Purpose:To evaluate improvements in image homogeneity in pelvic MR imaging at 3 Tesla (T) using two different dielectric pads.
Materials and Methods:A total of eight healthy females were scanned using a 3T MR scanner equipped with a body-array coil. Axial and sagittal fast spin-echo T2-weighted images (T2WI) (TR/TE ϭ 3200 msec/94 msec), axial fast spin-echo T1-weighted images (T1WI) (TR/TE ϭ 700 msec/11 msec), and sagittal half-Fourier acquisition single-shot turbo spin-echo (HASTE) images (TR/TE ϭ 3000 msec/100 msec) were performed for pelvic imaging. Sequences were repeated with dielectric pads (consisting of either ultrasound [US] gel or water), and without pads. Three or four regions of interest (ROIs) were placed on fatty tissues and the ratio of minimum to maximum signal intensity (RSI) was calculated as a marker of image homogeneity.Results: RSI was significantly higher on T2WI and T1WI when using dielectric pads than when no pad was used. A similar tendency was observed in RSI on HASTE. No significant difference was found between images with US gel pads and those with water pads. THE USE OF MR SYSTEMS at magnetic field strengths of 3 Tesla (3T) or higher is beneficial in obtaining increased signal-to-noise ratio (SNR), potentially leading to reduced scanning time or reduced voxel size in obtaining high-resolution images (1). These advantages have been demonstrated in numerous brain imaging studies (2-6) and in some studies on body MRI including coronary artery, MR cholangiopancreatography (MRCP), prostate, and the female pelvis (7-10).
ConclusionDespite improvements in image quality (1,7-10), 3T MR body imaging faces a number of challenging issues. The greater susceptibility effect, increased specific absorption rate (SAR), and radiofrequency (RF) field inhomogeneity are drawbacks of 3T MR systems; these problems are more pronounced for body MR imaging (1).RF field inhomogeneity, or B1 inhomogeneity, is related to the shorter RF wavelengths at 3T. The RF wavelength in water becomes 26 cm at 3T, which is half its length at 1.5T, and approximates the size of the body's dimensions. Because the RF penetration effect is inversely proportional to the RF wavelength, RF does not reach deep into the body at 3T and causes signal dropoff at the center of the body. In addition, shorter RF waves tend to cause more severe RF wave interferences in the body as well as RF field inhomogeneity and locally irregular flip angle. It can also lead to bright or dark areas; this is known as the dielectric resonance effect or standing wave effect. These artifacts are more prominent for a larger target relative to the RF wavelength. Further RF effects are generated by eddy currents induced in conductive regions of the body. The current acts like an electromagnet that opposes the changing magnetic field, thus attenuating the RF field. This poses problems for cases of pregnant women or patients with massive ascites, as in these cases the