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Online since: February 2013
Authors: A.M. Lider, E.V. Berezneeva, N.S. Pushilina, Ekaterina N. Stepanova, Ivan P. Chernov, S.V. Ivanova
Berezneeva 1,c, A.M.
Lider 1,d, I.
Fig. 1.
References [1] D.I.
Yang, Nanocrystalline and amorphous surface structure of 0.45%C steel produced by high current pulsed electron beam, Mater SCI. 41 (2006) 479-483
Lider 1,d, I.
Fig. 1.
References [1] D.I.
Yang, Nanocrystalline and amorphous surface structure of 0.45%C steel produced by high current pulsed electron beam, Mater SCI. 41 (2006) 479-483
Online since: January 2010
Authors: Zhuang Qi Hu, Xiao Feng Sun, Wen Zhen Wang, Tao Jin
The as-cast γ' morphology is shown in Fig. 1.
The incipient melting point and the heat treatment process is indicated in Table 1.
If the cuboidal γ' is forced to obtain, its edge length will exceed 1µm causing adverse effect on mechanical properties.
References [1] K.A.A1-Jarba, G.E.Fuchs: Mater.
A 479 (2008) 148-156 [7] D.Blavette, P.Caron, T.Khan: Scripta Mater. 20 (1986) 1395-1400 [8] D.Blavette, P.Caron, T.Khan: Superalloys 1988.
The incipient melting point and the heat treatment process is indicated in Table 1.
If the cuboidal γ' is forced to obtain, its edge length will exceed 1µm causing adverse effect on mechanical properties.
References [1] K.A.A1-Jarba, G.E.Fuchs: Mater.
A 479 (2008) 148-156 [7] D.Blavette, P.Caron, T.Khan: Scripta Mater. 20 (1986) 1395-1400 [8] D.Blavette, P.Caron, T.Khan: Superalloys 1988.
Online since: March 2017
Authors: Alan Iacopi, Dzung Viet Dao, Sima Dimitrijev, Ji Sheng Han, Afzaal Qamar, Toan Dinh, Hoang Phuong Phan
Figure 1(b) shows the rocking curve of 3C-SiC(200) peak with FWHM value of 1.47o which is a reasonable value for such a thin film.
Figure 1: XRD curve of the n-type 3C-SiC on Si(100) in conventional θ-2θ mode; (b) Rocking curve of the 3C-SiC(200) peak.
References [1].
Noraini Marsi, Burhanuddin Yeop Majlis, Azrul Azlan Hamzah, Faisal Mohd-Yasin: Energy Procedia, Volume 68 (2015), pp. 471-479
Rev., vol. 1 (2014), pp. 031301
Figure 1: XRD curve of the n-type 3C-SiC on Si(100) in conventional θ-2θ mode; (b) Rocking curve of the 3C-SiC(200) peak.
References [1].
Noraini Marsi, Burhanuddin Yeop Majlis, Azrul Azlan Hamzah, Faisal Mohd-Yasin: Energy Procedia, Volume 68 (2015), pp. 471-479
Rev., vol. 1 (2014), pp. 031301
Online since: June 2015
Authors: R. Srinivasan, M. Saravanan, S. Paul Singarayar, S. Joseph Dominic Vijayakumar
Paul Singarayar 4, d
1 Principal, Sri Subramanya college of Engineering & Technology, Palani, India
Table 1-3. lists the twelve different benchmark problems and the average RPD value for 10 different instances and the same plotted in the Fig 1-3.
Table 1.
References [1] K.
Maroto, A comprehensive review and evaluation of permutation flow shop heuristics, European Journal of Operational Research, 165 (2005) 479-494
Table 1-3. lists the twelve different benchmark problems and the average RPD value for 10 different instances and the same plotted in the Fig 1-3.
Table 1.
References [1] K.
Maroto, A comprehensive review and evaluation of permutation flow shop heuristics, European Journal of Operational Research, 165 (2005) 479-494
Online since: February 2013
Authors: Zhen Chen, Ling Yue Lv, Wen Hua Song, Fei Xie
The application and analysis of the risk assessment model
about BLEVE accident
Fei Xie1,2,a, Wen-hua Song1,b, Zhen Chen1,c,Ling-yue Lv1,d
1.Environment and Chemistry College, Tianjin Polytechnical Univeisity, Tianjin China
2.Tianjin City Public Security Fire Station, Hexi District Fire Brigade, Tianjin, China
ae-mail:xiefei820818@126.com
be-mail: songwenhuateam@sina.com
ce-mail: chenzhen3419@126.com
de-mail: yiqiandshowlove@126.com
Keywords:BLEVE; TNT equivalent method; 1,2-dichloropropane tank area; risk assessment; overpressure wave;
Abstract:The flammable vapor pressure inside the combustible liquid storage tanks in the fire environment elevates, and the of the tank wall the yield strength of enduring the heat decreases, which cause the collapse to occur soon, resulting in the happen of BLEVE.
The dike in the tank area is about 40meters long and 10 meters wide, 1 meter high, with the cover area of approximately 400m2.
REFERENCES [1] WuZongzhi.
[3] A.Wolf,Bleve kills two,NFPA J.92(6)(1998)1-8
[6] H.J.Chen,M.H.Lin,Modeling a boiling liquid expanding vapor explosion phenomenon with application to relief device design for liquefied ammonia storage,Ind.Eng.Chem.Res.38(1999)479–487
The dike in the tank area is about 40meters long and 10 meters wide, 1 meter high, with the cover area of approximately 400m2.
REFERENCES [1] WuZongzhi.
[3] A.Wolf,Bleve kills two,NFPA J.92(6)(1998)1-8
[6] H.J.Chen,M.H.Lin,Modeling a boiling liquid expanding vapor explosion phenomenon with application to relief device design for liquefied ammonia storage,Ind.Eng.Chem.Res.38(1999)479–487
Online since: October 2020
Authors: Svetlana Khashirova, Elina V. Khakyasheva, Albert S. Shabaev, Ruslan A. Shetov
Composition of studied samples PEEK + Hostаnox P-EPQ
Sample number
Composition
1
PEEK
2
PEEK + 0.5 % of Hostаnox P-EPQ
3
PEEK + 1 % of Hostаnox P-EPQ
4
PEEK + 1.5 % of Hostаnox P-EPQ
5
PEEK +2 % of Hostаnox P-EPQ
The study of the thermal-oxidative stability of the samples under in an oxygen medium showed that the amount of absorbed oxygen decreases significantly with increasing stabilizer concentration (Fig. 1).
Fig. 1.
References [1] A.S.
Stab. 91 (2006) 479
Jiang, Synthesis and thermal crosslinking behavior of poly(aryl ether ketone)s containing 1,4-naphthalene moieties, Chem.
Fig. 1.
References [1] A.S.
Stab. 91 (2006) 479
Jiang, Synthesis and thermal crosslinking behavior of poly(aryl ether ketone)s containing 1,4-naphthalene moieties, Chem.
Online since: March 2018
Authors: Radu G. Saulescu, Radu Velicu, Mihai Tiberiu Lates
In [4] is presented a comparative analysis for two wheels profiles (ISO 1395-1977 and ANSI ASA B29.1-1950) for a bush chain transmission.
By considering z = 60, the wheel’s profile geometrical parameters are determined (figure 1).
Table 1 presents the numerical values of the wheel’s geometry.
References [1] Sergeev, S.
Mechanisms and Machine Science 18 (2013) 471-479
By considering z = 60, the wheel’s profile geometrical parameters are determined (figure 1).
Table 1 presents the numerical values of the wheel’s geometry.
References [1] Sergeev, S.
Mechanisms and Machine Science 18 (2013) 471-479
Online since: March 2014
Authors: Mirosław M. Bućko, Jakub Domagała, Radosław Lach
The bed, once the reaction completed, was ground in a jaw crushed and sieved through a sieve with 1 mm sieve mesh.
After 15 days (360 h), the compacts were sintered at 1,750°C for 1 min in nitrogen flow.
Fig. 1.
References [1] J.W.
Soc. 62 (1979) 476-479
After 15 days (360 h), the compacts were sintered at 1,750°C for 1 min in nitrogen flow.
Fig. 1.
References [1] J.W.
Soc. 62 (1979) 476-479
Online since: February 2006
Authors: Manabu Enoki, Satoshi Nishinoiri
Application of Laser AE to Microfracture at Elevated Temperature
1
Enoki, M. and 2Nishinoiri, S.
1
Department of Materials Engineering, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo
113-8656, Japan,
2
Central Research Institute of Electric Power Industry, 2-11-1 Iwadokita, Komae-shi, Tokyo
201-8511, Japan,
enoki@rme.mm.t.u-tokyo.ac.jp, s-nishi@criepi.denken.or.jp
Keywords: Laser Interferometer, Microfracture, In-process monitoring
Abstract.
The experimental setup of in-process monitoring system is shown in Fig.1.
However, no AE could be detected in a specimen (No.1) in which maximum principal stress did not exceed the value of 45 MPa.
Typical AE behavior during cooling period after plasma spraying 0 20 40 60 80 10003 0 06 0 0 0 20 40 60 80 10003 0 06 0 0 Time, t / s Stress, σ/ MPa First AE No.6 No.5 No.4 No.3 No.2 No.1 Fig. 4.
References Enoki, M., Nishinoiri, S., Seki, T. and Kishimoto, A. (2004) "Non-contact measurement of acoustic emission in thin specimen by laser interferometer", Key Engineering Materials, Vol. 270-273, pp. 485-490 Enoki, M., Watanabe, M., Chivavibul, P. and Kishi, T. (2000) "Non-contact Measurement of Acoustic Emission in Materials by Laser Interferometry", Science and Technology of Advanced Materials, Vol. 1, No.3, pp. 157-165 Nagahisa, K., Iwamoto, K., Shinozaki, K., Sasaki, G., Enoki, M. and Yoshida, M. (2004) "Effect of thermal residual stress on matrix cracking strain and fracture behavior of the sintered SiC fiber reinforced SiO2-mullite composites", Journal of the Japan Institute of Metals, Vol. 68, Vol. 2, pp. 172-180 Nambu, S. and Enoki, M. (2004a) "Analysis of acoustic emission behavior in graphite materials for solid rocket motor", Key Engineering Materials, Vol. 270-273, pp. 479-484 Nambu, S. and Enoki, M. (2004b) "Strength and toughness of graphite
The experimental setup of in-process monitoring system is shown in Fig.1.
However, no AE could be detected in a specimen (No.1) in which maximum principal stress did not exceed the value of 45 MPa.
Typical AE behavior during cooling period after plasma spraying 0 20 40 60 80 10003 0 06 0 0 0 20 40 60 80 10003 0 06 0 0 Time, t / s Stress, σ/ MPa First AE No.6 No.5 No.4 No.3 No.2 No.1 Fig. 4.
References Enoki, M., Nishinoiri, S., Seki, T. and Kishimoto, A. (2004) "Non-contact measurement of acoustic emission in thin specimen by laser interferometer", Key Engineering Materials, Vol. 270-273, pp. 485-490 Enoki, M., Watanabe, M., Chivavibul, P. and Kishi, T. (2000) "Non-contact Measurement of Acoustic Emission in Materials by Laser Interferometry", Science and Technology of Advanced Materials, Vol. 1, No.3, pp. 157-165 Nagahisa, K., Iwamoto, K., Shinozaki, K., Sasaki, G., Enoki, M. and Yoshida, M. (2004) "Effect of thermal residual stress on matrix cracking strain and fracture behavior of the sintered SiC fiber reinforced SiO2-mullite composites", Journal of the Japan Institute of Metals, Vol. 68, Vol. 2, pp. 172-180 Nambu, S. and Enoki, M. (2004a) "Analysis of acoustic emission behavior in graphite materials for solid rocket motor", Key Engineering Materials, Vol. 270-273, pp. 479-484 Nambu, S. and Enoki, M. (2004b) "Strength and toughness of graphite