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Online since: October 2011
Authors: Yu Jie Wang, Xiao Na Li, Yun Wang, Dong Xiang Zhao, Jing Lin Gao, Zheng Qiang Peng
Unlike EAG results, males were attractive to (E)-2-octenal (10-2 and 10-1 μL /μL) and tridecane (10 μL /μL), and repelled by (E)-2-octenal (10-3, 1, 10 and 102 μL /μL) and tridecane (10-1 μL /μL) in the Y-tube olfactometer.
Odours were spotted on a strip of filter paper (1 cm × 1 cm) and placed in one of the jars of the bioassay apparatus.
In behavior assays, males repelled by (E)-2-octenal (10-3, 1, 10 and 102 μL /μL) and tridecane (10-1 μL /μL), while (E)-2-octenal (10-2 and 10-1 μL /μL) and tridecane (10 μL /μL) were attractive to males (Figs. 3-4).
Am. 78: 474-479
Zool. 42: 1-7
Odours were spotted on a strip of filter paper (1 cm × 1 cm) and placed in one of the jars of the bioassay apparatus.
In behavior assays, males repelled by (E)-2-octenal (10-3, 1, 10 and 102 μL /μL) and tridecane (10-1 μL /μL), while (E)-2-octenal (10-2 and 10-1 μL /μL) and tridecane (10 μL /μL) were attractive to males (Figs. 3-4).
Am. 78: 474-479
Zool. 42: 1-7
Online since: July 2023
Authors: Andrés Mauricio Nieves Chacón, Dany Sanchez Dominguez, Francisco Bruno Souza Oliveira
The data center industry consumes between 196 and 400 terawatt-hours annually, between 1% and 2% of the world's energy consumption.
Table 1.
Energy release components (see Table 1) were considered, coupled with the dimensions and positioning of each element.
(a) (b) Figure 1.
Equation (1) represents the relation between volumetric flow in (m3/s) and the fan speed: (1) where N2 and N1 represent the new and old speeds, respectively.
Table 1.
Energy release components (see Table 1) were considered, coupled with the dimensions and positioning of each element.
(a) (b) Figure 1.
Equation (1) represents the relation between volumetric flow in (m3/s) and the fan speed: (1) where N2 and N1 represent the new and old speeds, respectively.
Online since: January 2019
Authors: Xiao Li Xi, Yun He Zhang, Zhao Jie Huang, Li Wen Ma, Yue Hua Wang
Optimum conditions are observed at a phase ratio of 1:2 because with the change in the phase ratio, the ion loss rate is the lowest at a phase ratio of 1:2 and 1:3 (Fig. 2).
References [1] Gu F, Guo J, Yao X, et al.
Electrochimica Acta, 2004, 50(2–3): 479-483
Solid-state redox reactions of LiNi(1/2)Co(1/2)O2 (R3(bar) m) for 4 volt secondary lithium cells[J].
Electrochimica Acta, 1999, 45(1-2): 243-253
References [1] Gu F, Guo J, Yao X, et al.
Electrochimica Acta, 2004, 50(2–3): 479-483
Solid-state redox reactions of LiNi(1/2)Co(1/2)O2 (R3(bar) m) for 4 volt secondary lithium cells[J].
Electrochimica Acta, 1999, 45(1-2): 243-253
Online since: October 2010
Authors: Li Hua, Gia Kuan Yang, Hong Quan Zhang
Hua 1, a, 2, 3, G.
The solder alloys used in this investigation were cold rolled to columns with Φ1cm×1.5cm.
The percent of Germanium was 0.2, 0.5, 1, 2, 5, 8 wt.%, respectively, the number was 1#, 2#, 3#, 4#, 5#, 6#.
CHMT-5, 479 (1982)
R. 44, 1 (2004)
The solder alloys used in this investigation were cold rolled to columns with Φ1cm×1.5cm.
The percent of Germanium was 0.2, 0.5, 1, 2, 5, 8 wt.%, respectively, the number was 1#, 2#, 3#, 4#, 5#, 6#.
CHMT-5, 479 (1982)
R. 44, 1 (2004)
Online since: March 2023
Authors: B. Selvakumar, S. Vijayalakshmi, S. Arunachalam, Periasamy Palanisamy
Fig. 1.
Small peaks observed for PANI with h k l values at (1 2 1) (1 1 5) (0 0 6) (4 2 1) found increased for PANI\20wt% MnO2 composite materials.
Transmittance peaks at 1570 cm-1, 1500 cm-1,1397 cm-1, 1302 cm-1, 1142 cm-1, 816 cm-1 confirms the existence of PANI vibrational mode.
Table 1.
[16] S.L Suib, Porous Manganese Oxide Octahedral Molecular Sieves and Octahedral Layered Materials, Accounts of the Chemical Research. 41 (2008) 479-487
Small peaks observed for PANI with h k l values at (1 2 1) (1 1 5) (0 0 6) (4 2 1) found increased for PANI\20wt% MnO2 composite materials.
Transmittance peaks at 1570 cm-1, 1500 cm-1,1397 cm-1, 1302 cm-1, 1142 cm-1, 816 cm-1 confirms the existence of PANI vibrational mode.
Table 1.
[16] S.L Suib, Porous Manganese Oxide Octahedral Molecular Sieves and Octahedral Layered Materials, Accounts of the Chemical Research. 41 (2008) 479-487
Online since: February 2018
Authors: R. Rajesh, Duraisamy Thirumalaikumarasamy, V. Balasubramanian, S. Sree Sabari, Medha R. Elayidom
It was described in Fig. 1.
2.5.2.
Table 1.
Design matrix and Experimental Results Spray Condition Coded values Original value Porosity, vol.% Deposition Efficiency, (%) P S F P (kW) S (cm) F (gpm) 1 -1 -1 -1 19.4 10.6 20 12 10 2 1 -1 -1 23.6 10.6 20 7 17 3 -1 1 -1 19.4 12.4 20 14 9 4 1 1 -1 23.6 12.4 20 6 15 5 -1 -1 1 19.4 10.6 30 10 5 6 1 -1 1 23.6 10.6 30 9 7 7 -1 1 1 19.4 12.4 30 18 6 8 1 1 1 23.6 12.4 30 13 8 9 -1.682 0 0 18 11.5 25 14 6 10 1.682 0 0 25 11.5 25 5 18 11 0 -1.682 0 21.5 10 25 9 11 12 0 1.682 0 21.5 13 25 15 7 13 0 0 -1.682 21.5 11.5 15 8 17 14 0 0 1.682 21.5 11.5 35 12 9 15 0 0 0 21.5 11.5 25 5 21 16 0 0 0 21.5 11.5 25 6 23 17 0 0 0 21.5 11.5 25 5 23 18 0 0 0 21.5 11.5 25 6 21 19 0 0 0 21.5 11.5 25 5 23 20 0 0 0 21.5 11.5 25 5 23 Table 3.
References [1] G.L.
:Mater.Int. 22 (2012) 468-479
Table 1.
Design matrix and Experimental Results Spray Condition Coded values Original value Porosity, vol.% Deposition Efficiency, (%) P S F P (kW) S (cm) F (gpm) 1 -1 -1 -1 19.4 10.6 20 12 10 2 1 -1 -1 23.6 10.6 20 7 17 3 -1 1 -1 19.4 12.4 20 14 9 4 1 1 -1 23.6 12.4 20 6 15 5 -1 -1 1 19.4 10.6 30 10 5 6 1 -1 1 23.6 10.6 30 9 7 7 -1 1 1 19.4 12.4 30 18 6 8 1 1 1 23.6 12.4 30 13 8 9 -1.682 0 0 18 11.5 25 14 6 10 1.682 0 0 25 11.5 25 5 18 11 0 -1.682 0 21.5 10 25 9 11 12 0 1.682 0 21.5 13 25 15 7 13 0 0 -1.682 21.5 11.5 15 8 17 14 0 0 1.682 21.5 11.5 35 12 9 15 0 0 0 21.5 11.5 25 5 21 16 0 0 0 21.5 11.5 25 6 23 17 0 0 0 21.5 11.5 25 5 23 18 0 0 0 21.5 11.5 25 6 21 19 0 0 0 21.5 11.5 25 5 23 20 0 0 0 21.5 11.5 25 5 23 Table 3.
References [1] G.L.
:Mater.Int. 22 (2012) 468-479
Online since: October 2024
Authors: Anton Chernukha, Olga Skorodumova, Nataliia Lysak, Viacheslav Kurepin
Fig. 1.
Bands at 2330 cm–1 and 2360 cm–1 also appear on the spectra, which can characterize the oscillations of Р–Н bonds.
Peaks at 620, 670, 790 cm–1 also appear for all samples with phenol.
Fire resistance of reinforced concrete and steel structures, 1–166
Emen, The Use of Sol-Gel Method for Obtaining Fire-Resistant Elastic Coatings on Cotton Fabrics, Materials Science Forum. 1038 (2021) 468–479
Bands at 2330 cm–1 and 2360 cm–1 also appear on the spectra, which can characterize the oscillations of Р–Н bonds.
Peaks at 620, 670, 790 cm–1 also appear for all samples with phenol.
Fire resistance of reinforced concrete and steel structures, 1–166
Emen, The Use of Sol-Gel Method for Obtaining Fire-Resistant Elastic Coatings on Cotton Fabrics, Materials Science Forum. 1038 (2021) 468–479
Online since: November 2017
Authors: Bibiana Porto da Silva, Fernando Saccol, Nanton Roberto Caetano, Cristiane Pedrazzi, Nattan Roberto Caetano
The Decree 479 of March 20, 1992 obliges to keep the power factor as close to unity as possible (1.00), for both utilities and consumers.
The residue class E in mill 1 resulted in values close to 1.00 of the power factor.
References [1] R.
JOURNAL OF THE BRAZILIAN CHEMICAL SOCIETY. 00 (2017) 1-8
Revista Científica Eletrônica de Engenharia Florestal. 8 (2006) 1-9
The residue class E in mill 1 resulted in values close to 1.00 of the power factor.
References [1] R.
JOURNAL OF THE BRAZILIAN CHEMICAL SOCIETY. 00 (2017) 1-8
Revista Científica Eletrônica de Engenharia Florestal. 8 (2006) 1-9
Online since: September 2011
Authors: Krzysztof Biernacki
Methods of Increasing Loadability for the
Plastic Cycloidal Gears
Krzysztof Biernacki 1,a
1 Ul.
Fig. 1.
Material Young's modulus E [MPa] Yield point Re [MPa] 1.
References [1] S.
The Journal of Strain Analysis for Engineering Design, October 2010, vo.45, Issue 7, pages 465-479
Fig. 1.
Material Young's modulus E [MPa] Yield point Re [MPa] 1.
References [1] S.
The Journal of Strain Analysis for Engineering Design, October 2010, vo.45, Issue 7, pages 465-479
Online since: May 2025
Authors: Annamária Polyákné Kovács, Tamás József Szabó, Solmaz Hajialilou, Yitbarek Firew Minale, Márton Tomin, Balázs Gyore
Fig. 1.
Yield stress, according to the supplier, is 58 MPa, measured according to DIN ISO 527-1 [8].
A side peak induced by oxidative degradation can be observed at the 1750 cm-1 wavenumber range.
[21] Peter Larkin, Chapter 1 - Introduction: Infrared and Raman Spectroscopy, Infrared and Raman Spectroscopy, Peter Larkin, Ed., Oxford: Elsevier, 2011, pp. 1–5.doi: https://doi.org/10.1016/B978-0-12-386984-5.10001-1
[24] Peng He, Xiaoyang Zhao, Ling Wang, and Zhen Xu, Thermal degradation of syndiotactic polypropylene and the influence of stereoregularity on the thermal degradation behaviour by in situ FTIR spectroscopy, Polymer Degradation and Stability, vol. 88, no. 3, pp. 473–479, 2005, doi: https://doi.org/10.1016/j.polymdegradstab.2004.12.008
Yield stress, according to the supplier, is 58 MPa, measured according to DIN ISO 527-1 [8].
A side peak induced by oxidative degradation can be observed at the 1750 cm-1 wavenumber range.
[21] Peter Larkin, Chapter 1 - Introduction: Infrared and Raman Spectroscopy, Infrared and Raman Spectroscopy, Peter Larkin, Ed., Oxford: Elsevier, 2011, pp. 1–5.doi: https://doi.org/10.1016/B978-0-12-386984-5.10001-1
[24] Peng He, Xiaoyang Zhao, Ling Wang, and Zhen Xu, Thermal degradation of syndiotactic polypropylene and the influence of stereoregularity on the thermal degradation behaviour by in situ FTIR spectroscopy, Polymer Degradation and Stability, vol. 88, no. 3, pp. 473–479, 2005, doi: https://doi.org/10.1016/j.polymdegradstab.2004.12.008