流动颗粒流化浴设计与传热

M. Golob, C. Nguyen, S. Jeter, S. Abdel-Khalik, C. Ho
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引用次数: 1

摘要

任何提议的颗粒到工作流体热交换器作为CSP颗粒加热接收器系统的一部分是具有挑战性的。主要挑战是实现高温颗粒与工作流体(如sCO2)或管道或其他通道中流动的空气之间的充分热交换(HX)。为了减小所需的HX面积,需要较高的颗粒侧换热系数,而逆流始终是最佳的总体布置。因此,一种很有前途的方法是实现流化颗粒的开放通道流动,实际上是相对于工作流体以一般逆流的方式流动,工作流体包含在浸入通道中的管或通道中。这种布置提供了(1)优良的颗粒侧传热;(2)方便的颗粒再循环;(3)与工作流体几乎理想的逆流。为了提高人们对流态化换热的理解和支持,本文研究了颗粒流动路径对流态化换热的局部影响的可能性。为此,建立了一系列较小的流化床热交换器,利用轴向流动的开口通道作为流化颗粒的移动床。这些设计的特点是蛇形流道,代表了其他人提出的全尺寸HX设计。提出的蛇形流设计是基于现有的颗粒冷却系统;然而,人们对这种设计提出了一些尚未得到最终回答的问题,并推动了这项调查。支持这项研究的测试槽包含一个弯道,颗粒在离开热交换器之前绕其流动。这个大型仪器的目的是观察影响颗粒流稳定性或均匀性的变量,并提供对操作单元潜在问题的见解。试验台由两个堆叠的部分组成。下容器为流化空气静压室,通过上容器底平面提供均匀分布的气流。界面包括一个结构穿孔板,堆叠的滤纸层来平衡压降,以及一个精细的不锈钢丝网,以确保颗粒留在上部容器中。上面的容器代表颗粒流动面积。透明导电PETG聚合物壁用于流化浴,以减少静电积聚,同时仍然提供透明材料,可以观察流动。目前的设计使用空气输送机将颗粒从测试槽的一端再循环到另一端,关闭颗粒循环。所描述的试验研究了流化在蛇形路径特定区域的有效性。在这些区域进行了测量,以确定局部传热系数。这是通过插入一个已知功率输入和加热区域的盒式加热器来实现的,用细珠表面热电偶测量加热器表面温度。另外,两个探头浸在围绕筒式加热器的流化床中,以测量床内的自由流温度。流态化的空气输入和空气输送机的提升也被测量并记录为测试参数,以及每个区域的大致床层高度。除了流量的定量测量外,该试验装置还用于观察流化、床层高度和出口位置对颗粒轴向质量流量的影响。这些结果将在提议的文件中提出。展望未来,这种设置将允许测试系统的各种质量流量控制方案。目前,这种设计,与仪表加热器和自由流温度探头,允许测量局部传热特性在任何地方的粒子流动路径。目前的测试提供了流化浴设计中传热系数的局部图和流动行为的描述,这些将被报道和展示,以支持未来的明渠颗粒到sCO2热交换器的设计。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Flowing Particle Fluidized Bath Design and Heat Transfer
Any proposed particle to working fluid heat exchanger as part of a CSP Particle Heating Receiver system is challenging. A principal challenge is achieving adequate heat exchange (HX) from the high temperature particles to the working fluid such as sCO2 or air flowing in tubes or other passages. To reduce the required HX area, a high particle side heat transfer coefficient is needed, and counterflow is always the best overall arrangement. Consequently, a promising approach is implementing an open channel flow of fluidized particles actually flowing in a general counterflow with respect to the working fluid, which is contained in tubes or passages immersed in the channel. This arrangement provides (1) excellent particle side heat transfer, (2) convenient particle re-circulation, and (3) almost ideal counterflow with the working fluid. To advance the understanding and support the design and applications of such exchangers, this investigation has been conducted to study the possibility of local effects of the particle flow path on the fluidized heat transfer. To this end, a series of smaller fluidized bed heat exchangers were built utilizing an axially flowing open channel for the moving bed of fluidized particles. These designs featured a serpentine flow path representative the full scale HX design proposed by others. The proposed serpentine flow design is based on an existing particle cooling system; however, questions were raised about this design that had not yet been conclusively answered and promoted this investigation. The test bath supporting this investigation contains one bend around which the particulate flows prior to exiting the heat exchanger. The intent of this larger scale apparatus is to observe the variables affecting the stability or uniformity of the particle flow and provide insight into potential problems with the operational unit. The test rig consists of two stacked sections. The lower container is the fluidizing air plenum, which provides a uniformly distributed airflow through the bottom plane of the upper container. The interface comprises a structural perforated plate, stacked layers of filter paper to balance the pressure drop, and a fine stainless steel wire mesh to ensure that the particulate remains in the upper container. This upper container represents the particulate flow area. Clear conductive PETG polymer walls were used for the fluidized bath to reduce electrostatic buildup while still providing a transparent material through which the flow can be observed. The current design uses an air conveyor to recirculate the particulate from one end of the test bath back to the other closing the particle loop. The tests described investigate the effectiveness of fluidization in specific regions of the serpentine path. Measurements have been taken in these regions to determine the local heat transfer coefficient. This is accomplished by inserting a cartridge heater with a known power input and heated area, instrumented with a fine bead surface thermocouple to measure the heater surface temperature. In addition, two probes are immersed in the fluidized bed surrounding the cartridge heater to measure the free stream temperature in the bed. The air input for fluidization and air conveyor lift are also measured and recorded as test parameters along with approximate bed height in each region. In addition to the quantitative measurements of the flow, the test unit is used to observe the effect of fluidization, bed height, and outlet locations on the axial mass flow rate of the particulate. These results will be presented in the proposed paper. Going forward, this setup will allow for testing of various mass flow control schemes for the system. Currently this design, with the instrumented heater and free stream temperature probes, allows measurement of the local heat transfer properties anywhere in the particle flow path. The present tests provide a localized map of heat transfer coefficients in the fluidized bath design and a description of the flow behavior which will be reported and presented to support future open channel particle to sCO2 heat exchanger designs.
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