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Composite Materials Research Progress

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Eletromechanical Field Concentrations and Polarization Switching... 261<br />

For 90 ◦ switching in the x2x3 plane,<br />

U = 1<br />

2 (σ22ε22 + σ33ε33 +2σ32ε32 + D2E2) (29)<br />

The critical value of internal energy density is assumed in the following form:<br />

where ɛ T 33<br />

Uc = 1<br />

2 ɛT 33(Ec) 2<br />

is the dielectric permittivity at constant stress.<br />

The constitutive equations (10) and (11) during polarization switching are<br />

The new piezoelectric constant e ′ ikl<br />

by<br />

(30)<br />

σij = cijklε l kl − e ′ kijEk (31)<br />

D l i = e ′ iklε l kl + ɛikEk (32)<br />

is related to the elastic and direct piezoelectric constants<br />

e ′ 111 = d′ 111 c11 + d ′ 122 c12 + d ′ 133 c13<br />

e ′ 122 = d ′ 111c12 + d ′ 122c11 + d ′ 133c13<br />

e ′ 133 = d′ 111 c13 + d ′ 122 c13 + d ′ 133 c33<br />

e ′ 123 =2d ′ 123c44<br />

e ′ 131 =2d′ 131 c44<br />

e ′ 112 =2d ′ 112c66<br />

e ′ 211 = d′ 211 c11 + d ′ 222 c12 + d ′ 233 c13<br />

e ′ 222 = d ′ 211c12 + d ′ 222c11 + d ′ 233c13<br />

e ′ 233 = d′ 211 c13 + d ′ 222 c13 + d ′ 233 c33<br />

e ′ 223 =2d ′ 223c44<br />

e ′ 231 =2d′ 231 c44<br />

e ′ 212 =2d′ 212 c66<br />

e ′ 311 = d ′ 311c11 + d ′ 322c12 + d ′ 333c13<br />

e ′ 322 = d′ 311 c12 + d ′ 322 c11 + d ′ 333 c13<br />

e ′ 333 = d ′ 311c13 + d ′ 322c13 + d ′ 333c33<br />

e ′ 323 =2d′ 323 c44<br />

e ′ 331 =2d ′ 331c44<br />

e ′ 312 =2d′ 312 c66<br />

The components of the piezoelectricity tensor d ′ ikl are<br />

d ′<br />

�<br />

ikl = d33ninknl + d31(niδil − ninknl)+ 1<br />

2 d15(δiknl<br />

�<br />

− 2ninknl + δilnk)<br />

where ni is the unit vector in the poling direction, δij is the Kroneker delta, and d33 = d333,<br />

d31 = d311, d15 =2d131 are the direct piezoelectric constants.<br />

(33)<br />

(34)

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