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Some consideration Some consideration on the on the magnetoacoustic magnetoacoustic effect effect Nicolae Cretu Nicolae Cretu Mihail Pop Mihail Pop Physics Department Physics Department Transilvania University Brasov-ROMANIA Transilvania University Brasov-ROMANIA [email protected] [email protected] ; [email protected] ; [email protected]
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Some consideration on the magnetoacoustic effect Nicolae Cretu Mihail Pop Physics Department Transilvania University Brasov-ROMANIA [email protected]@unitbv.ro;

Mar 31, 2015

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Page 1: Some consideration on the magnetoacoustic effect Nicolae Cretu Mihail Pop Physics Department Transilvania University Brasov-ROMANIA cretu.c@unitbv.rocretu.c@unitbv.ro;

Some consideration on Some consideration on the magnetoacoustic the magnetoacoustic

effecteffectNicolae CretuNicolae Cretu

Mihail PopMihail PopPhysics DepartmentPhysics Department

Transilvania University Brasov-ROMANIATransilvania University [email protected]@unitbv.ro; [email protected]; [email protected]

Page 2: Some consideration on the magnetoacoustic effect Nicolae Cretu Mihail Pop Physics Department Transilvania University Brasov-ROMANIA cretu.c@unitbv.rocretu.c@unitbv.ro;

MFM image of magnetic MFM image of magnetic domains for Nidomains for Ni

H

Page 3: Some consideration on the magnetoacoustic effect Nicolae Cretu Mihail Pop Physics Department Transilvania University Brasov-ROMANIA cretu.c@unitbv.rocretu.c@unitbv.ro;

The MAE and BN profiles (Y.H.Xu et al/J.Magn.Mag. The MAE and BN profiles (Y.H.Xu et al/J.Magn.Mag. Mat. 219(2000)166-172)Mat. 219(2000)166-172)

The profiles of MAE and BN The profiles of MAE and BN are in general quite are in general quite different since its different since its important contribution of important contribution of MAE is 90MAE is 90oo domain wall domain wall motion and of BN is 180motion and of BN is 180o o

domain wall motiondomain wall motion For NDE is important to For NDE is important to

explore the region with explore the region with H>Hmax, because in the H>Hmax, because in the presence of deffects we presence of deffects we need strong magnetic need strong magnetic forces which can produce forces which can produce the abrupt irreversible the abrupt irreversible magnetic domain wall magnetic domain wall motion.motion.

Page 4: Some consideration on the magnetoacoustic effect Nicolae Cretu Mihail Pop Physics Department Transilvania University Brasov-ROMANIA cretu.c@unitbv.rocretu.c@unitbv.ro;

Ideea of our workIdeea of our work Is possible to obtain information about the internal deffects if we are Is possible to obtain information about the internal deffects if we are

able to produce the motion of the walls of the magnetic domains able to produce the motion of the walls of the magnetic domains pinning around the deffects.pinning around the deffects.

The necessary energy to produce wall mouvement of such domains The necessary energy to produce wall mouvement of such domains can be obtained from the stationary wave generated in the sample.can be obtained from the stationary wave generated in the sample.

The time-varying magnetic field has the same frequency as the The time-varying magnetic field has the same frequency as the eigenfrequencies of the sample. In this case the oscillations of eigenfrequencies of the sample. In this case the oscillations of magnetic field are correlated with the standing elastic wave from magnetic field are correlated with the standing elastic wave from the sample, and the domain wall motion become a forced oscillation. the sample, and the domain wall motion become a forced oscillation.

The exploration of the line shape, will give information about the The exploration of the line shape, will give information about the magnetoelastic interactions of the magnetic walls magnetoelastic interactions of the magnetic walls

The paper contain investigations on MAE in the standing wave state The paper contain investigations on MAE in the standing wave state of ferromagnetic carbon steel rods. The influence of the artificial of ferromagnetic carbon steel rods. The influence of the artificial defects on the shape of the velocity line is investigated.defects on the shape of the velocity line is investigated.

Page 5: Some consideration on the magnetoacoustic effect Nicolae Cretu Mihail Pop Physics Department Transilvania University Brasov-ROMANIA cretu.c@unitbv.rocretu.c@unitbv.ro;

Experimental setupExperimental setup The magnetoelastic signal The magnetoelastic signal

was detected by a noncontact was detected by a noncontact method using a Bruel&Kjaer method using a Bruel&Kjaer Laser Velocity Transducer Laser Velocity Transducer Type 3544 (with excellent Type 3544 (with excellent results in velocity results in velocity measurements) attached to a measurements) attached to a linear preamplifier RFT Type linear preamplifier RFT Type 20027 connected to a USB 20027 connected to a USB acquisition board NI DAQ acquisition board NI DAQ Pad6015. The spectral Pad6015. The spectral decomposition of the signals, decomposition of the signals, the filtering and other data the filtering and other data processing were obtained processing were obtained using the Signal Analysis using the Signal Analysis Module in Lab View and TEST Module in Lab View and TEST POINT.POINT.

Page 6: Some consideration on the magnetoacoustic effect Nicolae Cretu Mihail Pop Physics Department Transilvania University Brasov-ROMANIA cretu.c@unitbv.rocretu.c@unitbv.ro;

. . The shape of the amplitude of the velocity of MAE effect The shape of the amplitude of the velocity of MAE effect obtained by axial magnetostriction measurements for the first obtained by axial magnetostriction measurements for the first

fours eigenfrequenciesfours eigenfrequencies

Page 7: Some consideration on the magnetoacoustic effect Nicolae Cretu Mihail Pop Physics Department Transilvania University Brasov-ROMANIA cretu.c@unitbv.rocretu.c@unitbv.ro;

The Lorentzian shape formulaThe Lorentzian shape formula

2 222 0

0 2 2 20

2

20 2

20

( ) ( )

2( )

2

A A

A

Page 8: Some consideration on the magnetoacoustic effect Nicolae Cretu Mihail Pop Physics Department Transilvania University Brasov-ROMANIA cretu.c@unitbv.rocretu.c@unitbv.ro;

Linewidth obtained by fitting with the LorentzianLinewidth obtained by fitting with the Lorentzian

Page 9: Some consideration on the magnetoacoustic effect Nicolae Cretu Mihail Pop Physics Department Transilvania University Brasov-ROMANIA cretu.c@unitbv.rocretu.c@unitbv.ro;

The change of the area of resonance plot of MAE for The change of the area of resonance plot of MAE for

the first four natural frequenciesthe first four natural frequencies

Page 10: Some consideration on the magnetoacoustic effect Nicolae Cretu Mihail Pop Physics Department Transilvania University Brasov-ROMANIA cretu.c@unitbv.rocretu.c@unitbv.ro;

The influence of deffects (artificial created deffects)The influence of deffects (artificial created deffects)

Page 11: Some consideration on the magnetoacoustic effect Nicolae Cretu Mihail Pop Physics Department Transilvania University Brasov-ROMANIA cretu.c@unitbv.rocretu.c@unitbv.ro;

CONCLUSIONSCONCLUSIONS

The sources of MAE are the domain The sources of MAE are the domain wall motion, the domain wall wall motion, the domain wall nucleation and annihilationnucleation and annihilation

The strength of MAE is proportional to The strength of MAE is proportional to the magnetostriction[]the magnetostriction[]

The main parameters which can give The main parameters which can give information for NDE are :frequency information for NDE are :frequency change; peak hight exploration; line change; peak hight exploration; line width change in the presence of width change in the presence of defects defects

Page 12: Some consideration on the magnetoacoustic effect Nicolae Cretu Mihail Pop Physics Department Transilvania University Brasov-ROMANIA cretu.c@unitbv.rocretu.c@unitbv.ro;

ReferencesReferences [1] Hubert A and Schäfer R. Magnetic Domains, Berlin: Springer;1998[1] Hubert A and Schäfer R. Magnetic Domains, Berlin: Springer;1998 [2] McVitie S, White GS,Scott J, Warin P and Chapman JN. Quantitative imaging of [2] McVitie S, White GS,Scott J, Warin P and Chapman JN. Quantitative imaging of

magnetic domain walls in thin films using Lorentz and magnetic force microscopies, J magnetic domain walls in thin films using Lorentz and magnetic force microscopies, J Appl Phys 2001;90:5220-5227Appl Phys 2001;90:5220-5227

[3] Schneider CM. Soft X-ray photoemission electron microscopy as an element-[3] Schneider CM. Soft X-ray photoemission electron microscopy as an element-specific probe of magnetic microstructures. J Magn Magn Mat 1997;175:160-176specific probe of magnetic microstructures. J Magn Magn Mat 1997;175:160-176

[4] Kleiber M, Bode M, Ravlik R,Wiesendanger R. Topology-Induced Spin Frustrations [4] Kleiber M, Bode M, Ravlik R,Wiesendanger R. Topology-Induced Spin Frustrations at the Cr(001) Surface Studied by Spin-Polarized Scanning Tunneling Spectroscopy. at the Cr(001) Surface Studied by Spin-Polarized Scanning Tunneling Spectroscopy. Phys Rev Lett 2000;85:4606-4614Phys Rev Lett 2000;85:4606-4614

[5] Weber NB and Oldag H, Gomonaj H and Hillebrecht FU. Magnetostrictive Domain [5] Weber NB and Oldag H, Gomonaj H and Hillebrecht FU. Magnetostrictive Domain Walls in Antiferromagnetic NiO. Phys Rev Lett 2003;91:237205-1Walls in Antiferromagnetic NiO. Phys Rev Lett 2003;91:237205-1

[6] Park DG, Ok CI, Jeong HT,.Kuk IH,.Hong JH. Nondestructive evaluation of [6] Park DG, Ok CI, Jeong HT,.Kuk IH,.Hong JH. Nondestructive evaluation of irradiation effects in RPV steel using Barkhausen noise and magnetoacoustic irradiation effects in RPV steel using Barkhausen noise and magnetoacoustic emission signals. J Magn Magn Mat 1999;196-197:382-384emission signals. J Magn Magn Mat 1999;196-197:382-384

[7] Sullivan DO, Cotterell M, Cassidy S, Tanner DA, Meszaros I. Magneto-acoustic [7] Sullivan DO, Cotterell M, Cassidy S, Tanner DA, Meszaros I. Magneto-acoustic emission for the characterisation of ferritic stainless steel microstructural state. J emission for the characterisation of ferritic stainless steel microstructural state. J Magn Magn Mat 2004;271:381-389Magn Magn Mat 2004;271:381-389

[8] Xu YH, La L, Du FM, Ma XY, Ng L. Magnetoacoustic emission and Barkhausen noise [8] Xu YH, La L, Du FM, Ma XY, Ng L. Magnetoacoustic emission and Barkhausen noise of cobalt nickel oriented silicon steel and permalloy. J Magn Magn Mat 2000;219:166-of cobalt nickel oriented silicon steel and permalloy. J Magn Magn Mat 2000;219:166-172172

[9] Hatafuku H. Estimation of effective magnetic field in a nickel rod by the [9] Hatafuku H. Estimation of effective magnetic field in a nickel rod by the magnetoacoustic effect. J Magn Magn Mat 2002;239:94-96magnetoacoustic effect. J Magn Magn Mat 2002;239:94-96