By Fluegge S. (ed.)
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Extra info for Encyclopedia of physics, vol. 8-1. Fluid mechanics I
Sample text
28. L. Ginzburg, Zh. Eksp. Teor. Fiz. 23, 236, 1952. 29. L. Ginzburg, Zh. Eksp. Teor. Fiz. 34, 113, 1958 [Sov. Phys. JETP 7, 78, 1958]. 30. L. Ginzburg, Zh. Eksp. Teor. Fiz. 42, 299, 1962 [Sov. Phys. JETP 15, 207, 1962]. 31. L. Ginzburg, Zh. Eksp. Teor. Fiz. 36, 1930, 1959 [Sov. Phys. JETP 9, 1372, 1959]. 32. L. Ginzburg, Zh. Eksp. Teor. Fiz. 31, 202, 1956 [Sov. Phys. JETP 4, 153, 1957]. 33. F. Zharkov, Zh. Eksp. Teor. Fiz. 34, 412, 1958; 37, 1784, 1959 [Sov. Phys. JETP 7, 278, 1958; 10, 1257, 1959].
I try, however, to avoid this term, not out of false modesty but rather because in such cases the use of one’s own name is not conventional in Russian. D. P. A. Sobyanin (see Sect. 4). The article [29] is included in this book. 15) n −i ∇Ψ − AΨ = 0, c where n is the normal to the boundary (for more details, see [29] and Sect. 3). 15) refers to the case of a boundary between a superconductor and a vacuum or a dielectric. As regards the equation for A, under the condition div A = 0, and after variation of the integral FsH dV over A, it becomes ΔA = − 4π js, c js = − ie e2 (Ψ∗ ∇Ψ − Ψ∇Ψ∗ ) − |Ψ|2 A.
P. A. Sobyanin (see Sect. 4). The article [29] is included in this book. 15) n −i ∇Ψ − AΨ = 0, c where n is the normal to the boundary (for more details, see [29] and Sect. 3). 15) refers to the case of a boundary between a superconductor and a vacuum or a dielectric. As regards the equation for A, under the condition div A = 0, and after variation of the integral FsH dV over A, it becomes ΔA = − 4π js, c js = − ie e2 (Ψ∗ ∇Ψ − Ψ∇Ψ∗ ) − |Ψ|2 A. , the total current is superconducting. 15)]. 16). 15)].
Encyclopedia of physics, vol. 8-1. Fluid mechanics I by Fluegge S. (ed.)
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