VM247

VM247
Campbell Diagrams and Critical Speeds Using Symmetric Bearings

Overview

Reference:Nelson and McVaugh,"The Dynamics of Rotor-Bearing Systems Using Finite Elements", Journal of Engineering for Industry, May 1976.
Analysis Type(s):Modal analysis (ANTYPE =2)
Element Type(s):
3D Linear finite-strain beam element (BEAM188)
Structural mass element (MASS21)
Spring damper element (COMBIN14)
Input Listing:vm247.dat

Test Case

A rotor-bearing system is analyzed to determine the whirl speeds. The distributed rotor was modeled as a configuration of six elements with each element composed of subelements. See Table 10: Geometric Data of Rotor-Bearing Elements for a list of the geometrical data of the elements. Two undamped linear bearings were located at positions four and six. Modal analysis is performed on rotor bearing system with multiple load steps to determine the critical speeds and Campbell values for the system.

Figure 419: Rotor-bearing Configuration

Rotor-bearing Configuration

Figure 420: Isometric View of the Rotor Bearing System

Isometric View of the Rotor Bearing System

Table 10: Geometric Data of Rotor-Bearing Elements

Element No.Subelement No.Axial Distance to Subelement (cm)Inner Diameter (cm)Outer Diameter (cm)
110.00 0.51
21.27 1.02
215.08 0.76
27.62 2.03
318.89 2.03
210.16 3.30
310.671.523.30
411.431.782.54
512.70 2.54
613.46 1.27
4116.51 1.27
219.05 1.52
5122.86 1.52
226.67 1.27
6128.70 1.27
230.48 3.81
331.50 2.03
434.541.52203

Material PropertiesGeometric PropertiesLoading
Shaft
E11 = 2.078E11 Pa
G12 = 1.0E12 Pa
DENS = 7806 kg/m3
Mass Element
Mass = 1.401 kg
Polar inertia = .002 kg m2
Diametral inertia =.00136 kg m2
Bearing Element
Spring constant = 4.378E7 N/m
Rotational Velocity
Spin (1) = 0 rpm
Spin (2) = 35,000 rpm
Spin (3) = 70,000 rpm
Spin (4) = 105,000 rpm

Analysis Assumptions and Modeling Notes

A modal analysis is performed on a rotor bearing system with QR Damp method to determine the whirl speeds and Campbell values. The rotor shaft is modeled with BEAM188 elements with quadratic shape function and an internal node to enhance element accuracy. MASS21 element is used to model the rigid disk (concentrated mass) and COMBIN14 element is used to model symmetric bearings. No shear effect is included in the rotor-bearing system. The displacement along X as well as the rotation around X axis is constrained so that the rotor bearing system does not have any torsion or traction related displacements. The CORIOLIS command is activated in a stationary reference frame to apply gyroscopic effect to the rotating structure. The whirl speeds for slope (excitation per revolution) 1 and 4 are determined and compared with the numerical solution.


Note:  In the "Results Comparison" table below, the values listed from the reference article are the whirl speeds (frequencies) and not the critical speeds. Also, the definition of the ratio differs between the reference article and this application. In the article, the whirl ratio equals the rotational velocity divided by the frequency. In this application, the ratio is the slope, which is equal to the frequency divided by the rotational velocity. As a result, the values listed in the reference article for a whirl ratio of 1/4 (see the "Results Comparison" table below) are divided by 4 so that they can be compared to the critical speeds obtained from this application with a slope of 4.


Results Comparison

 TargetMechanical APDLRatio
Whirl speeds for slope = 1 (rpm)
Mode 115470.000015478.52471.001
Mode 217159.000017128.08420.998
Mode 346612.000046711.55851.002
Mode 449983.000050093.96401.002
Mode 564752.000064875.37911.002
Mode 696547.000095636.27380.991
Whirl speeds for slope = 4 (rpm)
Mode 14015.00004013.38571.000
Mode 24120.25004116.17170.999
Mode 311989.250012015.44491.002
Mode 412200.000012227.00101.002
Mode 518184.250018205.28451.001
Mode 620162.250020127.05700.998