Background: This article explains some simple experiments that can be used in undergraduate or graduate physics or biomedical engineering laboratory classes to learn how birdcage volume radiofrequency (RF) coils and magnetic resonance imaging (MRI) work. For a clear picture, and to do any quantitative MRI analysis, acquiring images with a high signal-to-noise ratio (SNR) is required. With a given MRI system at a given field strength, the only means to change the SNR using hardware is to change the RF coil used to collect the image. RF coils can be designed in many different ways including birdcage volume RF coil designs. The choice of RF coil to give the best SNR for any MRI study is based on the sample being imaged.
Results: The data collected in the simple experiments show that the SNR varies as inverse diameter for the birdcage volume RF coils used in these experiments. The experiments were easily performed by a high school student, an undergraduate student, and a graduate student, in less than 3 h, the time typically allotted for a university laboratory course.
Conclusions: The article describes experiments that students in undergraduate or graduate laboratories can perform to observe how birdcage volume RF coils influence MRI measurements. It is designed for students interested in pursuing careers in the imaging field.
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http://www.ncbi.nlm.nih.gov/pmc/articles/PMC5669019 | PMC |
http://dx.doi.org/10.1186/s13036-017-0084-1 | DOI Listing |
Quant Imaging Med Surg
December 2024
Department of Biomedical Engineering, State University of New York at Buffalo, Buffalo, NY, USA.
Background: Low-field open magnetic resonance imaging (MRI) systems, typically operating at magnetic field strengths below 1 Tesla, has greatly expanded the accessibility of MRI technology to meet a wide range of patient needs. However, the inherent challenges of low-field MRI, such as limited signal-to-noise ratios and limited availability of dedicated radiofrequency (RF) coils, have prompted the need for innovative coil designs that can improve imaging quality and diagnostic capabilities. In this work, we introduce a multimodal axial array resonator and its implementation in a volume coil, or referred to as a coupled stack-up volume coil, to address these challenges in low-field open MRI.
View Article and Find Full Text PDFPLoS One
December 2024
Physical Sciences Platform, Sunnybrook Research Institute, Toronto, ON, Canada.
MRI of patients with Deep Brain Stimulation (DBS) implants is constrained due to radiofrequency (RF) heating of the implant lead. However, "RF-shimming" parallel transmission (PTX) has the potential to reduce DBS heating during MRI. As part of using PTX in such a "safe mode", maps of the RF transmission field (B1+) are typically acquired for calibration purposes, with each transmit coil excited individually.
View Article and Find Full Text PDFJ Magn Reson
November 2024
MPA-Q, Los Alamos National Laboratory, Los Alamos, NM 87545, USA.
DNP-NMR and EPR experiments that operate at or greater than L-band (i.e., ν(e) = 1-2 GHz) are typically limited to maximum sample volumes of several hundred µL.
View Article and Find Full Text PDFMagn Reson Med
February 2025
CIBM Center for Biomedical Imaging, Lausanne, Switzerland.
Magn Reson Med
February 2025
Medical Physics in Radiology, German Cancer Research Center (DKFZ), Heidelberg, Germany.
Purpose: Transmit arrays for body imaging have characteristics of both volume and local transmit coils. This study evaluates two specific absorption rate (SAR) aspects, local and whole-body SAR, of arrays for body imaging at 7 T and also for a 3 T birdcage.
Methods: Simulations were performed for six antenna arrays at 7 T and one 3 T birdcage.
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