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Static characteristics and rotordynamic coefficients of a four-pad tilting-pad journal bearing with ball-in-socket pivots in load-between-pad configuration

机译:垫间载荷配置的四轴可倾式垫轴颈轴承的静态特性和转子动力系数,其中球窝式枢轴

摘要

Static characteristics and rotordynamic coefficients were experimentallydetermined for a four-pad tilting-pad journal bearing with ball-in-socket pivots in loadbetween-pad configuration. A frequency-independent [M]-[C]-[K] model fit themeasurements reasonably well, except for the cross-coupled damping coefficients. Testconditions included speeds from 4,000 to 12,000 rpm and unit loads from 0 to 1896 kPa(0 to 275 psi).The test bearing was manufactured by Rotating Machinery Technology (RMT),Inc. Though it has a nominal diameter of 101.78 mm (4.0070 in.), measurementsindicated significant bearing crush with radial bearing clearances of 99.6 ?m (3.92 mils)and 54.6 ?m (2.15 mils) in the axes 45? counterclockwise and 45? clockwise from theloaded axis, respectively. The pad length is 101.6 mm (4.00 in.), giving L/D = 1.00.The pad arc angle is 73?, and the pivot offset ratio is 65%. The preloads of the loadedand unloaded pads are 0.37 and 0.58, respectively.A bulk-flow Navier-Stokes model was used for predictions, using adiabaticconditions for the bearing fluid. Because the model assumes constant nominalclearances at all pads, the average of the measured clearances was used as an estimate.Eccentricities and attitude angles were markedly under predicted while power loss wasunder predicted at low speeds and very well predicted at high speeds. The maximum detected pad temperature was 71?C (160?F) and the rise from inlet to maximum bearingtemperature was over predicted by 10-40%.Multiple-frequency force inputs were used to excite the bearing. Direct stiffnessand damping coefficients were significantly over predicted, but addition of a simplestiffness-in-series model substantially improved the agreement between theory andexperiment. Direct added masses were zero or negative at low speeds and increasedwith speed up to a maximum of about 50 kg; they were normally greater in the unloadeddirection. Although significant cross-coupled stiffness terms were present, they alwayshad the same sign. The bearing had zero whirl frequency ratio netting unconditionalstability over all test conditions. Static stiffness in the y direction (obtained from steadystateloading) matched the rotordynamic stiffness Kyy (obtained from multiple-frequencyexcitation) reasonably at low loads but poorly at the maximum test load.
机译:静态特性和转子动力学系数是通过实验确定的,其中在垫间配置的情况下,球窝式枢轴的四垫可倾式垫轴颈轴承。除交叉耦合的阻尼系数外,与频率无关的[M]-[C]-[K]模型非常适合测量。测试条件包括转速从4,000到12,000 rpm,单位载荷从0到1896 kPa(0到275 psi)。测试轴承由美国旋转机械技术公司(RMT)制造。尽管其公称直径为101.78毫米(4.0070英寸),但测量结果表明轴承受到了严重挤压,在45?轴上的径向轴承游隙为99.6?m(3.92密耳)和54.6?m(2.15密耳)。逆时针和45?从加载的轴分别顺时针旋转。轴瓦长度为101.6毫米(4.00英寸),L / D = 1.00。轴瓦弧角为73°,枢轴偏移率为65%。加载和卸载垫的预载荷分别为0.37和0.58。使用大流量Navier-Stokes模型进行预测,使用了绝热条件下的轴承流体。由于该模型在所有垫块上均假定恒定的名义间隙,因此将测得间隙的平均值用作估计值。偏心率和姿态角明显低于预测值,而低速时预测的功率损耗较低,而高速时则预测的非常好。检测到的最高衬套温度为71?C(160?F),从入口到最高轴承温度的升高超出了预测的10-40%,并使用多频力输入来激励轴承。直接刚度和阻尼系数大大超出了预期,但是添加简单的串联刚度模型大大改善了理论和实验之间的一致性。在低速时,直接增加的质量为零或负,并随速度增加而增加,最大增加到约50 kg;它们通常在卸载方向上更大。尽管存在显着的交叉耦合刚度项,但它们始终具有相同的符号。在所有测试条件下,轴承的涡流频率比为零,因此无条件稳定。 y方向上的静态刚度(从稳态负载获得)与转子动态刚度Kyy(从多频励磁中获得)相当,在低负载下却不如在最大测试负载下。

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    Harris Joel Mark;

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  • 年度 2009
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