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Online since: February 2006
Authors: Han Cheol Choe, Yeong Mu Ko, Sun Jae Kim
The pit size and number of non coated
Co-Cr alloy is severely attacked along with grain boundaries
Centrifugal casting� High frequency induction casting Vacuum pressure casting
Non
(TiN) A alloy� B alloy C alloy A alloy B alloy C alloy A alloy B alloy C alloy
I corr
(A/�)�
1.88X10-7
(7.49X10-6)
1.42X10-6
(1.19X10-6)�
5.13X10-7
(8.14X10-6)�
1.65X10-7
(1.50X10-6)�
6.62X10-7
(5.93X10-7)�
1.39X10-7
(7.81X10-6)�
1.81X10-7
(6.78X10-6)�
8.87X10-7
(7.14X10-8)�
1.20X10-7
(6.80X10-6)�
I
300m
V
(A/�)�
1.06X10-6
(9.00X10-5)�
1.65X10-1
(8.64X10-5)
1.80X10-4
(1.20X10-4)
3.35X10-4
(2.24X10-6)
4.26XX10-2
(7.22X10-5)
1.09X10-4
(2.90X10-5)
4.19X10-4
(6.00X10-5)
2.58X10-2
(6.89X10-5)
1.43X10-4
(5.00X10-5)
E corr
(mV)�
-461
(-422)
-373
(-330)
-401
(-394)
-381
(-289)
-287
(-355)
-475
(-261)
-444
(-245)
-268
(-260)
- 436
(-309)
E pit
(mV)�
+720
(+830)�
+130
(+150)
+740
(+900)
References [1] BR Lanier, KD Rudd, RR Strunk: J.
Tech Vol 91(1997), p 1
Shreir, Corrosion Handbook Vol.1, Newnes-Butterworths Boston, (1979), p.3-31 [16] H.
Vol. 475-479 (2005), p.2287
References [1] BR Lanier, KD Rudd, RR Strunk: J.
Tech Vol 91(1997), p 1
Shreir, Corrosion Handbook Vol.1, Newnes-Butterworths Boston, (1979), p.3-31 [16] H.
Vol. 475-479 (2005), p.2287
Online since: February 2006
Authors: Chang Ho Lee, Sung Doo Hwang, Young Do Park, Yong Ho Park, Ik Min Park, Wang Kee Min, Young Seok Kim, Yang Do Kim
The XRD patterns show that the increase in intensity of (1 1 0)
plane are more notable than that of (1 0 10) and (0 0 15) plane.
According to the pole figures of (0 0 6) plane and (1 1 0) plane, the increased intensity of the (1 1 0) plane is favorable to improve the thermoelectric performance [15,16].
The electrical conductivity and thermal conductivity of hot extruded specimens are shown in Fig. 4. 20 30 40 50 60 Intensity (arb. unit) Cu (Kα ) 48 h 72 h 100 h 145 h 195 h (0 0 15) (0 2 10) (2 0 5) (1 1 0) (1 0 10) (0 1 5) 2θ (Deg ree) Figure 1.
It is also observed in the SEM fractographs 20 30 40 50 60 annealed annealed as-bulk as-bulk parallel perpoendicular (0 2 10) (2 0 5) (0 0 15) (1 0 10) (1 1 0) (0 1 5) Cu (Kα) Intensity (arb. unit) 2θ (Degree) Figure. 6.
Forum 475-479 (2005) p.1759 [11] K.Wakamura: J.
According to the pole figures of (0 0 6) plane and (1 1 0) plane, the increased intensity of the (1 1 0) plane is favorable to improve the thermoelectric performance [15,16].
The electrical conductivity and thermal conductivity of hot extruded specimens are shown in Fig. 4. 20 30 40 50 60 Intensity (arb. unit) Cu (Kα ) 48 h 72 h 100 h 145 h 195 h (0 0 15) (0 2 10) (2 0 5) (1 1 0) (1 0 10) (0 1 5) 2θ (Deg ree) Figure 1.
It is also observed in the SEM fractographs 20 30 40 50 60 annealed annealed as-bulk as-bulk parallel perpoendicular (0 2 10) (2 0 5) (0 0 15) (1 0 10) (1 1 0) (0 1 5) Cu (Kα) Intensity (arb. unit) 2θ (Degree) Figure. 6.
Forum 475-479 (2005) p.1759 [11] K.Wakamura: J.
Online since: March 2007
Authors: Z. Horita, Terence G. Langdon, Minoru Furukawa, Cheng Xu, Megumi Kawasaki
Summary and Conclusions
1.
W911NF-05-1-0046.
References [1] R.Z.
Kopylov, Russian Metall. 1 (1981), p. 99
Forum 475-479 (2005), p.2949
W911NF-05-1-0046.
References [1] R.Z.
Kopylov, Russian Metall. 1 (1981), p. 99
Forum 475-479 (2005), p.2949
Online since: October 2008
Authors: Yue Sheng Tong, Li Xin, Xing Wen Liang
(1)
1
n
jEK j j ji i
i
F X G
As can be seen from Eq.8 that the mass jm~ of equivalent SDOF system (Fig.3) is ji n i i T j j Xm MXm 1 }1]{[}{~
References [1] M.S.Medhekar, D.J.L.
Earthquake Engineering and Structural Dynamics, Vol.30(2001),pp:467-479 [3] Timothy White, Perry Adebar.
Journal of Building Structures, Vol.28 (2007)No.1,pp:101-106.
As can be seen from Eq.8 that the mass jm~ of equivalent SDOF system (Fig.3) is ji n i i T j j Xm MXm 1 }1]{[}{~
References [1] M.S.Medhekar, D.J.L.
Earthquake Engineering and Structural Dynamics, Vol.30(2001),pp:467-479 [3] Timothy White, Perry Adebar.
Journal of Building Structures, Vol.28 (2007)No.1,pp:101-106.
Online since: December 2014
Authors: Zhong De Shan, Wan Hua Cai, Bai Liang Zhuang, Yong Sheng Ye
The results are listed in Table 1.
Prod.Eng.Res.Devel. 2007(1)：149-15
Annals of the CIRP. 2007,56(1)：269-272
Engineering Failure Analysis, 2009, 16(1)：128-135.
Computer Aided Engineering, 2007, 1(1):85-89 [16] Zhuang Bai-liang, Shan Zhong-de, Jiang Chao, Rong Wen-juan.
Prod.Eng.Res.Devel. 2007(1)：149-15
Annals of the CIRP. 2007,56(1)：269-272
Engineering Failure Analysis, 2009, 16(1)：128-135.
Computer Aided Engineering, 2007, 1(1):85-89 [16] Zhuang Bai-liang, Shan Zhong-de, Jiang Chao, Rong Wen-juan.
Online since: January 2025
Authors: Adel Benidir
Table 1.
Three zones numbered from 1 to 3 are delimited to extract cores (Fig. 1).
Fig. 1.
Vol. 18, Issue 1, 2023
July, pp. 479–486, 2018
Three zones numbered from 1 to 3 are delimited to extract cores (Fig. 1).
Fig. 1.
Vol. 18, Issue 1, 2023
July, pp. 479–486, 2018
Online since: October 2014
Authors: Dumitru Nedelcu, Elena Puiu, Lucia Vrajitoriu
Therefore, fluids with non-linear viscous behaviors, as well as viscoelastic materials are complex fluids [1,2,3,4].
Therefore, the complex fluid is assimilated to a “rheological” fluid, whose dynamics are described by the complex velocities field, V, and by the imaginary viscosity type coefficient, iλ2τdtτ2DF-1.
References [1] Luis, G. (1993), Complex Fluids, Springer, Volume 415, 327-349 [2] Mitchell, M. (2009), Complexity: A guided tour.
Europhysics Letters 17 (6), 479 [8] Chen-Shiyi and Doolen Gary, D. (1998), Lattice Boltzmann methodd for fluid flows.
General relativity and gravitation, 40 (1), 35-55 [22] Agop, M.; Murgulet, C. (2007).
Therefore, the complex fluid is assimilated to a “rheological” fluid, whose dynamics are described by the complex velocities field, V, and by the imaginary viscosity type coefficient, iλ2τdtτ2DF-1.
References [1] Luis, G. (1993), Complex Fluids, Springer, Volume 415, 327-349 [2] Mitchell, M. (2009), Complexity: A guided tour.
Europhysics Letters 17 (6), 479 [8] Chen-Shiyi and Doolen Gary, D. (1998), Lattice Boltzmann methodd for fluid flows.
General relativity and gravitation, 40 (1), 35-55 [22] Agop, M.; Murgulet, C. (2007).
Online since: January 2013
Authors: Zhi Peng Xu, Xiao Ping Chen, Xi Hong Zhao, Xing Zhou Chen, Qing Yang
Fig 1.
Protein marker; 1.
Table 1.
References [1] T.
Plant Cell Rep 31: 479-94
Protein marker; 1.
Table 1.
References [1] T.
Plant Cell Rep 31: 479-94
Online since: June 2014
Authors: Xeniya Mikhailovna Rakova, Nikolay Sergeevich Bolshakov, Sergey Aleksandrovich Krivoy
Floors: 1 floor and 1 ground floor.
Fig. 1.
The following inputs have been used: Table 1.
References [1] A.S.
Vol. 1.
Fig. 1.
The following inputs have been used: Table 1.
References [1] A.S.
Vol. 1.
Online since: September 2020
Authors: Mohd Ambar Yarmo, Maratun Najiha Abu Tahari, Tengku Sharifah Marliza, Norliza Dzakaria, Azizul Hakim Lahuri, Mark Lee Wun Fui, Tengku Shafazila Tengku Saharuddin
XRD diffractograms for Fe2O3 and bimetal BeO/Fe2O3 are shown in Fig. 1.
BeO/Fe2O3-300 also obtain highest adsorption capacity of 5.85 mg/g among all adsorbents (Table 1) for physical CO2 adsorption isotherms at room temperature (25 °C) and 1 atm as shown in (Fig. 3 b).
The nature of adsorption is favorable based on dimensionless separation factor of 01.
The slope, 1/n, allows for understanding the adsorption process.
Forum. 888 (2017) 479-484
BeO/Fe2O3-300 also obtain highest adsorption capacity of 5.85 mg/g among all adsorbents (Table 1) for physical CO2 adsorption isotherms at room temperature (25 °C) and 1 atm as shown in (Fig. 3 b).
The nature of adsorption is favorable based on dimensionless separation factor of 0
The slope, 1/n, allows for understanding the adsorption process.
Forum. 888 (2017) 479-484