3)(*) and CO(2)(g) extended to 120 °C.

Stable carbon isotope fractionation data between H(2)CO(3)(*) and CO(2)(g) extended to 120 °C.
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DOI:
10.1002/rcm.6950
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发表时间:
2014-08
期刊:
Rapid communications in mass spectrometry : RCM
影响因子:
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通讯作者:
A. Myrttinen;V. Becker;Bernhard Mayer;Johannes A. C. Barth
A. Myrttinen;V. Becker;Bernhard Mayer;Johannes A. C. Barth
中科院分区:
其他
文献类型:
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作者:
A. Myrttinen;V. Becker;Bernhard Mayer;Johannes A. C. Barth

文献摘要

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理论依据关于H2 CO 3(*)(H2 CO 3 + CO2(aq))和气态CO2(CO2(g))之间实验得出的平衡稳定碳同位素分馏(10(3)lnα(13)C)的文献数据迄今为止仅在高达60 °C下可用,并且通常在大气压或接近大气压下测定。在这里,我们通过实验将该数据集扩展到接近CO2超临界状态的温度和压力条件。其目的是提高稳定碳同位素作为示踪剂在环境中的适用性,在这种情况下盛行。方法在钢制容器中进行了18个稳定碳同位素实验。将用盐酸(HCl,1 N)酸化至pH为2.4的去离子水用CO2(g)在55巴的压力(pCO 2)下平衡2至188小时的持续时间。实验在20、60、80、100和120 °C下进行。H2、CO 3(*)和CO2(g)分别取样,用同位素比值质谱法测定其碳同位素比值。结果在20 °C下,观察到平均10(3)In α(13)CH 2CO 3 * -CO2(g)值为-1.0 ± 0.1 ‰,优先使用H2 CO 3中的(12)C(*)与之前的研究一致。在120 °C的高温下,10(3)lnα(13)CH 2CO 3 * -CO2(g)值降至平均值-0.7 ± 0.1 ‰。H2 CO 3(*)和CO2(g)之间碳同位素分馏的温度依赖关系为10(3)lnα(13)CH 2CO 3 * -CO2(g)=(0.0025 ± 0.0004)T(℃)-(1.0 ± 0.03)‰。H2 CO 3(*)和CO2(g)之间的碳同位素平衡在反应时间18 h内达到,大部分在5 h或更短时间内达到。结论10(3)lnα(13)CH 2CO 3 * -CO2(g)数据现在可用于温度高达120 °C和压力高达55 bar的情况。结果表明,较高的pCO 2水平可能缩短碳同位素平衡时间。这些数据对于使用δ(13)C值作为示踪剂至关重要,例如在地质CO2封存地点和相应的天然类似物中。
RATIONALE Literature data on experimentally derived equilibrium stable carbon isotope fractionation (10(3) lnα(13) C) between H2 CO3 (*) (H2 CO3 + CO2(aq) ) and gaseous CO2 (CO2(g) ) are so far only available up to 60 °C and were typically determined at or near atmospheric pressures. Here we experimentally expand this dataset to temperature and pressure conditions close to the supercritical state for CO2 . The objective is to improve the applicability of stable carbon isotopes as a tracer in environments where such conditions prevail. METHODS Eighteen stable carbon isotope laboratory experiments were conducted in a steel vessel. Deionised water that was acidified with hydrochloric acid (HCl, 1 N) to a pH of 2.4 was equilibrated with CO2(g) at pressures (pCO2 ) of 55 bar for durations between 2 and 188 h. The experiments were conducted at 20, 60, 80, 100 and 120 °C. H2 CO3 (*) and CO2(g) were sampled separately and their carbon isotope ratios were determined by isotope ratio mass spectrometry. RESULTS At 20 °C, average 10(3) lnα(13) CH2CO3 * -CO2(g) values of -1.0 ± 0.1 ‰ were observed with a preference for (12) C in H2 CO3 (*) consistent with previous research. At elevated temperatures of 120 °C, 10(3) lnα(13) CH2CO3 * -CO2(g) values decreased to an average value of -0.7 ± 0.1 ‰. The resulting temperature dependence for carbon isotope fractionation between H2 CO3 (*) and CO2(g) was 10(3) lnα(13) CH2CO3 * -CO2(g) = (0.0025 ± 0.0004) T(°C) - (1.0 ± 0.03) ‰. Carbon isotope equilibrium between H2 CO3 (*) and CO2(g) was reached within reaction times of 18 h and mostly within 5 h or less. CONCLUSIONS 10(3) lnα(13) CH2CO3 * -CO2(g) data are now available for temperatures up to 120 °C and for pressures of up to 55 bar. The results suggest that higher pCO2 levels possibly shorten carbon isotope equilibration times. These data are critically important for using δ(13) C values as tracers, for instance at geological CO2 sequestration sites and corresponding natural analogues.