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提示:如果分析得出第一阶频率接近72.059就可以了,因为CosmosWorks(2006)在频率分析时没有办法设置旋转刚度软化的影响,所以不会得到后面那个target值。9 _6 q D% ]- m* }& K+ s1 q# F
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Title Vibration of a Rotating Cantilever Blade! q' ^% L8 [% [6 U: h* b# E
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Overview
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6 `2 A2 b. q+ \4 R) B| Reference: | W. Carnegie, “Vibrations of Rotating Cantilever Blading”, Journal Mechanical Engineering Science, Vol. 1 No. 3, 1959, pg. 239 | | Analysis Type(s): | Static Analysis
1 J6 N+ H% \" q: S: o3 kMode-frequency Analysis% J; X; T2 S2 G4 O6 B8 |; X
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' x0 \4 H+ q: rTest Case4 u N" s! C) x6 ^( c
* N: E3 M4 h7 _& L( g8 {A blade is cantilevered from a rigid rotating cylinder. Determine the fundamental frequency of vibration of the blade, f, when the cylinder is spinning at a rate of Ω .
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; l) _7 O6 T' ?7 r( O- ]2 rFigure 54.1 Rotating Cantilever Blade
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7 f+ L# f& ^% }" y( e3 a, J; J| Material Properties | | E = 217 E9 Pa | | ρ = 7850 kg/m3 | | υ = 0.3 |
| | Geometric Properties | | r = 150 mm | | l= 328 mm | | b = 28 mm | | t = 3mm |
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Analysis Assumptions and Modeling NotesThe problem is solved in two different ways:
1 q, m: p+ X1 j' i: |1 d* U& a1 ~- Using Elastic Shell Elements (SHELL63)
- Using 3-D Solid Shell Elements (SOLSH190)
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Spin (centrifugal) softening is used. Since the cylinder is rigid, the base of the blade has its displacements constrained. A static prestress analysis is performed to include the inertial effects resulting from the rotation of the cylinder.
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Results Comparison* ^$ Q4 h5 J, e6 h* C
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| Target | ANSYS | Ratio | | SHELL63 | | f, Hz | 52.75 | 52.01 | 0.986 | | SOLSH190 | | f, Hz | 52.75 | 51.80 | 0.982 |
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[ 本帖最后由 tigerdak 于 2007-11-9 15:25 编辑 ] |
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