By Haris S. Chrysikopoulos
Keywords Spin › Electromagnetic radiation › Resonance › Nucleus › Hydrogen › Proton › definite atomic nuclei own inherent magnetic allow us to summarize the MRI approach. Te sufferer homes referred to as spin, and will have interaction with electro- is positioned in a magnetic feld and turns into briefly 1 magnetic (EM) radiation via a technique known as magnetized. Resonance is accomplished during the - resonance. while such nuclei take up EM strength they plication of specifc pulses of EM radiation, that's continue to an excited, risky confguration. Upon absorbed through the sufferer. therefore, the surplus - go back to equilibrium, the surplus power is published, ergy is liberated and measured. Te captured sign generating the MR sign. Tese tactics aren't is processed via a working laptop or computer and switched over to a grey random, yet obey predefned principles. scale (MR) photograph. Te least difficult nucleus is that of hydrogen (H), con- Why can we have to position the sufferer in a m- sisting of just one particle, a proton. as a result of its web? as the earth’s magnetic feld is simply too susceptible to abundance in people and its powerful MR sign, H be clinically invaluable; it varies from zero. 3–0. 7 Gauss (G). is the main helpful nucleus for scientific MRI. Tus, foC r urrent medical MR structures function at low, mid or our reasons, MRI refers to MRI of hydrogen, and for h igh feld power starting from zero. 1 to 3.
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The lesion is “unmasked” by fat suppression, in c and d. Note that the lesion is more conspicuous in STIR than in c, despite an unfavorable large difference in TE (30 vs 112 ms). 56a–d Failure of selective fat suppression. A 60-year- old with knee pain. Axial a T1-w SE (465/14), b STIR (4,000/TI 120/30), and c fat-suppressed PD (2,823/33) images. The anterior cruciate ligament (ACL) is very thick (arrows). In c, fat suppression is successful only in the soft tissues posteriorly and partly in the lateral femoral condyle.
A 30-yearold woman with dysmenorrhea. Transaxial a T1-w TSE (690/20), b T2-w TSE (3,870/112), c fat-suppressed T1-w TSE (640/12), and d post-contrast T1-w TSE (690/20) slices. 5 cm in size) are present bilaterally (arrows). The right one has intermediate to high T1 and very low T2 signal intensity. It appears Ch a pter 2 0 very bright after fat saturation. The left lesion is moving in the opposite direction in all pulse sequences. Note the peripheral (rim) enhancement, which is more obvious on the left-hand side.
Hence, there is a need for rapid alternatives. Since imaging time is linearly related to TR, one would be tempted to compress TR for time savings. 38). The ingenious solution is to disengage tissue saturation and tissue contrast from the influence of TR, using excitation pulses (θ) less than 90° (partial flip angle). In this way, only a fraction of the longitudinal magnetization Mz is converted to transverse magnetization Mxy. A considerable portion of the macroscopic vector M is kept on the z-axis (at all times), available for successive TR cycles.