Abstract:The strength of magnetoelectric (ME) coupling at 10Hz–3MHz has been measured in trilayers of Fe, Co, or Ni and lead zirconate titanate (PZT). The strongest ME coupling is measured for trilayers with Ni and the weakest in Co. Data on ME voltage coefficient αE versus bias magnetic field H for Fe–PZT–Fe show unique features including zero crossing and sign reversal. Measurements of frequency dependence of αE reveal a giant ME coupling due to the electromechanical resonance at 200–300kHz for radial modes and at ∼2… Show more
“…It has been reported that ME output of Ni/PZT/Ni bulk ME sensor with 2-2 structure can have a value as high as 40-400 mV/cmÁOe. [22][23][24] The ME coefficient of our BiFeO 3 /Ni is much smaller than this value. It will be important to understand the limiting factors in order to maximize the ME output.…”
“…It has been reported that ME output of Ni/PZT/Ni bulk ME sensor with 2-2 structure can have a value as high as 40-400 mV/cmÁOe. [22][23][24] The ME coefficient of our BiFeO 3 /Ni is much smaller than this value. It will be important to understand the limiting factors in order to maximize the ME output.…”
“…[11][12][13][14][15][16][17]19,20 A resonance enhancement ͑ϳ100 times͒ of the ME voltage coefficient ͑V ME ͒ has been reported at the first longitudinal mode ͑f 0 ͒. [21][22][23] Such enhancement is potentially very important; however, it is limited to a relatively high frequency: for example, consider a 15 mm long Terfenol-D/PZT LT mode laminate, V ME Ϸ 18.5 V / cm Oe at f 0 Ϸ 80 kHz. 11 For ME laminates having a Terfenol-D layer͑s͒, a high resonant frequency of ജ10 kHz will result in significant eddy current losses due to the conductive nature of the Terfenol-D layer, which in turn will dramatically lower the efficiency of energy conversion.…”
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.
“…[11][12][13][14][15][16][17][18][19] In addition, most layered ME composite theoretical models stressed on the influence of thickness ratio of ferromagnetic and ferroelectric phases, but paid no attention on the influence of in-plane sizes on ME coefficient. [20][21][22][23] In fact, the magnetostrictivity is largely dependent on in-plane sizes due to shape demagnetization effect, so ME coefficients α E,31 and α E,32 would be different.…”
Magnetoelectric (ME) voltage coefficient was always considered independent on in-plane shape of plate layered magnetostrictive-piezoelectric composites due to the oversimplification in ME theoretical models. In this article, we present that in fact the ME voltage coefficient is largely dependent on the in-plane shape owing to shape demagnetization effect on magnetostrictivity. Theoretical analysis and experimental results both indicate that ME voltage coefficient changes notably with the variation of in-plane sizes (length and width) of layered ME properties. ME coefficient increases with the rise of in-plane sizes, and different aspect ratio will also result in different ME coefficient. Proper design of in-plane shape will greatly promote the development of ME devices.
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