{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"The available experimental results have been summarized concerning the effect of <span style=\"color:red\">grain</span> <span style=\"color:red\">size</span> on minimum creep rate.There are two types of creep rate-<span style=\"color:red\">grain</span> <span style=\"color:red\">size</span> relations.One is that there is a criti- cal <span style=\"color:red\">grain</span> <span style=\"color:red\">size</span> above which creep rate is independent of <span style=\"color:red\">grain</span> <span style=\"color:red\">size</span>,below which creep rate increases with the decrease of <span style=\"color:red\">grain</span> <span style=\"color:red\">size</span>.The other is that there is an intermediate <span style=\"color:red\">grain</span> <span style=\"color:red\">size</span> at which creep resistance is optimum.The first relation usually occurs at higher temperatures(>0.5 T_m),and intermediate stress ranges,while the second relation at interme- diate temperature ranges(0.4-0.5 T_m)and higher stresses.For the two types of creep rate-<span style=\"color:red\">grain</span> <span style=\"color:red\">size</span> relations,the increase of the creep rates with the de- crease of <span style=\"color:red\">grain</span> <span style=\"color:red\">size</span> for small <span style=\"color:red\">grain</span> sizes is all due to <span style=\"color:red\">grain</span> boundary sliding.For large <span style=\"color:red\">grain</span> sizes,a dis- location climb mechanism is dominant in creep deformation for the first relation,while a Hall-Perch <span style=\"color:red\">grain</span> boundary strengthening effect is believed to play an important role by dislocation glide mechanism for the second relation.","authors":[{"authorName":"LI Pei'en ** Institute of Materials Science and Engineering","id":"e40c6329-7ed8-44a4-9890-2e14279f7bf8","originalAuthorName":"LI Pei'en ** Institute of Materials Science and Engineering"},{"authorName":"Shanghai Jiaotong University","id":"4361bd10-f54c-458e-b92a-b3320afa646f","originalAuthorName":"Shanghai Jiaotong University"},{"authorName":"Shanghai 200030","id":"2fdc20e7-ebab-4e6a-9c6d-31b9cb1ff9ed","originalAuthorName":"Shanghai 200030"},{"authorName":"China+ To whom correspondence should be addressed.","id":"39b14400-db67-4e4f-8312-986dcdb02167","originalAuthorName":"China+ To whom correspondence should be addressed."}],"categoryName":"|","doi":"","fpage":"119","id":"20a0a2c9-cbbe-4323-a9bb-da5fdff60672","issue":"2","journal":{"abbrevTitle":"CLKXJSY","coverImgSrc":"journal/img/cover/JMST.jpg","id":"11","issnPpub":"1005-0302 ","publisherId":"CLKXJSY","title":"材料科学技术（英文）"},"keywords":[{"id":"0075c70d-ed70-4b02-9753-7bbaa31fd532","keyword":"<span style=\"color:red\">grain</span> <span style=\"color:red\">size</span>","originalKeyword":"grain size"},{"id":"e5abcdfc-2374-49d6-9672-f9facd6c3650","keyword":"null","originalKeyword":"null"}],"language":"en","publisherId":"1005-0302_1992_2_1","title":"On <span style=\"color:red\">Grain</span> <span style=\"color:red\">Size</span> Dependence of Minimum Creep Rate","volume":"8","year":"1992"},{"abstractinfo":"Most of the available methods for the calculation of the three dimensional(3D)<span style=\"color:red\">grain</span> <span style=\"color:red\">size</span> dis- tribution functions(SDF)are based on the S model and lead a grave systematical error.The origin is the basic supposition of spherical grains in the S model,which does not correspond with the feature of real grains.A new model called A model is developed based on the hypothe- sis of polvhedral grains.The probability functions of the A model and the method to calculate the 3D SDFs using the A model are given in the present paper.The theoretical analyses and experimental tests have demonstrated that the A model reduces the systematical error radical- ly.It is nearly as simple as the so far used S model,but gives much better results in repro- ducing of 3D SDFs from the measured ID or 2D SDFs.","authors":[{"authorName":"ZHAO Xinbing Zhejiang University","id":"766bfdbe-57d1-40ed-9cb9-0bc202f5e03e","originalAuthorName":"ZHAO Xinbing Zhejiang University"},{"authorName":"Hangzhou","id":"e0b83e8d-04a8-4b87-9ee1-4317f78b0ec8","originalAuthorName":"Hangzhou"},{"authorName":"China LCKEK Institut fur Metallkunde und Metallphysik der RWTH Aachen","id":"0964ed3c-b604-4b91-b21c-4bdbcf831092","originalAuthorName":"China LCKEK Institut fur Metallkunde und Metallphysik der RWTH Aachen"},{"authorName":"Germany Department of Materials Scicnce and Engineering","id":"4aa8b533-9334-4fa7-8146-6db319bcccbe","originalAuthorName":"Germany Department of Materials Scicnce and Engineering"},{"authorName":"Zhejiang Univer sity","id":"39140f88-a313-46cf-8ce1-edde87113a2e","originalAuthorName":"Zhejiang Univer sity"},{"authorName":"Hangzhou 310027","id":"1952b435-1018-49ed-a4ee-6bd0e714e305","originalAuthorName":"Hangzhou 310027"},{"authorName":"China","id":"070d05bb-bb1f-478a-aeb4-62baec504081","originalAuthorName":"China"}],"categoryName":"|","doi":"","fpage":"46","id":"69b2de51-b754-42da-81c8-a25b0f14d0e6","issue":"1","journal":{"abbrevTitle":"JSXBYWB","coverImgSrc":"journal/img/cover/amse.jpg","id":"49","issnPpub":"1006-7191","publisherId":"JSXBYWB","title":"金属学报(英文版)"},"keywords":[{"id":"5a875055-f398-400a-812b-b687f7adfa6a","keyword":"<span style=\"color:red\">grain</span> <span style=\"color:red\">size</span>","originalKeyword":"grain size"},{"id":"2ac6d4fe-89b5-4ef0-8da0-897a255a775b","keyword":"null","originalKeyword":"null"},{"id":"7c057482-4503-49df-8a3e-c73abe16c070","keyword":"null","originalKeyword":"null"},{"id":"4ff246ab-ca1e-46b4-ad61-30c21e699fa2","keyword":"null","originalKeyword":"null"}],"language":"en","publisherId":"1006-7191_1993_1_4","title":"GEOMETRIC MODEL AND APPLIED METHOD FOR THE CALCULATION OF <span style=\"color:red\">GRAIN</span> <span style=\"color:red\">SIZE</span> DISTRIBUTIONS","volume":"6","year":"1993"},{"abstractinfo":"In order to achieve the optimum conditions for electroplating nanocrystalline nickel coating from Watts-type bath, the effect of some process parameters namely, bath temperature, current density, and saccharin addition on <span style=\"color:red\">grain</span> <span style=\"color:red\">size</span> and texture coefficient (TC= <em>I</em><sub>(200)</sub> /<em>I</em><sub>(111)</sub> ) of the deposits were investigated by X-ray diffraction<br />\n(XRD). The results showed that in a bath containing 5 g/L saccharin, by increasing the bath temperature from 45&deg;C to 55&deg;C, the <span style=\"color:red\">grain</span> <span style=\"color:red\">size</span> decreased, whereas further increase of bath temperature resulted in a contrary effect. By increasing the current density from 10 to 75 mA/cm<sup>2</sup>, both the <span style=\"color:red\">grain</span> <span style=\"color:red\">size</span> and TC decreased, while further increase in current density had no significant effect on the <span style=\"color:red\">grain</span> <span style=\"color:red\">size</span>. At a given current density, the <span style=\"color:red\">grain</span> <span style=\"color:red\">size</span> and TC decreased rapidly by increasing the saccharin content before leveling off at 3 g/L of saccharin. Finally, based on the <span style=\"color:red\">grain</span> refining the optimum conditions for producing nanocrystalline nickel coating from Watts-type bath have been proposed.","authors":[{"authorName":"A.M. Rashidi A. Amadeh","id":"1718fce8-5f0d-405c-9012-f33aa093f793","originalAuthorName":"A.M. Rashidi A. Amadeh"}],"categoryName":"|","doi":"","fpage":"82","id":"59aa3698-2590-4ed5-a27a-af48e08fc560","issue":"1","journal":{"abbrevTitle":"CLKXJSY","coverImgSrc":"journal/img/cover/JMST.jpg","id":"11","issnPpub":"1005-0302 ","publisherId":"CLKXJSY","title":"材料科学技术（英文）"},"keywords":[{"id":"85909cdb-7322-422b-b641-d09a92e24c82","keyword":"Electroplating","originalKeyword":"Electroplating"},{"id":"b7dcadf5-1307-4494-87ea-140ae100114e","keyword":"<span style=\"color:red\">grain</span> <span style=\"color:red\">size</span>","originalKeyword":"grain size"},{"id":"a453f604-cfe3-4ec5-82b0-34d6d285cc2a","keyword":"Nanocrystalline Coating","originalKeyword":"Nanocrystalline Coating"}],"language":"en","publisherId":"1005-0302_2010_1_6","title":"Effect of Electroplating Parameters on Microstructure of Nanocrystalline Nickel Coatings","volume":"26","year":"2010"},{"abstractinfo":"Through combining an experimental investigation on the isothermal nanocrystallization thermodynamics of bulk amorphous selenium and a theoretical analysis, an easy and reliable way to derive the lower <span style=\"color:red\">grain-size</span> limit of polycrystalline materials was proposed. The <span style=\"color:red\">grain-size</span> limit for the polycrystalline selenium was determined to be about 4.0 nm. [S0163-1829(99)00310-0].","authors":[],"categoryName":"|","doi":"","fpage":"5987","id":"f18173b0-fcc2-41bd-9c70-0dce5999989e","issue":"9","journal":{"abbrevTitle":"PRB","id":"41d73232-e732-4216-a5f7-4b352bb955cf","issnPpub":"0163-1829","publisherId":"PRB","title":"Physical Review B"},"keywords":[{"id":"b9efce56-44d7-4180-a917-c7165eb332ac","keyword":"nanocrystalline materials;transition;silicon","originalKeyword":"nanocrystalline materials;transition;silicon"}],"language":"en","publisherId":"0163-1829_1999_9_1","title":"<span style=\"color:red\">Grain-size</span> limit of polycrystalline materials","volume":"59","year":"1999"},{"abstractinfo":"The effect of electric current pulses (ECP) on <span style=\"color:red\">grain</span> <span style=\"color:red\">size</span> in castings is considered. The relationship between <span style=\"color:red\">grain</span> <span style=\"color:red\">size</span> and electric current density is revealed. Numerical calculation shows that an electric current density with a magnitude of 10(3) A/cm(2) is needed to reduce the <span style=\"color:red\">grain</span> <span style=\"color:red\">size</span> by one order of magnitude for some pure metals, such as Ni, Sn, Pb, Cu, and Fe. The effects of Joule heating, skin, and pinch force are proved to be of lesser importance. The theory gives a good explanation for the experimental results reported by Conrad and co-workers.","authors":[],"categoryName":"|","doi":"","fpage":"77","id":"3009dcc2-c55b-43ed-a7cb-fe0e27beaef3","issue":"1","journal":{"abbrevTitle":"IJONP","id":"271e056f-652b-4524-9953-a84e4f1f2e41","issnPpub":"1368-9290","publisherId":"IJONP","title":"International Journal of Non-Equilibrium Processing"},"keywords":[{"id":"b7302d9f-99e5-4638-ada9-7635554a3578","keyword":"electric current pulse;<span style=\"color:red\">grain</span> <span style=\"color:red\">size</span>;nanocrystalline;conductors","originalKeyword":"electric current pulse;grain size;nanocrystalline;conductors"}],"language":"en","publisherId":"1368-9290_1998_1_1","title":"Effect of electric current pulses on <span style=\"color:red\">grain</span> <span style=\"color:red\">size</span> in castings","volume":"11","year":"1998"},{"abstractinfo":"Molecular dynamics simulations of high temperature annealing of copper bicrystals\nhave been carried out. The bicrystals have planar <span style=\"color:red\">grain</span> boundaries, and the gain\n<span style=\"color:red\">size</span> varies in nano range. An EAM(Embedded Atom Method) potential of FS type is\nused for calculating the interatomic forces. The results show that in nanocrystalline\ncopper, GB migration driven by inter-GB reaction can take place. A critical <span style=\"color:red\">grain</span>\n<span style=\"color:red\">size</span> is identi&macr;ed, below which the inter-GB reaction becomes strong enough to trigger\nGB motion, which accelerates rapidly and leads to annihilation of the <span style=\"color:red\">grain</span> bound-\naries. The critical <span style=\"color:red\">size</span> is found to be 16 atomic radii. A \\through intermediate <span style=\"color:red\">grain</span>\nmechanism\" is identi&macr;ed for the nano-<span style=\"color:red\">grain</span> boundary motion observed, which is never\nreported for GB migrations of conventional polycrystalline metals.","authors":[{"authorName":"L. Zhou","id":"c0825789-e9aa-4a18-96db-3698c0aee526","originalAuthorName":"L. Zhou"},{"authorName":" X.Q. Wei ","id":"c935e434-9cc3-406c-86f2-045ee26d57f9","originalAuthorName":" X.Q. Wei "},{"authorName":"  N.G. Zhou","id":"3c943edc-f333-4db1-b9b3-b05835359f81","originalAuthorName":"  N.G. Zhou"}],"categoryName":"|","doi":"","fpage":"11","id":"bb9da047-ae41-4b7e-a2cf-26f92fe83c1b","issue":"1","journal":{"abbrevTitle":"JSXBYWB","coverImgSrc":"journal/img/cover/amse.jpg","id":"49","issnPpub":"1006-7191","publisherId":"JSXBYWB","title":"金属学报(英文版)"},"keywords":[{"id":"f405a00d-40fc-4d0f-a5a3-9e36504b8d0b","keyword":"<span style=\"color:red\">grain</span> boundary migration","originalKeyword":"grain boundary migration"},{"id":"5934a7fa-371b-480f-9323-165f355879b1","keyword":"null","originalKeyword":"null"},{"id":"827485dd-e9d7-42d9-8e6e-b0b92acdaadf","keyword":"null","originalKeyword":"null"}],"language":"en","publisherId":"1006-7191_2004_1_18","title":"NANO <span style=\"color:red\">SIZE</span> EFFECT IN <span style=\"color:red\">GRAIN</span> BOUNDARY MIGRATION OF COPPER","volume":"17","year":"2004"},{"abstractinfo":"The relation between <span style=\"color:red\">grain</span> <span style=\"color:red\">size</span> and strength of the duplex stainless steels and influence of <span style=\"color:red\">grain</span> <span style=\"color:red\">size</span> on properties of hydrogen induced cracking in these steels have been investigated. The Hall-Petch relation between <span style=\"color:red\">grain</span> <span style=\"color:red\">size</span> and strength of the steels is also followed.The susceptibility to hydrogen induced cracking of the steels increases with increasing <span style=\"color:red\">grain</span> <span style=\"color:red\">size</span>.","authors":[{"authorName":"HE Jianhong Huazhong University of Science and Technology","id":"b23296da-2d44-4d31-a7f1-276af2f64c6b","originalAuthorName":"HE Jianhong Huazhong University of Science and Technology"},{"authorName":"Wuhan","id":"fe8eba65-88a2-4101-a8db-88e38ab66ce4","originalAuthorName":"Wuhan"},{"authorName":"ChinaTANG Xiangyun CHEN Nanping Tsinghua University","id":"f3f44811-838f-499f-9f47-b31601af07fe","originalAuthorName":"ChinaTANG Xiangyun CHEN Nanping Tsinghua University"},{"authorName":"Beijing","id":"d3c3c3df-1d39-4a3b-a871-1830568d169b","originalAuthorName":"Beijing"},{"authorName":"China Dept.of Materials Science and Engineering","id":"55e7924c-0b51-43ea-9000-1ca4e912ef52","originalAuthorName":"China Dept.of Materials Science and Engineering"},{"authorName":"Huazhong University of Science and Technology","id":"44dd275d-5571-46fb-940b-d0c796774c69","originalAuthorName":"Huazhong University of Science and Technology"},{"authorName":"Wuhan 430074","id":"a8baaa13-a4ae-4652-bb56-80f95d2fda99","originalAuthorName":"Wuhan 430074"},{"authorName":"China","id":"4f8b35e3-dfe3-4146-8997-6392a1439ab2","originalAuthorName":"China"}],"categoryName":"|","doi":"","fpage":"21","id":"e92c986d-484b-40af-a6b0-3097fe230533","issue":"1","journal":{"abbrevTitle":"JSXBYWB","coverImgSrc":"journal/img/cover/amse.jpg","id":"49","issnPpub":"1006-7191","publisherId":"JSXBYWB","title":"金属学报(英文版)"},"keywords":[{"id":"2e953c1b-41ba-4e28-8154-c70ef499c5a6","keyword":"duplex stainless steel","originalKeyword":"duplex stainless steel"},{"id":"55b03711-4be2-4904-b9c5-88c6f2b0a29a","keyword":"null","originalKeyword":"null"},{"id":"07a7addf-1c94-4d20-a629-11bf690f7e09","keyword":"null","originalKeyword":"null"}],"language":"en","publisherId":"1006-7191_1991_1_7","title":"INFLUENCE OF <span style=\"color:red\">GRAIN</span> <span style=\"color:red\">SIZE</span> ON STRENGTH AND HYDROGEN INDUCED CRACKING OF DUPLEX STAINLESS STEELS","volume":"4","year":"1991"},{"abstractinfo":"Porosity-free nanocrystalline element selenium (nc-Se) samples with the mean <span style=\"color:red\">grain</span> sizes ranging from 8 to 70 nm were: synthesized by complete crystallization of the melt-quenched amorphous Se solid. Mechanical properties including microhardness (H-nu) and elastic modulus (E) of the nc-Se samples were measured by means of nanoindentation tests and microhardness tests, respectively. With a reduction of <span style=\"color:red\">grain</span> <span style=\"color:red\">size</span>, the nc-Se samples were found to be substantially hardened. But the <span style=\"color:red\">grain</span> <span style=\"color:red\">size</span> dependence of H-nu does not follow a simple Hall-Fetch relation over the whole <span style=\"color:red\">grain</span> <span style=\"color:red\">size</span> range, exhibiting three distinct stages corresponding to three different Hall-Fetch slopes. The maximum Hall-Fetch slope was found to be in the <span style=\"color:red\">grain</span> <span style=\"color:red\">size</span> range of 15-20 nm, corresponding to large values of the: elastic modulus. This behavior can be explained in terms of the lattice distortion in the nc-Se samples that was experimentally determined by using quantitative x-ray diffraction measurements. A conclusion is drawn that the lattice structure of the nm-sized crystallites may play an important role in mechanical properties of nanocrystalline materials.","authors":[],"categoryName":"|","doi":"","fpage":"923","id":"1b9b6f6a-4171-4125-9f0d-7cbdd2c09eaf","issue":"4","journal":{"abbrevTitle":"JOMR","id":"155c387a-c8cb-4083-85f3-6b58aeef4116","issnPpub":"0884-2914","publisherId":"JOMR","title":"Journal of Materials Research"},"keywords":[{"id":"5c853508-96a7-4689-b7b3-7fd0c434173d","keyword":"hall-petch relationship;behavior;alloys;cu;ni;pd","originalKeyword":"hall-petch relationship;behavior;alloys;cu;ni;pd"}],"language":"en","publisherId":"0884-2914_1997_4_3","title":"<span style=\"color:red\">Grain</span> <span style=\"color:red\">size</span> dependence of mechanical properties in nanocrystalline selenium","volume":"12","year":"1997"},{"abstractinfo":"The apparent activation energy of serrated yielding was measured by two different methods for a commercial brass H68.The results showed that the apparent activation energy of serrat- ed yielding measured by a method involving(m+β)values increases with the <span style=\"color:red\">grain</span> <span style=\"color:red\">size</span>.In contrast,those measured by another method without involving(m+β)values are all the same for specimens with different <span style=\"color:red\">grain</span> sizes.Combining with the observation of the microstructures,the above phenomena have been explained.The method to measure the true activation energy of serrated yielding has also been proposed.","authors":[{"authorName":"XIAO Lingang QIAN Kuangwu Fuzhou University","id":"6effe586-fe16-479c-9232-a7b315419c69","originalAuthorName":"XIAO Lingang QIAN Kuangwu Fuzhou University"},{"authorName":"Fuzhou","id":"ecc99091-a13f-40f4-b5e3-b4080feede7d","originalAuthorName":"Fuzhou"},{"authorName":"Fujian","id":"c73ffeaa-cba7-4391-9adc-a65fe0f23bb7","originalAuthorName":"Fujian"},{"authorName":"China Correspondent:QIAN Kuangwu Professor","id":"b2abc6f0-a554-4bdc-ad9c-fe19f0777f9b","originalAuthorName":"China Correspondent:QIAN Kuangwu Professor"},{"authorName":"Institute for Materials Research","id":"e3452c80-586d-4e24-aeec-fdcbd75f8e3f","originalAuthorName":"Institute for Materials Research"},{"authorName":"Fuzhou University Fuzhou","id":"a121f785-d7fb-45fc-bd83-591607c58f4f","originalAuthorName":"Fuzhou University Fuzhou"},{"authorName":"Fujian 350002","id":"a8430d21-4910-41b9-a3fe-6b1a0b55ac30","originalAuthorName":"Fujian 350002"},{"authorName":"China","id":"5ad3352d-9f98-4d76-9633-1151d2b651e7","originalAuthorName":"China"}],"categoryName":"|","doi":"","fpage":"10","id":"3cafe7b8-c569-4ad4-9cbd-457ee70d3ea0","issue":"1","journal":{"abbrevTitle":"JSXBYWB","coverImgSrc":"journal/img/cover/amse.jpg","id":"49","issnPpub":"1006-7191","publisherId":"JSXBYWB","title":"金属学报(英文版)"},"keywords":[{"id":"37b87ca3-8f46-4996-92f2-ba2e2472fc13","keyword":"serrated yielding","originalKeyword":"serrated yielding"},{"id":"7409eacc-5129-4adf-b005-4f0df7fc473b","keyword":"null","originalKeyword":"null"},{"id":"4cc28b91-e5a8-48cd-b7b7-7adf713e91d0","keyword":"null","originalKeyword":"null"},{"id":"888cde9c-b7fa-4e39-b990-219918bc0e37","keyword":"null","originalKeyword":"null"}],"language":"en","publisherId":"1006-7191_1990_1_9","title":"<span style=\"color:red\">GRAIN</span> <span style=\"color:red\">SIZE</span> AND ACTIVATION ENERGY OF SERRATED YIELDING","volume":"3","year":"1990"},{"abstractinfo":"To promote effectively dynamic recrystallization and obtain a homogeneous distribution of ultrafine <span style=\"color:red\">grain</span> <span style=\"color:red\">size</span> in strip finish rolling process, the behavior of static and dynamic recrystallization must be appropriately designed to provide an ultrafine austenite microstructure without mixed <span style=\"color:red\">grain</span> <span style=\"color:red\">size</span>. The design of rolling schedule was analyzed based on the control of the recrystallization behavior to achieve ultrafine <span style=\"color:red\">grain</span> <span style=\"color:red\">size</span> in the strip rolling process of niobium microalloyed steel. The experimental simulations were presented to validate the twice dynamic recrystallization design to achieve ultrafine <span style=\"color:red\">grain</span> <span style=\"color:red\">size</span> control.","authors":[{"authorName":"ZHU Guohui","id":"5ef0b3d9-55b3-46f2-bed8-1e5224ab2ce3","originalAuthorName":"ZHU Guohui"},{"authorName":"S V Subramanian","id":"cfc6e6d3-1a07-4295-8f24-90a3855b8ea2","originalAuthorName":"S V Subramanian"}],"categoryName":"|","doi":"","fpage":"39","id":"e8a57991-df7f-422d-8b80-c42f5a10406d","issue":"1","journal":{"abbrevTitle":"GTYJXBYWB","coverImgSrc":"journal/img/cover/GTYJXBEN.jpg","id":"1","issnPpub":"1006-706X","publisherId":"GTYJXBYWB","title":"钢铁研究学报(英文版)"},"keywords":[{"id":"6fbac10c-ad5a-427c-941b-a0f8a06f698e","keyword":"twice dynamic recrystallization;critical strain;dynamic recrystallization;ultrafine <span style=\"color:red\">grain</span> <span style=\"color:red\">size</span>","originalKeyword":"twice dynamic recrystallization;critical strain;dynamic recrystallization;ultrafine grain size"}],"language":"en","publisherId":"1006-706X_2008_1_19","title":"Recrystallization Behavior Design for Controlling <span style=\"color:red\">Grain</span> <span style=\"color:red\">Size</span> in Strip Rolling Process","volume":"15","year":"2008"}],"totalpage":302,"totalrecord":3015}