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1998
DOI: 10.1006/jsvi.1998.1640
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A Continuous Cracked Beam Vibration Theory

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Cited by 444 publications
(246 citation statements)
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“…Figure 6 shows the first natural frequency ratio ( c ω ω ) versus the crack depth ratio α for a simply supported beam with a surface crack at mid-span. Compared with the predictions obtained using the damage finite element by Potirniche et al [1], the first natural frequency reduction predicted by the proposed improved two-dimensional finite element matches very well with the experiments results by Chondros et al [7]. , is considered.…”
Section: Simply Supported Beam With a Surface Cracksupporting
confidence: 76%
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“…Figure 6 shows the first natural frequency ratio ( c ω ω ) versus the crack depth ratio α for a simply supported beam with a surface crack at mid-span. Compared with the predictions obtained using the damage finite element by Potirniche et al [1], the first natural frequency reduction predicted by the proposed improved two-dimensional finite element matches very well with the experiments results by Chondros et al [7]. , is considered.…”
Section: Simply Supported Beam With a Surface Cracksupporting
confidence: 76%
“…An aluminium beam [7] , is considered. In the numerical study the crack depth ratio α ( a H ) is varied from 0 to 0.5.…”
Section: Simply Supported Beam With a Surface Crackmentioning
confidence: 99%
“…In both cases, a crack function representing the perturbation in the stress field induced by the crack is considered. Chondros et al [18] have developed a continuous cracked beam vibration theory. They considered that crack introduces a continuous change in the flexibility in its neighborhood and models it by incorporating a displacement field consistent with the singularity.…”
Section: Introductionmentioning
confidence: 99%
“…In 1978 Adams et al [2] investigated the case of damage that was modelled by an axial spring (axial damage model), but there is absent a calculating stiffness of the spring. Then transverse (rotational) model of damage has been developed and validated by a general theory of damaged beams [3] that makes it be possible to determine the stiffness of the equivalent spring as a function of damage depth. Using the transverse model of damage Rizos et al [4] have constructed the frequency equation for cantilever beam.…”
Section: Introductionmentioning
confidence: 99%
“…G . Chondros and A. D. Dimarogonas et al [3], we have If a parameter f3 = EI/KL is introduced for description of relative flexibility of the spring and called here damage magnitude, then (3=0 (K=oo) will correspond to the undamaged case and f3max =138.5 (h/ L), when a= h -to the completely damaged one. Furthermore, at the damage sit it's must be hold the condition…”
mentioning
confidence: 99%