低温氦气涡轮膨胀机凹凸型气体箔型推力轴承气动与热分析

J. Kumar, Ch. Rewant, Hitesh Kumar Sinha, Suraj K Behera
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摘要

气体箔轴承(gfb)用于几个高速应用,其顺应行为,以定制其阻尼和刚度。高速应用之一是低温涡轮膨胀器,它们用于液化器中的气流制冷。本文对用于支撑设计转速为240,000转/分的氦气涡轮膨胀机轴向载荷的碰撞型气体箔形推力轴承(BGFTBs)进行了气动和热力学分析。BGFTBs由非常薄的顶部和凹凸箔连接到轴承基础。轴颈和顶翼之间的楔入作用负责气动压力的发展,这种气动压力支持转子的轴向载荷。由于项圈和顶箔之间气体流动的收敛通道受到限制,过程气体可能会升高温度并扭曲轴承的薄箔。本文提出了一种分析bgftb气动和热特性的仿真方法。采用雷诺方程对气膜进行了建模。将结构方程和雷诺方程耦合在一起,预测了膜厚、压力分布和承载能力。此外,利用能量方程对气膜进行了建模,以预测其热特性。采用Couette近似法预测气膜的温度分布。这种近似有助于将能量方程与雷诺方程分离。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Aerodynamic and Thermal Analysis of Bump Type Gas Foil Thrust Bearing for Cryogenic Helium Turboexpander
Gas Foil Bearings (GFBs) are used for several high-speed applications for its compliant behavior to tailor its damping and stiffness. One of the high-speed application is the cryogenic turboexpander and they are used to refrigerate the gas stream in a liquefier. This article deals with the aerodynamic and thermodynamic analysis of bump type gas foil thrust bearings (BGFTBs), which are used to support the axial load of the helium turboexpander with a design speed of 2,40,000 rpm. The BGFTBs consists of very thin top and bump foils attached to the bearing base. The wedging action between the shaft collar and top foil is responsible for the development of aerodynamic pressure and this aerodynamic pressure supports the axial load of the rotor. Due to restricted converging passage for the gas flow between the collar and top foil, the process gas is likely to rise in temperature and distort the thin foils of the bearings. This paper presents a simulation method to analyze the aerodynamic and thermal behavior of the BGFTBs. The gas film is modeled using Reynold’s equation. The structural and Reynold’s equations are coupled together to predict the film thickness, pressure distribution and load carrying capacity. Further, the gas film is modeled by using an energy equation to predict the thermal characteristics. The Couette Approximation is used to predict the temperature distribution of the gas film. This approximation helps to delink the energy equation with Reynolds equation.
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