Abstract

New composite anisotropic materials (CM) glass, carbon and boric plastics are more and more frequently used in engineering construction. By tuning strength and stiffness characteristics of CM under tension or bending with their density or price it is possible to get laminated construction of maximum strength and stiffness and minimum mass or price. The purpose of this work is to analyse regularity of distribution of stiffness or strains and stresses in three-layer bars, subjected to tension or bending by changing geometric characteristics of layer, materials and their position in cross-section of bars. The bar layers were formed of carbon plastic (A), hot (Sk) and cold hardening (Sc) glass plastics and epoxy resin (D). Equations were obtained describing the alteration of bar and beam stiffness and the alteration of normal stresses, all depending on relative thichness Ψ of bar or beam. The relative thickness Ψ is the ratio of middle layer height to the whole height. It has been shown that maximum stresses in exterior and middle layers (with elasticity modules E1 and E2accordingly) become equal when Ψ = E1 /E2 . The intensity of stiffness alteration depends on the magnitude of | E2 —E1 |. In the case of positive magnitude, the bar or beam stiffness increases while increasing Ψ. In the opposite case the stiffness decreases with decrease of Ψ. For the example of structure A-Sk—A and Ψ = 0,5, the price economy for 42% and mass reduction for 4% have been shown and compared with carbon plastic beam.

Highlights

  • A-stiklo plastike (Sk) -A tipo trisluoksnes konstrukcijos su vidurinio sluoksnio storiu () 2 = O,SH duomenis palygin(( su gryno anglies plastiko sijos parametrais gauname, kad A-Sk -A sija yra 42% pigesne, 4% lengvesne, standumas D sumaieja 12%, standumas slyciai K padideja 40%, maksimalios normaliniq jtempiq reiksmes padideja 9%, o deformacijq - 4,5%

  • The bar layers were formed of carbon plastic (A), hot (S~c) and cold hardening (Sc) glassplastics and epoxy resin (D)

  • The relative thickness 'I' is the ratio of middle layer height to the whole height

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Summary

Konstrukciniq elementq charakteristika ir jq analitinis skaiciavimas

KeiCiant is siq medZiagq sudarytq sluoksniq padetis buvo nagrinejamos pirmqjq devyniq tipq simetrines konstrukcijos, kurios, naudojant raidinius mediiagq eymejimus, gall biiti pafymetos: 1. A-Sk-A; 4. KeiCiant is siq medZiagq sudarytq sluoksniq padetis buvo nagrinejamos pirmqjq devyniq tipq simetrines konstrukcijos, kurios, naudojant raidinius mediiagq eymejimus, gall biiti pafymetos: 1. Konstrukcijas, kuriose isoriniq sluoksniq mediiagos tamprumo modulis E 1 yra didesnis nei vidurinio sluoksnio E 2 - vadinsime "tiesioginemis" (1, 2, 3, 7, 9, 10 tipo konstrukcijose E1 > E2 ), o jei maiesnis "atvirkstinemis" (4, 5, 6, 8, 11, 12 tipo - E 1 < E 2 ). Siq trisluoksniq konstrukcijq isoriniai sluoksniai pagaminti is vienos medziagos, o jq storiai lygiis. Buvo naudojami staCiakampio skerspjiivio vienodo ploCio bandiniai (b=50 mm). Vidurinio ir isoriniq sluoksniq storiai buvo keiciami islaikant bendr~ bandinio auksti pastovq, t.y. H = _L8i = 12 mm =canst. Ltempimq ir deformacijq dydiiai buvo skaiciuojami gembinei sijai esant santykiniams apkrovq dydiiams F=100 N, M=100 Nm ltempimai skaiciuojami pagal formules [5]:.

Strypq stiprumas ir standumas
Sijq standumas ir deformacijos
ISvados
Findings
Summary
Full Text
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