1994
DOI: 10.1111/j.1460-2695.1994.tb00810.x
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Stress Intensity Factors for Cracks at Fastener Holes

Abstract: Transmission and reflection photoelasticity has been used to determine the stress intensity factors for artificial cracks emanating from a hole in two-dimensional tensile plates. Three geometries were investigated, namely a free hole, a pin-loaded hole and a hole with an interference-fit pin. All these cases relate to situations commonly found in aircraft structures. The results have been compared where possible with analytical data and a good correlation was found for these cases.

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Cited by 20 publications
(12 citation statements)
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“…By contrast, because photoelasticity provides only the elastic strain fields in the birefringent coating, it is mainly used to determine experimentally stress intensity factors for complex loading modes in components where the fields are predominantly linear elastic [24][25][26][27]. Because constraint effects that arise in elastic-plastic materials are then weak, such experimental data agree reasonably well with theoretical plane-stress solutions.…”
Section: Introductionsupporting
confidence: 73%
“…By contrast, because photoelasticity provides only the elastic strain fields in the birefringent coating, it is mainly used to determine experimentally stress intensity factors for complex loading modes in components where the fields are predominantly linear elastic [24][25][26][27]. Because constraint effects that arise in elastic-plastic materials are then weak, such experimental data agree reasonably well with theoretical plane-stress solutions.…”
Section: Introductionsupporting
confidence: 73%
“…For a crack propagating through elastic material, the crack flanks would be expected to open as if they were hinged at the crack tip, although in practice the ‘hinge’ is likely to be in the plastic zone ahead of the visible crack tip where void formation within a process zone previews the formation of the crack 42 . This behaviour is evident in the coupon with the unexpanded hole in which, for all crack lengths, the COD decreases approximately linearly from the edge of the hole to zero at a point between 0.6 mm and 1.2 mm ahead of the visible crack tip; values that lie between the plane stress estimate for plastic zone radius (1.83 to 2.6 mm) and plane strain estimates of the plastic zone radius (0.30 to 0.43 mm) 46,47 . In the coupon with the unexpanded hole, the maximum COD, which occurs at the edge of the hole in the UH coupon increases approximately linearly with crack length from about 0.02 mm at a = 1 mm to about 0.05 mm at a = 3.7 mm.…”
Section: Resultsmentioning
confidence: 83%
“…Transmission photoelasticity suffers from the drawback (particularly as far as fatigue cracks are concerned), that the material behaviour in the process zone will differ from that in the main classes of engineering materials. Reflection photoelasticity can, of course, be used to circumvent this, but is more complex experimentally [3]. Other experimental techniques employed have included caustics [4], interferometry [5], and point measurements with strain gauges [6].…”
Section: Introductionmentioning
confidence: 99%