ON THE EQUILIBRIUM OF FLUIDS IN AN ELECTROMAGNETIC FIELD

SHIZUWO SANO

doi:10.11429/subutsugaiyo1903.2.365

SHIZUWO SANO

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1905 Volume 2 Issue 24 Pages 365-380

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

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Published: 1905 Received: - Available on J-STAGE: March 27, 2006 Accepted: - Advance online publication: - Revised: -
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Date of correction: March 27, 2006 Reason for correction: - Correction: DTRECEIVED Details: Wrong : 19050617

Date of correction: March 27, 2006 Reason for correction: - Correction: AUTHOR Details: Wrong : Shizuwo Sano
Right : SHIZUWO SANO

Date of correction: March 27, 2006 Reason for correction: - Correction: CITATION Details: 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.

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