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STATIC PERFORMANCE CHARACTERISTICS AND ROTORDYNAMIC COEFFICIENTS FOR A FOUR-PAD BALL-IN-SOCKET TILTING PAD JOURNAL BEARING

机译:四垫球型倾斜垫纸张轴承的静态性能特性和旋转动力系数

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Static performance characteristics and rotordynamic coefficients were experimentally determined for a four-pad, spherical-seat, tilting-pad journal bearing in load-between-pad configuration. Measured static characteristics include journal static equilibrium position, estimated power loss, and trailing-edge pad temperatures. Rotordynamic coefficients were determined from curve fits of measured complex dynamic-stiffness coefficients as a functions of the excitation frequency. A frequency-independent [M]-[C]-[K] model did a good job of fitting the measurements. Test conditions included speeds from 4 to 12 krpm and unit loads from 0 to 1896 kPa (0 to 275 psi). The bearing uses cool inlet oil to decrease the pad operating temperatures and increase the bearing's load and speed capacity. The bearing has a nominal diameter of 101.78 mm (4.0070 in). Measurements indicated significant bearing crush with a radial bearing clearance of 99.63 μm (3.92 mils) in the axis 45° counterclockwise from the loaded axis and 54.60 μm (2.15 mils) in the axis 45° clockwise from the loaded axis. The pad length is 101.60 mm (4.00 in), giving L/D= 1.00. The pad arc angle is 73°, and the pivot offset ratio is 65%. Testing was performed using a test rig described by Kaul [1], and rotordynamic coefficients were extracted using a procedure adapted from Childs and Hale [2]. A bulk-flow Navier-Stokes model was used for predictions, using adiabatic conditions for the fluid in the bearings. However, the model assumes constant nominal clearances at all pads, and an average clearance was used based on measured clearances. Measured static eccentricities and attitude angles were significantly lower than predicted. Attitude angles varied from 6° to 39° and decreased with load. Power loss was well-predicted, with a maximum value of 25 kW (34 hp). The maximum detected pad temperature was 71°C (160°C) while the temperature rise from inlet to exit was over-predicted by 8°C (14℉). Direct stiffness and damping coefficients were significantly over-predicted, but the addition of a simple pivot-stiffness in series with the measured stiffness and damping values vastly improved the agreement between theory and experiment. Direct added masses were negative to a higher degree for M_(yy) (y load direction) at low speeds and increased with speed. With the exception of M_(yy) at zero load, they became positive before reaching 8,000 rpm. Although significant cross-coupled stiffness terms were present, they always had the same sign, producing a whirl frequency ratio of zero and netting unconditional stability over all test conditions.
机译:在焊盘构造之间的四个焊盘,球形座椅,倾斜垫轴颈轴承实验确定静态性能特性和旋转动力系数。测量的静态特性包括轴颈静态平衡位置,估计功率损耗和后缘焊盘温度。根据激发频率的功能,从测量的复杂动态刚度系数的曲线拟合确定旋转动力系数。频率无关的[M] - [C] - [K]模型在拟合测量时做得很好。测试条件包括4至12 krpm的速度,单位载荷为0至1896 kPa(0至275psi)。轴承使用凉爽的入口油来减少垫操作温度并提高轴承的负载和速度。轴承的标称直径为101.78 mm(4.0070英寸)。测量表明,在轴45°沿轴45°逆时针,在轴45°中逆时针,在轴45°中,从装载的轴线逆时针逆时针,测量值为99.63μm(3.92密耳)。焊盘长度为101.60毫米(4.00英寸),给出L / D = 1.00。垫弧角度为73°,枢轴偏移比为65%。使用Kaul [1]描述的试验台进行测试,并且使用从儿童和HALE的过程提取旋转动力系数[2]。使用轴承中的液体的绝热条件,使用散装流Navier-Stokes模型进行预测。然而,该模型假设所有垫处的恒定标称间隙,并且基于测量的间隙使用平均间隙。测量的静态偏心和姿态角度显着低于预测。姿态角度从6°变化到39°,随着负荷减小。功率损耗良好预测,最大值为25千瓦(34 HP)。最大检测焊盘温度为71°C(160°C),而从入口从入口升高到8°C(14°)的温度升高。直接刚度和阻尼系数显着过度预测,但是与测量的刚度和阻尼值串联的简单枢转刚度添加了理论和实验之间的协议。直接添加质量在低速下的M_(YY)(YY)(YY)(Y负载方向)的较高程度,随着速度的增加而增加。除了零负荷的M_(YY)外,在达到8,000 rpm之前,它们变为阳性。尽管存在显着的交叉耦合刚度术语,但它们总是具有相同的符号,在所有测试条件下产生零点和网络无条件稳定性的旋转频率比。

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