{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"人造织构表面在润滑条件下,较光滑表面提高了润滑性能,减少磨损.为了深入了解织构表面形貌对流体润滑影响的机理,本文提出了规则凹坑表面油膜<span style=\"color:red\">压力</span>的<span style=\"color:red\">计算</span>方案和公式,比较了粗糙表面与光滑表面的最小油膜厚度和<span style=\"color:red\">压力</span>分布.结果表明,低速、低载时,规则凹坑表面具有更大的最小油膜厚度,更接近弹流润滑的典型膜厚,而接触面间的最大油膜<span style=\"color:red\">压力</span>降低.","authors":[{"authorName":"李鹏","id":"c1850001-de09-461b-b1ad-82fa2ea4d5b5","originalAuthorName":"李鹏"},{"authorName":"李健","id":"b3dffb5f-038e-4179-aa99-efbdf3be3547","originalAuthorName":"李健"},{"authorName":"","id":"90753e3e-1a65-4b0d-a2b3-7adc18e02c28","originalAuthorName":""},{"authorName":"董光能","id":"2ee03522-b1c9-4c28-af7d-581d7cce7f4e","originalAuthorName":"董光能"}],"doi":"10.3969/j.issn.1001-1560.2004.z1.037","fpage":"123","id":"3388d076-b482-405d-895b-b2ebd0948aa5","issue":"z1","journal":{"abbrevTitle":"CLBH","coverImgSrc":"journal/img/cover/CLBH.jpg","id":"7","issnPpub":"1001-1560","publisherId":"CLBH","title":"材料保护"},"keywords":[{"id":"d644f1e7-bc94-4049-af0f-5f356cc968b5","keyword":"人造织构表面","originalKeyword":"人造织构表面"},{"id":"b972bb5c-74d3-4519-bb63-40ed2b9971a0","keyword":"弹流","originalKeyword":"弹流"},{"id":"b2d459fa-cf38-43ba-b31d-2a66a44eeea6","keyword":"润滑膜","originalKeyword":"润滑膜"},{"id":"0a5baf5a-6475-416c-bacc-d37d3725343c","keyword":"<span style=\"color:red\">压力计算</span>","originalKeyword":"压力计算"}],"language":"zh","publisherId":"clbh2004z1037","title":"不同速度、载荷下点接触弹流润滑<span style=\"color:red\">计算</span>","volume":"37","year":"2004"},{"abstractinfo":"运用BP网络建立了平整轧制<span style=\"color:red\">压力计算</span>方法,实际应用结果表明:BP网络建立了平整轧制<span style=\"color:red\">压力计算</span>方法比较简单,<span style=\"color:red\">计算</span>精度高,<span style=\"color:red\">计算</span>误差小于8 %,完全可以应用于工程实际.","authors":[{"authorName":"魏立群","id":"c1875393-43d0-420d-9c04-1cd7d2e38d40","originalAuthorName":"魏立群"},{"authorName":"卢冬华","id":"92bb13fe-a53b-4b0f-a2ea-c66a65f62141","originalAuthorName":"卢冬华"}],"doi":"","fpage":"33","id":"f2a93d8f-043f-4420-a9a6-c9a5af636f2b","issue":"12","journal":{"abbrevTitle":"GT","coverImgSrc":"journal/img/cover/GT.jpg","id":"27","issnPpub":"0449-749X","publisherId":"GT","title":"钢铁"},"keywords":[{"id":"27a9d0b7-9f0f-474f-b321-bc3560bd45c8","keyword":"BP网络","originalKeyword":"BP网络"},{"id":"62f5f807-94da-44b2-b9cd-453fa0a59e38","keyword":"平整","originalKeyword":"平整"},{"id":"9fd58fff-f01b-4111-89b7-3751bb8b5188","keyword":"轧制<span style=\"color:red\">压力</span>","originalKeyword":"轧制压力"}],"language":"zh","publisherId":"gt200212010","title":"基于BP网络的平整轧制<span style=\"color:red\">压力计算</span>","volume":"37","year":"2002"},{"abstractinfo":"本文以Watts提出的求解代数方程组的附加修正值法为基础,在油藏<span style=\"color:red\">压力</span>数值<span style=\"color:red\">计算</span>中,提出了一种加快油藏<span style=\"color:red\">压力计算</span>迭代收敛速度的分块修正技术.在<span style=\"color:red\">计算</span>过程中,将原来的整个<span style=\"color:red\">计算</span>区块一个修正值,改变成根据边界以及各<span style=\"color:red\">计算</span>区块孔隙度的不同,对不同的<span style=\"color:red\">计算</span>区域分块修正.通过<span style=\"color:red\">计算</span>表明,在同等<span style=\"color:red\">计算</span>条件下,分块修正技术较之单块修正明显加快了<span style=\"color:red\">计算</span>迭代收敛速度,最后本文对分块修正加快收敛速度的原因做了分析.","authors":[{"authorName":"贾欣鑫","id":"8393c15f-27fb-4fb1-8c2d-5b1c694ce701","originalAuthorName":"贾欣鑫"},{"authorName":"徐明海","id":"a41464ca-0432-4948-8edf-3c9f223aade3","originalAuthorName":"徐明海"},{"authorName":"王胜","id":"cf6e86b5-70cd-421e-a5d7-be2db6caf430","originalAuthorName":"王胜"},{"authorName":"胡国华","id":"45eef63a-53a0-45e8-906e-54185da8d280","originalAuthorName":"胡国华"},{"authorName":"梁卓","id":"07f66e9d-3578-4bb9-89a1-1a2cffa21be8","originalAuthorName":"梁卓"}],"doi":"","fpage":"545","id":"01c4e309-4375-4230-be00-8b70297e57e9","issue":"3","journal":{"abbrevTitle":"GCRWLXB","coverImgSrc":"journal/img/cover/GCRWLXB.jpg","id":"32","issnPpub":"0253-231X","publisherId":"GCRWLXB","title":"工程热物理学报   "},"keywords":[{"id":"699b6024-138c-42fd-a516-ee290536089b","keyword":"油藏数值模拟","originalKeyword":"油藏数值模拟"},{"id":"7eb1bdf2-b7ad-41a2-bc68-c9c05f9abe79","keyword":"<span style=\"color:red\">压力</span>修正","originalKeyword":"压力修正"},{"id":"fe7458ba-8b57-4c0a-8b05-042430977ee3","keyword":"多块修正","originalKeyword":"多块修正"},{"id":"0f9e5f04-f942-4267-8ecc-7568b27cf47d","keyword":"TDMA算法","originalKeyword":"TDMA算法"}],"language":"zh","publisherId":"gcrwlxb201403030","title":"加快油藏<span style=\"color:red\">压力计算</span>收敛速度的数值方法—分区块修正","volume":"35","year":"2014"},{"abstractinfo":"目前凝析气井井筒<span style=\"color:red\">压力计算</span>仍在沿用常规气井的方法,由于对井筒相态考虑不充分,<span style=\"color:red\">计算</span>精度无法满足动态分析和生产管理的需求.本文从凝析气井井筒相态特性出发,结合井筒温度分布,以气液相平衡<span style=\"color:red\">计算</span>为基础,建立了凝析气井生产过程综合考虑井筒温度、相态变化的<span style=\"color:red\">压力计算</span>模型,运用隐式差分格式并结合具体实例对凝析气井生产过程井筒<span style=\"color:red\">压力</span>分布进行了研究和<span style=\"color:red\">计算</span>.从<span style=\"color:red\">计算</span>结果看,该方法考虑了井筒温度及相态变化,因而井底<span style=\"color:red\">压力</span>的<span style=\"color:red\">计算</span>结果与实际情况更接近,可以解决<span style=\"color:red\">压力计</span>无法下入产层中部或不能正常测试的问题,作为凝析气井<span style=\"color:red\">压力</span>测试的替代手段,在仅进行井口参数测量的情况下能够帮助完成凝析气井常规的生产动态分析工作,从而节省测试所需的大量人力、物力.","authors":[{"authorName":"孟悦新","id":"53bd09e9-2ac1-4a03-ab19-81522f7ba5e6","originalAuthorName":"孟悦新"},{"authorName":"李相方","id":"7e6ac335-0d2e-4545-bd80-afbe83f9c26c","originalAuthorName":"李相方"},{"authorName":"尹邦堂","id":"4743974b-b22f-4232-ac7f-d1769ac1e12e","originalAuthorName":"尹邦堂"},{"authorName":"齐明明","id":"1c0727bb-9103-43a9-924f-762648dc6d22","originalAuthorName":"齐明明"}],"doi":"","fpage":"1508","id":"c1f6bea1-92ba-44d7-84fc-a59e021c3be9","issue":"9","journal":{"abbrevTitle":"GCRWLXB","coverImgSrc":"journal/img/cover/GCRWLXB.jpg","id":"32","issnPpub":"0253-231X","publisherId":"GCRWLXB","title":"工程热物理学报   "},"keywords":[{"id":"1e04fb44-9f83-457a-b994-2c7eb17ead54","keyword":"凝析气井","originalKeyword":"凝析气井"},{"id":"bf15ae67-7746-45d8-9ff9-feef2604e748","keyword":"相平衡","originalKeyword":"相平衡"},{"id":"b6130f4f-f63f-4939-986a-c717009dd5a3","keyword":"温度","originalKeyword":"温度"},{"id":"5359f0f7-42d9-459c-9aab-e07d32d95a29","keyword":"流压","originalKeyword":"流压"},{"id":"7a4f612c-d922-4dcb-9b86-6d935a6f9e35","keyword":"差分","originalKeyword":"差分"}],"language":"zh","publisherId":"gcrwlxb201009017","title":"凝析气井井筒流动<span style=\"color:red\">压力</span>分布<span style=\"color:red\">计算</span>方法","volume":"31","year":"2010"},{"abstractinfo":"采用轧制-拉伸法建立了铸轧铝坯的变形抗力模型;根据实测轧制<span style=\"color:red\">压力</span>并利用 Hill 显式估算得出铝箔粗轧机和中轧机轧制过程的摩擦系数;提出了变形速度系数的算法;推导了 Hill 显式的无解条件及最小可轧厚度公式.","authors":[{"authorName":"吴瑞峰","id":"53824b71-1a8e-403a-8d21-34800cb76903","originalAuthorName":"吴瑞峰"},{"authorName":"林大为","id":"6a543641-bbb0-488c-bae1-038c0ca195c3","originalAuthorName":"林大为"}],"doi":"10.3969/j.issn.1001-7208.2003.04.008","fpage":"36","id":"940a98d5-4404-4cc4-b522-e6f17f96f02e","issue":"4","journal":{"abbrevTitle":"SHJS","coverImgSrc":"journal/img/cover/SHJS.jpg","id":"59","issnPpub":"1001-7208","publisherId":"SHJS","title":"上海金属"},"keywords":[{"id":"84612fc6-b1be-4ea7-b8fb-c9699995b091","keyword":"铝箔","originalKeyword":"铝箔"},{"id":"415e1b21-dc9e-4bf9-b7d0-c201508a49d8","keyword":"轧制<span style=\"color:red\">压力</span>","originalKeyword":"轧制压力"},{"id":"7025437e-73a5-402b-b4c4-ab80c9d2eb7c","keyword":"Hill","originalKeyword":"Hill"},{"id":"b334b4a5-aa54-4a04-b9d5-63a4c9e6d59f","keyword":"显式<span style=\"color:red\">计算</span>","originalKeyword":"显式计算"},{"id":"e7aceb5e-bae4-41f8-bf48-a19bed8411fe","keyword":"最小可轧厚度","originalKeyword":"最小可轧厚度"}],"language":"zh","publisherId":"shjs200304008","title":"铝箔轧制<span style=\"color:red\">压力</span>的<span style=\"color:red\">计算</span>","volume":"25","year":"2003"},{"abstractinfo":"本文建立了均质形核条件下<span style=\"color:red\">压力</span>与温度对形核率影响的数学方程,用此方程<span style=\"color:red\">计算</span>了Betol<span style=\"color:red\">压力</span>下结晶的形核数。得出在<span style=\"color:red\">压力</span>不变条件下,形核率-温度曲线出现一峰值,增加<span style=\"color:red\">压力</span>此峰值向高温方向移动。对于结晶时体积收缩的晶体物质,在温度不变的条件下,形核率-<span style=\"color:red\">压力</span>曲线也出现峰值,温度升高此峰值向高压方向移动。","authors":[{"authorName":"齐丕骧","id":"71134ff8-a2bb-43e3-a7f8-50d2cef5d6c4","originalAuthorName":"齐丕骧"}],"categoryName":"|","doi":"","fpage":"465","id":"ca2208c5-9df4-4042-9f25-71401293f14f","issue":"6","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[],"language":"zh","publisherId":"0412-1961_1984_6_10","title":"对<span style=\"color:red\">压力</span>下结晶形核率的理论<span style=\"color:red\">计算</span>","volume":"20","year":"1984"},{"abstractinfo":"用于固体火箭发动机壳体和工业贮罐的纤维缠绕<span style=\"color:red\">压力</span>容器，爆破压强是重要的设计参数。本文基于网络理论，给出了纤维缠绕圆筒<span style=\"color:red\">压力</span>容器圆筒和封头爆破压强的<span style=\"color:red\">计算</span>方法，给出了用模拟实验<span style=\"color:red\">压力</span>容器确定纤维发挥强度的方法。算例表明，<span style=\"color:red\">计算</span>值与实测结果符合良好。这些方法可供纤维缠绕<span style=\"color:red\">压力</span>容器设计者参考或直接应用。","authors":[{"authorName":"陈汝训","id":"80fb394b-fb06-47fa-856e-baf7e4df694b","originalAuthorName":"陈汝训"}],"doi":"10.3969/j.issn.1007-2330.2000.06.006","fpage":"28","id":"6be30c3b-9e73-4476-87cc-c79b942f0c92","issue":"6","journal":{"abbrevTitle":"YHCLGY","coverImgSrc":"journal/img/cover/YHCLGY.jpg","id":"77","issnPpub":"1007-2330","publisherId":"YHCLGY","title":"宇航材料工艺   "},"keywords":[{"id":"3cb064c1-03b9-41fe-833f-4760de5d79e4","keyword":"纤维缠绕","originalKeyword":"纤维缠绕"},{"id":"c39cebc6-d706-450a-abed-24a930ca9044","keyword":"<span style=\"color:red\">压力</span>容器","originalKeyword":"压力容器"},{"id":"869ecb08-d188-461b-9386-14ebc23c62cc","keyword":"爆破压强","originalKeyword":"爆破压强"},{"id":"4b33a707-b8e0-4788-8ac1-0a45912b6d7b","keyword":"发挥强度","originalKeyword":"发挥强度"}],"language":"zh","publisherId":"yhclgy200006006","title":"纤维缠绕<span style=\"color:red\">压力</span>容器爆破压强<span style=\"color:red\">计算</span>","volume":"30","year":"2000"},{"abstractinfo":"本文通过Franc3D软件,<span style=\"color:red\">计算</span>了<span style=\"color:red\">压力</span>容器表面裂纹失稳扩展的临界尺寸及不同尺寸的初始裂纹的扩展,发现当容器表面的初始椭圆形裂纹尺寸小于3 mm×20 mm及5 mm×10 mm时,在裂纹穿透壁厚之前,裂纹尖端的应力强度因子都小于<span style=\"color:red\">压力</span>容器用钢的断裂韧性KIC,故该裂纹不会发生失稳扩展,且上述两个初始裂纹穿透容器壁厚时的循环载荷次数分别为40 688、45 560次.","authors":[{"authorName":"常磊","id":"5cad8b07-9a80-46da-8ad5-440a74d42f4a","originalAuthorName":"常磊"},{"authorName":"邓春锋","id":"11959918-33cc-432e-8d93-13add6086633","originalAuthorName":"邓春锋"},{"authorName":"任方杰","id":"b5f70623-89b6-4f19-9336-04ce2fd7ec6b","originalAuthorName":"任方杰"},{"authorName":"邵飞","id":"2563acd2-7ffa-45a9-beae-a971f7cac37a","originalAuthorName":"邵飞"},{"authorName":"武春学","id":"ec7ea1e0-5420-42df-aa6f-d5dfc92ee4b1","originalAuthorName":"武春学"},{"authorName":"梅鹏程","id":"03349200-c94a-4da0-ae2b-ee31cf38ee49","originalAuthorName":"梅鹏程"}],"doi":"","fpage":"95","id":"a5327513-7b54-4729-9d7d-fd0110f5c566","issue":"5","journal":{"abbrevTitle":"CLKFYYY","coverImgSrc":"journal/img/cover/CLKFYYY.jpg","id":"10","issnPpub":"1003-1545","publisherId":"CLKFYYY","title":"材料开发与应用"},"keywords":[{"id":"38c66c26-006f-4881-95e8-8f1300ac2fd1","keyword":"数值<span style=\"color:red\">计算</span>","originalKeyword":"数值计算"},{"id":"1cdb4a07-b43b-4e98-94cf-c72139c73fc9","keyword":"疲劳裂纹扩展","originalKeyword":"疲劳裂纹扩展"},{"id":"5267bc6d-ed1c-476c-a045-60cb9ed4267a","keyword":"FRANC3D","originalKeyword":"FRANC3D"}],"language":"zh","publisherId":"clkfyyy201305021","title":"<span style=\"color:red\">压力</span>容器表面裂纹疲劳扩展的数值<span style=\"color:red\">计算</span>","volume":"28","year":"2013"},{"abstractinfo":"本文将利用RNG κ-ε湍流模型对轴流式模型水轮机进行了全流道三维非定常湍流<span style=\"color:red\">计算</span>,预测模型水轮机的<span style=\"color:red\">压力</span>脉动性能.同时,本文对轴流式模型水轮机进行了<span style=\"color:red\">压力</span>脉动试验,通过对模型水轮机<span style=\"color:red\">压力</span>脉动试验结果与数值<span style=\"color:red\">计算</span>结果的对比,以验证数值<span style=\"color:red\">计算</span>预测<span style=\"color:red\">压力</span>脉动性能的准确性和可行性.","authors":[{"authorName":"邵杰","id":"903c66ce-5338-47ba-8c0a-12989ffc45ef","originalAuthorName":"邵杰"},{"authorName":"刘树红","id":"aedfac22-192d-4d99-92f5-3d1bd623159c","originalAuthorName":"刘树红"},{"authorName":"吴墒锋","id":"d7991d4d-7ebc-4964-bb34-71dc72aa2c29","originalAuthorName":"吴墒锋"},{"authorName":"吴玉林","id":"f52d03de-ca89-4891-9fa8-d553f462d7c4","originalAuthorName":"吴玉林"}],"doi":"","fpage":"783","id":"60714b5e-fbac-4d62-8e4a-fc761cc33af5","issue":"5","journal":{"abbrevTitle":"GCRWLXB","coverImgSrc":"journal/img/cover/GCRWLXB.jpg","id":"32","issnPpub":"0253-231X","publisherId":"GCRWLXB","title":"工程热物理学报   "},"keywords":[{"id":"cb5656b8-3142-49c2-99b3-6ab1cb812bbd","keyword":"RNG κ-ε湍流模型","originalKeyword":"RNG κ-ε湍流模型"},{"id":"4bce7e02-2302-45ca-8ee8-0f5e1f06fd54","keyword":"轴流式水轮机","originalKeyword":"轴流式水轮机"},{"id":"642cf3af-4a51-44e9-ba6e-6ce31e9a45c0","keyword":"<span style=\"color:red\">压力</span>脉动","originalKeyword":"压力脉动"}],"language":"zh","publisherId":"gcrwlxb200805016","title":"轴流式模型水轮机<span style=\"color:red\">压力</span>脉动试验与数值<span style=\"color:red\">计算</span>预测","volume":"29","year":"2008"},{"abstractinfo":"把钢卷径向弹性模量作变量处理,同时考虑卷取过程中卷筒的缩径,从而建立了卷取过程钢卷内部应力分布以及卷取机卷筒单位<span style=\"color:red\">压力计算</span>的数学模型,与实际情况较吻合.","authors":[{"authorName":"白振华","id":"cc416185-8ce8-4f6d-aebc-5bd716064a72","originalAuthorName":"白振华"},{"authorName":"连家创","id":"bc58d26b-2a0c-4e32-b0fb-fe81cbc93184","originalAuthorName":"连家创"}],"doi":"10.3969/j.issn.1001-7208.2002.02.002","fpage":"6","id":"3027d750-5bc1-4e25-bebd-d5e86f8af624","issue":"2","journal":{"abbrevTitle":"SHJS","coverImgSrc":"journal/img/cover/SHJS.jpg","id":"59","issnPpub":"1001-7208","publisherId":"SHJS","title":"上海金属"},"keywords":[{"id":"4a23c740-c123-4831-af77-8896ed32c969","keyword":"钢卷","originalKeyword":"钢卷"},{"id":"943d73ff-d3c2-44f3-bac3-63697f75939d","keyword":"卷取","originalKeyword":"卷取"},{"id":"e7396fd4-697d-426f-8b8b-583c6b483e65","keyword":"应力","originalKeyword":"应力"},{"id":"5ff7fdc8-9ddb-416a-9fb9-170bb76a3b51","keyword":"卷筒","originalKeyword":"卷筒"}],"language":"zh","publisherId":"shjs200202002","title":"卷取过程中钢卷内部应力的<span style=\"color:red\">计算</span>","volume":"24","year":"2002"}],"totalpage":2470,"totalrecord":24698}