Abstract:Resonant bending-mode Tb1−xDyxFe2−y∕elastic-steel∕Pb(Zr,Ti)O3 magnetoelectric (ME) laminate composites have been investigated. An elastic-steel layer with a relatively high Qm significantly increases the resonant enhancement of the ME coefficient due to an increased effective Qm of the laminate. The three-phase ME laminates have a low first-order bending frequency of ∼5kHz, with a resonance-enhanced ME coefficient of ∼40V∕cmOe.
“…A steel phase with a high mechanical Q increased the ME coefficient, while lowering the resonant frequency without increasing the size of the magnetostrictive phase. 11 In this case, lower resonance frequencies offer the potential to enhance the ME coefficient for applications such as small magnetic field sensors.…”
A Pb(Zr,Ti)O3-bimorph/NdFeB laminate device has a giant magnetoelectric (ME) effect. Our results reveal a giant ME coefficient of 16V∕cmOe or 62nC∕cmOe at a low (subresonant) frequency of 10Hz, and one of 250V∕cmOe or 960nC∕cmOe at a first order resonant bending mode frequency of ∼60Hz. The findings show a simple means by which to achieve magnetoelectric effects, without the use of magnetostrictive material.
“…A steel phase with a high mechanical Q increased the ME coefficient, while lowering the resonant frequency without increasing the size of the magnetostrictive phase. 11 In this case, lower resonance frequencies offer the potential to enhance the ME coefficient for applications such as small magnetic field sensors.…”
A Pb(Zr,Ti)O3-bimorph/NdFeB laminate device has a giant magnetoelectric (ME) effect. Our results reveal a giant ME coefficient of 16V∕cmOe or 62nC∕cmOe at a low (subresonant) frequency of 10Hz, and one of 250V∕cmOe or 960nC∕cmOe at a first order resonant bending mode frequency of ∼60Hz. The findings show a simple means by which to achieve magnetoelectric effects, without the use of magnetostrictive material.
“…[3][4][5][6][7][8][9][10] The said laminated ME composites have ME voltage coefficients much larger than any other ME materials. It has accordingly been designated as a giant ME effect.…”
Laminated magnetoelectric (ME) composites consisting of magnetostrictive and piezoelectric layers are an important class of magnetic sensors. Here, we will present a means to design ME sensors with in-built capabilities to cancel environmental noise, based on designing the sensor signal and the noise in different fundamental modes. We then show that some composite designs offer unique capabilities to reject acoustic or thermal noise sources.
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