首页> 外文会议>ASME International Conference on Energy Sustainability;ASME Heat Transfer Conference >OPTICAL RAY-TRACING PERFORMANCE MODELING OF QUARTZ HALF-SHELL TUBES APERTURE COVER FOR FALLING PARTICLE RECEIVER
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OPTICAL RAY-TRACING PERFORMANCE MODELING OF QUARTZ HALF-SHELL TUBES APERTURE COVER FOR FALLING PARTICLE RECEIVER

机译:坠落接收器的石英半壳管孔径盖的光学跟踪性能建模

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A 1 MW_t falling particle receiver prototype was designed, built and is being evaluated at Sandia National Laboratories, National Solar Thermal Test Facility (NSTTF). The current prototype has a 1 m~2 aperture facing the north field. The current aperture configuration is susceptible to heat and particle losses through the receiver aperture. Several options are being considered for the next design iteration to reduce the risk of heat and particle losses, in addition to improving the receiver efficiency to target levels of ~90%. One option is to cover the receiver aperture with a highly durable and transmissive material such as quartz glass. Quartz glass has high transmittance for wavelengths less than 2.5 microns and low transmittance for wavelengths greater than 2.5 microns to help trap the heat inside the receiver. To evaluate the receiver optical performance, ray-tracing models were set up for several different aperture cover configurations. The falling particle receiver is modeled as a box with a 1 m~2 aperture on the north side wall. The box dimensions are 1.57 m wide × 1.77 m tall × 1.67 m deep. The walls are composed of RSLE material modeled as Lambertian surfaces with reflectance of either 0.9 for the pristine condition or 0.5 for soiled walls. The quartz half-shell tubes are 1.46 m long with 105 mm and 110 mm inner and outer diameters, respectively. The half-shell tubes are arranged vertically and slant forward at the top by 30 degrees. Four configurations were considered: concave side of the half-shells facing away from the receiver aperture with (1) no spacing and (2) high spacing between the tubes, and concave side of the half-shells facing the aperture with (3) no spacing and (4) high spacing between the tubes. The particle curtain, in the first modeling approach, is modeled as a diffuse surface with transmittance. reflectance, and absorptance values, which are based on estimates from previous experiments for varying particle flow rates. The incident radiation is from the full NSTTF heliostat field with a single aimpoint at the center of the receiver aperture. The direct incident rays and reflected and scattered rays off the internal receiver surfaces are recorded on the internal walls and particle curtain surfaces as net incident irradiance. The net incident irradiances on the internal walls and particle curtain for the different aperture cover configuration are compared to the baseline configuration. In all cases, just from optical performance alone, the net incident irradiance is reduced from the baseline. However, it is expected that the quartz half-shells will reduce the convective and thermal radiation losses through the aperture. These ray-tracing results will be used as boundary conditions in computational fluid dynamics (CFD) analyses to determine the net receiver efficiency and optimal configuration for the quartz half-shells that minimize heat losses and maximize thermal efficiency.
机译:设计,制造了一个1 MW_t的降落粒子接收器原型,并在桑迪亚国家实验室的国家太阳能热测试设施(NSTTF)中进行评估。当前的样机面向北场的孔径为1 m〜2。当前的光圈配置易于通过接收器光圈散失热量和颗粒。除了将接收器效率提高到90%左右的目标水平外,下一次设计迭代还考虑了几种选择,以降低热量和颗粒损失的风险。一种选择是用高度耐用且可透射的材料(例如石英玻璃)覆盖接收器孔。石英玻璃对于小于2.5微米的波长具有高透射率,对于大于2.5微米的波长具有低透射率,以帮助将热量收集在接收器内部。为了评估接收器的光学性能,针对几种不同的光圈盖配置建立了射线追踪模型。下落的粒子接收器被建模为一个在北侧壁上具有1 m〜2的孔径的盒子。盒子尺寸为1.57 m宽×1.77 m高×1.67 m深。墙壁由建模为朗伯表面的RSLE材料组成,对于原始状态,反射率为0.9;对于弄脏的墙壁,反射率为0.5。石英半壳管长1.46 m,内径和外径分别为105 mm和110 mm。半壳管垂直排列,并在顶部向前倾斜30度。考虑了四种配置:半壳的凹面背向接收器孔,(1)无间距,(2)管之间的间距大;半壳的凹面背向接收器孔,(3)无。间距和(4)管之间的高间距。在第一种建模方法中,粒子幕被建模为具有透射率的漫射表面。反射率和吸收率值,这些值是基于先前实验对各种颗粒流速的估算得出的。入射辐射来自整个NSTTF定日镜场,其单个瞄准点位于接收器孔径的中心。离开内部接收器表面的直接入射光线以及反射和散射光线记录为内壁和粒子幕表面上的净入射辐照度。将不同孔径盖配置的内壁和粒子幕上的净入射辐照度与基线配置进行比较。在所有情况下,仅从光学性能而言,净入射辐照度都比基线降低。但是,可以预期的是,石英半壳将减少通过孔的对流和热辐射损失。这些射线追踪结果将在计算流体动力学(CFD)分析中用作边界条件,以确定净接收器效率和石英半壳的最佳配置,从而将热量损失最小化并将热效率最大化。

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