{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"本文报道一种新型的、准球形的有机分子材料TPR-1(四(吡咯-1-基-甲基)甲烷).这种有机分子含有四个吡咯基团,容易通过真空热蒸发成膜.在紫外光作用下,还可以原位交联,形成较稳定的半导体薄膜.实验中,分别用Cu或Al作为顶底电极,制作夹层器件,发现样品导电能力随外加电压变化存在明显的<span style=\"color:red\">非线性</span>变化特征,开关斜率比最高可达50倍,频率相应范围在50Hz～10kHz,并具有良好的重复性和稳定性.","authors":[{"authorName":"蔡永挚","id":"6050b156-c5b4-4f2c-840e-db47d894bf6c","originalAuthorName":"蔡永挚"},{"authorName":"郭鹏","id":"fe3447ba-a691-4d02-8c11-884862b6aba8","originalAuthorName":"郭鹏"},{"authorName":"刘春明","id":"a1be0fe7-2de4-448b-a0f5-d3144fe2467f","originalAuthorName":"刘春明"},{"authorName":"吕银祥","id":"c52b0ebe-9435-4703-aa20-f9a746db60ff","originalAuthorName":"吕银祥"},{"authorName":"徐伟","id":"8a2c14fc-c7ab-4986-bd87-2dfb9d474025","originalAuthorName":"徐伟"},{"authorName":"潘星龙","id":"e2700369-b687-4f95-8baf-8d573396781b","originalAuthorName":"潘星龙"},{"authorName":"华中一","id":"5ac648bd-6c82-4408-bf03-47f6fa2a4d82","originalAuthorName":"华中一"}],"doi":"","fpage":"1867","id":"9e3776cc-9857-46f1-890e-d8b747aeab71","issue":"z1","journal":{"abbrevTitle":"GNCL","coverImgSrc":"journal/img/cover/GNCL.jpg","id":"33","issnPpub":"1001-9731","publisherId":"GNCL","title":"功能材料"},"keywords":[{"id":"e47351d0-28a7-4798-a25e-e2b4ddbd2892","keyword":"有机分子材料","originalKeyword":"有机分子材料"},{"id":"c3376fb3-df98-4836-8f8a-8491b4feb942","keyword":"原位聚合","originalKeyword":"原位聚合"},{"id":"266d5ccd-753d-4a1f-92fd-7948d00724a1","keyword":"紫外辐照","originalKeyword":"紫外辐照"},{"id":"d48854f1-66c7-4aa2-9c6c-0e4243e089f8","keyword":"有机半导体薄膜","originalKeyword":"有机半导体薄膜"},{"id":"57a6b988-bd02-4819-ae16-1ea67b9f44e3","keyword":"<span style=\"color:red\">非线性</span><span style=\"color:red\">电阻</span>","originalKeyword":"非线性电阻"}],"language":"zh","publisherId":"gncl2004z1520","title":"有机薄膜的场效应<span style=\"color:red\">非线性</span><span style=\"color:red\">电阻</span>特性","volume":"35","year":"2004"},{"abstractinfo":"固相烧结SiC(SSiC)陶瓷大多数用于结构陶瓷材料,用于电子和<span style=\"color:red\">电阻</span>元器件的研究很少.实验以添加不同C含量的致密SSiC陶瓷材料为研究对象,研究了添加不同C含量SSiC陶瓷的伏安特性、<span style=\"color:red\">电阻</span>率与电流密度的变化关系及<span style=\"color:red\">电阻</span>率与温度的变化关系.研究结果表明:SSiC陶瓷表现出明显的<span style=\"color:red\">非线性</span>电学特性,其<span style=\"color:red\">电阻</span>率随着电流的增大而降低;对于添加3wt％C含量的SSiC陶瓷,当电场强度超过15.8 V/mm时,晶界势垒被击穿;对于添加6wt％C含量的SSiC陶瓷,当电场强度超过70.7 V/mm时,晶界势垒被击穿,它们的<span style=\"color:red\">电阻</span>率将为晶粒所控制,<span style=\"color:red\">电阻</span>率较小;同时在电场强度1 V/mm条件下,SSiC陶瓷<span style=\"color:red\">电阻</span>率随着温度的升高而降低,表现出很好热敏特性,从常温的106 Ω·cm变化为400℃的5 Ω·cm左右.","authors":[{"authorName":"陈健","id":"675b18db-847e-401a-a1b5-c853d62dca08","originalAuthorName":"陈健"},{"authorName":"殷杰","id":"9581d9db-4d04-40e1-8c2d-cbf808952855","originalAuthorName":"殷杰"},{"authorName":"朱云洲","id":"e32b33d3-56a5-463a-a051-7483284a3e0b","originalAuthorName":"朱云洲"},{"authorName":"杨勇","id":"d98f0a79-9518-4325-beab-0e72a4ef9f85","originalAuthorName":"杨勇"},{"authorName":"陈忠明","id":"f54fc1fd-bd66-4f49-a5fb-a87d6b706e88","originalAuthorName":"陈忠明"},{"authorName":"张景贤","id":"64f4c7c9-7613-45d0-bcd0-a4881f30f893","originalAuthorName":"张景贤"},{"authorName":"刘学建","id":"af66f475-a581-43d0-bddc-4a0ff4fbbd9d","originalAuthorName":"刘学建"},{"authorName":"黄政仁","id":"68f8199e-b75b-455a-a3da-8e9deee70c7e","originalAuthorName":"黄政仁"}],"doi":"10.15541/jim20160171","fpage":"45","id":"9b2c59f0-98f2-4b81-9b18-aa5062db65c1","issue":"1","journal":{"abbrevTitle":"WJCLXB","coverImgSrc":"journal/img/cover/WJCLXB.jpg","id":"62","issnPpub":"1000-324X","publisherId":"WJCLXB","title":"无机材料学报"},"keywords":[{"id":"4f9b01d9-cfae-4d63-a0f0-3366e468de31","keyword":"SiC","originalKeyword":"SiC"},{"id":"48b1ca54-4936-4c52-a511-18d919a45af4","keyword":"固相烧结","originalKeyword":"固相烧结"},{"id":"bc2331fb-0adf-4270-a163-8565247411c9","keyword":"<span style=\"color:red\">非线性</span><span style=\"color:red\">电阻</span>","originalKeyword":"非线性电阻"},{"id":"b446c5e3-63a3-4903-b0cd-3307a0df66bc","keyword":"热敏<span style=\"color:red\">电阻</span>","originalKeyword":"热敏电阻"}],"language":"zh","publisherId":"wjclxb201701007","title":"固相烧结SiC陶瓷的<span style=\"color:red\">非线性</span>电学行为研究","volume":"32","year":"2017"},{"abstractinfo":"研究了碳纤维水泥基材料(CFRC) <span style=\"color:red\">非线性</span><span style=\"color:red\">电阻</span>的伏安特性,并着重讨论了不同的碳纤维掺量和温度对CFRC材料电压-<span style=\"color:red\">电阻</span>关系的影响.结果表明:在较小外加电压下(＜2V)CFRC材料的电压-<span style=\"color:red\">电阻</span>曲线会出现明显的平台区,随着电压的进一步增大,其<span style=\"color:red\">电阻</span>逐渐降低呈现<span style=\"color:red\">非线性</span>特性.相同纤维掺量的水泥基材料随温度的升高其电压-<span style=\"color:red\">电阻</span>曲线下降斜率基本保持不变,但初始<span style=\"color:red\">电阻</span>值下降;而在温度保持不变时,随碳纤维掺量的增加,<span style=\"color:red\">电阻</span>随电压下降的趋势逐渐减缓.","authors":[{"authorName":"姚武","id":"42680602-ab6d-4479-aad3-7ea738ecc004","originalAuthorName":"姚武"},{"authorName":"徐晶","id":"2b4d0842-30e0-4352-95a2-de6168a4a6a5","originalAuthorName":"徐晶"}],"doi":"","fpage":"632","id":"f43d4fa2-0b4d-48f1-935c-1f3a5801930f","issue":"4","journal":{"abbrevTitle":"GNCL","coverImgSrc":"journal/img/cover/GNCL.jpg","id":"33","issnPpub":"1001-9731","publisherId":"GNCL","title":"功能材料"},"keywords":[{"id":"3a9fe0c8-8725-46af-af67-3a0022d97333","keyword":"碳纤维","originalKeyword":"碳纤维"},{"id":"fa7de6c2-a1ab-4a4c-bf2b-a783178bb72d","keyword":"水泥基材料","originalKeyword":"水泥基材料"},{"id":"7b71b733-dd30-4707-906d-30de2993a2d8","keyword":"电压","originalKeyword":"电压"},{"id":"dcdc7d2a-9ac8-45a4-a042-bf4867da39f9","keyword":"<span style=\"color:red\">电阻</span>","originalKeyword":"电阻"},{"id":"662c8470-2e2e-46bd-a13b-ddf43ac85548","keyword":"<span style=\"color:red\">非线性</span>","originalKeyword":"非线性"}],"language":"zh","publisherId":"gncl200604038","title":"碳纤维水泥基材料<span style=\"color:red\">电阻</span>的<span style=\"color:red\">非线性</span>研究","volume":"37","year":"2006"},{"abstractinfo":"制备的ZnO/Co2O3敏感<span style=\"color:red\">电阻</span>单元材料同时具有伏安(V-I)<span style=\"color:red\">非线性</span>特性及负温<span style=\"color:red\">电阻</span>(NTC)效应.两种效应的形成与烧结过程900℃热处理温度密切相关.差热分析(DTA)曲线表明:Co2O3在904℃有一相变吸收峰.在该温度点保温热处理的ZnO/Co2O3敏感<span style=\"color:red\">电阻</span>单元材料获得相对大的伏安<span style=\"color:red\">非线性</span>和NTC效应.电子自旋共振谱(ESR)证明,Co离子由烧结热处理前的Co3+价变成热处理后的Co2+价,其中最大敏感<span style=\"color:red\">电阻</span>和伏安<span style=\"color:red\">非线性</span>参数样品与最强Co2+离子ESR信号对应.变温过程ESR动态观察显示,Co2+与Co3+可逆变换,说明被Co2+离子束缚的电子存在禁锢与脱离的可逆过程.这是ZnO/Co2O3敏感<span style=\"color:red\">电阻</span>单元材料在电场、热场下产生V-I<span style=\"color:red\">非线性</span>及NTC效应的基础.","authors":[{"authorName":"徐国跃","id":"387f69cf-d35b-4070-a143-7599c6a0427e","originalAuthorName":"徐国跃"},{"authorName":"马立新","id":"c289af60-f611-4cc6-95e3-eec19950479a","originalAuthorName":"马立新"},{"authorName":"谢国治","id":"bcb532c7-0f68-4d15-b550-e6a7502cb970","originalAuthorName":"谢国治"},{"authorName":"骆心怡","id":"31a21eef-f562-4dfc-9abe-c48946363a88","originalAuthorName":"骆心怡"}],"doi":"","fpage":"516","id":"ce65c4c0-e0a1-4f0c-97e4-bd73420b0663","issue":"5","journal":{"abbrevTitle":"GNCL","coverImgSrc":"journal/img/cover/GNCL.jpg","id":"33","issnPpub":"1001-9731","publisherId":"GNCL","title":"功能材料"},"keywords":[{"id":"6fe77349-e9ba-44a4-89e8-3376ae55cb53","keyword":"ZnO","originalKeyword":"ZnO"},{"id":"1f53a421-e579-4dbd-82b5-20c68a98a845","keyword":"压敏陶瓷","originalKeyword":"压敏陶瓷"},{"id":"1226ec01-246e-4f1d-ba5e-d0da266f718d","keyword":"V-I<span style=\"color:red\">非线性</span>","originalKeyword":"V-I非线性"},{"id":"1d91cdec-3e56-4450-82a0-1249b3dda6af","keyword":"NTC效应","originalKeyword":"NTC效应"}],"language":"zh","publisherId":"gncl200005026","title":"ZnO/Co2O3敏感<span style=\"color:red\">电阻</span>单元材料V-I<span style=\"color:red\">非线性</span>及NTC效应","volume":"31","year":"2000"},{"abstractinfo":"粒子群优化算法是一种启发式的全局优化算法，将其与 BP 神经网络结合，能够有效地改善 BP 神经网络在进行<span style=\"color:red\">电阻</span>率层析反演中的收敛速度和求解质量。提出一种基于混沌振荡的粒子群算法，使用混沌振荡曲线来自适应调整惯性权重w以提高PSO算法的全局寻优能力，并使用其训练和优化BP神经网络的权值和阈值。比较不同隐含层节点数目和惯性权重w值对反演结果的影响，并给出混沌振荡PSO-BP算法<span style=\"color:red\">非线性</span>反演的具体实现方案。对均匀半空间中异常体理论模型进行反演，实验结果表明：混沌振荡PSO-BP不依赖初始模型，在稳定性和准确性上优于BP反演和标准PSO-BP反演，成像质量优于最小二乘法反演的。","authors":[{"authorName":"戴前伟","id":"1d81e9b5-b973-4076-8619-0e35fc6f92f6","originalAuthorName":"戴前伟"},{"authorName":"江沸菠","id":"b4541ca2-a85d-4406-87e7-21a6b83d800a","originalAuthorName":"江沸菠"}],"doi":"","fpage":"2897","id":"a3f0eb60-9e25-41e6-853e-af9a83eb7aad","issue":"10","journal":{"abbrevTitle":"ZGYSJSXB","coverImgSrc":"journal/img/cover/ZGYSJSXB.jpg","id":"88","issnPpub":"1004-0609","publisherId":"ZGYSJSXB","title":"中国有色金属学报"},"keywords":[{"id":"0f52a786-3d48-431d-9cd1-650a70d4a0cb","keyword":"<span style=\"color:red\">电阻</span>率层析成像","originalKeyword":"电阻率层析成像"},{"id":"e7cc4c78-4910-45a3-b10a-3daab72fee68","keyword":"<span style=\"color:red\">非线性</span>反演","originalKeyword":"非线性反演"},{"id":"f53e73fb-1882-4764-bca3-ba424a615471","keyword":"粒子群优化","originalKeyword":"粒子群优化"},{"id":"156be7da-43b4-4963-90a4-fd12b213e05b","keyword":"反向传播网络","originalKeyword":"反向传播网络"},{"id":"ea0a6c83-3c68-43ad-805e-f9bd51ff43ec","keyword":"混沌序列","originalKeyword":"混沌序列"}],"language":"zh","publisherId":"zgysjsxb201310023","title":"基于混沌振荡PSO-BP算法的<span style=\"color:red\">电阻</span>率层析成像<span style=\"color:red\">非线性</span>反演","volume":"","year":"2013"},{"abstractinfo":"本文根据全矢量模型首先对背景材料取为 silica 材料的六角形光子晶体光纤(PCF)结构,在不同空气孔直径下对基模<span style=\"color:red\">非线性</span>系数的影响进行数值研究,在此基础上,进一步将光子晶体背景材料折射率取为 -1.45 进行仿真数值研究,探究负折射率介质材料在不同空气孔直径下对基模<span style=\"color:red\">非线性</span>系数影响的物理规律性,数值研究发现,无论背景材料的折射率为正,还是为负,增大空气孔的直径d都会使<span style=\"color:red\">非线性</span>系数增大;不同的是,当背景材料取为负折射率材料时,会出现负的<span style=\"color:red\">非线性</span>系数,这将对设计不同要求的<span style=\"color:red\">非线性</span>微结构光纤提供有效的理论依据.","authors":[{"authorName":"潘波","id":"78ba7f52-5340-4446-8677-b95661c322c0","originalAuthorName":"潘波"}],"doi":"","fpage":"1204","id":"21fe332e-7766-4aa2-afbb-449591e9d68e","issue":"6","journal":{"abbrevTitle":"GSYTB","coverImgSrc":"journal/img/cover/GSYTB.jpg","id":"36","issnPpub":"1001-1625","publisherId":"GSYTB","title":"硅酸盐通报   "},"keywords":[{"id":"028655f0-2402-434b-962d-68c95129e064","keyword":"光子晶体光纤","originalKeyword":"光子晶体光纤"},{"id":"29c5215a-eb6c-42dc-b519-d697cc248197","keyword":"负折射率材料","originalKeyword":"负折射率材料"},{"id":"c0852a7e-ffdb-457f-bf93-c8dfaecb113b","keyword":"<span style=\"color:red\">非线性</span>系数","originalKeyword":"非线性系数"},{"id":"4c341993-5408-44aa-aa4e-d9c765ef1512","keyword":"全矢量模型","originalKeyword":"全矢量模型"}],"language":"zh","publisherId":"gsytb200806024","title":"光子晶体光纤的<span style=\"color:red\">非线性</span>研究","volume":"27","year":"2008"},{"abstractinfo":"在模拟线棒上绕包一层防晕材料，测试其<span style=\"color:red\">电阻</span>在场强变化下的<span style=\"color:red\">非线性</span>特性，探讨防晕材料<span style=\"color:red\">非线性</span>特性的测试及计算方法，并对比了部分国内外防晕材料的<span style=\"color:red\">非线性</span>特性。结果表明：国外某公司的防晕高阻带A的<span style=\"color:red\">非线性</span>特性较好，防晕高阻带B的<span style=\"color:red\">非线性</span>特性较好，而自制高阻带C的<span style=\"color:red\">非线性</span>特性一般。","authors":[{"authorName":"曾柏顺","id":"a98e52f6-e990-4871-9e5c-451feaa345bf","originalAuthorName":"曾柏顺"},{"authorName":"费巍峰","id":"c1c1eade-1e4e-456f-8231-d7ce8df9f62f","originalAuthorName":"费巍峰"},{"authorName":"舒氧","id":"adc90a8a-a134-42fe-8f4b-59fe2d506a80","originalAuthorName":"舒氧"},{"authorName":"夏宇","id":"c6e4a605-6b7c-45fd-bb84-643479851c25","originalAuthorName":"夏宇"}],"doi":"","fpage":"57","id":"df4fa412-5b3b-45ee-9e7e-61f62acf83d8","issue":"5","journal":{"abbrevTitle":"JYCL","coverImgSrc":"journal/img/cover/JYCL.jpg","id":"50","issnPpub":"1009-9239","publisherId":"JYCL","title":"绝缘材料"},"keywords":[{"id":"c1d0f090-5a16-44fe-ab41-f7bc6d543acf","keyword":"碳化硅","originalKeyword":"碳化硅"},{"id":"44da45da-6eaf-4bcf-ac04-8b416e3fe254","keyword":"防晕材料","originalKeyword":"防晕材料"},{"id":"c12d38a9-c48e-420f-ace9-85181431b0c7","keyword":"<span style=\"color:red\">非线性</span>特性","originalKeyword":"非线性特性"}],"language":"zh","publisherId":"jycltx201505013","title":"高压电机用防晕材料<span style=\"color:red\">非线性</span>特性比较分析","volume":"","year":"2015"},{"abstractinfo":"综述了碳化硅<span style=\"color:red\">非线性</span>导电特性的意义和碳化硅材料的特性、<span style=\"color:red\">非线性</span>导电特性的测试及计算方法,讨论了α-SiC和β-SiC的<span style=\"color:red\">非线性</span>导电特性及其影响因素.前人研究结果表明,对于α-SiC,颗粒越粗,<span style=\"color:red\">电阻</span>率ρ 0越低、<span style=\"color:red\">非线性</span>系数β越大;颗粒越细,<span style=\"color:red\">电阻</span>率ρ 0越高、<span style=\"color:red\">非线性</span>系数β越小;不同种类,不同工厂生产的碳化硅的<span style=\"color:red\">电阻</span>率ρ 0和<span style=\"color:red\">非线性</span>系数β是不同的;α-SiC制成防晕带后<span style=\"color:red\">电阻</span>率升高,β值下降,颗粒越粗,β值下降越大;防晕带与粉料的<span style=\"color:red\">非线性</span>性质有相似的规律 ,而β-SiC具有比α-SiC低得多的<span style=\"color:red\">电阻</span>率和较大的<span style=\"color:red\">非线性</span>系数,并且其<span style=\"color:red\">电阻</span>率和<span style=\"color:red\">非线性</span>系数受到粉料的粒径、合成温度和涂层有机物含量等因素的直接影响.","authors":[{"authorName":"郭磊","id":"6560dfe4-f45c-49f0-a0ae-7fcf6185de5d","originalAuthorName":"郭磊"},{"authorName":"宁叔帆","id":"f8b6457f-e7c6-4ab3-aeb9-b1238eb61794","originalAuthorName":"宁叔帆"},{"authorName":"于开坤","id":"b466d00a-db9b-43b1-adb3-30264325bf4c","originalAuthorName":"于开坤"},{"authorName":"李红岩","id":"f80e55b8-3df9-412f-838e-2ba80aa4b9e4","originalAuthorName":"李红岩"},{"authorName":"赵丽华","id":"aba3d290-00fd-4a24-bece-0ddc0fa13e29","originalAuthorName":"赵丽华"},{"authorName":"刘斌","id":"eb71f20e-625a-4e7c-839d-15a79ba73f65","originalAuthorName":"刘斌"},{"authorName":"陈寿田","id":"8e2bdf72-65a5-4c22-a001-6780c03405c8","originalAuthorName":"陈寿田"}],"doi":"10.3969/j.issn.1009-9239.2005.03.019","fpage":"60","id":"3b65a76d-47af-40aa-983d-071abde20d76","issue":"3","journal":{"abbrevTitle":"JYCL","coverImgSrc":"journal/img/cover/JYCL.jpg","id":"50","issnPpub":"1009-9239","publisherId":"JYCL","title":"绝缘材料"},"keywords":[{"id":"4b936368-e56b-4c45-bc6b-4c95b2985929","keyword":"碳化硅","originalKeyword":"碳化硅"},{"id":"a46fb23b-acc8-422b-9995-1ed9422b1f50","keyword":"<span style=\"color:red\">电阻</span>率","originalKeyword":"电阻率"},{"id":"4308f332-08da-4f8c-86fc-208a40f90958","keyword":"<span style=\"color:red\">非线性</span>系数","originalKeyword":"非线性系数"},{"id":"a66f05d9-55c7-4574-8de4-2f1ae81c17f8","keyword":"应用","originalKeyword":"应用"}],"language":"zh","publisherId":"jycltx200503019","title":"碳化硅<span style=\"color:red\">非线性</span>导电特性的研究进展","volume":"38","year":"2005"},{"abstractinfo":"对于芯区为克尔型<span style=\"color:red\">非线性</span>介质，衬底和包层为<span style=\"color:red\">线性</span>介质的LNL型<span style=\"color:red\">非线性</span>光波导，给出了各层介质中的场分布和功率分布的数学表达式，纠正了Boardman和Egan在1986年发表的文章中的几处差错，给出了正确的色散方程，并对该文中所引的典型实例进行了计算，给出了正确的数据和曲线.所得结果的正确性已采用数值分析法进行过核验.","authors":[{"authorName":"王照明","id":"e238f678-d25d-48d7-93db-241626ba5abd","originalAuthorName":"王照明"},{"authorName":"佘守宪","id":"403e6d6e-ef3e-4a1c-853b-02f7563548dc","originalAuthorName":"佘守宪"},{"authorName":"林铁生","id":"433a76b1-e427-4c5e-825c-7dfde87f5162","originalAuthorName":"林铁生"},{"authorName":"王薇","id":"4df8fa3b-e43a-4a8b-9c54-72e977c1fd28","originalAuthorName":"王薇"}],"doi":"10.3969/j.issn.1007-5461.2001.02.008","fpage":"130","id":"edbea309-ebd7-4d3b-b61b-b2f312381481","issue":"2","journal":{"abbrevTitle":"LZDZXB","coverImgSrc":"journal/img/cover/LZDZXB.jpg","id":"53","issnPpub":"1007-5461","publisherId":"LZDZXB","title":"量子电子学报   "},"keywords":[{"id":"43cc2f9c-6257-4b7a-bf01-b508fd8bbc6a","keyword":"<span style=\"color:red\">非线性</span>光波导","originalKeyword":"非线性光波导"},{"id":"03e20aff-be95-4cc0-98bc-3d287f17b79c","keyword":"克尔型光学介质","originalKeyword":"克尔型光学介质"}],"language":"zh","publisherId":"lzdzxb200102008","title":"<span style=\"color:red\">非线性</span>薄膜中的导模","volume":"18","year":"2001"},{"abstractinfo":"通过分析力敏炭黑填充导电橡胶（力敏导电炭黑/橡胶）＂负<span style=\"color:red\">电阻</span>-压力系数＂（NPCR）的主因,研究了基于炭黑填充导电橡胶的力传感器<span style=\"color:red\">非线性</span>特性。研究表明,当炭黑体积分数接近临界渗流体积分数时,NPCR<span style=\"color:red\">非线性</span>的主因为<span style=\"color:red\">电阻</span>率的<span style=\"color:red\">非线性</span>减小;炭黑体积分数在渗流区时,NPCR<span style=\"color:red\">非线性</span>的主因为<span style=\"color:red\">电阻</span>率的<span style=\"color:red\">非线性</span>减小和导电橡胶应力-应变关系的<span style=\"color:red\">非线性</span>;若炭黑体积分数在传导区时,NPCR<span style=\"color:red\">非线性</span>的主因为应力-应变关系的<span style=\"color:red\">非线性</span>。随着炭黑体积分数的增大,力敏导电炭黑/橡胶的NPCR<span style=\"color:red\">非线性</span>逐渐减弱。此外,由于界面压阻效应以及导电橡胶近似不可压缩体的性质,用于获取NPCR效应的电极分布形式也对NPCR效应的<span style=\"color:red\">非线性</span>特性存在影响。","authors":[{"authorName":"刘平","id":"28ed1d81-9917-4f38-a193-d843f8b5e82a","originalAuthorName":"刘平"},{"authorName":"黄英","id":"017e64b5-a2c1-4b13-b449-10a6eba51413","originalAuthorName":"黄英"},{"authorName":"廉超","id":"3797d9f9-8edb-40ea-9b2b-e7385b342b53","originalAuthorName":"廉超"},{"authorName":"蒋红生","id":"bf20c23c-e660-49bb-9411-1b4031e264e6","originalAuthorName":"蒋红生"},{"authorName":"刘秀梅","id":"db6be1b4-5205-45c9-8486-17e9c4c1a779","originalAuthorName":"刘秀梅"},{"authorName":"赵小文","id":"e8366188-74b6-41df-95e2-c74ae0343038","originalAuthorName":"赵小文"}],"doi":"","fpage":"72","id":"02cacd22-0d29-46c2-9410-efa717c9e5ba","issue":"8","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":"95b6069e-8d70-43d8-a1f1-2b16e984ae8b","keyword":"<span style=\"color:red\">非线性</span>","originalKeyword":"非线性"},{"id":"f5556169-5e80-4276-bc20-7e8bd4d7ee86","keyword":"炭黑","originalKeyword":"炭黑"},{"id":"3fe8e993-a425-476f-9d9e-9c2f725fa480","keyword":"导电橡胶","originalKeyword":"导电橡胶"},{"id":"ed26b013-1933-4ea5-bdfe-51ed1cfc031f","keyword":"触觉传感器","originalKeyword":"触觉传感器"}],"language":"zh","publisherId":"gfzclkxygc201208018","title":"基于炭黑填充导电橡胶的压力传感器<span style=\"color:red\">非线性</span>特性","volume":"28","year":"2012"}],"totalpage":1358,"totalrecord":13575}