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8 G9 j: z' d1 f0 G4 R0 I提示:屈曲分析(特征值法)。% H! |# o3 I! q4 H& ]
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Title Buckling of a Bar with Hinged Ends (Line Elements)0 A7 u; x, Y% W3 E+ b# D
9 ?5 h- w( U; w& Z/ \Overview
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5 S- D6 w' B; O0 p3 o$ Z| Reference: | S. Timoshenko, Strength of Material, Part II, Elementary Theory and Problems, 3rd Edition, D. Van Nostrand Co., Inc., New York, NY, 1956, pg. 148, article 29. | | Analysis Type(s): | Buckling Analysis
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Test Case, F, s5 u) J, T- Z% I8 W
% U: o: M4 n% l: f8 ^ P* oDetermine the critical buckling load of an axially loaded long slender bar of length L with hinged ends. The bar has a cross-sectional height h, and area A.
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# j' A8 t& y. pFigure 127.1 Buckling Bar Problem Sketch; _" j6 V3 O7 b5 i% J; [) z8 a
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| Material Properties | | E = 30E6 psi |
| | Geometric Properties | | l = 200 in | | A = 0.25 in2 | | h = 0.5 in |
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Analysis Assumptions and Modeling NotesOnly the upper half of the bar is modeled because of symmetry. The boundary conditions become free-fixed for the half symmetry model. A total of 10 master degrees of freedom in the X-direction are selected to characterize the buckling mode. The moment of inertia of the bar is calculated as I = Ah2/12 = 0.0052083 in4 .; \8 H5 y0 R2 `5 n1 {) B+ J, i
( b* h& T/ r3 i4 u1 r: r. A$ @4 b3 mResults Comparison | Target | ANSYS | Ratio | | Fcr, lb | 38.553 | 38.553 [1] | 1.000 | 6 l7 s5 [: M: |( V; s* J1 c
- Fcr = Load Factor (1st mode).
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) z9 t" B/ P, E[ 本帖最后由 tigerdak 于 2007-11-8 18:44 编辑 ] |
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