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We measured the electrical resistivity of face-centered-cubic (fcc) structured iron hydrides at high pressures up to 65 GPa and high temperatures in a laser-heated diamond anvil cell. The results indicate that the resistivity of stoichiometric fcc FeHx (x ~ 1.0) is smaller than that of fcc Fe at the same pressure and temperature conditions. The same behavior was also observed in fcc FeNiHx (x ~ 1.0). On the other hand, hydrogen-poor fcc FeHx (x < 0.77) showed a resistivity comparable to that of the fcc phase of pure iron. Therefore, we conclude that the stoichiometric fcc Fe (–Ni) hydride is more conductive than Fe (–Ni) with the same crystal symmetry, and the impurity resistivity of hydrogen in Fe is vanishingly small. Even if hydrogen is the major light element in the Earth's core, it would have little influence on the electrical and thermal conductivity of Fe–Ni alloys, and hence the thermal evolution of the core. 相似文献
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Kay I. Ohshima Genta Mizuta Motoyo Itoh Yasushi Fukamachi Tatsuro Watanabe Yasushi Nabae Koukichi Suehiro Masaaki Wakatsuchi 《Journal of Oceanography》2001,57(4):451-460
In the southwestern part of the Okhotsk Sea, oceanographic and sea-ice observations on board the icebreaker Soya were carried out in February 1997. A mixed layer of uniform temperature nearly at the freezing point extending down to a
depth of about 300 m was observed. This is much deeper than has previously been reported. It is suggested that this deep mixed
layer originated from the north (off East Sakhalin), being advected along the shelf slope via the East Sakhalin Current, accompanied
with the thick first-year ice (average thickness 0.6 m). This vertically uniform winter water, through mixing with the surrounding
water, makes the surface water more saline (losing a characteristic of East Sakhalin Current Water) and the water in the 100–300
m depth zone less saline, colder, and richer in oxygen (a characteristic of the intermediate Okhotsk Sea water). The oceanographic
structure and a heat budget analysis suggest that new ice zone, which often appears at ice edges, can be formed through preconditioning
of thick ice advection and subsequent cooling by the latent heat release due to its melting.
This revised version was published online in August 2006 with corrections to the Cover Date. 相似文献
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