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Temperatures of continuously operated mobile x-ray focal spots

机译:连续操作的移动X射线焦点的温度

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摘要

We use the adjective "mobile" to describe a focal spot in an x‐ray tube which moves cyclically in a closed path relative to the target surface on which it is generated quite without reference to whether the spot be fixed or in motion with respect to the tube. Alex Müller and also A. Bouwers have made calculations of the thermal effects in such spots energized for very short fractions of one cycle of motion. This paper treats the case where the focal spot is energized continuously so that a "steady" state of thermal oscillation is set up. The solutions obtained refer only to conditions after this steady state of oscillation is reached. Only the ideal case of a spot of uniform intensity with sharp boundaries is treated. For simplicity the flow of heat from front target surface to cooling water is assumed one dimensional and normal to the front surface over an everywhere uniform thickness d. Curves are plotted showing the ratio of temperature rise in moving spots to that in fixed spots of the same size as a function of r the size of the spot relative to the length of path it describes and of θ a variable depending on the speed of rotation, the thickness d and the thermal constants of the target material. Curves of the ratio of permissible energy input for moving and fixed spots, respectively, as a function of the aforementioned variables are also shown. The paper gives a solution reduced to figures and curves of the heat flow equation for certain boundary conditions which to the author's knowledge has never before been obtained and therefore has some interest beyond its immediate application to x‐ray tubes. Certain mathematical difficulties of practical interest are also overcome in a way which may be helpful in other problems of similar nature. For the reader uninterested in mathematics the results are independently discussed in a separate section. Approximate methods are given for applying the results of the paper to targets consisting of two materials such as tungsten and copper.
机译:我们使用形容词“移动”来描述X射线管中的焦点,该焦点相对于在其上生成目标表面的闭合路径循环运动,而完全不考虑该点是相对于目标固定还是运动。管。亚历克斯·穆勒(AlexMüller)和A.布沃斯(A. ​​Bouwers)已计算出在一个运动周期的非常短的时间内通电的此类点的热效应。本文讨论了持续向焦点供电以建立热振荡的“稳定”状态的情况。获得的解仅涉及达到此稳定振荡状态后的条件。仅处理强度均匀,边界清晰的光斑的理想情况。为简单起见,假设热量从前目标表面流到冷却水的方向是一维且垂直于前表面,且处处都是均匀的厚度d。绘制了曲线图,显示了相同大小的移动点与固定点的温升之比,其与点的大小相对于其描述的路径长度的函数r和随旋转速度而变化的θa有关,厚度d和目标材料的热常数。还示出了根据上述变量的分别用于运动点和固定点的允许能量输入的比率的曲线。本文针对某些边界条件给出了热流方程的图和曲线的简化解,据作者所知,这是从未获得的,因此,除了将其立即应用于X射线管外,还有一些兴趣。某些实际实用的数学难题也可以通过对类似性质的其他问题有所帮助的方式来克服。对于对数学不感兴趣的读者,结果将在单独的部分中单独进行讨论。给出了将纸的结果应用于由两种材料(例如钨和铜)组成的靶材的近似方法。

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