32 21 JOURNAL OF VIBRATION AND SHOCK Vol. 32 No. 21 213 ANSYS - - 29BAG12A1 - K1-3 212-9 - 3 212-11 - 28 1987 1929 11624 ANSYS - UPF - - - - - - - - ANSYS UPF U211. 9 A Seimic repone analyi of a time-varying high peed train -rail-bridge ytem baed on ANSYS LIU Chang-liang YIN Xun-qiang LIN Gao LI Jian-bo HU Zhi-qiang Laboratory of Earthquake State Key Laboratory of Coatal and Offhore Engineering Dalian Univerity of Technology Dalian 11624 China Abtract Uing ANSYS oftware platform a time-variant wheel-rail coupled element with artificial node wa introduced combining application of uer programmable feature UPF a dynamic FE model for the eimic repone analyi of a high-peed vehicle-rail-bridge ytem wa formed and embedded in the popular finite element oftware ANSYS. With the propoed approach the dynamic interaction of rail and bridge wa modeled with ma-pring-dahpot ytem the vehicle ubytem wa modeled a a rigid-body dynamic model. The vehicle-rail-bridge ytem wa aembled through atifying the geometric compatibility and balance of the interaction force on the connected node. Earthquake acceleration time hitorie a the input excitation to the ytem were applied to the rail-bridge ubytem with the largema method. Finally the reliability and good erviceability of the propoed time-varying ytem were verified through numerical example and it application to actual engineering project. It wa hown that thi time-varying ytem model ha the potential to olve ophiticated and real engineering problem combined with the rich element library and nonlinear olver available in the commercial finite element oftware ANSYS. Key word high-peed train time-varying ytem eimic repone analyi ANSYS UPF - - 1-6 - 7
21 ANSYS - - 59 - - 1. 1 Yang 8 1 2 4 NEWMARK - 2 - v c z φ c c v t φ t t v w w 1 9-1 APDL AN- k y1 k y2 c y1 c y2 SYS - l l c l t - Lagrange - 11 - - - ANSYS UPF M uu M uw uu M wu M C uu C uw uu ww u C w wu C ww uw K uu K uw u K wu K u F ww u = u w F T u w T R 1 w 1 - - u w M C K 1 - u F - R - T T u = - - 1 Newmark x y z 2 Fig. 2 Sketch of train ubytem model 1 - - Fig. 1 Sketch map of high peed train-tail-bridge time-variant ytem ubjected to eimic excitation 3 - Fig. 3 Sketch of rail-bridge ubytem model
6 213 32 1. 2-4 1 - R = T -1 w M ww u * w C ww u * w K ww u * w M wu u u C wu u u K wu u u - F w 5 u * w =? Г?N v? 1 u r1 r x 1 Г?N v? i u ri r x i? T * uw Bemoulli-Euler * uw 3-5 k bx k by c bx - c by 2 12 - M * r ur C M r ur M b M C r C - C M u b M * r - C ur L u - C r L u - C T b C b C T b C b C ub u K * r - K u b K r K - K u - K T K b r F K u r - R - K = b F 2 b M u L T K b r F K u r R = b F * 6 b M L u g g M r b * r = M r - - δ nw N v i T -1 w M wwij Γ?N v? j 7a w = 1 R C * r = C u g M L r C δ nw N v i T -1 w C wwij Γ?N v? j 7b w = 1 - - K * r = K r K Hermitian δ nw N v i T -1 w K wwij Γ?N v? j 7c C = ne c bx l N u?n u?dx c by l w = 1 N v?n v?dx 3a R * r = - N v i T -1 w K wwi r x i el = 1 K = ne k bx l N u?n u?dx k by el = 1 l M wui u ui C wu u ui K wui u ui F wi 7d N v?n v?dx 3b δ δ = 1 N u N v δ = nw l ne 6 - - M L M b 1 6-1. 3 1 i u wi = Г?N v? i u ri r x i 4 Г Newmark r x u ri -
21 ANSYS - - 61 2 ANSYS ANSYS 5 - - Fig. 5 Activated of time-variant wheel-rail coupling element - - ANSYS - ANSYS Rayleigh α β - - 2. 1-7b c * r = δ N v t -1 w c ww - αm ww - βk ww Γ?N v? 9-4 ANSYS ANSYS i j i 1 1 j 1 - - 2 3 2. 2-2 - ANSYS - 4 - Fig. 4 Time-variant wheel-rail - coupling element with virtual node UerElem. f 2 k k * - k = 5 - k T k B c c 7c * - c k = - c T c - k - β - k T k 1 k c k * r = k r δ N v ξ c t -1 w k ww Γ?N v ξ c? 8 2. 3 k r δ = 1-7 a - 7 b A C δ = ANSYS ANSYS ANSYS UerElem. f 13 ANSYS UPF FORTRAN
62 213 32 Newmark 6 L = 25 m I = 2. 9 m 4 E = 2. 87E9 Pa m = 2 33 kg /m ν =. 2 - M v = 5 75 kg k v = 1 595 kn /m 2. 4 ANSYS 1-5 kg I t = 1 kg m 4 M w = 1-5 kg k y1 = 1 1 kn /m ANSYS - k y2 =. 5 k v = 797. 5 kn /m c y1 = c y2 = kn /m - l c = l t = l = m E r = 21 GPa v r =. 3 I r = 1-1 m 4 m r = 1-1 kg /m k by = 1 1 kn /m 2 c by = kn / m 2 E b = E = 2. 87 GPa v b = v =. 3 I b = I = 2. 9 m 4 m b = m = 233 kg /m ANSYS APDL 1 BEAM3 ANSYS 14 7 8 1 1 ANSYS - - Tab. 1 Flowchart of the etablihment of propoed model 1. - APDL 2. Uer1. f 3. - - 1 5 Uer2. f APDL 2 - UerElem. f 1-2 - 6 2 3 37 4 7 Fig. 7 The midpoint diplacement of the beam 5 8 7 6 1-7 3 - ANSYS 4 1 Uer2. f 4. APDL 3 v = 27. 78 m / M c = M v = 5 75 kg = 1 kg m 4 M t = 7 6 I c - 8 Fig. 6 A imple beam ubjected to a moving pring-ma train model Fig. 8 The acceleration repone of the prung ma
21 ANSYS - - 63 8-1. 11 mm 1. 71 mm. 159 mm. 16 mm - 4 1. 75 4. 1 mm 1. 193 mm 3 15 ANSYS 1. 844 mm - - 2. 173 mm 12 32 m 1 5 1. 86 m / 2. 248 m / 2 m 5. 5 m 2. 3 m. 52 m / 2. 112 m / 2 15 beam3. 17 m / 2. 118 m / 2 ma21. 53 m / 2. 85 m / 2 CP - - ma21 - Rayleigh. 5 15 El Centro 8 gal 9 9 El Centro Fig. 9 Acceleration time domain of El Centro earthquake 1 Fig. 1 The vertical diplacement repone at the midpoint of 3rd bridge with and without eimic extraction 4. 2 1 3 km /h 11 3 Fig. 11 The vertical diplacement repone at the midpoint 11 of 3rd rail with and without eimic extraction 1 15 12 1-11 5 - -
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