The dynamic model of the five shaft geared rotor system is shown in Fig。 2。 kiL , ciL and kiR, ciR are the stiffness parameters and damping parameters of the left TPJBs and right TPJBs on the five shafts respectively, which are dependent on the loading charac- teristic。 Fi is the meshing force。 Unlike the traditional one-to-one gear pair's transmission, the geared system in Fig。 2 is consisted of a bull-gear (M) and four pinion gears, and the bull-gear meshes with the other four gears at the same time, which cause a much stronger coupling effect。 This compact structure can offer several advantages such as smaller floor space, lower energy consump- tion, and higher power density。 However, it also means that much more critical speeds must disperse in a certain interval of speed, which brings much more difficulties in critical speed designing。
3。6-DOFs dynamic modeling method of geared rotor system
The finite element method is used to set up the dynamic model of the geared rotor system shown in Fig。 3, and the assumptions
Fig。 4。 Rotating rigid discs model。
and simplifications are introduced as follows: (1) All the shafts are linear elastic。 (2) The bearing houses are rigid。 (3) A gear pair is represented by linear equivalent stiffness along its pressure line。
(4) A shaft section with a larger radius can be simplified as rigid disc。
The beam element shown in Fig。 3 is chosen to describe shafts, which has 12 degrees of freedom (DOFs) and is defined as
uij ¼ h xi yi zi θxi θyi θzi xj yj zj θxj θyj θzj i
The dynamic equation of the beam element is described as
Fig。 5。 The dynamic model of gear mesh effect。
section is simplified to the combination of the rectangular section
Mbu€ ij þðCb þ ΩGbÞu_ ij þ Kbuij ¼ Fb ð2Þ
where Ω is the rotating speed around axes-x; Fb is the force vector of the beam element; Mb, Cb , Gb and Kb are the mass matrix, damping matrix, gyroscopic matrix and stiffness matrix respec-
where Fmesh is the mesh force acting on the tooth; δBr is the
tively, where Cb is defined as Rayleigh damping and described as
Cb ¼ α U Mb þβ U Kb ð3Þ
where α and β are the scaling factors。
The impellers, wheels and gears are regarded as rigid rotating discs (with gyroscopic effect), and simplified to be lumped mass and moment of inertia acting on the corresponding node, which is shown in Fig。 4。 The rigid disc has 6 degrees of freedom, which is defined as
corresponding bending deformation of rectangular section; δBt is the corresponding bending deformation of trapezoid section; δs is the corresponding shear deformation; and δG is the corresponding elasticity deformation caused by the root tilting。 Assume i and j are
the nodes of the gear pair, where i is on the driving pinion, which is shown in Fig。 5。 ψ ij is defined as the angle between the tangent plane of the gear contact surfaces and the axis-z and described as
( ϕij þαij driving gear rotate counterclockwise
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