ON THE EQUILIBRIUM OF FLUIDS IN AN ELECTROMAGNETIC FIELD

SHIZUWO SANO

doi:10.11429/subutsugaiyo1903.2.365

SHIZUWO SANO

著者情報

ジャーナルフリー

1905 年 2 巻 24 号 p. 365-380

DOI https://doi.org/10.11429/subutsugaiyo1903.2.365

詳細

Published: 1905 Received: - Available on J-STAGE: 2006/03/27 Accepted: - Advance online publication: - Revised: -
訂正情報
訂正日: 2006/03/27 訂正理由: - 訂正箇所: 論文受付日訂正内容: 訂正前 : 19050617

訂正日: 2006/03/27 訂正理由: - 訂正箇所: 著者情報訂正内容: 訂正前 : 佐野静雄

訂正日: 2006/03/27 訂正理由: - 訂正箇所: 引用文献情報訂正内容: Wrong : It was pointed out by H. v. Helmholtz that the contact electricity diminishes the surface tensions, (Monatsber, d. Berl. Akad, Nov. 1881; Ges. Abb. 1, p. 945, Leipzing 1882.)
See. W. Gieses, Wied. Ann. 37, p. 576, 1889.
See P. Duhem, Ann. Sc. de Pecole norm. sup. (3) 7, p. 289, 1890.
D. Hurmezeascu, C. R. 119, p. 1006. 1894; Jour. d. Phys. (3) 4, p. 118, 1895 ; Rapports présenté au Congrés international de Physique 2, p. 557, Paris, 1900. This problem was also treated by P. Duhem. (Ann. d. la Fac. Sc. d. Toulouse 2, 1888-89.) but I had not access to his paper.
A. Einstein, Ann. d. Phys. 8, p. 802, equation (2), 1902. The impressed force considered by him is more general than the case of gruvity.
W. Nernst, Zeitscchr. f. phys. Chem. 9, p. 137, 1892.
See W. Nernst, Zeitschr. f. phys. Chem. 4, p. 129, 1889 ; Theoretische Chemie 4th Edition, p. 705, Stuttgart, 1903.
G. Jäger, Ber. 108, Abth. 2a, p. 1499, 1899.

Right : * Here it will be understood that in the case in which there are convertible components F₀ is not the actual value of the free energy per unit volume when the electric and magnetic forces vanish under the same condition of temperature and volume, but it is the value which F would assume on the supposition that ρ₁, ρ₂,...ρ_n, θ do not vary; i.e. if F≡F(ρ₁, ρ₂,...ρ_n, θ, X, Y, Z, α, β, γ), then F₀ stands for F(ρ₁, ρ₂,....ρ_n, θ, 0, 0, 0, 0, 0, 0), where ρ₁, ρ₂,...ρ_n refer to the case in which the substance is placed in the field.
* It was pointed out by H. v. Helmholtz that the contact electricity diminishes the surface tension, (Monatsber, d. Berl. Akad, Nov. 1881; Ges. Abh. 1, p. 925, Leipzig, 1882.)
* See W. Giese, Wied. Ann. 37, p. 576, 1889.
† See P. Duhem, Ann, Sc, de l'Ecole norm. sup. (3) 7, p. 289, 1890.
* D. Hurmezescu, C. R. 119, p. 1006, 1894; Jour. d. Phys. (3) 4, p. 118, 1895; Rapports présenté au Congrès international de Physique 2, p. 557, Paris, 1900. This problem was also treated by P. Duhem, (Ann. d. la Fac. d. Sc. d. Toulouse 2, 1888-89,) but I had not access to his paper.
* A. Einstein, Ann. d. Phys. 8, p. 802, equation (2), 1902. The impressed force considered by him is more general than the case of gravity.
* W. Nernst, Zeitschr. f. phys. Chem. 9, p. 137, 1892.
* See W. Nernst, Zeitschr. f. phys. Chem. 4, p. 129, 1889.
* Theoretische Chemie, 4th Edition, p. 705, Stuttgart, 1903.
* G. Jäger, Wien. Ber. 108, Abth, 2a, p. 1499, 1899.

訂正日: 2006/03/27 訂正理由: - 訂正箇所: PDFファイル訂正内容: -

責任著者(Corresponding author)

訂正情報

J-STAGEへの登録はこちら（無料）