Abstract:Residual stresses play an important role in controlling fracture behavior in ion-exchanged glass. In this work, the internal tensile stress resulting from ion exchange is measured using conventional birefringence methods. By progressively etching thin layers from the glass surface, the compressive stress in the removed layer can then be determined from the change in the compensating internal tensile stress, producing a stress profile as a function of depth. Specimen geometry, surface roughness, and configurati… Show more
“…Equation (24) was formulated in such a way by Brodland and Dolovich [34] in order to produce symmetric, self-equilibrating stress distributions, like those that typically arise in a uniformly strengthened glass plate, for specimens that extend from y = 0 to y = 2D. Stress equilibrium through the thickness is granted:…”
“…We suggest replacing the measurement of central core tensile stresses with gradient scattered light method instead of currently used transmission photoelasticity [24] or originally used scattered light method [11]. Each time when a layer with thickness of 1-2 lm is etched away using HF acid the alternation of full stress profile is induced.…”
Section: Possible Additional Applications New Enhanced Version Of Bramentioning
confidence: 99%
“…In order to achieve increased accuracy, Abrams et al [24] replaced the scattered light measurement with transmission photoelasticity for central tension measurement in the Bradshaw's method. Sglavo et al [12] introduced curvature measurements for determining the stress profile in chemically strengthened glass.…”
Section: Introductionmentioning
confidence: 99%
“…Two separate fringe patterns are recorded-one for the extraordinary ray (also referred to as TM-wave) and other for the ordinary ray (TE-wave). The DSR method presented by Kishii [13] assumes that the stress profile is linear, which makes it unsuitable for measuring stress profiles with complex shape encountered in chemically strengthened lithium aluminosilicate glass or double ion-exchanged [24][25][26][27] glass. The method of surface refractometry can be considered as indirect measurement because no info is gathered from specific depth, but it relies on analysis of fringe pattern produced by resurgent light.…”
A new non-destructive gradient scattered light method is presented for micronscale stress profile measurement in chemically strengthened (chemically tempered, ion exchanged) glass. Direct non-destructive stress measurement in the surface layer (\100 lm) of chemically strengthened glass is reported for the first time. This is accomplished by passing a narrow laser beam through the surface layer of the glass at a considerably large incidence angle of 81.9°. The theory of gradient scattered light method is based on the ray tracing of ordinary and extraordinary rays in chemically strengthened glass and calculating the optical retardation distribution along the curved ray path. The experimental approach relies on recording the scattered light intensity and calculating the optical retardation distribution from it. The stress profile is measured in a chemically strengthened (8 h at 480°C in a salt mixture of 80 mol% KNO 3 and 20 mol% NaNO 3 ) lithium aluminosilicate glass plate to illustrate the capability of the method. Measured surface compressive stress was -1053 MPa and case depth 365 lm. Method is validated with transmission photoelasticity. The method could also be used for stress profile measurement in all transparent flat materials (such as very thin thermally tempered glass slabs or polymers). Additional new applications could be: (1) enhanced version of Bradshaw's surface layer etching method for stress profile measurement in case of ultra-thin case depths \20 lm;(2) micron-scale non-destructive tomography of layered polymeric gradient-refractive-index materials. The experimental procedure is developed to the level of full automation and the measurement time is less than 10 s.
“…Equation (24) was formulated in such a way by Brodland and Dolovich [34] in order to produce symmetric, self-equilibrating stress distributions, like those that typically arise in a uniformly strengthened glass plate, for specimens that extend from y = 0 to y = 2D. Stress equilibrium through the thickness is granted:…”
“…We suggest replacing the measurement of central core tensile stresses with gradient scattered light method instead of currently used transmission photoelasticity [24] or originally used scattered light method [11]. Each time when a layer with thickness of 1-2 lm is etched away using HF acid the alternation of full stress profile is induced.…”
Section: Possible Additional Applications New Enhanced Version Of Bramentioning
confidence: 99%
“…In order to achieve increased accuracy, Abrams et al [24] replaced the scattered light measurement with transmission photoelasticity for central tension measurement in the Bradshaw's method. Sglavo et al [12] introduced curvature measurements for determining the stress profile in chemically strengthened glass.…”
Section: Introductionmentioning
confidence: 99%
“…Two separate fringe patterns are recorded-one for the extraordinary ray (also referred to as TM-wave) and other for the ordinary ray (TE-wave). The DSR method presented by Kishii [13] assumes that the stress profile is linear, which makes it unsuitable for measuring stress profiles with complex shape encountered in chemically strengthened lithium aluminosilicate glass or double ion-exchanged [24][25][26][27] glass. The method of surface refractometry can be considered as indirect measurement because no info is gathered from specific depth, but it relies on analysis of fringe pattern produced by resurgent light.…”
A new non-destructive gradient scattered light method is presented for micronscale stress profile measurement in chemically strengthened (chemically tempered, ion exchanged) glass. Direct non-destructive stress measurement in the surface layer (\100 lm) of chemically strengthened glass is reported for the first time. This is accomplished by passing a narrow laser beam through the surface layer of the glass at a considerably large incidence angle of 81.9°. The theory of gradient scattered light method is based on the ray tracing of ordinary and extraordinary rays in chemically strengthened glass and calculating the optical retardation distribution along the curved ray path. The experimental approach relies on recording the scattered light intensity and calculating the optical retardation distribution from it. The stress profile is measured in a chemically strengthened (8 h at 480°C in a salt mixture of 80 mol% KNO 3 and 20 mol% NaNO 3 ) lithium aluminosilicate glass plate to illustrate the capability of the method. Measured surface compressive stress was -1053 MPa and case depth 365 lm. Method is validated with transmission photoelasticity. The method could also be used for stress profile measurement in all transparent flat materials (such as very thin thermally tempered glass slabs or polymers). Additional new applications could be: (1) enhanced version of Bradshaw's surface layer etching method for stress profile measurement in case of ultra-thin case depths \20 lm;(2) micron-scale non-destructive tomography of layered polymeric gradient-refractive-index materials. The experimental procedure is developed to the level of full automation and the measurement time is less than 10 s.
“…17 As-received plates were cut to dimensions of 100 mm × 50 mm, and polished to improve optical transmission, then processed in the ion exchange salt baths, producing a compressive surface stress and a compensating internal tensile stress. The tensile stresses in the interior of each specimen were measured using conventional optical retardation techniques.…”
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