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

机译:四垫套球式垫板滑动轴承的静态性能特性和转子动力学系数

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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 thetemperature 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:静态性能特征和转子动力学系数是通过实验确定了四块球面,球形座,可倾瓦块轴颈轴承在两块瓦块之间的配置的。测得的静态特性包括轴颈静态平衡位置,估计的功率损耗和后缘垫板温度。根据测得的复杂动态刚度系数的曲线拟合确定转子动力系数,并将其作为激励频率的函数。频率无关的[M]-[C]-[K]模型在拟合测量值方面做得很好。测试条件包括速度从4到12 krpm,单位负载从0到1896 kPa(0到275 psi)。 轴承使用凉爽的入口油来降低轴瓦的工作温度,并增加轴承的负载和速度。轴承的公称直径为101.78毫米(4.0070英寸)。测量结果表明轴承受到了严重挤压,径向轴承间隙在与负载轴成逆时针方向45°的轴上为99.63μm(3.92 mils),在与负载轴成顺时针45°方向上的径向轴承间隙为54.60μm(2.15 mils)。垫的长度为101.60毫米(4.00英寸),L / D = 1.00。垫弧角为73°,枢轴偏移率为65%。使用Kaul [1]描述的测试台进行测试,并使用Childs and Hale [2]改编的程序提取转子动力系数。 使用大流量Navier-Stokes模型进行预测,其中使用了轴承中流体的绝热条件。但是,该模型假定所有垫片的名义间隙均恒定,并且根据测量的间隙使用了平均间隙。测得的静态偏心距和姿态角显着低于预期。姿态角从6°到39°不等,并随负载而减小。功率损耗可以很好地预测,最大值为25 kW(34 hp)。检测到的最高焊盘温度为71°C(160°C),而 从入口到出口的温度升高被高估了8°C(14℉)。 直接的刚度和阻尼系数被大大地高估了,但是与测量的刚度和阻尼值串联的简单枢轴刚度的添加极大地改善了理论与实验之间的一致性。在低速时,M_(yy)(y负载方向)的直接附加质量在较大程度上为负,并随速度增加。除了零负载下的M_(yy)以外,它们在达到8,000 rpm之前变为正值。尽管存在显着的交叉耦合刚度项,但是它们始终具有相同的符号,从而在所有测试条件下产生零的旋转频率比并获得无条件的稳定性。

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