Issue 10 Volume 41 May 16, 2003
Issue 10 Volume 41 May 16, 2003
Issue 10 Volume 41 May 16, 2003
- TAGS
- volume
- 202.118.250.135
You also want an ePaper? Increase the reach of your titles
YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.
26<br />
METALS AND METALLIC MATERIALS<br />
Includes physical, chemical, and mechanical properties of metals and metallic materials; and metallurgy.<br />
<strong>2003</strong>0032265 Pennsylvania State Univ., University Park, PA, USA<br />
3D Finite Element Analysis of Particle-Reinforced Aluminum<br />
Shen, H.; Lissenden, C. J.; February 01, 2002; 6 pp.; In English; Original contains black and white illustrations<br />
Contract(s)/Grant(s): NCC3-848; RTOP 706-85-24<br />
Report No.(s): E-13677; No Copyright; Avail: CASI; A02, Hardcopy<br />
Deformation in particle-reinforced aluminum has been simulated using three distinct types of finite element model: a<br />
three-dimensional repeating unit cell, a three-dimensional multi-particle model, and two-dimensional multi-particle models.<br />
The repeating unit cell model represents a fictitious periodic cubic array of particles. The 3D multi-particle (3D-MP) model<br />
represents randomly placed and oriented particles. The 2D generalized plane strain multi-particle models were obtained from<br />
planar sections through the 3D-MP model. These models were used to study the tensile macroscopic stress-strain response and<br />
the associated stress and strain distributions in an elastoplastic matrix. The results indicate that the 2D model having a particle<br />
area fraction equal to the particle representative volume fraction of the 3D models predicted the same macroscopic stress-strain<br />
response as the 3D models. However, there are fluctuations in the particle area fraction in a representative volume element.<br />
As expected, predictions from 2D models having different particle area fractions do not agree with predictions from 3D<br />
models. More importantly, it was found that the microscopic stress and strain distributions from the 2D models do not agree<br />
with those from the 3D-MP model. Specifically, the plastic strain distribution predicted by the 2D model is banded along lines<br />
inclined at 45 deg from the loading axis while the 3D model prediction is not. Additionally, the triaxial stress and maximum<br />
principal stress distributions predicted by 2D and 3D models do not agree. Thus, it appears necessary to use a multi-particle<br />
3D model to accurately predict material responses that depend on local effects, such as strain-to-failure, fracture toughness,<br />
and fatigue life.<br />
Author<br />
Aluminum Alloys; Finite Element Method; Strain Distribution; Triaxial Stresses; Stress-Strain Relationships; Tensile Stress;<br />
Computerized Simulation; Elastic Deformation<br />
<strong>2003</strong>0032927 NASA Glenn Research Center, Cleveland, OH, USA<br />
Specific Hardening Function Definition and Characterization of a Multimechanism Generalized Potential-Based<br />
Viscoelastoplasticity Model<br />
Arnold, S. M.; Saleeb, A. F.; February <strong>2003</strong>; 38 pp.; In English; Original contains black and white illustrations<br />
Contract(s)/Grant(s): NCC3-808; 22-713-82-35<br />
Report No.(s): NASA/TM-<strong>2003</strong>-212219; NAS 1.15:212219; E-13833; No Copyright; Avail: CASI; A03, Hardcopy<br />
Given the previous complete-potential structure framework together with the notion of strain- and stress-partitioning in<br />
terms of separate contributions of several submechanisms (viscoelastic and viscoplastic) to the thermodynamic functions<br />
(stored energy and dissipation) a detailed viscoelastoplastic multimechanism characterization of a specific hardening<br />
functional form of the model is presented and discussed. TIMETAL 21S is the material of choice as a comprehensive test<br />
matrix, including creep, relaxation, constant strain-rate tension tests, etc. are available at various temperatures. Discussion of<br />
these correlations tests, together with comparisons to several other experimental results, are given to assess the performance<br />
and predictive capabilities of the present model particularly with regard to the notion of hardening saturation as well as the<br />
interaction of multiplicity of dissipative (reversible/irreversible) mechanisms.<br />
Author<br />
Elastoplasticity; Viscoelasticity; Viscoplasticity; Hardening (Materials); Models; Thermodynamics; Titanium Alloys<br />
<strong>2003</strong>0033070 NASA Goddard Space Flight Center, Greenbelt, MD, USA<br />
The FERRUM Project: Experimental Transition Probabilities of [Fe II] and Astrophysical Applications<br />
Hartman, H.; Derkatch, A.; Donnelly, M. P.; Gull, T.; Hibbert, A.; Johannsson, S.; Lundberg, H.; Mannervik, S.; Norlin, L.<br />
-O.; Rostohar, D.; November <strong>16</strong>, 2002; 8 pp.; In English<br />
Contract(s)/Grant(s): GR/L20276; HST-7302; Copyright; Avail: CASI; A02, Hardcopy<br />
We report on experimental transition probabilities for thirteen forbidden [Fe II] lines originating from three different<br />
metastable Fe II levels. Radiative lifetimes have been measured of two metastable states by applying a laser probing technique<br />
on a stored ion beam. Branching ratios for the radiative decay channels, i.e. M1 and E2 transitions, are derived from observed<br />
48