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Direct Energy, 2018a

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3 PYROELECTRICS AND ELECTRO-OPTICS 65<br />

3.4. The rst gure below shows the displacement ux density<br />

a function of the strength of an appliedelectric eldintensity<br />

in a non-electro-optic material.<br />

displacement ux density<br />

∣ −→ ∣<br />

D<br />

∣ −→ ∣<br />

E<br />

∣ −→ D<br />

as<br />

∣ −→ E ∣<br />

The secondgure below shows the<br />

∣ as a function of the strength of an<br />

appliedelectric eldintensity ∣ in a ferroelectric electro-optic material.<br />

The solidline corresponds to an unpoledmaterial. The dotted<br />

line corresponds to the material after it has been poled in the â z direction,<br />

andthe dashedline corresponds to the material after it has<br />

been poledin the −â z direction.<br />

(a) For the non-electro-optic material, ndthe relative permittivity,<br />

ɛ r . Also ndthe magnitude of the material polarization, −→ P.<br />

(b) Assume the ferroelectric electro-optic material is poledby a<br />

strong external electric eld, andthen the eldis removed. Find<br />

∣ after the exter-<br />

the magnitude of the material polarization<br />

nal eldis removed.<br />

∣ −→ ∣<br />

P<br />

(c) Assume the ferroelectric material is poledin the −â z direction by<br />

a strong external eld, and then the eld is removed. A dierent<br />

external electric eldgiven by −→ E = 100â z<br />

V<br />

m<br />

is applied. Find<br />

the approximate relative permittivity of the material.<br />

−→ DinC/m<br />

2<br />

400 · ɛ 0<br />

200 · ɛ 0<br />

100<br />

−→ EinV/m

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