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During the launching stage,hydrodynamic pressure and adapters’ reaction loads can influence the vehicle’s rigid motion as well as cause its structural vibration,which is a typical rigid-flexible coupling dynamic problem. This paper presents a 2-D rigid-flexible coupling model to calculate the vehicle’s dynamic responses in that period.The vehicle was equivalent to a flexure beam with axial deformation. Hybrid coordinate and modal superposition methods were used to describe its large rigid displacement and small deformation. By the second Lagrange equation,the vehicle centroid’s displacements,rotational angle and modal coordinates were chosen as generalized coordinates and then the vehicle ’s rigid-flexible coupling dynamic equations were obtained. By numerical simulation,the results of vehicle’s motion parameters and transverse internal loads were acquired.The calculation results showed that differences of the vehicle’s motion parameters between the rigid-flexible coupling model and the rigid body assumption are noticeable and the peak magnitude of the vehicle’s transverse internal loads in the rigid-flexible coupling model is higher remarkably than that in the rigid body assumption.
During the launching stage, hydrodynamic pressure and adapters’ reaction loads can influence the vehicle’s rigid motion as well as cause as its structural vibration, which is a typical rigid-flexible coupling dynamic problem. This paper presents a 2-D rigid-flexible coupling model to calculate the vehicle’s dynamic responses in that period. The vehicle was equivalent to modal superposition methods were used to describe its large rigid displacement and small deformation. By the second Lagrange equation, the vehicle centroid’s displacements, rotational numerical and modal coordinates were chosen as generalized coordinates and then the vehicle ’s rigid-flexible coupling dynamic equations were obtained. By numerical simulation, the results of vehicle’s motion parameters and transverse internal loads were acquired. vehicle’s motion parameters between the rigid-flexible coupling model and th e rigid body assumption are the peak magnitude of the vehicle’s transverse internal loads in the rigid-flexible coupling model is noticeably than that in the rigid body assumption.