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首页> 外文期刊>Journal of Nuclear Materials: Materials Aspects of Fission and Fusion >Effect of proton beam profile on stress in JSNS target vessel
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Effect of proton beam profile on stress in JSNS target vessel

机译:质子束轮廓对JSNS靶血管应力的影响

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摘要

A cross-flow type (CFT) mercury target with flow guide blades hits been developed for JSNS that suppresses the generation of a stagnant flow region near the beam window where the peak power density is generated due to the spallation reaction. In addition, a flat type beam window has been applied to the CFT target that Suppresses dynamic stress caused by pressure waves, that have been estimated with an elastic model for mercury.Recent experimental results obtained by using a proton beam incident to mercury targets suggested. that using it cutoff pressure model for mercury would be appropriate for predicting it dynamic stress behavior in a target vessel. Dynamic stress analyses were carried out with the cutoff pressure model in which the negative pressure less than -0.15 MPa could not be sustained. The dynamic stress generated in the flat beam window became much larger than that in a semi-cylindrical type window as a result of using the cut-off pressure model. Regardless, even the stress generated in the semi-cylindrical type beam window exceeded the allowable stress of SS316L. under the peak power density of 668 MW/m(3). In order to decrease the dynamic stress in the semi-cylindrical beam window. the incident proton beam was defocused to reduce the peak power density down to 218 MW/m(3), Although the dynamic stress could be suppressed to less than the allowable stress, the high power density generated on the end of the flow guide blades due to defocus of the proton beam caused high thermal stress exceeding the allowable stress, Several shapes, of blade ends were studied analytically to decrease the thermal stress. that did not affect the mercury flow distribution, A simple thin-end blade showed low thermal stress below the allowable stress. (c) 2005 Elsevier B.V. All rights reserved.
机译:针对JSNS开发了带有导流叶片的错流型(CFT)汞靶,该靶可抑制束流窗口附近停滞的流动区域的产生,在该区域中由于散裂反应而产生峰值功率密度。另外,在CFT靶上已经应用了扁平型射束窗口,该窗口可以抑制由压力波引起的动态应力,该压力是通过汞的弹性模型估算得出的。建议通过使用质子束入射到汞靶上获得的最新实验结果。使用汞的截断压力模型将适合预测目标容器中的动态应力行为。使用截止压力模型进行了动态应力分析,其中不能维持小于-0.15 MPa的负压。由于使用了截止压力模型,因此在平光束窗口中产生的动应力变得比在半圆柱型窗口中产生的动应力大得多。无论如何,即使在半圆柱形梁窗口中产生的应力也超过了SS316L的允许应力。峰值功率密度为668 MW / m(3)。为了减少半圆柱梁窗口中的动应力。入射质子束散焦以将峰值功率密度降低到218 MW / m(3),尽管可以将动应力抑制到小于允许应力,但由于导流叶片末端产生的高功率密度为了使质子束散焦而导致高的热应力超过允许的应力,对叶片端部的几种形状进行了分析研究,以减小热应力。不会影响汞的流量分布,一个简单的薄端刀片显示出低于允许应力的低热应力。 (c)2005 Elsevier B.V.保留所有权利。

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