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Selective Proton/Deuteron Transport through NafionlGraphenelNafion Sandwich Structures at High Current Density

机译:高电流密度下通过NafionlGraphenelNafion夹心结构的选择性质子/氘核传输

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摘要

Ion current densities near 1 A cm~(–2) at modest bias voltages (<200 mV) are reported for proton and deuteron transmission across single-layer graphene in polyelectrolyte-membrane (PEM)-style hydrogen pump cells. The graphene is sandwiched between two Nafion membranes and covers the entire area between two platinum–carbon electrodes, such that proton transfer is forced to occur through the graphene layer. Raman spectroscopy confirms that buried graphene layers are single-layer and relatively free of defects following the hot-press procedure used to make the sandwich structures. Area-normalized ion conductance values of approximately 29 and 2.1 S cm~(–2) are obtained for proton and deuteron transport, respectively, through single-layer graphene, following correction for contributions to series resistance from Nafion resistance, contact resistance, etc. These ion conductance values are several hundred to several thousand times larger than in previous reports on similar phenomena. A ratio of proton to deuteron conductance of 14 to 1 is obtained, in good agreement with but slightly larger than those in prior reports on related cells. Potassium ion transfer rates were also measured and are attenuated by a factor of many thousands by graphene, whereas proton transfer is attenuated by graphene by only a small amount. Rates for hydrogen and deuterium ion exchange across graphene were analyzed using a model whereby each hexagonal graphene hollow site is assumed to transmit ions with a specific per-site ion-transfer self-exchange rate constant. Rate constant values of approximately 2500 s~(–1) for proton transfer and 180 s~(–1) for deuteron transfer per site through graphene are reported.
机译:据报道,在适度的偏置电压(<200 mV)下,离子电流密度接近1 A cm〜(-2),用于质子和氘核在聚电解质膜(PEM)型氢泵电池中跨单层石墨烯的传输。石墨烯夹在两个Nafion膜之间,并覆盖两个铂-碳电极之间的整个区域,从而迫使质子转移穿过石墨烯层。拉曼光谱法证实,按照用于制造三明治结构的热压程序,埋入的石墨烯层为单层且相对没有缺陷。通过对Nafion电阻,接触电阻等对串联电阻的贡献进行校正,分别通过单层石墨烯获得质子和氘核传输的面积归一化离子电导率值分别约为29和2.1 S cm〜(–2)。这些离子电导率值是以前关于类似现象的报告的数百至数千倍。质子与氘核的电导比为14:1,与先前有关细胞的报道相吻合,但略有增加。还测量了钾离子的传输速率,并且通过石墨烯将钾离子的传输速率衰减了数千倍,而通过石墨烯将质子的传输仅衰减了少量。使用模型分析氢和氘离子在整个石墨烯上的交换速率,其中假设每个六边形石墨烯空心位点以特定的每位离子转移自交换速率常数传输离子。据报道,每个位置通过石墨烯的质子转移速率常数约为2500 s〜(-1),氘核的速率常数约为180 s〜(-1)。

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  • 来源
    《Journal of the American Chemical Society》 |2018年第5期|1743-1752|共10页
  • 作者单位

    Department of Chemistry, Clemson University, Clemson, South Carolina 29634, United States;

    Department of Chemistry, Texas Tech University, Lubbock, Texas 79409, United States;

    Department of Chemistry, Texas Tech University, Lubbock, Texas 79409, United States;

    Department of Chemistry, University of Utah, Salt Lake City, Utah 84112, United States;

    Department of Chemistry, Clemson University, Clemson, South Carolina 29634, United States;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);美国《化学文摘》(CA);
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  • 正文语种 eng
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