核技术
覈技術
핵기술
Nuclear Techniques
2015年
9期
090201-1-090201-5
,共1页
张催%李公平%潘小东%魏绪波%商宏杰%饶松%郑赛春%张益海
張催%李公平%潘小東%魏緒波%商宏傑%饒鬆%鄭賽春%張益海
장최%리공평%반소동%위서파%상굉걸%요송%정새춘%장익해
强度分布%X 射线机%工业 CT%阳极效应
彊度分佈%X 射線機%工業 CT%暘極效應
강도분포%X 사선궤%공업 CT%양겁효응
Intensity distribution%X-ray machine%Industrial CT%Anode effect
X 射线机是工业 CT 中使用最广泛的 X 射线源,但因阳极效应以及自身结构的限制,其射线强度空间分布不均匀,系统的研究和测量其射线强度分布对于实际应用十分必要。利用 CsI(Tl)光电二极管探测器测量了射线强度在不同轴线上随角度的分布,给出了理论分析,并与蒙特卡罗法计算结果做了对比,提出了“展宽效应”,解释了边界射线强度分布展宽的现象。比较了大、小焦点射线强度分布的情况,给出了其在阴极末端出现差异的原因。结合其在竖直方向的射线强度分布以及对称性,给出了 X 射线强度的二维分布。结果表明,在张角20°(–10°–+10°)的范围内,射线强度分布均匀(最大相对偏差4.59%),张角越大均匀性越差,在阴极端边界射线分布出现外延。
X 射線機是工業 CT 中使用最廣汎的 X 射線源,但因暘極效應以及自身結構的限製,其射線彊度空間分佈不均勻,繫統的研究和測量其射線彊度分佈對于實際應用十分必要。利用 CsI(Tl)光電二極管探測器測量瞭射線彊度在不同軸線上隨角度的分佈,給齣瞭理論分析,併與矇特卡囉法計算結果做瞭對比,提齣瞭“展寬效應”,解釋瞭邊界射線彊度分佈展寬的現象。比較瞭大、小焦點射線彊度分佈的情況,給齣瞭其在陰極末耑齣現差異的原因。結閤其在豎直方嚮的射線彊度分佈以及對稱性,給齣瞭 X 射線彊度的二維分佈。結果錶明,在張角20°(–10°–+10°)的範圍內,射線彊度分佈均勻(最大相對偏差4.59%),張角越大均勻性越差,在陰極耑邊界射線分佈齣現外延。
X 사선궤시공업 CT 중사용최엄범적 X 사선원,단인양겁효응이급자신결구적한제,기사선강도공간분포불균균,계통적연구화측량기사선강도분포대우실제응용십분필요。이용 CsI(Tl)광전이겁관탐측기측량료사선강도재불동축선상수각도적분포,급출료이론분석,병여몽특잡라법계산결과주료대비,제출료“전관효응”,해석료변계사선강도분포전관적현상。비교료대、소초점사선강도분포적정황,급출료기재음겁말단출현차이적원인。결합기재수직방향적사선강도분포이급대칭성,급출료 X 사선강도적이유분포。결과표명,재장각20°(–10°–+10°)적범위내,사선강도분포균균(최대상대편차4.59%),장각월대균균성월차,재음겁단변계사선분포출현외연。
Background: X-ray machine is the most-extensively-used X-ray source in industrial CT, due to its anode effect and the restrictions of its own structure, the radiation intensity distribution is not uniform. Purpose: The aim is to research and measure the radiation intensity distribution of X-ray machine as a vital part of imaging correction and the foundation for the precise application of X-ray machine. Methods: The CsI(Tl) scintillation and photodiode detector is used to measure the radiation intensity distribution of the MXR225/22 X-ray machine (made by Swiss COMET Inc.) along with various angles on different axis. At the same time, the radiation intensity distribution is simulated by Monte Carlo method. Results: The “broadening effect” is observed, and the boundary radiation intensity distribution broadening phenomena can be explained thereby. The radiation intensity distributions of the large and small focal are compared, and the reason for the difference in the cathode ends is analyzed. And the 2D radiation intensity distribution of X-ray machine is given. Conclusion: The results showed that in the 20° opening angle range (–10°–+10°), the radiation intensity distributes uniformly, the larger opening angle, the worse distribution uniformity. The radiation distribution extension occurs at the boundary of cathode side.