匡威
纤维素
衍射
X射线晶体学
压电
小角X射线散射
材料科学
化学
结晶学
高分子化学
光学
复合材料
散射
有机化学
物理
数学
几何学
作者
Wolfgang Gindl‐Altmutter,Gerhard Emsenhuber,Johannes Plackner,Johannes Konnerth,Jozef Kečkéš
出处
期刊:Biomacromolecules
[American Chemical Society]
日期:2010-03-30
卷期号:11 (5): 1281-1285
被引量:25
摘要
The converse piezoelectric effect in cellulose I was studied by exposing thin pine wood slices to an electric field. Macroscopically, a strong extension of wood was observed in its transverse anatomical direction (grain angle 90 degrees), perpendicular to the direction of the electric field. The same effect, albeit to a lesser extent, was observed for specimens with a 45 degree grain angle, whereas no measurable dimensional change was observed for specimens with grain oriented parallel to the testing direction (0 degree grain angle). The measured extension in the transverse direction was proportional to the intensity of the applied electric field and amounted to 0.0278% on average at a field intensity of 1 MV m(-1), which results in a piezoelectric charge constant of 278 pm V(-1). At the nanoscale, changes in the cellulose crystallites due to the applied electric field were studied by means of wide-angle X-ray diffraction using the same specimens as in macroscopic experiments. Significant radial shifts of the scattering intensity peak attributed to the cellulose 200 crystallographic plane toward smaller scattering angles were observed, while the electric field was applied. These peak shifts were attributed to an increase in the spacing of the 200 crystallographic planes of cellulose I. At an electric field intensity of 1 MV m(-1), a crystallite strain epsilon(perpendicular 200) normal to the 200 reflection plane of 0.2% was estimated from Bragg's law.
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