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At a temperature of -271 °C the internal coil of the dipole magnet becomes supraconductive and can therefore be used for the generation of a magnetic field with a strength of approx. 8 Tesla.

INTO JAPANESE

-271°Cの温度では、双極子磁石の内部コイルは超伝導性になるため、約1〜2の強さの磁場の生成に使用できます。 8テスラ。

BACK INTO ENGLISH

At temperatures of -271 ° C, the internal coil of the dipole magnet becomes superconducting and can be used to generate a magnetic field with a strength of about 1-2. 8 Tesla.

INTO JAPANESE

-271°Cの温度では、双極子磁石の内部コイルは超伝導になり、約1〜2の強度の磁場を生成するために使用できます。 8テスラ。

BACK INTO ENGLISH

At temperatures of -271 ° C, the internal coil of the dipole magnet becomes superconducting and can be used to generate a magnetic field with an intensity of about 1-2. 8 Tesla.

INTO JAPANESE

-271°Cの温度では、双極子磁石の内部コイルは超伝導になり、約1〜2の強度の磁場を生成するために使用できます。 8テスラ。

BACK INTO ENGLISH

At temperatures of -271 ° C, the internal coil of the dipole magnet becomes superconducting and can be used to generate a magnetic field with an intensity of about 1-2. 8 Tesla.