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作 者:胡小博 Takahiro OTSUKA Toru IWAO Tsuginori INABA
机构地区:[1]Chuo University,Tokyo 112-8551,Japan [2]Toko Electric Corporation,Saitama 349-0192,Japan [3]Musashi Institute of Technology,Tokyo 158-8557,Japan
出 处:《Plasma Science and Technology》2007年第6期752-755,共4页等离子体科学和技术(英文版)
摘 要:When a lightning current is impressed through a copper wire, the copper wire would be melted. A straight thin copper wire with a diameter of 0.1 mm,~ is melted due to the specific melting Joule heating (j^2t)m in an adiabatic condition. However, it has been recognized in the experiment that the thicker copper wires of φ1 mm are not completely melted, but sheared mainly at the connecting terminal by a relatively low impulse current. Electro-magnetic mechanical shearing stress, etc. are discussed in addition to the conventional Joule heating. New broken mechanisms were presumed and proved in the additional experiments.When a lightning current is impressed through a copper wire, the copper wire would be melted. A straight thin copper wire with a diameter of 0.1 mm,~ is melted due to the specific melting Joule heating (j^2t)m in an adiabatic condition. However, it has been recognized in the experiment that the thicker copper wires of φ1 mm are not completely melted, but sheared mainly at the connecting terminal by a relatively low impulse current. Electro-magnetic mechanical shearing stress, etc. are discussed in addition to the conventional Joule heating. New broken mechanisms were presumed and proved in the additional experiments.
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