51 research outputs found
Modified Norris–Landzberg Model and Optimum Design of Temperature Cycling ALT
Accelerated life testing (ALT) is an effective way to assess the lifetime of a product. Due to the complex nature of its testing profile, it is difficult to carry out temperature cycling ALT. This paper establishes a modified Norris–Landzberg model as acceleration model, and proposes the optimum design method of temperature cycling ALT. First, the FEA method is used to study the influence of temperature cycling profile parameters on the thermal fatigue life of 63Sn–37Pb solder joints. Then, a modified Norris–Landzberg model is proposed by introducing ramp time and dwell time with an added weight value. Finally, the temperature cycling ALT is regarded as a special multi-stress ALT to study its optimum design method. The uniform design theory is used to determine the combined mode. The optimum model is established with the objective of minimizing the asymptotic variance of the estimation of median lifetime under normal use conditions, and the simulation example shows the workability of the proposed method
Body-centered-cubic Ni and its magnetic properties
The body-centered-cubic (bec) phase of Ni, which does not exist in nature, has been achieved as a thin film on GaAs(001) at 170 K via molecular beam epitaxy. The bec Ni is ferromagnetic with a Curie temperature of 456 K and possesses a magnetic moment of 0.52 \uc2\ub1 0.08 \uce\ubcB/atom. The cubic magneto-crystalline anisotropy of bec Ni is determined to be +4.0 \uc3\u97 105 ergs \uc2\ub7 cm-3, as opposed to -5.7 \uc3\u97 10 4 ergs \uc2\ub7 cm-3 for the naturally occurring face-centered-cubic (fcc) Ni. This sharp contrast in the magnetic anisotropy is attributed to the different electronic band structures between bec Ni and fcc Ni, which are determined using angle-resolved photoemission with synchrotron radiation
Relationship Between the Thermodynamic Parameters, Structure, and Anticorrosion Properties of Al-Zr-Ni-Fe-Y Alloys
The influence of the chemical composition on the crystallization process, amorphous phase
formation, and the anticorrosion properties of Al-Zr-Ni-Fe-Y alloys are presented. To reduce
the number of experiments, a thermodynamic approach was applied in which the entropy and
Gibbs free energy of representative alloys were optimized. The low glass-forming ability of
Al-Zr-Ni-Fe-Y alloy systems was related to the crystallization of the Al3Zr phase from the melt.
The structural analysis showed that phases containing Ni and Fe, such as Al19Ni5Y3, Al10Fe2Y,
and Al23Ni6Y4, played a key role in the formation of amorphous alloys. According to this, the
simultaneous addition of Ni/Fe and Y is important to prevent the crystallization of Al-based
alloys in the melt. The formation of an amorphous phase in Al80Zr5Ni5Fe5Y5 alloys and the
complete amorphization of Al85Ni5Fe5Y5 alloys were responsible for the high corrosion
resistance compared with fully crystalline alloys. Moreover, the addition of Y had a significant
impact on the anticorrosion properties. The XPS results showed that the alloys tended to form a
passive Al2O3 and Y2O3 layer on the surface
Covariance differencing‐based angle estimation method for bistatic multiple‐input–multiple‐output radar in unknown coloured noise
Geochemistry and Sr–Nd–Hf isotopes of Middle Devonian igneous rocks of the Sarsuk polymetallic Au deposit: implications for understanding the tectonic evolution of the south Altay Orogenic Belt, Northwest China
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