Residual Strength and Fatigue Lifetime of ... - Solid Mechanics

Residual Strength and Fatigue Lifetime of ... - Solid Mechanics Residual Strength and Fatigue Lifetime of ... - Solid Mechanics

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(2.2) where and for plane stress and plane strain, respectively. E and are Young’s modulus and Poisson’s ratio, respectively. Normal force and moment in the TSD specimen can be determined from the vertical force P and the tilt angle by (2.3) (2.4) For the reduced formulation where ==0 Finally, the energy release rate can be calculated by Regarding the mode-mixity it was revealed that the mode-mixity for a conventional TSD specimen remains quite unaffected by the tilt angle (Li and Carlsson, 2001). Furthermore, it was discovered that the unreinforced TSD specimens display positive mode-mixity phase angles for tilt angles up to around 80 for all analysed PVC core materials, thus provoking the crack to kink into the core (Berggreen and Carlsson, 2010). To increase the range of achieved mode-mixities by the TSD specimen, two modified designs of the TSD specimen were proposed by Berggreen and Carlsson (2010). In the first modified design the upper face sheet of the TSD specimen is reinforced by a thick stiff steel plate to increase the stiffness of the loaded face sheet as shown in Figure 2.10. It was shown that by reinforcing the upper face sheet with a stiff steel plate the range of phase angles is expanded because of increasing shear loading and crack tip root rotation in the specimen. 24 (2.5) (2.6) (2.7)

Figure 2.10: Schematic presentation of the first modified TSD specimen. Further modifications were made by reducing the global shear deformation of the core by reinforcing the left edge of the TSD specimen by placing a metal block, see Figure 2.11. To avoid compression failure of the core at the right end of the reinforced TSD specimen due to rotation of the reinforced face sheet, a short link is pin-attached between the rigid base of the test rig and the centre of the steel reinforcement bar on both sides of the TSD specimen, see Figure 2.11. Figure 2.11: Schematic presentation of the second modified TSD specimen. 25

(2.2)<br />

where <strong>and</strong> for plane stress <strong>and</strong> plane strain, respectively. E <strong>and</strong> are<br />

Young’s modulus <strong>and</strong> Poisson’s ratio, respectively. Normal force <strong>and</strong> moment in the TSD<br />

specimen can be determined from the vertical force P <strong>and</strong> the tilt angle by<br />

(2.3)<br />

(2.4)<br />

For the reduced formulation where ==0<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

Finally, the energy release rate can be calculated by<br />

<br />

<br />

<br />

<br />

<br />

Regarding the mode-mixity it was revealed that the mode-mixity for a conventional TSD<br />

specimen remains quite unaffected by the tilt angle (Li <strong>and</strong> Carlsson, 2001). Furthermore, it was<br />

discovered that the unreinforced TSD specimens display positive mode-mixity phase angles for<br />

tilt angles up to around 80 for all analysed PVC core materials, thus provoking the crack to kink<br />

into the core (Berggreen <strong>and</strong> Carlsson, 2010). To increase the range <strong>of</strong> achieved mode-mixities<br />

by the TSD specimen, two modified designs <strong>of</strong> the TSD specimen were proposed by Berggreen<br />

<strong>and</strong> Carlsson (2010). In the first modified design the upper face sheet <strong>of</strong> the TSD specimen is<br />

reinforced by a thick stiff steel plate to increase the stiffness <strong>of</strong> the loaded face sheet as shown in<br />

Figure 2.10. It was shown that by reinforcing the upper face sheet with a stiff steel plate the<br />

range <strong>of</strong> phase angles is exp<strong>and</strong>ed because <strong>of</strong> increasing shear loading <strong>and</strong> crack tip root rotation<br />

in the specimen.<br />

24<br />

(2.5)<br />

(2.6)<br />

(2.7)

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