1957
DOI: 10.1007/bf00621091
|View full text |Cite
|
Sign up to set email alerts
|

The analogue of Kelvin's theorem in hydromagnet.es

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1

Citation Types

0
1
0

Year Published

1963
1963
1963
1963

Publication Types

Select...
1

Relationship

0
1

Authors

Journals

citations
Cited by 1 publication
(1 citation statement)
references
References 1 publication
0
1
0
Order By: Relevance
“…As a special case, one may choose r to be a closed line of B, say rB. In this case the second term in (27) vanishes and one is left with (De 1957) T o illalce the hydrodynamical equation (23) suitable, as a second step one introduces the generalized hj-clrodynamical or Clebsch potentials x, q, l defined by (Ito 1953;Lamb 1953) These are particularly convenient, because one can always visualize the lines of the generalized vorticity = VqXVt as the lines of intersection of the surfaces q = coilstant and 6 = constant. The generalized Clebsch potentials reduce to the ordinary Clebsch potentials when the magnetic illduction B…”
Section: ~-;~V [~+ + + V ( V +~-~B X P ) ]mentioning
confidence: 99%
“…As a special case, one may choose r to be a closed line of B, say rB. In this case the second term in (27) vanishes and one is left with (De 1957) T o illalce the hydrodynamical equation (23) suitable, as a second step one introduces the generalized hj-clrodynamical or Clebsch potentials x, q, l defined by (Ito 1953;Lamb 1953) These are particularly convenient, because one can always visualize the lines of the generalized vorticity = VqXVt as the lines of intersection of the surfaces q = coilstant and 6 = constant. The generalized Clebsch potentials reduce to the ordinary Clebsch potentials when the magnetic illduction B…”
Section: ~-;~V [~+ + + V ( V +~-~B X P ) ]mentioning
confidence: 99%