Journal of Mechanics of Materials and Structures vol. 5 (2010 ... - MSP

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814 YING LI AND CHANG-JUN CHENG Figure 3. Variation of deflection W and void moment ψ of EVB with X, for various a1. Figure 4. Variation of deflection W and void moment ψ of TEVB with X, for various a1. Figure 5. Variation of deflection W and void moment ψ of TEVB with X, for various a3. Figure 6. Variation of deflection W and void moment ψ of EVB with X, for various a4.
A NONLINEAR MODEL OF THERMOELASTIC BEAMS WITH VOIDS, WITH APPLICATIONS 815 Figure 7. Variation of deflection W and void moment ψ of TEVB with X, for various a4. Figure 8. Variation of deflection W of EVB and void moment ψ of TEVB with X, for various a2. Figure 9. Variation of deflection W and void moment ψ of TEVB with X, for various a5. deflection of TEB increases with an increase in a2, as seen in Figure 8a, and so does the deflection of TEVB. In contrast, the void moment of TEVB decreases with an increase in a2, as seen in Figure 8b. Effect of a5. The parameter a5 is a coupling one of volume fraction and temperature field. Figure 9 shows that the deflection of TEVB varies from negative to positive with an increase in a5, while the void moment varies from positive to negative. Effect of a10 and a11. When a10 = 0, the boundary of the beam is adiabatic, meanwhile, the temperature is independent of a11 but just dependent of the thickness-length ratio of the beam. When a10 → ∞, the
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Journal of Mechanics of Materials a
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AXIAL COMPRESSION OF HOLLOW ELASTIC
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JOURNAL OF MECHANICS OF MATERIALS A
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GENETIC MODELING OF COMPRESSIVE STR
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Journal of Mechanics of Materials and Structures vol. 5 (2010 ... - MSP

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