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Stress state in tempered glass plate and determination of heat-transfer rate

Three-dimensional stress state in thermally tempered glass plate, determination of the stress components and a photoelastic method of evaluating heat-transfer rate during tempering are described

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Abstract

Thermal tempering is widely used to manufacture safety glass for economic as well as for certain safety measures. Laboratory investigations of the tempering process and the resultant strengthening effect are generally limited to rectangular specimens. Results are, therefore, appropriate for this particular geometry. This paper describes a simple stress-state model of a tempered flat glass specimen. the model, developed using photoelastic equations to determine the three-dimensional stress components, was used to predict the transient birefringence in a rectangular glass specimen subjected to uniform and symmetrical heat-transfer conditions, at a temperature where glass behaves as a perfect elastic material with no stress relaxation within the experimental time. A method of determining the coefficient of heat-transfer rate was then developed based on the analysis of the transient birefringence. This technique uses the glass specimen as an optical transducer, and does not affect, in any way, the natural flow of heat by forced convection or contact cooling.

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Abbreviations

C o :

stress-optical coefficient

c :

subscript for central mid-plane value, specific heat

Δd :

scattered-light fringe separation

E :

Young's modulus

h 1 ,h 2 ,h 3 :

coefficient of heat-transfer rate in directionsx 1 ,x 2 andx 3 , respectively

K :

constant

k :

true thermal conductivity

\(2\ell _1 \) :

length

\(2\ell _2 \) :

width

\(2\ell _3 \) :

thickness

s :

subscript for surface value, half thickness

R 1 ,R 2 ,R 3 :

relative retardations in polarized light propagating alongx 1 ,x 2 andx 3 respectively

x 1 ,x 2 ,x 3 :

Cartesian coordinates

α:

coefficient of linear thermal expansion

\(\beta = \frac{k}{{\rho c}}\) :

thermal diffusivity

θ:

excess temperature over the ambient at any time

θ i :

initial excess temperature

ϱ:

density

σ1, σ2, σ3 :

principal stresses

σ i j, σ i k :

components of principal stress σ i alongi due to the heat flow alongj andk, respectively,i # j # k

λ:

wavelength of light

ν:

Poisson's ratio

τ:

time in seconds

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Sinha, N.K. Stress state in tempered glass plate and determination of heat-transfer rate. Experimental Mechanics 18, 25–34 (1978). https://doi.org/10.1007/BF02326554

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  • DOI: https://doi.org/10.1007/BF02326554

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