{"title":"Magnetic backprojection imaging","authors":"H. Hong, M. Fox","doi":"10.1109/IEMBS.1993.978658","DOIUrl":null,"url":null,"abstract":"The assessment of the vascular lumen is of intense interest to clinicians because of the importance of early detection and quantification of atherosclerosis. We have developed a new technique (to our knowledge) for the assessment of anomalies in electrically conductive tubular smctures like blood vessels. We inject current (minimally invasive and potentially noninvasive) into the vessel, detect the resulting magnetic flux and then backproject to show any deviations from the linear flow of blood. which can indicate the narrowing of the vascular lumen by atheromatous plaque. Preliminary results on a phantom show that attainable resolution is within 1.02 mm. Introduction The measurement of the magnetic field from the human body (biomagnetism) has been used to detect the natural current flow especially around the brain and spinal cord. The magnetic energy is not significantly distorted or attenuated by human tissues, according to both electromagnetic field theory and experiment [11. The detection of natural biomagnetism requires ultrasensitive SQUID (Superconducting Quantum Interference Devices) magnetic sensors. However the SQUID needs cryogenic conditions, which leads to a high cost of manufacturing and maintenance. The system we developed also measures the magnetic field outside of the body, as in biomagnetism, but utilizes a Hall effect sensor which is small, cost effective and easy to maintain at m m temperature. The system we are developing uses injected c m n t which is high enough to generate a magnetic field detectable by a Hall sensor, but safe enough (less than 100 mA of IO kI-k ac current) for diagnostic screening use (21. The BiotSavart law and the preliminary results of our biomagnetism studies suggest that the direction and location of current generating a magnetic field can be determined from the magnetic flux pauem. Our hypothesis is that because of plasma electrolytes, the resistivity of blood (1.75 ohm m) is much lower than that of the wall layers, i.e., tunica intima, media and adventitia (200 ohm m), of the blood vessel [31. Therefore, injected current would flow along the blood stream. The blood vessel wall works as an insuIator like in electric cable. Therefore, the backprojection lines of magnetic flux would meet at one single point which is on the center line of current carrying conductor (blood). Any abnormality in the blood vessel corresponds to a deviation from the major center line of the blood stream, which is detectable by backprojection of magnetic flux. Our model studies were directed at confming this hypothesis in vitro. Method When the current injected into the blood, i, generates a magnetic field (Ampere’s law) like that shown in Fig.1, the magneric flux density, B. is given by the vectorial form of the Biot-Savart law: where B, I, and a, are vectors and X denotes vector cross product. Therefore, the direction of B is determined by the angIe formed between dl (direction of the blood vessel) and ar (unit vector) along the direction €rom the center of blood vessel to the measuring point with a distance of r. Current flows normal to the plane of the magnetic field and the direction of magnetic field (flux density), B, is tangential to the circle of radius, r, and perpendicular to a,. Therefore, the backprojection chords L B P ~ and L B P ~ (shown in Fig.1) meet at one single point, which is the center of the current carrier (position 0 in Fig.1). The Hall effect Sensor is sensitive to the flux density. B, and generates the output voltage, VH, in which the k, d. I. and q are respectively, the gain of Hall sensor, depth, lenglh of Hall element and the electron charge. Depending on the geometry between the bias current, I, and the flux density, B, VH represents only the horizontal (Va) or vertical ( V H ~ ) component of B, i.e., B,, By. From the fact that the backprojection Line should be normal to the magnetic flux, the corresponding center location (xc, yc) of the current carrying blood stream is determined as.","PeriodicalId":408657,"journal":{"name":"Proceedings of the 15th Annual International Conference of the IEEE Engineering in Medicine and Biology Societ","volume":"78 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1993-10-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Proceedings of the 15th Annual International Conference of the IEEE Engineering in Medicine and Biology Societ","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/IEMBS.1993.978658","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 1
Abstract
The assessment of the vascular lumen is of intense interest to clinicians because of the importance of early detection and quantification of atherosclerosis. We have developed a new technique (to our knowledge) for the assessment of anomalies in electrically conductive tubular smctures like blood vessels. We inject current (minimally invasive and potentially noninvasive) into the vessel, detect the resulting magnetic flux and then backproject to show any deviations from the linear flow of blood. which can indicate the narrowing of the vascular lumen by atheromatous plaque. Preliminary results on a phantom show that attainable resolution is within 1.02 mm. Introduction The measurement of the magnetic field from the human body (biomagnetism) has been used to detect the natural current flow especially around the brain and spinal cord. The magnetic energy is not significantly distorted or attenuated by human tissues, according to both electromagnetic field theory and experiment [11. The detection of natural biomagnetism requires ultrasensitive SQUID (Superconducting Quantum Interference Devices) magnetic sensors. However the SQUID needs cryogenic conditions, which leads to a high cost of manufacturing and maintenance. The system we developed also measures the magnetic field outside of the body, as in biomagnetism, but utilizes a Hall effect sensor which is small, cost effective and easy to maintain at m m temperature. The system we are developing uses injected c m n t which is high enough to generate a magnetic field detectable by a Hall sensor, but safe enough (less than 100 mA of IO kI-k ac current) for diagnostic screening use (21. The BiotSavart law and the preliminary results of our biomagnetism studies suggest that the direction and location of current generating a magnetic field can be determined from the magnetic flux pauem. Our hypothesis is that because of plasma electrolytes, the resistivity of blood (1.75 ohm m) is much lower than that of the wall layers, i.e., tunica intima, media and adventitia (200 ohm m), of the blood vessel [31. Therefore, injected current would flow along the blood stream. The blood vessel wall works as an insuIator like in electric cable. Therefore, the backprojection lines of magnetic flux would meet at one single point which is on the center line of current carrying conductor (blood). Any abnormality in the blood vessel corresponds to a deviation from the major center line of the blood stream, which is detectable by backprojection of magnetic flux. Our model studies were directed at confming this hypothesis in vitro. Method When the current injected into the blood, i, generates a magnetic field (Ampere’s law) like that shown in Fig.1, the magneric flux density, B. is given by the vectorial form of the Biot-Savart law: where B, I, and a, are vectors and X denotes vector cross product. Therefore, the direction of B is determined by the angIe formed between dl (direction of the blood vessel) and ar (unit vector) along the direction €rom the center of blood vessel to the measuring point with a distance of r. Current flows normal to the plane of the magnetic field and the direction of magnetic field (flux density), B, is tangential to the circle of radius, r, and perpendicular to a,. Therefore, the backprojection chords L B P ~ and L B P ~ (shown in Fig.1) meet at one single point, which is the center of the current carrier (position 0 in Fig.1). The Hall effect Sensor is sensitive to the flux density. B, and generates the output voltage, VH, in which the k, d. I. and q are respectively, the gain of Hall sensor, depth, lenglh of Hall element and the electron charge. Depending on the geometry between the bias current, I, and the flux density, B, VH represents only the horizontal (Va) or vertical ( V H ~ ) component of B, i.e., B,, By. From the fact that the backprojection Line should be normal to the magnetic flux, the corresponding center location (xc, yc) of the current carrying blood stream is determined as.
由于动脉粥样硬化的早期检测和量化的重要性,对血管腔的评估是临床医生非常感兴趣的。我们已经开发了一种新技术(据我们所知)来评估导电管状结构(如血管)的异常。我们将电流(微创和潜在的非侵入性)注入血管,检测产生的磁通量,然后反向投影以显示血液线性流动的任何偏差。这表明血管腔因动脉粥样硬化斑块而变窄。在一个模型上的初步结果表明,可达到的分辨率在1.02毫米以内。人体磁场的测量(生物磁学)已被用于检测自然电流,特别是在大脑和脊髓周围。根据电磁场理论和实验,磁场能量不会被人体组织明显扭曲或衰减[11]。天然生物磁学的检测需要超灵敏的超导量子干涉装置磁传感器。然而,SQUID需要低温条件,这导致制造和维护成本高。我们开发的系统也可以测量身体外的磁场,就像生物磁学一样,但使用的是霍尔效应传感器,它体积小,成本效益高,易于在m - m温度下保持。我们正在开发的系统使用注入c m nt的高磁场,足以产生霍尔传感器检测到的磁场,但足够安全(小于100 mA的IO kI-k交流电流),用于诊断筛查(21)。BiotSavart定律和我们的生物磁学研究的初步结果表明,产生磁场的电流的方向和位置可以由磁通量来确定。我们的假设是,由于血浆电解质的存在,血液的电阻率(1.75欧姆)远低于血管壁层,即内膜、中膜和外膜的电阻率(200欧姆)[31]。因此,注入的电流将沿着血流流动。血管壁像电缆一样起着绝缘体的作用。因此,磁通量的反投影线会在载流导体(血)的中心线上的一个单点相交。血管中的任何异常都与血液主要中心线的偏离相对应,这是通过磁通的反向投影检测到的。我们的模型研究旨在在体外证实这一假设。方法当注入血液的电流i产生如图1所示的磁场(安培定律)时,磁通密度B用比奥-萨瓦定律的矢量形式给出,其中B、i、a为矢量,X为矢量外积。因此,B的方向由dl(血管方向)和ar(单位矢量)沿从血管中心到测量点距离r的方向€形成的夹角决定。电流垂直于磁场平面,磁场方向(磁通密度)B与半径r圆相切,垂直于a。因此,反投影弦L B P ~和L B P ~(如图1所示)相交于一个单点,即电流载波的中心(图1中位置0)。霍尔效应传感器对磁通密度很敏感。B,产生输出电压VH,其中k、d、i、q分别为霍尔传感器增益、霍尔元件深度、霍尔元件长度和电子电荷。根据偏置电流I和磁通密度B之间的几何形状,VH仅表示B的水平(Va)或垂直(V H ~)分量,即B, By。根据反投影线应与磁通量垂直,确定载流血流的相应中心位置(xc, yc)为。