Strain Rate Concentration Factor for Round and Flat Test Specimens

2018 ◽  
pp. 521-529
Author(s):  
Nao-Aki Noda ◽  
Rei Takaki ◽  
Yunong Shen ◽  
Akane Inoue ◽  
Yoshikazu Sano ◽  
...  
Keyword(s):  
Strain Rate ◽  
Concentration Factor

Strain rate concentration factor for flat notched specimen to predict impact strength for polymeric materials

2019 ◽  
Vol 131 ◽  
pp. 141-157 ◽  
Author(s):  
Nao-Aki Noda ◽  
Rei Takaki ◽  
Yunong Shen ◽  
Akane Inoue ◽  
Yoshikazu Sano ◽  
...  
Keyword(s):  
Impact Strength ◽  
Strain Rate ◽  
Concentration Factor ◽  
Polymeric Materials ◽  
Notched Specimen

scholarly journals Strain rate concentration factor in comparison with stress concentration factor of a circumferential notch in a round bar specimen

2017 ◽  
Vol 83 (851) ◽  
pp. 17-00034-17-00034
Author(s):  
Nao-Aki NODA ◽  
Daichi AKAGI ◽  
Yunong SHEN ◽  
Rei TAKAKI ◽  
Tomohiro IKEDA ◽  
...  
Keyword(s):  
Stress Concentration ◽  
Strain Rate ◽  
Stress Concentration Factor ◽  
Concentration Factor ◽  
Round Bar ◽  
Circumferential Notch

Strain rate concentration factor in comparison with stress concentration factor of notched flat bar specimens

2018 ◽  
Vol 2018.71 (0) ◽  
pp. D11
Author(s):  
Akane INOUE ◽  
Nao-Aki NODA ◽  
Yunong SHEN ◽  
Rei TAKAKI ◽  
Yoshikazu SANO ◽  
...  
Keyword(s):  
Stress Concentration ◽  
Strain Rate ◽  
Stress Concentration Factor ◽  
Concentration Factor

Relationship between Strain Rate Concentration Factor and Stress Concentration Factor for Round and flat Test Specimens

2019 ◽  
Vol 2019.72 (0) ◽  
pp. G25
Author(s):  
Rei TAKAKI ◽  
Nao-Aki NODA ◽  
Yunong SHEN ◽  
Akane INOUE ◽  
Yoshikazu SANO ◽  
...  
Keyword(s):  
Stress Concentration ◽  
Strain Rate ◽  
Stress Concentration Factor ◽  
Concentration Factor

Relationship between strain rate concentration factor and stress concentration factor

2017 ◽  
Vol 90 ◽  
pp. 218-227 ◽  
Author(s):  
Nao-Aki Noda ◽  
Yunong Shen ◽  
Rei Takaki ◽  
Daichi Akagi ◽  
Tomohiro Ikeda ◽  
...  
Keyword(s):  
Stress Concentration ◽  
Strain Rate ◽  
Stress Concentration Factor ◽  
Concentration Factor

Dislocation Substructures Produced During Tensile, Creep, and Fatigue Deformation of Ti3Al at 700°C

1977 ◽  
Vol 35 ◽  
pp. 272-273
Author(s):  
S. M. L. Sastry
Keyword(s):  
Intermetallic Compound ◽  
Strain Rate ◽  
Tensile Creep ◽  
Slip Systems ◽  
Slip Vector ◽  
Superlattice Structure ◽  
Slip Activity ◽  
Dislocation Arrangement ◽  
Ordered Intermetallic ◽  
Tangled Dislocation

Ti3Al is an ordered intermetallic compound having the DO19-type superlattice structure. The compound exhibits very limited ductility in tension below 700°C because of a pronounced planarity of slip and the absence of a sufficient number of independent slip systems. Significant differences in slip behavior in the compound as a result of differences in strain rate and mode of deformation are reported here.Figure 1 is a comparison of dislocation substructures in polycrystalline Ti3Al specimens deformed in tension, creep, and fatigue. Slip activity on both the basal and prism planes is observed for each mode of deformation. The dominant slip vector in unidirectional deformation is the a-type (b) = <1120>) (Fig. la). The dislocations are straight, occur for the most part in a screw orientation, and are arranged in planar bands. In contrast, the dislocation distribution in specimens crept at 700°C (Fig. lb) is characterized by a much reduced planarity of slip, a tangled dislocation arrangement instead of planar bands, and an increased incidence of nonbasal slip vectors.

Quantitative analysis of in situ straining experiments in the case of strong frictional forces

1978 ◽  
Vol 36 (1) ◽  
pp. 570-571
Author(s):  
F. Louchet ◽  
L.P. Kubin
Keyword(s):  
Strain Rate ◽  
Radiation Effects ◽  
Dislocation Line ◽  
Critical Length ◽  
Local Strain ◽  
Local Flow ◽  
Double Kink ◽  
Dislocation Densities ◽  
Frictional Forces ◽  
Local Strain Rate

Investigation of frictional forces -Experimental techniques and working conditions in the high voltage electron microscope have already been described (1). Care has been taken in order to minimize both surface and radiation effects under deformation conditions.Dislocation densities and velocities are measured on the records of the deformation. It can be noticed that mobile dislocation densities can be far below the total dislocation density in the operative system. The local strain-rate can be deduced from these measurements. The local flow stresses are deduced from the curvature radii of the dislocations when the local strain-rate reaches the values of ∿ 10-4 s-1.For a straight screw segment of length L moving by double-kink nucleation between two pinning points, the velocity is :where ΔG(τ) is the activation energy and lc the critical length for double-kink nucleation. The term L/lc takes into account the number of simultaneous attempts for double-kink nucleation on the dislocation line.

Observations of dislocation interactions with recrystallized grain boundaries

1988 ◽  
Vol 46 ◽  
pp. 628-629
Author(s):  
C. W. Price
Keyword(s):  
Dislocation Density ◽  
Grain Boundary ◽  
Strain Rate ◽  
Grain Boundaries ◽  
Dislocation Structure ◽  
Hot Deformation ◽  
Static Recrystallization ◽  
High Dislocation Density ◽  
High Angle ◽  
Dislocation Interactions

Little evidence exists on the interaction of individual dislocations with recrystallized grain boundaries, primarily because of the severely overlapping contrast of the high dislocation density usually present during recrystallization. Interesting evidence of such interaction, Fig. 1, was discovered during examination of some old work on the hot deformation of Al-4.64 Cu. The specimen was deformed in a programmable thermomechanical instrument at 527 C and a strain rate of 25 cm/cm/s to a strain of 0.7. Static recrystallization occurred during a post anneal of 23 s also at 527 C. The figure shows evidence of dissociation of a subboundary at an intersection with a recrystallized high-angle grain boundary. At least one set of dislocations appears to be out of contrast in Fig. 1, and a grainboundary precipitate also is visible. Unfortunately, only subgrain sizes were of interest at the time the micrograph was recorded, and no attempt was made to analyze the dislocation structure.

Observation of dislocations in dynamically loaded Cu-SiO2

1986 ◽  
Vol 44 ◽  
pp. 424-425
Author(s):  
D. S. Pritchard
Keyword(s):  
Electron Microscope ◽  
Strain Rate ◽  
Single Crystal ◽  
Transmission Electron Microscope ◽  
Volume Fraction ◽  
Screw Dislocations ◽  
Spherical Inclusions ◽  
Transmission Electron ◽  
Crystal Dispersion ◽  
Strain Rate Loading

The effect of varying the strain rate loading conditions in compression on a copper single crystal dispersion-hardened with SiO2 particles has been examined. These particles appear as small spherical inclusions in the copper lattice and have a volume fraction of 0.6%. The structure of representative crystals was examined prior to any testing on a transmission electron microscope (TEM) to determine the nature of the dislocations initially present in the tested crystals. Only a few scattered edge and screw dislocations were viewed in those specimens.

The effects of strain and strain rate on residual microstructures in copper

1986 ◽  
Vol 44 ◽  
pp. 420-421
Author(s):  
M. F. Stevens ◽  
P. S. Follansbee
Keyword(s):  
Strain Rate ◽  
Applied Stress ◽  
Threshold Stress ◽  
Rate Sensitivity ◽  
Viscous Drag ◽  
Strain Rates ◽  
Strain And Strain Rate ◽  
Threshold Strength ◽  
Mechanism Transition ◽  
Intrinsic Strength

The strain rate sensitivity of a variety of materials is known to increase rapidly at strain rates exceeding ∼103 sec-1. This transition has most often in the past been attributed to a transition from thermally activated guide to viscous drag control. An important condition for imposition of dislocation drag effects is that the applied stress, σ, must be on the order of or greater than the threshold stress, which is the flow stress at OK. From Fig. 1, it can be seen for OFE Cu that the ratio of the applied stress to threshold stress remains constant even at strain rates as high as 104 sec-1 suggesting that there is not a mechanism transition but that the intrinsic strength is increasing, since the threshold strength is a mechanical measure of intrinsic strength. These measurements were made at constant strain levels of 0.2, wnich is not a guarantee of constant microstructure. The increase in threshold stress at higher strain rates is a strong indication that the microstructural evolution is a function of strain rate and that the dependence becomes stronger at high strain rates.

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