{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"为探讨硅橡胶/镍粉复合材料的<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>性能,研究了不同掺量镍粉填充硅橡胶复合材料试样的电阻随拉应力、压应力的变化规律,并结合扫描电镜观察进行了机理分析.研究结果表明,所制备的硅橡胶/镍粉复合材料试样的电阻随拉、压应力的增加而减小,镍粉掺量越大,电阻对应力变化越敏感;在2 MPa的拉、压应力作用下,硅橡胶/绦粉复合材料试样的电阻变化最大分别可达11个和12个数量级.硅橡胶/镍粉复合材料优异的<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>效应是由量子隧道效应导致的.","authors":[{"authorName":"韩宝忠","id":"e1ff88f0-fc13-45c0-9e2d-b31851026b82","originalAuthorName":"韩宝忠"},{"authorName":"周道成","id":"383eb8cd-1e2c-428f-ac0e-6e7fd8737cee","originalAuthorName":"周道成"},{"authorName":"韩宝国","id":"bc50b9ee-5c40-4833-8c6a-4df416cfb277","originalAuthorName":"韩宝国"},{"authorName":"张扬","id":"28a8de0d-eda1-4eec-956f-2676849e7eb9","originalAuthorName":"张扬"},{"authorName":"盛伯瑶","id":"2631c232-4f86-46c0-8b90-6af4cefdb7cb","originalAuthorName":"盛伯瑶"}],"doi":"","fpage":"97","id":"96ef4f57-ebdf-442f-b4a1-7eaf5a63dff4","issue":"11","journal":{"abbrevTitle":"GFZCLKXYGC","coverImgSrc":"journal/img/cover/GFZCLKXYGC.jpg","id":"31","issnPpub":"1000-7555","publisherId":"GFZCLKXYGC","title":"高分子材料科学与工程"},"keywords":[{"id":"cc24706d-036a-4aca-ae44-4d3396b49dd8","keyword":"镍粉","originalKeyword":"镍粉"},{"id":"689cdcae-3a1f-4439-843b-e57360884344","keyword":"硅橡胶","originalKeyword":"硅橡胶"},{"id":"45825192-03cd-4a76-b251-457bf0026328","keyword":"<span style=\"color:red\">力</span><span style=\"color:red\">敏</span><span style=\"color:red\">性</span>","originalKeyword":"力敏性"},{"id":"7b3bb0aa-5d5f-4860-b4c5-8126bf4087a1","keyword":"应力","originalKeyword":"应力"},{"id":"2f15a260-e125-4330-bf98-8330641120a8","keyword":"电阻","originalKeyword":"电阻"}],"language":"zh","publisherId":"gfzclkxygc201011026","title":"硅橡胶/镍粉复合材料的<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>性能","volume":"26","year":"2010"},{"abstractinfo":"从碳纤维增强水泥基(CFRC)材料导电机理出发,建立了一个描述CFRC材料导电<span style=\"color:red\">性</span>的数学模型,并推破导了这种材料电导率与材料内部微观结构参数、载流子运动参数的关系.以该模型分析CFRC材料的<span style=\"color:red\">力</span><span style=\"color:red\">敏</span><span style=\"color:red\">性</span>,其理论规律与实验结果基本一致,从而验证了CRFC导电模型的合理性.","authors":[{"authorName":"姚武","id":"8a825e36-1fd6-448b-906e-03492d9e42d2","originalAuthorName":"姚武"},{"authorName":"王瑞卿","id":"a3600bea-d94d-465a-874d-6e576f2e8d0d","originalAuthorName":"王瑞卿"}],"doi":"10.3321/j.issn:1000-3851.2006.05.023","fpage":"121","id":"3fca105a-ff9f-40b0-990b-65891bc9703b","issue":"5","journal":{"abbrevTitle":"FHCLXB","coverImgSrc":"journal/img/cover/FHCLXB.jpg","id":"26","issnPpub":"1000-3851","publisherId":"FHCLXB","title":"复合材料学报"},"keywords":[{"id":"d80efadf-1657-4707-b8a5-3307523052f9","keyword":"隧道效应","originalKeyword":"隧道效应"},{"id":"55f3f3c7-0f71-47b9-9e21-e949722c11be","keyword":"数学模型","originalKeyword":"数学模型"},{"id":"db1bb405-547f-4128-8008-a54ab704ffaa","keyword":"电导率","originalKeyword":"电导率"},{"id":"25675239-1805-4d94-8ca8-9f506b342c43","keyword":"<span style=\"color:red\">力</span><span style=\"color:red\">敏</span><span style=\"color:red\">性</span>","originalKeyword":"力敏性"}],"language":"zh","publisherId":"fhclxb200605023","title":"基于隧道效应的CFRC材料的导电模型","volume":"23","year":"2006"},{"abstractinfo":"以300目非晶 Fe73 Si18 B9粉体为敏感组元,硅橡胶为基体,制得了粉体含量为25%,75%及83.3%(质量分数),厚度200μm 复合薄膜；采用LYYL-500N高档型微机控制压力实验机对薄膜试样进行连续加载卸载实验,同时,使用TH2816LCR 数字电桥采集薄膜在测试频率为1 kHz,压应力加载速度分别为0.05,0.1和0.5 mm/min条件下的阻抗值Z,研究了不同粉体含量的复合薄膜的<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>特性,比较了纳米晶 FeCuNbSiB 粉体/硅橡胶复合薄膜和非晶FeSiB粉体/硅橡胶复合薄膜<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>特性。研究表明,复合薄膜在连续加载/卸载速度≤0.1 mm/min,测试频率1 kHz、压应力0.03~1.0 MPa时,具有良好的<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>稳定性和灵敏<span style=\"color:red\">性</span>。薄膜对于小于0.2 MP a 应力更加灵敏,在此应力范围内,薄膜中粉体含量增加,薄膜的<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>特性变化趋势相同,但薄膜的<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>敏感度增大。当薄膜中粉体含量为83.3%(质量分数),压应力由0.03增大到0.2 MPa 时,在加载过程中薄膜的 SI%由36.51%增大到82.48%,k 值由42.91减小到1.889；当应力为0.2~0.7 MPa 时,薄膜的k 值在1.889~0.6之间,应力继续增大至1 MPa 时,k 值逐渐接近0。","authors":[{"authorName":"乔宝英","id":"a1bb1f35-14ac-4ea1-8535-e02970b813d6","originalAuthorName":"乔宝英"},{"authorName":"朱正吼","id":"3a8cb430-d5a8-4fe3-841d-d8607a6b984a","originalAuthorName":"朱正吼"},{"authorName":"杜康","id":"6e0aa263-2c4e-4526-ba46-bed7c5f085af","originalAuthorName":"杜康"},{"authorName":"周佳","id":"816e96b7-03ea-46b4-9224-3c20b8569468","originalAuthorName":"周佳"},{"authorName":"黄渝鸿","id":"76602cd6-0542-4276-a8d1-210ed5c8974c","originalAuthorName":"黄渝鸿"},{"authorName":"付远","id":"21bc381b-d78c-4bdd-bf47-dad512b749fe","originalAuthorName":"付远"}],"doi":"10.3969/j.issn.1001-9731.2014.08.012","fpage":"8056","id":"028232f8-72f7-483c-9adf-1c2d122306d8","issue":"8","journal":{"abbrevTitle":"GNCL","coverImgSrc":"journal/img/cover/GNCL.jpg","id":"33","issnPpub":"1001-9731","publisherId":"GNCL","title":"功能材料"},"keywords":[{"id":"c79cb66c-3954-4418-b8f6-3fce06a8c853","keyword":"<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>薄膜","originalKeyword":"力敏薄膜"},{"id":"8b629537-2c9f-4738-b565-5030de629cc7","keyword":"阻抗","originalKeyword":"阻抗"},{"id":"d20493dc-9a54-4fa1-bb76-01fb0a2c34be","keyword":"非晶","originalKeyword":"非晶"}],"language":"zh","publisherId":"gncl201408012","title":"FeSiB粉体/硅橡胶复合薄膜<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>特性研究","volume":"","year":"2014"},{"abstractinfo":"以 Fe73.5 Cu1 Nb3 Si13.5 B9粉体为复合相,硅橡胶为基体,制得粉体含量为83%(质量分数)、厚度200μm的复合薄膜；采用 TH2816LCR 数字电桥测试频率1kHz下薄膜的阻抗Z 随压应力σ的变化情况,用LYYL-500N高档型微机控制压力试验机对薄膜体系进行程序控制加载；薄膜采用电容方式连接。研究了复合薄膜在压应力连续加载/卸载和压应力保持加载/卸载状况下的<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>特性。研究表明,复合薄膜在连续加载/卸载速度≤0.5mm/min 和保压加载/卸载条件下,当测试频率1kHz、压应力0.2~1.0MPa 时,具有良好的<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>稳定性和灵敏<span style=\"color:red\">性</span>。随着应力σ增大,阻抗Z 呈非线性下降,SI%值为6%~23%,灵敏精度k值为2~0.2,测试标准偏差稳定在0.02~0.05,薄膜对于<0.3MPa应力更加灵敏。增加测试频率可以提高薄膜体系的<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>灵敏度。在压应力0.2~1.0MPa范围内,薄膜弹性后效现象显著,导致薄膜加载Z-σ曲线与卸载曲线不重合。","authors":[{"authorName":"周佳","id":"572b905b-4297-4acf-9c2e-369a428d31fc","originalAuthorName":"周佳"},{"authorName":"朱正吼","id":"8374f602-8e14-4052-89ff-690a7f7ae43b","originalAuthorName":"朱正吼"},{"authorName":"杜康","id":"179bfb8a-1ae1-461e-9d79-448899abbc99","originalAuthorName":"杜康"},{"authorName":"付远","id":"88850d68-eaf3-47d8-86f0-db443c345131","originalAuthorName":"付远"},{"authorName":"黄渝鸿","id":"cc5bb46e-2533-4a6b-84c8-34835c286e79","originalAuthorName":"黄渝鸿"},{"authorName":"乔宝英","id":"9a499cf3-6d88-4ef0-8112-d68ade11946b","originalAuthorName":"乔宝英"}],"doi":"10.3969/j.issn.1001-9731.2013.21.014","fpage":"3117","id":"51274d9d-2077-46dc-aeb4-6f018cb316f0","issue":"21","journal":{"abbrevTitle":"GNCL","coverImgSrc":"journal/img/cover/GNCL.jpg","id":"33","issnPpub":"1001-9731","publisherId":"GNCL","title":"功能材料"},"keywords":[{"id":"7bab567d-8348-44f3-9039-06acca988b64","keyword":"<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>薄膜","originalKeyword":"力敏薄膜"},{"id":"8cf31c68-67b9-46d1-a3d9-8d3c1977cefc","keyword":"阻抗","originalKeyword":"阻抗"},{"id":"11805b59-1f42-4873-945f-4b4150873a22","keyword":"弹性后效","originalKeyword":"弹性后效"}],"language":"zh","publisherId":"gncl201321014","title":"83wt%FeCuNbSiB粉体/硅橡胶复合薄膜<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>特性","volume":"","year":"2013"},{"abstractinfo":"以粒径为45μm 的 Fe73.5 Cu1 Nb3 Si13.5 B9非晶粉体为复合相,丁基橡胶为基体相,利用模压成型法制备了粉体含量为85%、厚度为150和200μm 的复合薄膜。采用LYYL-500N高档型微机控制压力试验机对薄膜试样进行连续加载/卸载实验(速度分别为0.1,0.5和1.0 mm/min),用 TH2816LCR 数字电桥测试频率1和50 kHz下薄膜的阻抗Z 值。研究了加载/卸载速度、测试频率、薄膜厚度和环境温度对 Fe-CuNbSiB粉体/丁基橡胶<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>特性的影响。研究表明,复合薄膜在v=0.1 mm/min 时,其重复性最好,在加载过程中,应力灵敏度|k|值随着应力的增大呈现先增大后减小的变化趋势,卸载过程中,|k|值随着应力的逐渐减小而增大。在1 kHz测试频率下复合薄膜的<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>灵敏度高于50 kHz。相同测试条件下,厚度为200μm的复合薄膜的<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>灵敏<span style=\"color:red\">性</span>略优于150μm 的。在39.5~80℃温度范围内,随着温度的升高复合薄膜的灵敏度越高。","authors":[{"authorName":"周佳","id":"3b6925cc-0dad-4406-a1b0-31512ceeee7d","originalAuthorName":"周佳"},{"authorName":"朱正吼","id":"373daa0a-d9c5-41db-a24b-8e6f0b173c80","originalAuthorName":"朱正吼"},{"authorName":"付远","id":"96e260b6-14ba-4706-a3c6-144cbf87dd65","originalAuthorName":"付远"},{"authorName":"乔宝英","id":"4898f5fc-6055-474b-9581-ba3760c7f304","originalAuthorName":"乔宝英"},{"authorName":"杜康","id":"be093a9e-3323-4031-97e4-5cf33a28f98d","originalAuthorName":"杜康"}],"doi":"10.3969/j.issn.1001-9731.2014.10.014","fpage":"10067","id":"e04ff339-8d62-48aa-b75a-38a6a08f1829","issue":"10","journal":{"abbrevTitle":"GNCL","coverImgSrc":"journal/img/cover/GNCL.jpg","id":"33","issnPpub":"1001-9731","publisherId":"GNCL","title":"功能材料"},"keywords":[{"id":"e8c30ff0-f310-4233-98b3-a4eed8b36655","keyword":"FeCuNbSiB 粉体","originalKeyword":"FeCuNbSiB 粉体"},{"id":"05964ad7-202d-49c5-9765-a3e177523f6b","keyword":"丁基橡胶","originalKeyword":"丁基橡胶"},{"id":"e33afa51-c9d2-4e96-815c-e68742104df1","keyword":"阻抗","originalKeyword":"阻抗"},{"id":"b68bffb4-5297-4605-9bd9-1028feb104a9","keyword":"<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>特性","originalKeyword":"力敏特性"}],"language":"zh","publisherId":"gncl201410014","title":"FeCuNbSiB非晶粉体/丁基橡胶复合薄膜的<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>特性","volume":"","year":"2014"},{"abstractinfo":"以 Fe73.5 Cu1 Nb3 Si13.5 B9粉体为复合相,丁基橡胶为基体,制得粉体质量含量为80%、厚度为200μm的复合薄膜；采用 TH2816LCR 数字电桥测试频率1 kHz下薄膜的阻抗Z 随压应力σ的变化情况,用LYYL-500N高档型微机控制压力试验机对薄膜体系进行程序控制加载；薄膜体系采用电容方式连接。研究了复合薄膜在3种不同的压应力条件下连续加载/卸载的<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>特性。研究表明,复合薄膜在连续加载/卸载速度≤0.5 mm/min和保压加载/卸载条件下、测试频率1 kHz、压应力0.1~1.0 MPa 时,复合薄膜具有良好的<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>稳定性和灵敏<span style=\"color:red\">性</span>。随着应力σ增大,阻抗Z 呈非线性下降,SI%值为6%~23%,灵敏精度k=Z’(σ)值范围1.9~0.02,测试标准偏差稳定在0.02~0.01,薄膜对于<0.3 MPa 应力更加灵敏。增加测试频率可以提高薄膜体系的<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>灵敏度。在压应力0.2~1.0 MPa范围内,薄膜弹性后效现象显著,导致薄膜加载Z-σ曲线与卸载曲线不重合。","authors":[{"authorName":"付远","id":"28a4af76-07c5-4055-8df2-63ef0ca9e85e","originalAuthorName":"付远"},{"authorName":"朱正吼","id":"cacf5ab9-2a8f-4a35-a6cb-80886b324c72","originalAuthorName":"朱正吼"},{"authorName":"乔宝英","id":"de1ccf4b-2283-44bb-bfd3-d55c49709266","originalAuthorName":"乔宝英"}],"doi":"10.3969/j.issn.1001-9731.2013.24.005","fpage":"3540","id":"f89982f2-6337-492b-b28d-aaee5ea07c9b","issue":"24","journal":{"abbrevTitle":"GNCL","coverImgSrc":"journal/img/cover/GNCL.jpg","id":"33","issnPpub":"1001-9731","publisherId":"GNCL","title":"功能材料"},"keywords":[{"id":"c1b69f58-cdda-4a71-aa9b-284e5e8347e6","keyword":"<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>薄膜","originalKeyword":"力敏薄膜"},{"id":"6126589a-366b-4c44-8519-f85297887003","keyword":"阻抗","originalKeyword":"阻抗"},{"id":"e6f56767-7966-499a-8b8a-9fabf58ad7c5","keyword":"弹性后效","originalKeyword":"弹性后效"},{"id":"ee601eb0-edad-4346-bf6c-4b72d2167d83","keyword":"丁基橡胶","originalKeyword":"丁基橡胶"}],"language":"zh","publisherId":"gncl201324005","title":"FeCuNbSiB粉体/丁基胶复合薄膜<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>特性","volume":"","year":"2013"},{"abstractinfo":"根据目前接触压力测量的研究现状和发展趋势,提出了一种新型柔性<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>导电胶敏感材料用于接触压力测量的思想.研究了柔性<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>导电胶的导电机理和<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>效应,对炭黑/硅橡胶/纳米二氧化硅复合体系的压阻特性,迟滞特性及时间响应特性进行了实验和分析.表明了这种可液体成型的新型<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>导电胶敏感材料具有较好的电学和力学性能,且工艺简单,成本低,可任意成型,适应于接触压力特别是柔性接触压力的测量场合.","authors":[{"authorName":"黄英","id":"478d05e7-ffa9-462f-960b-b6efe3db2608","originalAuthorName":"黄英"},{"authorName":"高峰","id":"89cfddbf-c3e0-44da-8605-53fcc56ee6dc","originalAuthorName":"高峰"},{"authorName":"仇怀利","id":"f07cc771-9417-40de-baa3-3a33e8347ecf","originalAuthorName":"仇怀利"},{"authorName":"付秀兰","id":"27aca30a-67f9-476a-aaf2-3acf33f59325","originalAuthorName":"付秀兰"},{"authorName":"余晓芬","id":"dd0335af-aacf-44ea-bb38-b04524020258","originalAuthorName":"余晓芬"}],"doi":"","fpage":"177","id":"bc396b03-a44a-470c-b333-b60062908502","issue":"2","journal":{"abbrevTitle":"GNCL","coverImgSrc":"journal/img/cover/GNCL.jpg","id":"33","issnPpub":"1001-9731","publisherId":"GNCL","title":"功能材料"},"keywords":[{"id":"376f0589-51cb-4817-807f-3590b6995305","keyword":"柔性","originalKeyword":"柔性"},{"id":"17038280-7fa6-42af-9416-1e74a17627bc","keyword":"接触压力","originalKeyword":"接触压力"},{"id":"5751c416-cb27-46f7-bbf4-452cc0ec5ac0","keyword":"<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>导电胶","originalKeyword":"力敏导电胶"}],"language":"zh","publisherId":"gncl200802001","title":"用于接触压力测量的柔性<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>导电胶研究","volume":"39","year":"2008"},{"abstractinfo":"以通用有效介质理论为基础，给出了炭黑填充导电橡胶（炭黑／橡胶）的<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>传感器灵敏系数计算方程。采用该方程并结合应变和压阻效应对“负压力一电阻特性”（NPC）的影响程度，分析了<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>导电炭黑／橡胶的灵敏系数和工作原理。结果表明：炭黑体积分数在临界体积分数附近时，<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>导电炭黑／橡胶的灵敏系数在2．5-13之间，其工作原理主要为压阻效应。当炭黑体积分数在渗流区时，灵敏系数在2．5-4．5之间，其工作原理与接触压力的大小有关。压力较小时，其工作原理主要为压阻效应；压力较大时，其工作原理主要为应变效应。炭黑体积分数在传导区时，灵敏系数在2．O-2．5之间，其工作原理主要为应变效应。","authors":[{"authorName":"刘平","id":"bec970be-7d3a-4f3e-91d5-0a7f443daae8","originalAuthorName":"刘平"},{"authorName":"黄英","id":"55bc746c-7d94-4ae6-a0fa-9de91d85f36f","originalAuthorName":"黄英"},{"authorName":"廉超","id":"e273478c-6951-4aee-b30f-41a1340eab51","originalAuthorName":"廉超"},{"authorName":"蒋红生","id":"830c30c7-37b1-4ca3-9dbb-72e265f05999","originalAuthorName":"蒋红生"},{"authorName":"葛运建","id":"e42ed543-0711-49da-ac2d-5a4196d32710","originalAuthorName":"葛运建"}],"doi":"","fpage":"16","id":"9afcae55-ecdc-4314-bb29-2420c96eff01","issue":"1","journal":{"abbrevTitle":"FHCLXB","coverImgSrc":"journal/img/cover/FHCLXB.jpg","id":"26","issnPpub":"1000-3851","publisherId":"FHCLXB","title":"复合材料学报"},"keywords":[{"id":"732572cf-29b9-41b7-bb61-b169a131cb42","keyword":"应变效应","originalKeyword":"应变效应"},{"id":"163d28a9-d3d7-41a7-88be-5c2256174420","keyword":"压阻效应","originalKeyword":"压阻效应"},{"id":"41013375-a9ba-41ff-a192-a161ea0c5bb0","keyword":"炭黑","originalKeyword":"炭黑"},{"id":"476fea83-fd8e-4c61-917a-5d88e8482cc4","keyword":"导电橡胶","originalKeyword":"导电橡胶"},{"id":"f5f706ed-1d61-4e68-9eec-207a149d6b19","keyword":"灵敏系数","originalKeyword":"灵敏系数"},{"id":"4a706368-61e0-4b73-8377-81ddb6d67327","keyword":"传感器","originalKeyword":"传感器"}],"language":"zh","publisherId":"fhclxb201201003","title":"炭黑填充导电橡胶的<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>传感器灵敏系数","volume":"29","year":"2012"},{"abstractinfo":"以通用有效介质理论为基础,给出了,炭黑填充导电橡胶(炭黑/橡胶)的<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>传感器灵敏度计算方程.采用该方程并结合形变和压阻效应,分析了影响<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>导电炭黑/橡胶的灵敏度的主要参数.结果表明:炭黑体积分数是影响<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>导电炭黑/橡胶的灵敏度的主要参数.当炭黑体积分数在临界体积分数附近时,<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>导电炭黑/橡胶的灵敏度为0.1～11.5 MPa-1,其敏感机制主要为压阻效应.当炭黑体积分数在渗流区时,灵敏度为0.2～3.6 MPa-1,其敏感机制还与接触压力的大小有关,压力较小时,主要为压阻效应；压力较大时,主要为应变效应.若炭黑体积分数在传导区,灵敏度为0.3～1.7 MPa-1,其敏感机制主要为应变效应.","authors":[{"authorName":"刘平","id":"f3dcf098-2f33-42c6-bd30-21df9bad1c3e","originalAuthorName":"刘平"},{"authorName":"黄英","id":"99f69030-4cab-4207-a5de-3ca31c6e4a84","originalAuthorName":"黄英"},{"authorName":"刘秀梅","id":"da48f116-8262-4eaf-a7ba-3836a21ba8ee","originalAuthorName":"刘秀梅"},{"authorName":"蔡文婷","id":"e2489f0e-5573-41f1-9c92-aa859fb6afcf","originalAuthorName":"蔡文婷"},{"authorName":"李锐琦","id":"1ff94367-4cc0-4c84-9a59-dea476b778a6","originalAuthorName":"李锐琦"},{"authorName":"王大月","id":"7db5ad57-b271-40fd-b862-3805a51689a3","originalAuthorName":"王大月"}],"doi":"","fpage":"51","id":"69a94a12-4be8-4425-b99a-4fe63b5302a3","issue":"3","journal":{"abbrevTitle":"FHCLXB","coverImgSrc":"journal/img/cover/FHCLXB.jpg","id":"26","issnPpub":"1000-3851","publisherId":"FHCLXB","title":"复合材料学报"},"keywords":[{"id":"5a3c1de0-468a-48bb-b757-f1c84321e67d","keyword":"复合材料","originalKeyword":"复合材料"},{"id":"7f807cc1-7821-427c-beb0-353eb655ee2c","keyword":"灵敏度","originalKeyword":"灵敏度"},{"id":"a8f7a25f-9425-4a34-8ca8-c1f3556a0613","keyword":"压力","originalKeyword":"压力"},{"id":"9fc90614-190d-45c9-b1e2-0e70c87fcf91","keyword":"炭黑","originalKeyword":"炭黑"},{"id":"59844735-e965-499d-8d18-7cd9ed0b98e9","keyword":"导电橡胶","originalKeyword":"导电橡胶"},{"id":"366680f9-decd-45d1-a42c-744bc2c5a2aa","keyword":"柔性触觉传感器","originalKeyword":"柔性触觉传感器"}],"language":"zh","publisherId":"fhclxb201303009","title":"基于炭黑填充导电橡胶的<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>传感器的灵敏度","volume":"30","year":"2013"},{"abstractinfo":"以60~100 nm 的 FeNi 粉体为应力敏感元、硅橡胶为柔性基体,压制成型了粉体分布均匀、粉体含量30．6％(质量分数)、厚度200μm 的薄膜,在连续加载/卸载速度为0．1 mm/min、测试频率1 kHz 条件下,研究了正应力和综合应力两种受力条件下薄膜的<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>特性.研究结果表明,通过过渡溶剂液相混合方法可实现纳米级FeNi粉体在薄膜中均匀分布；在正应力条件下,加载过程中σ＜0．2 MP a 时,薄膜的灵敏精度|k|值＞50,当σ为0．2~0．4 MPa,|k|值介于37~49之间,薄膜对＜0．2 MPa的正应力敏感；当综合应力σ＜0．1 MPa 时,薄膜灵敏精度|k|值在60以上,薄膜对＜0．1 MP a的综合应力敏感；在综合应力加载/卸载条件下,薄膜的弹性后效现象显著,导致力<span style=\"color:red\">敏</span>稳定性较差；在正应力条件下的<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>特性优于综合应力条件下的<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>特性.","authors":[{"authorName":"赵辉","id":"287cf3c9-8cda-4f81-8d22-5a89bbd918b5","originalAuthorName":"赵辉"},{"authorName":"朱正吼","id":"e21df57e-2b30-454f-8cee-293f19f90094","originalAuthorName":"朱正吼"}],"doi":"10.3969/j.issn.1001-9731.2015.11.021","fpage":"11098","id":"ea041137-47bb-413b-87df-fd563f1585a8","issue":"11","journal":{"abbrevTitle":"GNCL","coverImgSrc":"journal/img/cover/GNCL.jpg","id":"33","issnPpub":"1001-9731","publisherId":"GNCL","title":"功能材料"},"keywords":[{"id":"f4adefa8-7c5c-4646-8583-6aa66717c07a","keyword":"FeNi 粉体","originalKeyword":"FeNi 粉体"},{"id":"401da673-1ef8-4d43-a5af-92387b39c456","keyword":"纳米级","originalKeyword":"纳米级"},{"id":"0621aaa3-5349-41c7-acc6-51ac53423748","keyword":"液体硅橡胶","originalKeyword":"液体硅橡胶"},{"id":"fa08cad0-8086-400c-b9ec-bccf19440e6a","keyword":"<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>特性","originalKeyword":"力敏特性"}],"language":"zh","publisherId":"gncl201511021","title":"纳米级FeNi粉体/SiR薄膜的制备及<span style=\"color:red\">力</span><span style=\"color:red\">敏</span>特性研究?","volume":"","year":"2015"}],"totalpage":5119,"totalrecord":51181}