Sort by:
Publication Type:
Open access:
Publication Date:
Periodicals:
Search results
Online since: February 2012
Authors: Lander Galdos, Jon Larrañaga, Eneko Sáenz de Argandoña, Aritz Legarda
Materials and tensile data
Three different steel grades, a DC01 low strength steel, a DP600 medium strength steel and a MS1200
high strength steel have been used in the present investigation.
The tendency is towards a reduction of the springback when the gap between the rolls is smaller.
The tendency is towards a reduction of the springback when the gap between the rolls is smaller.
Online since: December 2005
Authors: Wolfgang Skorupa, A. Nazarov, T. Gebel, I.N. Osiyuk, J.M. Sun, S. Prucnal, M. Helm, L. Rebohle
The method of analysing the trapping data is described elsewhere [7,8].
The scattering of hot electrons by both the charged defects and the Si nanoclusters results in a reduction of the average energy and the average impact excitation cross section of the Er centers around the negatively charged nanoclusters.
The scattering of hot electrons by both the charged defects and the Si nanoclusters results in a reduction of the average energy and the average impact excitation cross section of the Er centers around the negatively charged nanoclusters.
Online since: April 2013
Authors: Horst Meier, Jun Hong Zhu, Bolko Buff, Christian Magnus
These circumstances result in a reduction of the conducting cross-sectional area and a reduced conductivity compared to a uniform conductor.
In this connection, further materials have been tested in order to get data for referencing.
In this connection, further materials have been tested in order to get data for referencing.
Online since: February 2016
Authors: Yuriy Sharkeev, Valentina V. Chebodaeva, Ekaterina G. Komarova, Maria Sedelnikova
However, there are conflicting data about biocompatible properties of substrate materials.
Rough surface profile leads to reduction of the attractive forces of liquid molecules inside the material which create surface energy.
Rough surface profile leads to reduction of the attractive forces of liquid molecules inside the material which create surface energy.
Online since: April 2004
Authors: Soon Jong Yoon, Jae Ho Jung, Won Sup Jang
From the numerical analysis on the data obtained for the case of plate with FS boundary
conditions (kFS), the simplified form of equation for this case was obtained as Eq. (6), and the
simplified form of equation for the case of plate with SS boundary conditions (kSS) was simply
estimated as Eq. (7), subsequently.
3
2
FS 005.0103.0186.0025.37 E E
E R
R
R
k !
(8) ( ) u rc F EEk t b 2112 2211 112 �� �" � #In Eq. (8), "rc (0.7 for the structural steel) is the reduction factor to account for the imperfections of material such as residual stresses, initial crookedness of plate components, nonuniform distribution and waviness of reinforcing fibers, etc.
(8) ( ) u rc F EEk t b 2112 2211 112 �� �" � #In Eq. (8), "rc (0.7 for the structural steel) is the reduction factor to account for the imperfections of material such as residual stresses, initial crookedness of plate components, nonuniform distribution and waviness of reinforcing fibers, etc.
Online since: January 2013
Authors: Hans J. Maier, Elena Panchenko, Haluk E. Karaca, Ibrahim Karaman, Thomas Niendorf, Jayaram Dadda, Jan Lackmann, James A. Monroe
The reduction of the transformation strains and the increase of the thermal hysteresis under both stress states is attributed to the number and resulting interaction of martensite variants that form at higher stress levels, which will trigger stress-induced martensite along with the thermally-induced martensite [14].
The curves for Ms in Fig. 2 follow the Clausius-Clapeyron (CC) relationship with slopes of 0.9 MPa/°C and 1.5 MPa/°C for tension and compression, respectively, which is in good agreement with the data reported in literature [13].
The curves for Ms in Fig. 2 follow the Clausius-Clapeyron (CC) relationship with slopes of 0.9 MPa/°C and 1.5 MPa/°C for tension and compression, respectively, which is in good agreement with the data reported in literature [13].
Online since: January 2006
Authors: Michael Josef Zehetbauer, V.V. Stolyarov, Wolfgang Lacom, Bernhard Mingler, Hans Peter Karnthaler
The thickness reduction for one pass depended on the structure state and was 3 . 10-4 m for
the CG state and 1
. 10
-4 m for the UFG state.
Tensile properties In Table 1 the mechanical data of CG (ECAP(0)) Ti and those of UFG (ECAP(8)) Ti subjected to CR are presented.
Tensile properties In Table 1 the mechanical data of CG (ECAP(0)) Ti and those of UFG (ECAP(8)) Ti subjected to CR are presented.
Online since: December 2024
Authors: Nouman Bashir, Kaleem Akram, Aamir Nusair Khan, Ali Haider
Benefit of NdFeB magnet is the significant reduction in volume and improved efficiency.
The magnetic properties weakened with increase in temperature. 19.89°C 50.80°C 80.36°C 108.3°C Fig. 3 Demagnetization curve of NdFeB sample at varying temperatures Measurements data shows that increase in temperature affects the magnetic characteristics and performance of the NdFeB magnets declines.
The magnetic properties weakened with increase in temperature. 19.89°C 50.80°C 80.36°C 108.3°C Fig. 3 Demagnetization curve of NdFeB sample at varying temperatures Measurements data shows that increase in temperature affects the magnetic characteristics and performance of the NdFeB magnets declines.