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TWO REGIMES OF HYDRODYNAMIC FLOW IN CONVECTIVE CONDUCTIVITY. / Stishkov, Yu K.; Ostapenko, A. A.

In: Magnetohydrodynamics New York, N.Y., Vol. 15, No. 4, 01.01.1979, p. 396-401.

Research output: Contribution to journalArticlepeer-review

Harvard

Stishkov, YK & Ostapenko, AA 1979, 'TWO REGIMES OF HYDRODYNAMIC FLOW IN CONVECTIVE CONDUCTIVITY.', Magnetohydrodynamics New York, N.Y., vol. 15, no. 4, pp. 396-401.

APA

Stishkov, Y. K., & Ostapenko, A. A. (1979). TWO REGIMES OF HYDRODYNAMIC FLOW IN CONVECTIVE CONDUCTIVITY. Magnetohydrodynamics New York, N.Y., 15(4), 396-401.

Vancouver

Stishkov YK, Ostapenko AA. TWO REGIMES OF HYDRODYNAMIC FLOW IN CONVECTIVE CONDUCTIVITY. Magnetohydrodynamics New York, N.Y. 1979 Jan 1;15(4):396-401.

Author

Stishkov, Yu K. ; Ostapenko, A. A. / TWO REGIMES OF HYDRODYNAMIC FLOW IN CONVECTIVE CONDUCTIVITY. In: Magnetohydrodynamics New York, N.Y. 1979 ; Vol. 15, No. 4. pp. 396-401.

BibTeX

@article{2ba6897e69104e748138edea8465628c,
title = "TWO REGIMES OF HYDRODYNAMIC FLOW IN CONVECTIVE CONDUCTIVITY.",
abstract = "Two regimes of electrohydrodynamic flow are investigated for two groups of electrodes of various sizes in two liquids which differ greatly in viscosity. The mechanisms of these regimes are not connected with the change of the hydrodynamics of the flow (e. g. , with the transition from the laminar to turbulent region), but are explained by the change of the current-carrying mechanism from drift to convective. The nature of the electrohydrodynamic flow in the strongly and weakly nonuniform field is the same, and is clearly determined by the electrochemical processes near the electrodes.",
author = "Stishkov, {Yu K.} and Ostapenko, {A. A.}",
year = "1979",
month = jan,
day = "1",
language = "English",
volume = "15",
pages = "396--401",
journal = "Magnetohydrodynamics",
issn = "0024-998X",
publisher = "Издательство Латвийского университета",
number = "4",

}

RIS

TY - JOUR

T1 - TWO REGIMES OF HYDRODYNAMIC FLOW IN CONVECTIVE CONDUCTIVITY.

AU - Stishkov, Yu K.

AU - Ostapenko, A. A.

PY - 1979/1/1

Y1 - 1979/1/1

N2 - Two regimes of electrohydrodynamic flow are investigated for two groups of electrodes of various sizes in two liquids which differ greatly in viscosity. The mechanisms of these regimes are not connected with the change of the hydrodynamics of the flow (e. g. , with the transition from the laminar to turbulent region), but are explained by the change of the current-carrying mechanism from drift to convective. The nature of the electrohydrodynamic flow in the strongly and weakly nonuniform field is the same, and is clearly determined by the electrochemical processes near the electrodes.

AB - Two regimes of electrohydrodynamic flow are investigated for two groups of electrodes of various sizes in two liquids which differ greatly in viscosity. The mechanisms of these regimes are not connected with the change of the hydrodynamics of the flow (e. g. , with the transition from the laminar to turbulent region), but are explained by the change of the current-carrying mechanism from drift to convective. The nature of the electrohydrodynamic flow in the strongly and weakly nonuniform field is the same, and is clearly determined by the electrochemical processes near the electrodes.

UR - http://www.scopus.com/inward/record.url?scp=0018524156&partnerID=8YFLogxK

M3 - Article

AN - SCOPUS:0018524156

VL - 15

SP - 396

EP - 401

JO - Magnetohydrodynamics

JF - Magnetohydrodynamics

SN - 0024-998X

IS - 4

ER -

ID: 40623309