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Frontiers of Mechanical Engineering

ISSN 2095-0233

ISSN 2095-0241(Online)

CN 11-5984/TH

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2018 Impact Factor: 0.989

Front Mech Eng    2011, Vol. 6 Issue (3) : 277-286    https://doi.org/10.1007/s11465-011-0234-y
RESEARCH ARTICLE
Separation mechanism for double cylinder with shrink fitting system used for ceramics conveying rollers
Wenbin LI(), Hiromasa SAKAI, Shota HARADA, Yasushi TAKASE, Nao-Aki NODA
Department of Mechanical Engineering, Kyusyu Institute of Technology, Fukuoka 804-8550, Japan
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Abstract

Steel conveying rollers used in hot rolling mills must be exchanged frequently at great cost because hot conveyed strips induce wear and deterioration on the surface of roller in short periods. In previous studies, new roller structure was considered which has a ceramics sleeve connected with two steel shafts at both ends by shrink fitting. Here, although the ceramics sleeve can be used for many years, the steel shafts sometimes have to be exchanged for maintenance and reconstruction under the corrosive atmosphere. Since the thermal expansion coefficient of steel is about five times larger than that of ceramics, it is necessary to investigate how to separate the shrink fitting system by heating outside of sleeve and cooling inside of the shaft. Although how to separate the real roller has been discussed in the previous study, the separation mechanism has not been clarified yet. Therefore, in this study, several types of more fundamental models are investigated to understand the separation mechanism of real roller by the application of the finite element method. The results may be useful for designs of new rollers.

Keywords contact      ceramics      thermal stress      heating      finite element method     
Corresponding Author(s): LI Wenbin,Email:wenbin-li@hotmail.com   
Issue Date: 05 September 2011
 Cite this article:   
Wenbin LI,Hiromasa SAKAI,Shota HARADA, et al. Separation mechanism for double cylinder with shrink fitting system used for ceramics conveying rollers[J]. Front Mech Eng, 2011, 6(3): 277-286.
 URL:  
https://academic.hep.com.cn/fme/EN/10.1007/s11465-011-0234-y
https://academic.hep.com.cn/fme/EN/Y2011/V6/I3/277
Fig.1  Layout of conveying rollers
Fig.2  Roller structure. (a) Conventional roller; (b) shrink fitting roller; (c) new shrink fitting roller (model A); (d) new shrink fitting roller (model B or real roller model)
Fig.3  Double cylinder model
Fig.4  Model A initially considered. (a) Dimensions (mm); (b) boundary condition
Fig.5  Atmosphere temperature
Fig.6  Real roller model with coordinate (mm)
Heat (Forced convection, Radiation)r=135, z=590-800 α=50 W/(m2·K)?=0.4
Water cool (Forced convection)r=75, z=±590-800 r=20-75, z=±800-1150=1.163×104 W/(m2·K) ?=0
Air cool (Natural convection)r=105, z=0-±590 r=135, z=0-±590 r=75-105, z=±590 r=105-135, z=±800 r=50-105, z=±800-1150 (Shaft out side surface)=50 W/(m2·K)?=0
Insulationr=105-135, z=0 r=20-50, z=±1150
Tab.1  Values of heat transfer coefficient and emissivity along the , (mm) coordinate in Fig. 6
Fig.7  Double cylinder models with 5 different boundary conditions. (a) Dimensions (mm); (b) thermal boundary condition; (c) mechanical boundary condition
Fig.8  Double cylinder model with coordinate (mm)
Heat (Forced convection, radiation)r=135, z=±0-210 α=50 W/(m2·K) ?=0.4
Water cool (Forced convection)r=105, z=±0-210 α=1.163×104 W/(m2·K) ?=0
Insulationr=75-135, z=0,210
Tab.2  Values of heat transfer coefficient and emissivity along the , (mm) coordinate in Fig. 8
Ceramics HSteel (HV200)
Young’s modulus/Gpa300210
Poisson’s ratio0.280.3
Tensile strength/MPa500600
Mass density/(kg·m-3)32007800
T.hermal conductivity/(W·m-1K-1)62.5(393 K) 12.5(1273 K)25
Thermal expansion coefficient/K-13.0×10-61.45×10-5
Specific heat/(J·kg-1·K-1)680477
Emissivity0.40.4
Tab.3  Material properties
Fig.9  three atmosphere temperature
Fig.10  Time vs / for three atmosphere temperature
Fig.11  Separation history of contact area
Fig.12  Temperature distribution along contact area when 5000 s
Fig.13  along the contact area
Fig.14  along the contact area
Modelsδ/d (×10-3)
0.10.20.3
1.6219282
11954045No separation
No separation
Tab.4  Separation finishing time (s) (models 1, 2, 3)
Fig.15  Temperature along contact area when 5000 s. (a) Model 4; (b) model 5
Fig.16  along the contact area. (a) Model 4; (b) model 5
Fig.17  along the contact area. (a) Model 4; (b) model 5
Fig.18  Thermal deformation of steel single cylinder model (magnification of displacement: 50 mm)
Fig.19  Thermal deformation of double cylinder model (magnification of displacement: 50 mm). (a) Model 4; (b) model 5
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