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一般相対性理論 - 九州大学（KYUSHU UNIVERSITY）
1.1.2 Galilei の相対性原理 Galilei2 の相対性原理 「どの慣性座標系を基準にとっても Newton の力学法則は同じ形式 に書き表される．」 まず，ある慣性座標系を平行移動しても回転しても，慣性座標系とな
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野村 清英 - 九州大学（KYUSHU UNIVERSITY）
maya.phys.kyushu-u.ac.jp1 第0章 序 0.1 諸定数 アボガドロ(Avogadro)定数：NA = 6:022140857(74) 1023mol 1 ボルツマン(Boltzmann)定数：kB = 1:38064852(79) 10 23m2kgs 1K 1(J K 1) 気体定数: R= NAkB = 8:3144598(48)JK 1mol 1 プランク(Planck)定数: h= 6:626070040(81) 10 34m2kg=s(J s);ℏ = h=(2ˇ) 電子の静止質量：me = 9:10938356(11) 10 31kg 電子の素電荷: e= 1:6021766208(98) 10 19C
相転移の統計力学
maya.phys.kyushu-u.ac.jp1 第0章 序論 0.1 相転移と臨界現象 1次相転移: 1. 自由エネルギーの1階微分が不連続、潜熱や密度変化 2. 例としては、固体ー液体の融解など
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