Summary
A method of determining the thermal stresses in a flat rectangular isotropic plate of constant thickness with arbitrary temperature distribution in the plane of the plate and with no variation in temperature through the thickness is presented. The thermal stress have been obtained in terms of Fourier series and integrals that satisfy the differential equation and the boundary conditions. Several examples have been presented to show the application of the method.
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Abbreviations
- x, y :
-
rectangular coordinates
- σ x, σy :
-
direct stresses
- τ xy :
-
shear stress
- ø :
-
Airy's stress function
- E :
-
Young's modulus of elasticity
- α :
-
coefficient of thermal expansion
- T :
-
temperature
- ▽ 2 :
-
Laplace operator: \( - \left( {\frac{{\partial ^2 }}{{\partial x^2 }} + \frac{{\partial ^2 }}{{\partial y^2 }}} \right)\)
- ▽ 4 :
-
biharmonic operator \(\left( {\frac{{\partial ^4 }}{{\partial x^4 }} + 2\frac{{\partial ^4 }}{{\partial x^2 \partial y^2 }} + \frac{{\partial ^4 }}{{\partial y^4 }}} \right)\)
- 2a :
-
length of the plate
- 2b :
-
width of the plate
- a/b :
-
aspect ratio
- a mr, bms, cnr, dns :
-
Fourier coefficients defined in equation (6)
- α m=mπ/a m=1, 2, 3, ...:
-
β n=nπ/2a n=1, 3, 5, ...
- γ r=rπ/b r=1, 2, 3, ...:
-
δ s=sπ/2b s=1, 3, 5, ...
- A m, Bm, Cn, Dn, Er, Fr, Gs, Hs :
-
Fourier coefficients
- K rand L s :
-
Fourier coefficients defined in equation (20)
- σ∞ :
-
direct stress at infinity
- T 1(x, y):
-
temperature distribution symmetrical in x and y
- T 2(x, y):
-
temperature distribution symmetrical in x and antisymmetrical in y
- T 3(x, y):
-
temperature distribution antisymmetrical in x and symmetrical in y
- T 4(x, y):
-
temperature distribution antisymmetrical in x and y
References
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Sundara Raja Iyengar, K.T., Chandrashekhara, K. Thermal stresses in rectangular plates. Appl. sci. Res. 15, 141–160 (1966). https://doi.org/10.1007/BF00411552
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DOI: https://doi.org/10.1007/BF00411552