Apparatus for Quasihydrostatic Measurement of Piezoelectric dhCoefficient

K. Schoch, A. Dereggi, S. Roth
{"title":"Apparatus for Quasihydrostatic Measurement of Piezoelectric dhCoefficient","authors":"K. Schoch, A. Dereggi, S. Roth","doi":"10.1109/ISAF.1986.201241","DOIUrl":null,"url":null,"abstract":"Measurement of piezoelectric response of materials (dh) by a pressure pulse technique is described in this article. The sample is placed in a fluid-filled chamber fitted with a piston at one end. Impact on the piston creates a pressure pulse in the chamber, the duration and shape of which can be controlled. This method is effective with composite samples as well as polymer film samples. Introduction This paper describes a convenient and reliable method for measuring the hydrostatic piezoelectric coefficient of materials, dh. In this technique the sample is placed in a fluidfilled chamber and a hydrostatic pulse is applied by impacting a piston in the chamber. Pulse height, duration, and shape can be controlled readily, and in principle, information about frequency response can also be obtained. Automated data acquisition makes possible accurate calculation of response over the entire pressure pulse. Results on samples of various PbTiOj-based composites and poly(viny1idene fluoride)(PVF2) will be discussed. Other transient and ramp methods for measuring dh are described in the literature.[ll Experimental A . Pressure Generation The apparatus required for measurement is shown in Figure 1, and consists of a fluid-filled cell (Fiugre 2) containing the sample and a calibrated pressure transducer. The apparatus is an improved version of apparatus described previously, with digital processing added.[2,3] The cell was made by cutting a cylindrical chamber 3 inches long and 2 inches in diameter into a 4inch diameter 303 stainless steel rod. A calibrated pressure transducer was placed with the sensing diaphragm at the bottom of the chamber, and provision was made to connect a sample electrically to the outside of the chamber via a BNC connector. A piston of armoloy-plated brass was made to fit in the chamber for applying the pressure pulse. This sample cell containing the sample and a suitable fluid is placed in a drop tester, used to generate pulses reproducibly. Fig. 1-System block diagram Figure 2. Pressure Pulse Measurement Cell Pulses can be shaped by judicious selection of a material to be placed on top of the piston. The compliance of this coupling slug will determine the pulse length and shape. For example, a relatively soft material like a rubber vacuum hose produces a relatively long pulse of 10-15 msec duration. Harder materials produce shorter pulses of 1-5 msec duration. Some unusual pulse shapes can also be generated, depending on the resilience of the intermediate material. Pulse shapes for some typical materials are shown in Figure 3.","PeriodicalId":302681,"journal":{"name":"Sixth IEEE International Symposium on Applications of Ferroelectrics","volume":"15 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1986-06-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Sixth IEEE International Symposium on Applications of Ferroelectrics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/ISAF.1986.201241","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0

Abstract

Measurement of piezoelectric response of materials (dh) by a pressure pulse technique is described in this article. The sample is placed in a fluid-filled chamber fitted with a piston at one end. Impact on the piston creates a pressure pulse in the chamber, the duration and shape of which can be controlled. This method is effective with composite samples as well as polymer film samples. Introduction This paper describes a convenient and reliable method for measuring the hydrostatic piezoelectric coefficient of materials, dh. In this technique the sample is placed in a fluidfilled chamber and a hydrostatic pulse is applied by impacting a piston in the chamber. Pulse height, duration, and shape can be controlled readily, and in principle, information about frequency response can also be obtained. Automated data acquisition makes possible accurate calculation of response over the entire pressure pulse. Results on samples of various PbTiOj-based composites and poly(viny1idene fluoride)(PVF2) will be discussed. Other transient and ramp methods for measuring dh are described in the literature.[ll Experimental A . Pressure Generation The apparatus required for measurement is shown in Figure 1, and consists of a fluid-filled cell (Fiugre 2) containing the sample and a calibrated pressure transducer. The apparatus is an improved version of apparatus described previously, with digital processing added.[2,3] The cell was made by cutting a cylindrical chamber 3 inches long and 2 inches in diameter into a 4inch diameter 303 stainless steel rod. A calibrated pressure transducer was placed with the sensing diaphragm at the bottom of the chamber, and provision was made to connect a sample electrically to the outside of the chamber via a BNC connector. A piston of armoloy-plated brass was made to fit in the chamber for applying the pressure pulse. This sample cell containing the sample and a suitable fluid is placed in a drop tester, used to generate pulses reproducibly. Fig. 1-System block diagram Figure 2. Pressure Pulse Measurement Cell Pulses can be shaped by judicious selection of a material to be placed on top of the piston. The compliance of this coupling slug will determine the pulse length and shape. For example, a relatively soft material like a rubber vacuum hose produces a relatively long pulse of 10-15 msec duration. Harder materials produce shorter pulses of 1-5 msec duration. Some unusual pulse shapes can also be generated, depending on the resilience of the intermediate material. Pulse shapes for some typical materials are shown in Figure 3.
压电系数的准静压测量装置
本文介绍了用压力脉冲技术测量材料压电响应(dh)的方法。样品被放置在一端装有活塞的充满流体的腔室中。对活塞的冲击在腔室中产生压力脉冲,其持续时间和形状是可以控制的。该方法对复合材料样品和聚合物薄膜样品均有效。介绍了一种方便可靠的测量材料静压系数dh的方法。在这种技术中,样品被放置在充满流体的腔室中,通过冲击腔室中的活塞施加静流体脉冲。脉冲的高度、持续时间和形状可以很容易地控制,原则上,也可以获得有关频率响应的信息。自动数据采集使得精确计算整个压力脉冲的响应成为可能。讨论了各种pbtioj基复合材料和聚氟乙烯(PVF2)样品的结果。文献中描述了测量dh的其他瞬态和斜坡方法。[2]实验的;测量所需的设备如图1所示,由一个充满液体的容器(图2)和一个校准的压力传感器组成。该装置是先前描述的装置的改进版本,增加了数字处理。[2,3]细胞是通过将一个3英寸长、2英寸直径的圆柱形腔切割成直径4英寸的303不锈钢棒制成的。经过校准的压力传感器与感应膜片一起放置在腔室底部,并通过BNC连接器将样品电连接到腔室外部。一个镀黄铜的活塞被制成适合于施加压力脉冲的腔室。将含有样品和适当液体的样品池放置在跌落测试仪中,用于可重复地产生脉冲。图1系统框图压力脉冲测量单元可以通过明智地选择放置在活塞顶部的材料来形成脉冲。这种耦合段塞的顺应性将决定脉冲的长度和形状。例如,一种相对柔软的材料,如橡胶真空软管,会产生持续10-15毫秒的相对较长的脉冲。较硬的材料产生较短的脉冲,持续时间为1-5毫秒。根据中间材料的弹性,也可以产生一些不寻常的脉冲形状。一些典型材料的脉冲形状如图3所示。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
求助全文
约1分钟内获得全文 求助全文
来源期刊
自引率
0.00%
发文量
0
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
确定
请完成安全验证×
copy
已复制链接
快去分享给好友吧!
我知道了
右上角分享
点击右上角分享
0
联系我们:info@booksci.cn Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。 Copyright © 2023 布克学术 All rights reserved.
京ICP备2023020795号-1
ghs 京公网安备 11010802042870号
Book学术文献互助
Book学术文献互助群
群 号:604180095
Book学术官方微信