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Titlebook: MRI Physics for Radiologists; A Visual Approach Alfred L. Horowitz Book 19922nd edition Springer-Verlag New York, Inc. 1992 Magnetic Resona

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發(fā)表于 2025-3-21 18:14:30 | 只看該作者 |倒序?yàn)g覽 |閱讀模式
書(shū)目名稱MRI Physics for Radiologists
副標(biāo)題A Visual Approach
編輯Alfred L. Horowitz
視頻videohttp://file.papertrans.cn/621/620242/620242.mp4
圖書(shū)封面Titlebook: MRI Physics for Radiologists; A Visual Approach Alfred L. Horowitz Book 19922nd edition Springer-Verlag New York, Inc. 1992 Magnetic Resona
描述When this book was initially published three years ago, it was my goal to delineate the principles of magnetic resonance imaging in a format that could be understood without a sophisticated physics or mathematics back- ground. That is still my goal. However, in the interim, it has become clear to me that many magnetic resonance techniques that we now routinely use are inadequately understood by many of us. Therefore, I have re-structured and expanded the book in the following way. There are now three main sections: of the sections one and two deal with the contrast and spatial characteristics image, as they did in the original text; and an additional section deals with various peripheral but significant magnetic resonance topics. Sections one and two still provide the "meat" of the material through the guise of the spin-echo pulse sequence; but section three goes beyond by explaining other pulse cycles and devices that are commonly used in today‘s imaging centers. To begin with, since fast scanning has now become a widely used tech- nique, that chapter has been significantly expanded, and now includes a complete but non-mathematical explanation of what a gradient echo is and how fa
出版日期Book 19922nd edition
關(guān)鍵詞Magnetic Resonance Imaging (MRI; Radiologists; angiography; fat; imaging; magnetic resonance; magnetic res
版次2
doihttps://doi.org/10.1007/978-1-4684-0428-9
isbn_ebook978-1-4684-0428-9
copyrightSpringer-Verlag New York, Inc. 1992
The information of publication is updating

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Radiofrequency Pulseurrent through a wire, we create an electromagnetic field. That is, we have both an electrical field and a magnetic field at the same time, which means that either a charged particle or a “magnetizable” substance would experience a force when placed in this region. Now if we make that current an . c
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Gradientshow these different intensities are arranged in space to produce an image. There are a number of ways of doing this, but in this section, we will be concerned only with the most widely used method: two dimensional Fourier transform (“2DFT”) reconstruction.
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The Slice Select Gradientdient imposes a gradual change in the main magnetic field from the head to the foot end of the patient. If we graph the z gradient with the magnitude of the magnetic field on the y axis and the position along the long axis of the body on the x axis, then we obtain the straight line shown in the grap
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The Phase Encoding Gradiention just as we did for the x axis. However, if we did that, then we would not be able to uniquely specify whether a given frequency belonged to the x or the y axis, and the computer would get confused and render us an improper image reconstruction. So we must do something else, and in fact, all comm
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Wrapping up Basic Conceptsrequency change; and the y gradient produces a phase change. It is important to realize that each gradient is the same physical phenomenon: a change in the magnetic field from one point in space to another. Also, each gradient produces the same basic effect on protons: the vector precession frequenc
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Motion devices used to control motion artifacts and MR angiography. Although we will try to explain every phenomenon in terms of the principles that we have already learned, this may not always be possible because of the complexity of this subject. However, we will be able to explain most things; and we w
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