Extensive critical current density ##IMG## [http://ej.iop.org/images/0953-2048/33/10/104006/sustabaebeieqn1.gif] {${J_{\text{c}}}$} measurements are reported as a function of magnetic field ##IMG## [http://ej.iop.org/images/0953-2048/33/10/104006/sustabaebeieqn2.gif] {$B$} , temperature ##IMG## [http://ej.iop.org/images/0953-2048/33/10/104006/sustabaebeieqn3.gif] {$T$} , angle ##IMG## [http://ej.iop.org/images/0953-2048/33/10/104006/sustabaebeieqn4.gif] {$\theta $} between the applied field and the surface of the tape, and strain ##IMG## [http://ej.iop.org/images/0953-2048/33/10/104006/sustabaebeieqn5.gif] {$\varepsilon $} , on a REBCO coated conductor. The strain, ##IMG## [http://ej.iop.org/images/0953-2048/33/10/104006/sustabaebeieqn6.gif] {${\varepsilon _{{\text{peak}}}}\left( {B,T,\,\theta } \right)$} , at which ##IMG## {${J_{\text{c...}

中文翻译：

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高温超导体涂层导体REBCO的临界电流密度与角度的关系微弱出现

广泛的临界电流密度## IMG ## [http://ej.iop.org/images/0953-2048/33/10/104006/sustabaebeieqn1.gif] {$ {J _ {\ text {c}}} $}测量结果报告为磁场的函数## IMG ## [http://ej.iop.org/images/0953-2048/33/10/104006/sustabaebeieqn2.gif] {$ B $}，温度## IMG ## [http://ej.iop.org/images/0953-2048/33/10/104006/sustabaebeieqn3.gif] {$ T $}，角度## IMG ## [http：//ej.iop .org / images / 0953-2048 / 33/10/104006 / sustabaebeieqn4.gif] {$ \ theta $}在所施加的电场和胶带表面之间，并应变## IMG ## [http：// ej。 iop.org/images/0953-2048/33/10/104006/sustabaebeieqn5.gif] {$ \ varepsilon $}，在REBCO涂层导体上。菌株## IMG ## [http://ej.iop.org/images/0953-2048/33/10/104006/sustabaebeieqn6.gif] {$ {\ varepsilon _ {{\ text {peak}}} } \ left（{B，T，\，\ theta} \ right）$}，其中## IMG ## {$ {J _ {\ text {c ...}