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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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楼主: odometer
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Frequency GradientSo far, we have shown how we select an image plane, which represents only the first of the three coordinates that we must specify. To complete our image, we must understand how the other two orthogonal gradients specify the other two coordinates of each point in a given plane.
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The Phase Encoding Gradientor 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 commercial scanners available today make use of “phase encoding”. This rather difficult concept will now be explained in depth.
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Some other Pulse Cycles and Proceduresstanding of what they mean. And in fact, the author wishes to point out that at least one MR equipment vendor had for some time caused confusion by using the term “partial saturation” to refer to its T1 weighted single echo spin-echo. Fortunately, this has been rectified.
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Motion 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 will be sure to acknowledge those instances where we fall short of an adequate explanation.
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Book 19922nd editiond 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 expa
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Radiofrequency Pulseticle or a magnetizable substance would experience will vary in time from a maximum in one direction to a maximum in the opposite direction. It turns out that this variation in time can be mathematically described with a simple sine or cosine function.
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