The effect of magnetic fields applied on magnetic metals electrodeposition was examined. Nickel deposits obtained from a Watt solution with coumarin, at cathodic potentials of Ϫ1000, Ϫ1200, and Ϫ1300 mV/SCE, without and with, both, perpendicular and parallel oriented to the electrode surface low applied magnetic fields ͑up to 500 Oe͒ were examined by scanning electron microscopy ͑SEM͒ technique. At a potential of Ϫ1300 mV/SCE, a dramatic difference was observed between nickel morphologies obtained with a perpendicular oriented magnetic field ͑zero MHD effect͒ and those obtained in the absence of one. The nickel deposit obtained with perpendicular oriented magnetic fields was a very developed 3D arboreous-bead-dendritic structure. On the other hand, the nickel deposit obtained without the presence of magnetic field was very rough, with a clearly visible clustered structure. The obtained nickel morphologies are then compared with copper morphologies. Based on the fact that copper deposits obtained with and without a perpendicular oriented magnetic field were dendritic structures, the observed difference between nickel deposits with and those without a perpendicular oriented field, is essentially ascribed to the magnetoresistance effect on the magnetic deposits, which are nonexistent in nonmagnetic materials. We also have done experiments with iron deposits.The effect of an applied magnetic field on metal electrodeposition has been a subject of many investigations. 1-8 It was shown that an imposed magnetic field realizes various effects on electrolytic processes and in particular on the morphology and structure of metals or alloys prepared by electrodeposition. Morphologies of electrochemically obtained metal deposits are often strongly changed if metal electrodeposition was performed in the presence of a magnetic field. For example, a dense and compact deposit can be obtained in the presence of a magnetic field instead of dendritic one obtained without a magnetic field. 8 Changes in morphology of metal deposits were ascribed to the Lorentz force. 5 This force, F, exerted by an electromagnetic field B on the ions of charge q moving at the velocity v within an electric field E can be presented by Eq. 1 1,5During electrolysis, this force acts on the migration of ions and induces convective flow of electrolyte close to the electrode surface. This effect on the electrodeposition process is known as the magnetohydrodynamic ͑MHD͒ effect. The magnetohydrodynamic flow in electrochemical systems is conveniently described by the force per unit volume acting on the solution, F MHD ͑in N/m 3 ͒, and which is given by Eq. 2, 9 where J ͑in C/m 2 ͒ is the local flux of ionsThe largest effect of this force, and consequently, the largest effect on convective mass transport of the electrolyte, can be realized when magnetic field B is applied parallel to the electrode surface ͑i.e., an external magnetic field is oriented perpendicular to the direction of the ion flux͒. 9 This expectation is generally observed in investigations that hav...