Issue 19

P. K. Pradhan et alii, Frattura ed Integrità Strutturale, 19 (2012) 51-60; DOI: 10.3221/IGF-ESIS.19.05 59 Figure 16 : Void coalescence in front of crack. Figure 17 : Multi-crack formation. For specimen with smaller holes (of size 0.5mm), slip phenomena are observed as shown in Fig. 18. In this case, during slipping, load increases slightly and then decreases when fracture starts. As a very close approximation, the slip or glide can be considered analogous to the distortion produced in the pile of cards when it pushed from one end. Slip phenomena occur due to micro voids and dislocation movement in the materials. That slip phenomena promote for crack formation and propagation, which may be considered as Mode-II fracture. (a) Slip plane area near the bottom most hole (b) Crack tends to form by slip plane Figure 18 : Slipping Phenomena in the specimen with 0.5 mm hole. C ONCLUSIONS he following conclusions are drawn from the present experimental study: I. If a material is initially unloaded beyond yield point, then in reloading its Young’s Modulus value decreases but the elastic limit increases. II. During tensile deformation beyond UTS two or more cracks may be created independently by coalescence of micro void instead of single crack growth. III. Though the grain boundaries of the material are brittle, the grains are ductile in nature. IV. During the progress of crack, the crack path is not truly linear, it moves in a zigzag path by joining the voids present just in front of the crack front. V. The mechanical properties of specimen with holes decreases, compared to specimen without any hole. VI. By increasing the angle of orientation to the tensile axis, the YP, UTS, E and fracture strain increase upto 45° and then decreases. It indicates that with same amount of voids, present in different positions, the mechanical properties of the material are altered. VII. The specimen with square array holes at 0° (or 90°) to the tensile axis exhibits least mechanical properties. Shear band is not found in this case. VIII. No yield point phenomenon is observed in specimen with holes. T