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Online since: October 2023
Authors: Akshat Mahajan, Sahil Jaggi, Banda Lakshmi Sai Karthik
(Hamad & Dawi, 2017) (Güneyisi et al., 2012; Megat Johari et al., 2011) [1,2, 3].
Coarse aggregates used in this study were evaluated by the standard procedures of IS 2386 Part 1.
Table 1: Physical Property of Ordinary Portland Cement S.No Physical properties Results obtained 1 Specific gravity 3.11 2 Standard consistency (%) 31.3 3 Initial Setting time (min) 56 4 Final Setting time (min) 247 Fig. 1: Metakaolin Fig. 2: Silica Fume Table 2: Typical Properties of Normal and Coarse Granite Aggregates S.No Properties Normal Aggregates Granite Aggregates 1.
References [1] Mazloom, M., Ramezanianpour, A.
Construction and Building Materials, 30, 470–479. https://doi.org/10.1016/j.conbuildmat.2011.12.050 [4] Güneyisi, E., Gesoǧlu, M., Karaoǧlu, S., & Mermerdaş, K. (2012).
Coarse aggregates used in this study were evaluated by the standard procedures of IS 2386 Part 1.
Table 1: Physical Property of Ordinary Portland Cement S.No Physical properties Results obtained 1 Specific gravity 3.11 2 Standard consistency (%) 31.3 3 Initial Setting time (min) 56 4 Final Setting time (min) 247 Fig. 1: Metakaolin Fig. 2: Silica Fume Table 2: Typical Properties of Normal and Coarse Granite Aggregates S.No Properties Normal Aggregates Granite Aggregates 1.
References [1] Mazloom, M., Ramezanianpour, A.
Construction and Building Materials, 30, 470–479. https://doi.org/10.1016/j.conbuildmat.2011.12.050 [4] Güneyisi, E., Gesoǧlu, M., Karaoǧlu, S., & Mermerdaş, K. (2012).
Online since: February 2026
Authors: Muhammad Nizam, Mufti Reza Aulia Putra, Warindi Warindi
Table 1 Summarized recent findings on various thermal management techniques for batteries in high-temperature scenarios.
Triyono, “Mini Review of Thermoelectric and their Potential Applications as Coolant in Electric Vehicles to Improve System Efficiency,” Evergreen, vol. 10, no. 1, pp. 469–479, Mar. 2023
Liu et al., “Changes in performance and thermal stability of Ni0.8Co0.1Al0.1/graphite batteries with excessive water,” IET energy systems integration, 2024
Nielsen, “Automotive battery pack manufacturing – a review of battery to tab joining,” Journal of Advanced Joining Processes, vol. 1, Mar. 2020
Qu, “Battery thermal management using phase-change material,” Elsevier BV, 2024, pp. 1–40
Triyono, “Mini Review of Thermoelectric and their Potential Applications as Coolant in Electric Vehicles to Improve System Efficiency,” Evergreen, vol. 10, no. 1, pp. 469–479, Mar. 2023
Liu et al., “Changes in performance and thermal stability of Ni0.8Co0.1Al0.1/graphite batteries with excessive water,” IET energy systems integration, 2024
Nielsen, “Automotive battery pack manufacturing – a review of battery to tab joining,” Journal of Advanced Joining Processes, vol. 1, Mar. 2020
Qu, “Battery thermal management using phase-change material,” Elsevier BV, 2024, pp. 1–40
Online since: February 2012
Authors: F. Suárez-García, J.I. Paredes, M. Pérez-Mendoza, J. Nauroy, A. Martínez-Alonso, J.M.D. Tascón
The reaction rates calculated from these slopes are 4.0 Í 10-4 g g-1 min-1 for series obtained from fresh CNFs, 1.5 Í 10-3 and 1.9 Í 10-3 g g-1 min-1 for samples prepared from CNFs impregnated with 1 wt.% of K2CO3 and 1% KOH, respectively.
Figure 1.
Surface areas given in m2 g-1; pore volumes given in cm3 g-1.
Surface areas given in m2 g-1; pore volumes given in cm3 g-1.
Do, The preparation of active carbons from coal by chemical and physical activation, Carbon 34 (1996) 471-479
Figure 1.
Surface areas given in m2 g-1; pore volumes given in cm3 g-1.
Surface areas given in m2 g-1; pore volumes given in cm3 g-1.
Do, The preparation of active carbons from coal by chemical and physical activation, Carbon 34 (1996) 471-479
Online since: December 2004
Authors: Henrik Strandlund, Henrik Larsson
When Eq. 22 has been solved for all species it will be found that, in general, � xk �=1.
In10 −12 −10 −8 −6 −4 −2 0 −3 −2 −1 0 1 2 3 4 5 Kirkendall shift [µm] ∆C 0 Cr [at%] Calculated values Son and Morral (1989) Fig. 1: Measured and calculated values of the Kirkendall shift in Ni-8.8Cr-8.8Al/Ni(8.8 − ∆C0Cr)-5Al (at-%).
Fig. 1 the measured and calculated Kirkendall shift is compared.
Trans., Vol. 1, pp. 499-505,1970
[26] Chen, Q., Engstr¨om A., H¨oglund, L., Strandlund, H., Sundman, B., "Thermo-Calc Program Interface and Their Applications - Direct Insertion of Thermodynamic and Kinetic Data into Modelling of Materials Processing, Structure and Property", Materials Science Forum, Vols. 475- 479, pp. 3145-3148, 2005
In10 −12 −10 −8 −6 −4 −2 0 −3 −2 −1 0 1 2 3 4 5 Kirkendall shift [µm] ∆C 0 Cr [at%] Calculated values Son and Morral (1989) Fig. 1: Measured and calculated values of the Kirkendall shift in Ni-8.8Cr-8.8Al/Ni(8.8 − ∆C0Cr)-5Al (at-%).
Fig. 1 the measured and calculated Kirkendall shift is compared.
Trans., Vol. 1, pp. 499-505,1970
[26] Chen, Q., Engstr¨om A., H¨oglund, L., Strandlund, H., Sundman, B., "Thermo-Calc Program Interface and Their Applications - Direct Insertion of Thermodynamic and Kinetic Data into Modelling of Materials Processing, Structure and Property", Materials Science Forum, Vols. 475- 479, pp. 3145-3148, 2005
Online since: February 2021
Authors: Hong Tan, Yuan Qing Song, Yan Ma, Xin Li, Peng Chen, Feng Luo, Jie Hua Li, Zhen Li, Lie Yang, Zong Guang Zhou, Wen Kai Liu
Fig 1.
(a)the full spectra; (b)amplified regions from 1300cm-1 to 2000cm-1.
Table 1.
That is, the characteristic peak at 1722cm-1 and 1659cm-1 move to 1675cm-1 and 1619cm-1, respectively.
Near-infrared absorbing mesoporous carbon nanoparticle as an intelligent drug carrier for dual-triggered synergistic cancer therapy, Carbon. 82 (2015), 479-488
(a)the full spectra; (b)amplified regions from 1300cm-1 to 2000cm-1.
Table 1.
That is, the characteristic peak at 1722cm-1 and 1659cm-1 move to 1675cm-1 and 1619cm-1, respectively.
Near-infrared absorbing mesoporous carbon nanoparticle as an intelligent drug carrier for dual-triggered synergistic cancer therapy, Carbon. 82 (2015), 479-488
Online since: February 2016
Authors: Emanuele Baravelli, Pasquale Maiorano, Antonio Gnudi, Susanna Reggiani, Giorgio Baccarani, Elena Gnani
Eq. (1) shows that
the drain conductance can be close to its maximum value (2q2/h) Tsc only if (ηvs − µs) ≫ 1 and if
(η(0)cd − µs) ≪ 1.
On the other hand, the subthreshold swing SS can be expressed as SS = ln(10) kBT q ln (T−1 sc ) ηcs − ηcc + f(ηcc − µs) − f(ηcc − µd) ln (1 + exp(µs − ηcc) 1 + exp(µs − ηvs) 1 + exp(µd − ηvs) 1 + exp(µd − ηcc)) −1 (2) Eq. (2) shows that, if the factor in braces is substantially higher than 1, the subthreshold swing SS can be smaller than 60 mV/dec.
(ηvs −µs) ≫ 1 and ηcc is close to ηvs, the second term in braces tends to 1 and SS can be at most 60 mV/dec.
References [1] K.
Riel, "Tunnel field-effect transistors as energy-efficient electronic switches", Nature, 479, (2011) pp. 329-337
On the other hand, the subthreshold swing SS can be expressed as SS = ln(10) kBT q ln (T−1 sc ) ηcs − ηcc + f(ηcc − µs) − f(ηcc − µd) ln (1 + exp(µs − ηcc) 1 + exp(µs − ηvs) 1 + exp(µd − ηvs) 1 + exp(µd − ηcc)) −1 (2) Eq. (2) shows that, if the factor in braces is substantially higher than 1, the subthreshold swing SS can be smaller than 60 mV/dec.
(ηvs −µs) ≫ 1 and ηcc is close to ηvs, the second term in braces tends to 1 and SS can be at most 60 mV/dec.
References [1] K.
Riel, "Tunnel field-effect transistors as energy-efficient electronic switches", Nature, 479, (2011) pp. 329-337