Question 11.4: A [(02/90)2]s graphite–epoxy laminate is cured at 175°C and ...

A [(0_2/90)2]_s graphite–epoxy laminate is cured at 175°C and then cooled to room temperature (20°C). After cooling, the flat laminate is trimmed to in-plane dimensions of 300 × 150 mm and mounted in an assembly that provides type S4 simple supports along all four edges. The x-axis is defined parallel to the 300 mm edge (i.e., a = 0.3 m, b = 0.15 m).
The laminate is then subjected to a uniform in-plane tensile loading N_{xx} = N_{yy} = 50 kN/m and uniform transverse loading q(x,y) = 100 kPa. Temperature remains constant and no change in moisture content occurs (ΔM = 0). Plot the out-of-plane displacements induced along the centerline defined by y = 0.075 m. Use the properties listed for graphite– epoxy in Table 3.1, and assume each ply has a thickness of 0.125 mm.

TABLE 3.1
Typical Properties of Common Unidirectional Composites

Property Glass/ Epoxy Kevlar/ Epoxy Graphite/ Epoxy
E_{11} 55 GPa 100 GPa 170 GPa
(8.0 Msi) (15 Msi) (25 Msi)
E_{22} 16 GPa 6 GPa 10 GPa
(2.3 Msi) (0.90 Msi) (1.5 Msi)
ν_{12} 0.28 0.33 0.3
G_{12} 7.6 GPa 2.1 GPa 13 GPa
(1.1 Msi) (0.30 Msi) (1.9 Msi)
 \sigma _{11}^{fT} 1050 MPa 1380 MPa 1500 MPa
(150 ksi) (200 ksi) (218 ksi)
\sigma _{11}^{fC} 690 MPa 280 MPa 1200 MPa
(100 ksi) (40 ksi) (175 ksi)
\sigma _{22}^{ff} 45 MPa 35 MPa 50 MPa
(5.8 ksi) (2.9 ksi) (7.25 ksi)
\sigma _{22}^{fC} 120 MPa 105 MPa 100 MPa
(16 ksi) (15 ksi) (14.5 ksi)
\tau ^f_{22} 40 MPa 40 MPa 90 MPa
(4.4 ksi) (4.0 ksi) (13.1 ksi)
\alpha _{11} 6.7 μm/m−°C −3.6 μm/m−°C −0.9 μm/m−°C
(3.7 μin./in.\boxtimes  °F) (−2.0 μin./in.−°F) (−0.5 μin./in.−°F)
\alpha _{22} 25 μm/m−°C 58 μm/m−°C 27 μm/m−°C
(14 μin./in.−°F) (32 μin./in.−°F) (15 μin./in.−°F)
\beta _{11} 100 μm/m−%M 175 μm/m−%M 50 μm/m−%M
(100 μin./in.−%M) (175 μin./in.−%M) (50 μin./in.−%M)
\beta _{22} 1200 μm/m−%M 1700 μm/m−%M 1200 μm/m−%M
(1200 μin./in.−%M) (1700 μin./in.−%M) (1200 μin./in.−%M)
Ply 0.125 mm 0.125 mm 0.125 mm
Thickness (0.005 in.) (0.005 in.) (0.005 in.)
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A [(0_2/90)2]_s graphite–epoxy laminate was also considered in Example Problem 11.1, and numerical values for the [ABD] matrix are listed there.
As before, the 12-ply laminate has a total thickness t = 1.5 mm and aspect ratio R = a/b = 2.0.

The double Fourier series expansion of a uniform transverse loading was discussed in Section 10.4. The coefficients in the Fourier series expansion were found to be

q_{mn}=\frac{16q_0}{\pi ^2mn},m,n= odd integers

Combining these coefficients with Equation 11.28c

w(x,y)=\frac{R^4b^4}{\pi^4} \sum\limits_{m=1}^{\infty }{}\sum\limits_{n=1}^{\infty }{\frac{q_{mn}sin(m\pi x/a)sin(n\pi y/b)}{\left[D_{11}m^4+2(D_{12}+2D_{66})(mnR)^2+D_{22}(nR)^4+(a^2/\pi ^2)\left\{N_{xx}m^2+N_{yy}(nR)^2\right\} \right] } }        (11.28c)

allows prediction of out-of-plane displacements. A plot of these displacements along the centerline of the plate defined by y = b/2 = 0.075 m is shown in Figure 11.7. Curves are shown based on a 1-term expansion (i.e., m, n = 1), a 4-term expansion (m, n = 1, 3), and a 9-term expansion (m, n = 1, 3, 5). As would be expected due to symmetry, out-of-plane displacement is maximum at the center of the plate. The solution converges rapidly. The maximum displacement predicted on the basis of a 1-, 4-, and 9-term expansion equals 5.27, 4.71, and 4.78   mm^3  , respectively. If 100 terms were used (m, n = 1,3, . . ., 19) the maximum predicted displacement is 4.77 mm.

 

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