Imaging of Soft Tissues Adjacent to Orthopedic Hardware: Comparison of 3-T and 1.5-T MRI

Size: px
Start display at page:

Download "Imaging of Soft Tissues Adjacent to Orthopedic Hardware: Comparison of 3-T and 1.5-T MRI"

Transcription

1 Musculoskeletal Imaging Original Research Farrelly et al. MRI of Orthopedic Hardware Musculoskeletal Imaging Original Research Cormac Farrelly 1 Amir Davarpanah 2 Stephen Brennan 3 Mathew Sampson 4 Stephen J. Eustace 1 Farrelly C, Davarpanah A, Brennan S, Sampson M, Eustace SJ Keywords: 1.5 T, 3 T, artifact reduction, MRI, susceptibility DOI: /AJR Received August 27, 2008; accepted after revision July 6, Department of Radiology, Cappagh National Orthopaedic Hospital, Finglas, Dublin 11, Republic of Ireland. Address correspondence to C. Farrelly (farrellycormac@ gmail.com). 2 Department of Radiology, Northwestern University Hospital, Feinberg School of Medicine, Chicago, IL. 3 Department of Orthopedic Surgery, Cappagh National Orthopaedic Hospital, Finglas, Dublin, Republic of Ireland. 4 Department of Radiology, Sports Surgery Clinic, Santry Demesne, Dublin, Republic of Ireland. WEB This is a Web exclusive article. AJR 2010; 194:W60 W X/10/1941 W60 American Roentgen Ray Society Imaging of Soft Tissues Adjacent to Orthopedic Hardware: Comparison of 3-T and 1.5-T MRI OBJECTIVE. The purpose of this study was to compare metal artifact reduction techniques at 1.5-T and 3-T MRI. MATERIALS AND METHODS. A titanium plate with steel screws was placed in a freshly harvested pig leg. The leg was imaged with 1.5-T and 3-T MRI. A T2-weighted turbo spin-echo sequence was used with echo-train lengths of 8, 16, 32, and 64 and a constant readout bandwidth of 31.2 khz. The images were compared qualitatively, and the optimal echotrain length was selected. Images were acquired at the optimal echo-train length with four different readout bandwidths. Artifact was measured quantitatively, and image quality was ranked qualitatively. The qualitatively best image acquired at 1.5 T was compared with the qualitatively highest-ranked image acquired at 3 T. RESULTS. At both 1.5 T and 3 T, optimal images of equal quality were produced at echotrain lengths of 8 and 16. At higher readout bandwidths, there was quantitatively less artifact. The qualitatively best images were acquired at a readout bandwidth of 31.2 khz at 1.5 T and 62.5 khz at 3 T (Cronbach s α = 1.00). The optimal image at 3 T was qualitatively superior to that at 1.5 T. CONCLUSION. Optimizing image acquisition parameters in this phantom model resulted in similar quantitative susceptibility artifact at 3 T and 1.5 T and better qualitative images at 3 T than at 1.5 T. J oint replacements such as total hip arthroplasty are among the most commonly performed operations worldwide. With an aging population and as the clinical threshold for surgery decreases, this number will continue to rise [1]. The rate of complications requiring surgical revision after total hip arthroplasty has been reported to be as high as 17.5% in certain centers [2]. MRI of these complications can be difficult because metallic substances in a magnetic field induce magnetic field inhomogeneity, which induces a number of artifacts. These artifacts are often collectively referred to as susceptibility artifact. Gradient-recalled echo sequences are particularly prone to metallic artifact because of intravoxel dephasing [3] (Fig. 1). In regions of steep changes in the local magnetic field, such as those adjacent to metallic prostheses, the magnetic field that acts on protons within a single voxel can vary strongly. Unlike spin-echo sequences, gradient-recalled echo acquisitions do not entail use of a 180 refocusing pulse and therefore do not cor- rect for static field inhomogeneities. The result is marked dephasing of transverse spins and local signal loss (Fig. 1) that is more pronounced at higher field strengths because local distortions are directly proportional to the strength of the main magnetic field. Standard spin-echo and turbo spin-echo (TSE) sequences are less prone to artifact from static magnetic field inhomogeneity because of their refocusing 180 pulses. They are, however, prone to artifact due to variable magnetic field inhomogeneity. This includes signal void in the vicinity of the prosthesis caused by dephasing from randomly diffusing proton spins and characteristic lines of signal void and signal increase due to spatial misregistration artifact. The use of TSE with smaller interecho spacing, in which the frequency-encoding direction is oriented away from the tissues of interest and the readout bandwidth is increased, can reduce the effect of these artifacts [4 18]. With these methods, 1.5-T MRI can be clinically useful in evaluating complications after spinal surgery [4, 5] and total hip arthroplasty [6 12]. The purpose of W60 AJR:194, January 2010

2 MRI of Orthopedic Hardware Fig. 1 Pig leg with titanium plate prosthesis and two stainless steel nails in situ. Gradient-echo 3-T MR image (TR/TE, 375/10; flip angle, 20 ) shows marked susceptibility artifact due to constant and variable distortions in local magnetic field induced by metallic orthopedic prosthesis. this phantom study was to image orthopedic hardware in an animal cadaver leg to compare quantitative measurements of susceptibility artifact and qualitative measurements of overall image quality of 1.5-T and 3-T MRI after optimization of sequence parameters for both field strengths. Materials and Methods A titanium plate was surgically attached with two steel screws to the tibia of a freshly harvested pig leg. This leg was imaged with 1.5-T MRI (Signa HDx system, GE Healthcare) followed immediately by 3-T MRI (Signa HDx system). A standard transmit receive knee coil was used for each MRI unit. Ethical approval for this animal cadaver study was not required at our institution. Imaging parameters were kept as near identical as possible for the 1.5-T and 3-T MRI units. A matrix, slice thickness of 4 mm, and spacing of 1 mm were used. The field of view was selected to fit the size and orientation of the pig leg in the coronal plane. T2-weighted TSE (TR/TE, 2,540 13,940/70) and a frequency-encoding direction oriented away from the tissues of interest were selected. Each image was evaluated at standard window settings of center 6,500 and width 18,000. The pig leg was weighed (8.5 kg), and the specific absorption rate (SAR) limitations were entered into the MRI acquisition protocols. An estimated SAR of 3 W/kg, average coil SAR of 3 W/ kg, and peak SAR of 6 W/kg were selected. Echo-train length (ETL) and readout bandwidth were varied at 1.5 T and 3 T. Readers were blinded to magnetic field strength and sequence. The leg was initially imaged at ETLs of 8, 16, 32, and 64 with a constant readout bandwidth of 31.2 khz. The images were qualitatively ranked from 1 to 4. The ETL producing the optimal image quality (rank 1) was selected. The ETL then was kept constant at the optimal length (rank 1), and the leg was imaged at readout bandwidths of 15.6, 31.2, 62.5, and 125 khz. Objective Image Quality Parameters Quantitative measurements were made by two experienced radiologists using standard software. The readers assessed the images quantitatively by measuring the thickness of the artifact caused by the titanium plate at a predefined location at one of the screw orifices, measuring the maximal marrow thickness of the tibia in the transverse plane, and calculating the ratio between the two values (Fig. 2). The ratio measurements and calculations were repeated for all sequences at the optimal ETL in identical slice positions. The mean of the measurements recorded by the readers for each sequence was the final measurement for the results. The ratio of artifact to marrow thickness was directly comparable between the sequences imaged on the same unit because the phantom was not moved between sequences. One blinded reader repeated all measurements 5 months later, and intraobserver variability was recorded. Subjective Image Quality Parameters The images were ranked qualitatively from 1 to 4. Two readers with at least 5 years of radiology experience evaluated the images. Qualitative assessment involved comparing the image quality of the four sequences with differing ETLs and the four sequences with differing readout bandwidths at both 1.5 T and 3 T. The images from each sequence were loaded into a workstation and directly compared side by side. For each group of four sequences, the readers were asked to take into account three specific factors: amount of identifiable susceptibility artifact caused by the prosthesis, appreciable image noise or mottle, and lack of definition or sharpness in the periprosthetic tissues. Fig. 2 Pig leg with orthopedic hardware in situ. Example of quantitative measurement. Turbo spinecho MR image (TR/TE, 5,120/70; ETL, 16; readout bandwidth, 15.6 khz) shows increased susceptibility artifact involving periprosthetic soft tissues compared with higher readout bandwidth used for Figure 4B. Thickness of artifact due to titanium plate was measured at predefined location (distal screw orifice, short line), and marrow thickness was measured in transverse plane at thickest level (long line). These two measurements were repeated for all sequences with echo-train length of 16 at identical slice position. Ratio of artifact to marrow thickness (0.8 in this case) was directly comparable between sequences imaged with same MRI unit because phantom was not moved between sequences. After taking these three factors into account, the readers decided on which images they would prefer to report and ascribed a ranking score of 1 4 to each group, 1 representing superior image quality with the best visualization of periprosthetic soft tissue and 4 being the worst in that group. For each group the observers commented on which one of the three artifacts predominated as the respective scores worsened. If they were found to be of equal quality for visualization of the periprosthetic soft tissues, the images were ranked with the same number. Finally, the highest-ranked qualitative images (rank 1) at 1.5 T and 3 T were compared and ranked qualitatively in the same manner. Statistical Analysis Analysis was performed with statistical software (SPSS version 17.0, SPSS). Agreement on qualitative image ranking and quantitative artifact measurement was determined with reliability statistics including intraclass correlation coefficient based on the Cronbach alpha model. Interreader and intrareader agreement was calculated for the quantitative measurements. Agreement of more than 0.41, 0.61, and 0.81 was considered moderate, good, and very good, respectively. Results In the qualitative analysis, varying ETL produced images of equal quality at ETLs of 8 and 16 (Table 1). This was true at 1.5 T and 3 T. When the ETL was increased to 32 and 64, the readers commented that bone and softtissue definition was progressively worse (subjectively more blurred) at 1.5 T and 3 T (Fig. 3). Agreement between the readers was very good (α = 1.00). At both 1.5 T and 3 T, an ETL of 16 (rank 1) was selected. As the readout bandwidth was increased, there was quantitatively less artifact from the titanium plate (Table 2) (Fig. 2). Both interreader (α = 0.991) and intrareader (α = 0.995) agreement on quantitative measurements were very good. AJR:194, January 2010 W61

3 Farrelly et al. TABLE 1: Qualitative Ranks of Images at Varied Echo-Train Lengths and Constant Readout Bandwidth of 31.2 khz Echo-Train Length Rank Echo-Train Length Rank Note Readers comments stated that definition of periprosthetic tissues worsened progressively with more blurring as echo-train length increased. TABLE 2: Quantitative Measurements of Images With Varied Readout Bandwidths and Constant Echo-Train Length of 16 Readout Bandwidth (khz) Ratio Readout Bandwidth (khz) Ratio Note At both field strengths, the thickness of the susceptibility artifact decreased in relation to marrow thickness of the tibia as the readout bandwidth increased. These measurements are directly comparable between sequences on the same MRI unit but not between sequences at different field strengths (Fig. 2). A According to the comments by the readers regarding the qualitative ranking, noise increased subjectively as readout bandwidth was increased. The optimal compromise between artifact reduction and signal-to-noise ratio (SNR), determined with the qualitative ranking scores, was readout bandwidths of 31.2 khz (1.5 T) and 62.5 khz (3 T). There was no difference in qualitative scores between the two readers (α = 1.00) (Table 3). Both readers ranked the optimal image obtained at 3 T (ETL, 16; readout bandwidth, 62.5 khz) qualitatively superior to the optimal image obtained at 1.5 T (ETL, 16; readout bandwidth, 31.2 khz) (Fig. 4), commenting that there was less image noise and mottle and better definition of the periprosthetic soft tissues at 3 T. Discussion MRI at 1.5 T is clinically useful for evaluating periprosthetic tissue [6, 7]. White et Fig. 3 Pig leg with titanium plate prosthesis and two stainless steel nails in situ. A, Turbo spin-echo 3-T MR image (TR/TE, 6,050/70; echo-train length, 32; readout bandwidth, 31.2 khz) shows more blurring (less sharpness) of periprosthetic soft tissues than in B. B, Turbo spin-echo 3-T MR image (4,400/70; echo-train length, 16; readout bandwidth, 31.2 khz ) shows less blurring than A. B al. [6] found complications in 11 of 14 patients with pain after total hip arthroplasty. Johnston et al. [7] imaged 28 patients, all of whom had undergone previous imaging with other techniques and had persistent unexplained pain after total hip arthroplasty. In 15 cases, the cause of the pain was explained by MRI findings, and in 11 of the 15 cases, the complications were managed locally without open revision surgery. The clinical use of 3-T MRI is increasing. Doubling the field strength offers a potential doubling of SNR. There is concern, however, that imaging of orthopedic hardware at 3 T can increase susceptibility artifact [19, 20]. Our study showed that methods similar to those used to reduce susceptibility artifact at 1.5 T, such as using TSE sequences, can be used at 3 T. In addition, although there is potentially more susceptibility artifact from surgical hardware at higher field strengths, this artifact can be offset by the use of higher readout bandwidth. Metallic hardware in a magnetic field acquires magnetism proportional to the strength of the main magnetic field. Adjacent protons and water molecules then precess under the influence of the local magnetic field and either have a different frequency or rapidly dephase. Signal is localized in space by frequency and phase. The phase-encoding direction is less prone to produce geometric distortions induced by magnetic field inhomogeneity. Susceptibility artifact represents a combination of intravoxel dephasing, diffusion-related signal loss, and spatial misregistration. Therefore, susceptibility artifact acquires an oval configuration elongated in the frequency plane [8, 9]. To compare artifacts at 1.5 T and 3 T, an imaging plane (coronal) that depicts the entire length of a prosthesis was selected. All other parameters were selected to minimize artifact on both MRI units. Previous reports [4 18] have described numerous methods of decreasing susceptibility artifact at 1.5 T. These methods include use of TSE sequences, orienting the frequency-encoding direction away from the tissue of interest, increasing readout gradient strength, decreasing field of view and voxel size, and using parallel imaging techniques. We used a matrix size in this study. The frequency-encoding direction was oriented along the long axis of the tibia to allow optimal visualization of the periprosthetic soft tissue, and the field of view was determined by the size of the prosthesis. Parallel imaging technique was not used. W62 AJR:194, January 2010

4 MRI of Orthopedic Hardware TABLE 3: Qualitative Ranking of Images With Varied Readout Bandwidths and Constant Echo-Train Length of 16 Readout Bandwidth (khz) Rank Readout Bandwidth (khz) Rank Note Observers commented that at lower readout bandwidth, artifact from the prosthesis predominated but that at higher bandwidths, image noise and mottle were more prominent. Use of a TSE sequence, which has a long, closely spaced train of refocusing 180 pulses, reduces susceptibility artifact compared with use of a standard spin-echo sequence [4 18]. Randomly diffusing proton spins adjacent to metallic devices cause dephasing of spinning protons. This effect is inversely proportional to the distance from the prosthesis and is more pronounced at T2-weighted imaging because longer TEs allow increased dephasing. Use of TSE helps to reduce diffusion-related signal loss relative to use of standard spin-echo technique because multiple 180 refocusing pulses are applied within a single TR. The resulting shorter effective TE (echo spacing) allows less time for dephasing before the spins are refocused. With longer ETLs, however, the echoes at the end of the echo train are more susceptible to dephasing. High-frequency data responsible for image detail are acquired at the beginning and at the end of the echo train, if conventional linear filling of the k-space is used. Therefore, more blurring (less image sharpness) is expected with longer ETLs because of progressive dephasing. At 3 T more signal is available but spins dephase more quickly. Although one might expect increased blurring at 3 T compared with 1.5 T MRI, this study showed, at similar ETLs, no qualitatively appreciable blurring at 1.5-T or 3 T with ETLs up to 16. Increasing the ETL above this number led to progressively worse image quality at both magnetic field strengths. Receiver bandwidth is the range of frequencies used to sample an MR signal. It is the rate at which the MR signal is converted from analog to digital by the digital converter. As receiver bandwidth is increased, the time needed to sample the echo is decreased. The adjustment is made by increasing the amplitude of the frequency-encoding gradient and keeping the field of view constant. A steeper frequency-encoding gradient increases the speed of rephasing. Thus the echo forms faster, the sampling time decreases, and the sampling rate increases. In this study, increasing the readout bandwidth decreased the quantitative susceptibility artifact. This effect occurred because increasing the readout bandwidth shortened the interval between echoes in the echo train and therefore less time was available for signal intensity to decline before refocusing occurred. In addition, increasing the readout bandwidth increases the number of frequencies sampled per pixel. Therefore, signal misregistration occurred in fewer pixels. A theoretical, although less marked, effect of increasing readout bandwidth and decreasing effective TE at 3 T is improvement in T2-weighted image contrast. This effect occurs because at higher field strengths, the T2 decay times of various tissues shorten [20 22]. Thus maintaining image contrast requires a decrease in TE. However, increasing readout bandwidth decreases SNR. This A effect occurs because for a given a voxel size and static field strength, the number of excited spins is defined and therefore so is the maximum amount of MR signal available for sampling. The readout of the MR signal can take more or less time, depending on the receiver bandwidth. A broad bandwidth corresponds to fast sampling of the MR signal and a high-intensity readout gradient. Background noise has a constant intensity at all frequencies (white noise). Therefore, the larger the receiver bandwidth, the more noise is sampled relative to the MR signal and the lower is the SNR. In this study, the optimal qualitative readout bandwidth at 1.5 T was 31.2 khz. At readout bandwidths greater than this value, images became progressively more grainy and noisy. At 3 T, it was possible to double the readout bandwidth to 62.5 khz while maintaining a qualitatively adequate SNR. The optimal image obtained at 3 T (ETL, 16; readout bandwidth, 62.5 khz) was qualitatively superior to that obtained at 1.5 T (ETL, 16; readout bandwidth, 31.2 khz). This somewhat counterintuitive finding can be explained because SNR is directly proportional to the main magnetic field strength and SNR is proportional to 1/readout bandwidth. Therefore at 3 T and double the readout bandwidth, in this case 62.5 khz, the SNR is approximately 40% ( 2) greater than at 1.5 T and 31.2 khz. Yet at 3 T and double the readout bandwidth, the susceptibility artifact is approximately the same as at 1.5 T Fig. 4 Pig leg with titanium plate prosthesis and two stainless steel nails in situ. A, MR image obtained at 1.5 T (TR/TE, 4,370/70; echo-train length, 16; readout bandwidth, 31.2 khz) and ranked 1. Thickness of signal void caused by titanium plate is similar to that in B. B, MR image obtained at 3 T (3,680/70; echo-train length, 16; readout bandwidth, 62.4 khz) and ranked 1. Imaging slice position is near identical to A. Susceptibility artifact includes signal void and lines of high signal intensity due to misregistration of protons. Thickness of signal void caused by titanium plate is similar to that in A. Although signal void owing to steel screw in superior aspect is more prominent, high-signal-intensity artifact is decreased. There is improved signal-to-noise ratio, and improved definition of soft tissues adjacent to orthopedic hardware. B AJR:194, January 2010 W63

5 Farrelly et al. because the amount of susceptibility (spatial misregistration and diffusion-related signal loss) approximates linear proportionality to the field strength [5, 23]. Therefore, the SNR increase due to the higher field strength dominates the signal loss due to the increased readout bandwidth. In our experience, imaging a prosthesis, once it has been cemented or surgically fixed with screws, is safe and does not cause movement at 1.5 T or 3 T. It must be stated, however, that the required safety testing should be performed for each piece of hardware at 3 T. The SAR safety limitations were not exceeded despite being set to the weight of the pig leg (8.5 kg). It is therefore likely that in a heavier human patient, the SAR limits also would not be exceeded. This study had limitations. Comparing 1.5- T and 3-T images entails comparing images obtained with different machines. Although both MRI units used in this study were made by the same manufacturer, it is possible that differences in image quality might have been due to differences in hardware design not related to the different field strengths. Second, susceptibility artifact on images is present in two dimensions (oval configuration in the frequency plane), but the measurements used to quantify susceptibility artifact in this study were in one plane only. Although the quantitative measurements used were in the direction of the tissues of interest, that is, into the periprosthetic tissues and not along the length of the bone, this limitation remains. Third, insofar as possible, the observers were blinded to whether the images were obtained with a 1.5-T or a 3-T unit. However, inherent qualitative differences in the acquired images might have allowed the observers to determine which images were obtained with the 1.5-T unit and which with the 3-T unit. This is a potential source of bias. Finally, because of slight differences in imaging planes, quantitative measurements were directly comparable between images obtained on the same MRI unit only. As such, qualitative scoring was used for comparing the highest-ranked image obtained at 1.5 T with the highestranked image obtained at 3 T. We conclude that although more artifact from metal prostheses is present on images obtained at higher field strengths, if all imaging parameters are kept the same, optimizing imaging parameters at 3 T by use of TSE and doubling the readout bandwidth will cause susceptibility artifact similar to that at 1.5-T MRI and improve qualitative measurements of soft-tissue visualization adjacent to orthopedic hardware. References 1. Birrell F, Johnell O, Silman A. Projecting the need for hip replacement over the next three decades: influence of changing demography and threshold for surgery. Ann Rheum Dis 1999; 58: Skutek M, Bourne RB, MacDonald SJ. International epidemiology of revision THR. Curr Orthop 2006; 20: Port JD, Pomper MG. Quantification and minimization of magnetic susceptibility artifacts on GRE images. J Comput Assist Tomogr 2000; 24: Tartaglino LM, Flanders AE, Vinitski S, Friedman DP. Metallic artifact on MR images of the postoperative spine: reduction with fast spin-echo techniques. Radiology 1994; 190: Petersilge CA, Lewin JS, Duerk JL, Yoo JU, Ghaneyem AJ. Optimizing imaging parameters for MR evaluation of the spine with titanium pedicle screws. AJR 1996; 166: White LM, Kim JK, Lee MJ, et al. Complications of total hip arthroplasty: MR imaging initial experience. Radiology 2000; 215: Johnston C, Kerr J, Ford S, O Byrne J, Eustace S. MRI as a problem-solving tool in unexplained failed total hip replacement following conventional assessment. Skeletal Radiol 2007; 36: Suh JS, Jeong EK, Shin KH, et al. Minimizing artifacts caused by metallic implants at MR imaging: experimental and clinical studies. AJR 1998; 171: Eustace S, Jara H, Goldberg R, et al. A comparison of conventional spin-echo and turbo spinecho imaging of soft tissues adjacent to orthopedic hardware. AJR 1998; 170: Eustace S, Shah B, Mason M. Imaging orthopedic hardware with an emphasis on hip prostheses. Orthop Clin North Am 1998; 29: Potter HG, Nestor BJ, Sofka CM, Ho ST, Peters LE, Salvati EA. Magnetic resonance imaging after total hip arthroplasty: evaluation of periprosthetic soft tissue. J Bone Joint Surg Am 2004; 86: Twair A, Ryan M, O Connell M, Powell T, O Byrne J, Eustace S. MRI of failed total hip replacement caused by abductor muscle avulsion. AJR 2003; 181: Naraghi AM, White LM. Magnetic resonance imaging of joint replacements. Semin Musculoskelet Radiol 2006;10: Törmänen J, Tervonen O, Koivula A, Junila J, Suramo I. Image technique optimization in MR imaging of a titanium alloy joint prosthesis. J Magn Reson Imaging 1996; 6: Eustace S, Goldberg R, Williamson D, et al. MR imaging of soft tissues adjacent to orthopaedic hardware: techniques to minimize susceptibility artifact. Clin Radiol 1997; 52: Olsen RV, Munk PL, Lee MJ, et al. Metal artifact reduction sequence: early clinical applications. RadioGraphics 2000; 20: Viano AM, Gronemeyer SA, Haliloglu M, Hoffer FA. Improved MR imaging for patients with metallic implants. Magn Reson Imaging 2000; 18: Buckwalter KA. Optimizing imaging techniques in the postoperative patient. Semin Musculoskelet Radiol 2007; 11: Lee MJ, Kim S, Lee SA, et al. Overcoming artifacts from metallic orthopedic implants at highfield strength MR imaging and multidetector CT. RadioGraphics 2007; 27: Bolog N, Nanz D, Weishaupt D. Muskuloskeletal MR imaging at 3.0 T: current status and future perspectives. Eur Radiol 2006; 16: Gold GE, Han E, Stainsby J, Wright G, Brittain J, Beaulieu C. Musculoskeletal MRI at 3.0 T: relaxation times and image contrast. AJR 2004; 183: Gold GE, Suh B, Sawyer-Glover A, Beaulieu C. Musculoskeletal MRI at 3.0 T: initial clinical experience. AJR 2004; 183: King KF. Signal acquisition and k-space sampling. In: Bernstein MA, ed. Handbook of MRI pulse sequences. Boston, MA: Academic Press, 2004: W64 AJR:194, January 2010

MRI Metal Artifact Reduction

MRI Metal Artifact Reduction MRI Metal Artifact Reduction PD Dr. med. Reto Sutter University Hospital Balgrist Zurich University of Zurich OUTLINE Is this Patient suitable for MR Imaging? Metal artifact reduction Is this Patient suitable

More information

Pulse Sequence Design and Image Procedures

Pulse Sequence Design and Image Procedures Pulse Sequence Design and Image Procedures 1 Gregory L. Wheeler, BSRT(R)(MR) MRI Consultant 2 A pulse sequence is a timing diagram designed with a series of RF pulses, gradients switching, and signal readout

More information

Pulse Sequence Design Made Easier

Pulse Sequence Design Made Easier Pulse Sequence Design Made Easier Gregory L. Wheeler, BSRT(R)(MR) MRI Consultant gurumri@gmail.com 1 2 Pulse Sequences generally have the following characteristics: An RF line characterizing RF Pulse applications

More information

Background (~EE369B)

Background (~EE369B) Background (~EE369B) Magnetic Resonance Imaging D. Nishimura Overview of NMR Hardware Image formation and k-space Excitation k-space Signals and contrast Signal-to-Noise Ratio (SNR) Pulse Sequences 13

More information

Advanced MSK MRI Protocols at 3.0T. Garry E. Gold, M.D. Associate Professor Department of Radiology Stanford University

Advanced MSK MRI Protocols at 3.0T. Garry E. Gold, M.D. Associate Professor Department of Radiology Stanford University Advanced MSK MRI Protocols at 3.0T Garry E. Gold, M.D. Associate Professor Department of Radiology Stanford University Outline Why High Field for MSK? SNR and Relaxation Times Technical Issues Example

More information

H 2 O and fat imaging

H 2 O and fat imaging H 2 O and fat imaging Xu Feng Outline Introduction benefit from the separation of water and fat imaging Chemical Shift definition of chemical shift origin of chemical shift equations of chemical shift

More information

(N)MR Imaging. Lab Course Script. FMP PhD Autumn School. Location: C81, MRI Lab B0.03 (basement) Instructor: Leif Schröder. Date: November 3rd, 2010

(N)MR Imaging. Lab Course Script. FMP PhD Autumn School. Location: C81, MRI Lab B0.03 (basement) Instructor: Leif Schröder. Date: November 3rd, 2010 (N)MR Imaging Lab Course Script FMP PhD Autumn School Location: C81, MRI Lab B0.03 (basement) Instructor: Leif Schröder Date: November 3rd, 2010 1 Purpose: Understanding the basic principles of MR imaging

More information

1 Introduction. 2 The basic principles of NMR

1 Introduction. 2 The basic principles of NMR 1 Introduction Since 1977 when the first clinical MRI scanner was patented nuclear magnetic resonance imaging is increasingly being used for medical diagnosis and in scientific research and application

More information

Module 2. Artefacts and Imaging Optimisation for single shot methods. Content: Introduction. Phase error. Phase bandwidth. Chemical shift review

Module 2. Artefacts and Imaging Optimisation for single shot methods. Content: Introduction. Phase error. Phase bandwidth. Chemical shift review MRES 7005 - Fast Imaging Techniques Module 2 Artefacts and Imaging Optimisation for single shot methods Content: Introduction Phase error Phase bandwidth Chemical shift review Chemical shift in pixels

More information

MR Basics: Module 8 Image Quality

MR Basics: Module 8 Image Quality Module 8 Transcript For educational and institutional use. This transcript is licensed for noncommercial, educational inhouse or online educational course use only in educational and corporate institutions.

More information

M R I Physics Course. Jerry Allison Ph.D., Chris Wright B.S., Tom Lavin B.S., Nathan Yanasak Ph.D. Department of Radiology Medical College of Georgia

M R I Physics Course. Jerry Allison Ph.D., Chris Wright B.S., Tom Lavin B.S., Nathan Yanasak Ph.D. Department of Radiology Medical College of Georgia M R I Physics Course Jerry Allison Ph.D., Chris Wright B.S., Tom Lavin B.S., Nathan Yanasak Ph.D. Department of Radiology Medical College of Georgia M R I Physics Course Magnetic Resonance Imaging Spatial

More information

HETERONUCLEAR IMAGING. Topics to be Discussed:

HETERONUCLEAR IMAGING. Topics to be Discussed: HETERONUCLEAR IMAGING BioE-594 Advanced MRI By:- Rajitha Mullapudi 04/06/2006 Topics to be Discussed: What is heteronuclear imaging. Comparing the hardware of MRI and heteronuclear imaging. Clinical applications

More information

MRI Summer Course Lab 2: Gradient Echo T1 & T2* Curves

MRI Summer Course Lab 2: Gradient Echo T1 & T2* Curves MRI Summer Course Lab 2: Gradient Echo T1 & T2* Curves Experiment 1 Goal: Examine the effect caused by changing flip angle on image contrast in a simple gradient echo sequence and derive T1-curves. Image

More information

Phantom based qualitative and quantitative evaluation of artifacts in MR images of metallic hip prostheses.

Phantom based qualitative and quantitative evaluation of artifacts in MR images of metallic hip prostheses. Phantom based qualitative and quantitative evaluation of artifacts in MR images of metallic hip prostheses. Månsson, Sven; Müller, Gunilla; Wellman, Fredrik; Nittka, Mathias; Lundin, Björn Published in:

More information

2014 M.S. Cohen all rights reserved

2014 M.S. Cohen all rights reserved 2014 M.S. Cohen all rights reserved mscohen@g.ucla.edu IMAGE QUALITY / ARTIFACTS SYRINGOMYELIA Source http://gait.aidi.udel.edu/res695/homepage/pd_ortho/educate/clincase/syrsco.htm Surgery is usually recommended

More information

Cerclage Passer. For minimally invasive application of cerclage cables.

Cerclage Passer. For minimally invasive application of cerclage cables. Cerclage Passer. For minimally invasive application of cerclage cables. Handling Technique Cable application This publication is not intended for distribution in the USA. Instruments and implants approved

More information

Image Quality/Artifacts Frequency (MHz)

Image Quality/Artifacts Frequency (MHz) The Larmor Relation 84 Image Quality/Artifacts (MHz) 42 ω = γ X B = 2πf 84 0.0 1.0 2.0 Magnetic Field (Tesla) 1 A 1D Image Magnetic Field Gradients Magnet Field Strength Field Strength / Gradient Coil

More information

Cardiac MR. Dr John Ridgway. Leeds Teaching Hospitals NHS Trust, UK

Cardiac MR. Dr John Ridgway. Leeds Teaching Hospitals NHS Trust, UK Cardiac MR Dr John Ridgway Leeds Teaching Hospitals NHS Trust, UK Cardiac MR Physics for clinicians: Part I Journal of Cardiovascular Magnetic Resonance 2010, 12:71 http://jcmr-online.com/content/12/1/71

More information

3T Unlimited. ipat on MAGNETOM Allegra The Importance of ipat at 3T. medical

3T Unlimited. ipat on MAGNETOM Allegra The Importance of ipat at 3T. medical 3T Unlimited ipat on MAGNETOM Allegra The Importance of ipat at 3T s medical ipat on MAGNETOM Allegra The Importance of ipat at 3T The rise of 3T MR imaging Ultra High Field MR (3T) has flourished during

More information

MR Advance Techniques. Flow Phenomena. Class II

MR Advance Techniques. Flow Phenomena. Class II MR Advance Techniques Flow Phenomena Class II Flow Phenomena In this class we will explore different phenomenona produced from nuclei that move during the acquisition of data. Flowing nuclei exhibit different

More information

MR Basics: Module 6 Pulse Sequences

MR Basics: Module 6 Pulse Sequences Module 6 Transcript For educational and institutional use. This transcript is licensed for noncommercial, educational inhouse or online educational course use only in educational and corporate institutions.

More information

ISSN X CODEN (USA): PCHHAX. The role of dual spin echo in increasing resolution in diffusion weighted imaging of brain

ISSN X CODEN (USA): PCHHAX. The role of dual spin echo in increasing resolution in diffusion weighted imaging of brain Available online at www.derpharmachemica.com ISSN 0975-413X CODEN (USA): PCHHAX Der Pharma Chemica, 2016, 8(17):15-20 (http://derpharmachemica.com/archive.html) The role of in increasing resolution in

More information

2015 Spin echoes and projection imaging

2015 Spin echoes and projection imaging 1. Spin Echoes 1.1 Find f0, transmit amplitudes, and shim settings In order to acquire spin echoes, we first need to find the appropriate scanner settings using the FID GUI. This was all done last week,

More information

Pulse Sequences: Rapid Gradient Echo

Pulse Sequences: Rapid Gradient Echo Pulse Sequences: Rapid Gradient Echo M229 Advanced Topics in MRI Holden H. Wu, Ph.D. 2018.04.17 Department of Radiological Sciences David Geffen School of Medicine at UCLA Class Business Office hours -

More information

Magnetic Resonance Imaging Principles, Methods, and Techniques

Magnetic Resonance Imaging Principles, Methods, and Techniques Magnetic Resonance Imaging Principles, Methods, and Techniques Perry Sprawls Jr., Emory University Publisher: Medical Physics Publishing Corporation Publication Place: Madison, Wisconsin Publication Date:

More information

MR in RTP. MR Data for Treatment Planning: Spatial Accuracy Issues, Protocol Optimization, and Applications (Preview of TG117 Report) Acknowledgements

MR in RTP. MR Data for Treatment Planning: Spatial Accuracy Issues, Protocol Optimization, and Applications (Preview of TG117 Report) Acknowledgements MR Data for Treatment Planning: Issues, Protocol Optimization, and s (Preview of TG117 Report) Debra H. Brinkmann Mayo Clinic, Rochester MN Acknowledgements TG-117 Use of MRI Data in Treatment Planning

More information

High Field MRI: Technology, Applications, Safety, and Limitations

High Field MRI: Technology, Applications, Safety, and Limitations High Field MRI: Technology, Applications, Safety, and Limitations R. Jason Stafford, Ph.D. The University of Texas M. D. Anderson Cancer Center, Houston, TX Introduction The amount of available signal

More information

Magnetic Resonance Imaging

Magnetic Resonance Imaging Magnetic Resonance Imaging Principles, Methods, and Techniques Perry Sprawls, Ph.D., FACR, FAAPM, FIOMP Distinguished Emeritus Professor Department of Radiology Emory University Atlanta, Georgia Medical

More information

Simultaneous Multi-Slice (Slice Accelerated) Diffusion EPI

Simultaneous Multi-Slice (Slice Accelerated) Diffusion EPI Simultaneous Multi-Slice (Slice Accelerated) Diffusion EPI Val M. Runge, MD Institute for Diagnostic and Interventional Radiology Clinics for Neuroradiology and Nuclear Medicine University Hospital Zurich

More information

Downloaded from by on 02/07/18 from IP address Copyright ARRS. For personal use only; all rights reserved

Downloaded from  by on 02/07/18 from IP address Copyright ARRS. For personal use only; all rights reserved Downloaded from www.ajronline.org by 46.3.192.5 on 02/07/18 from IP address 46.3.192.5. Copyright RRS. For personal use only; all rights reserved C oil sensitivity encoding (SENSE) is a new technique that

More information

BOLD fmri: signal source, data acquisition, and interpretation

BOLD fmri: signal source, data acquisition, and interpretation BOLD fmri: signal source, data acquisition, and interpretation Cheryl Olman 4 th year student, Department of Neuroscience and Center for Magnetic Resonance Research Discussion series Week 1: Biological

More information

Metal-Induced Artifacts in MRI

Metal-Induced Artifacts in MRI Musculoskeletal Imaging Review Hargreaves et al. Metal-Induced rtifacts in MRI Musculoskeletal Imaging Review Downloaded from www.ajronline.org by 46.3.206.43 on 03/02/18 from IP address 46.3.206.43. opyright

More information

Works-in-Progress package Version 1.0. For the SIEMENS Magnetom. Installation and User s Guide NUMARIS/4VA21B. January 22, 2003

Works-in-Progress package Version 1.0. For the SIEMENS Magnetom. Installation and User s Guide NUMARIS/4VA21B. January 22, 2003 Works-in-Progress package Version 1.0 For the Installation and User s Guide NUMARIS/4VA21B January 22, 2003 Section of Medical Physics, University Hospital Freiburg, Germany Contact: Klaus Scheffler PhD,

More information

Experience in implementing continuous arterial spin labeling on a commercial MR scanner

Experience in implementing continuous arterial spin labeling on a commercial MR scanner JOURNAL OF APPLIED CLINICAL MEDICAL PHYSICS, VOLUME 6, NUMBER 1, WINTER 2005 Experience in implementing continuous arterial spin labeling on a commercial MR scanner Theodore R. Steger and Edward F. Jackson

More information

Gradient Spoiling. Average balanced SSFP magnetization Reduce sensitivity to off-resonance. FFE, FISP, GRASS, GRE, FAST, Field Echo

Gradient Spoiling. Average balanced SSFP magnetization Reduce sensitivity to off-resonance. FFE, FISP, GRASS, GRE, FAST, Field Echo Gradient Spoiling Average balanced SSFP magnetization Reduce sensitivity to off-resonance FFE, FISP, GRASS, GRE, FAST, Field Echo 1 Gradient-Spoiled Sequence (GRE, FFE, FISP, GRASS) RF TR G z G y G x Signal

More information

Passive Tracking Exploiting Local Signal Conservation: The White Marker Phenomenon

Passive Tracking Exploiting Local Signal Conservation: The White Marker Phenomenon Passive Tracking Exploiting Local Signal Conservation: The White Marker Phenomenon Jan-Henry Seppenwoolde,* Max A. Viergever, and Chris J.G. Bakker Magnetic Resonance in Medicine 50:784 790 (2003) This

More information

MRI: From Signal to Image

MRI: From Signal to Image MRI: From Signal to Image Johannes Koch physics654 2013-05-06 1 / 27 Tomography Magnetic Resonance Tomography Tomography: tomos: section graphein: to write Signal measured as function of space 2 / 27 Tomography

More information

HCS 1.5. The countersinkable compression screw.

HCS 1.5. The countersinkable compression screw. HCS 1.5. The countersinkable compression screw. Surgical Technique This publication is not intended for distribution in the USA. Instruments and implants approved by the AO Foundation. Table of Contents

More information

RAD 229: MRI Signals and Sequences

RAD 229: MRI Signals and Sequences RAD 229: MRI Signals and Sequences Brian Hargreaves All notes are on the course website web.stanford.edu/class/rad229 Course Goals Develop Intuition Understand MRI signals Exposure to numerous MRI sequences

More information

MRI Anatomy and Positioning Series Module 12: Fat Suppression Techniques

MRI Anatomy and Positioning Series Module 12: Fat Suppression Techniques MRI Anatomy and Positioning Series Module 12: Fat Suppression Techniques 1 Introduction... 3 RF FatSat... 4 HOAST... 4 FatSat... 5 Segment FS... 8 PhaseCycle... 9 Water Excitation... 10 STIR... 12 FatSep...

More information

Principles of MRI EE225E / BIO265. Lecture 21. Instructor: Miki Lustig UC Berkeley, EECS. M. Lustig, EECS UC Berkeley

Principles of MRI EE225E / BIO265. Lecture 21. Instructor: Miki Lustig UC Berkeley, EECS. M. Lustig, EECS UC Berkeley Principles of MRI Lecture 21 EE225E / BIO265 Instructor: Miki Lustig UC Berkeley, EECS Question What is the difference between the images? Answer Both T1-weighted spin-echo gradient-echo Lower SNR Meniscus

More information

Spiral MRI on a 9.4T Vertical-bore Superconducting Magnet Using Unshielded and Self-shielded Gradient Coils

Spiral MRI on a 9.4T Vertical-bore Superconducting Magnet Using Unshielded and Self-shielded Gradient Coils Magn Reson Med Sci doi:10.2463/mrms.tn.2016-0049 Published Online: March 27, 2017 TECHNICAL NOTE Spiral MRI on a 9.4T Vertical-bore Superconducting Magnet Using Unshielded and Self-shielded Gradient Coils

More information

MR in Tx Planning. Acknowledgements. Outline. Overview MR in RTP

MR in Tx Planning. Acknowledgements. Outline. Overview MR in RTP MR Data for Treatment Planning and Stereotactic Procedures: Sources of Distortion, Protocol Optimization, and Assessment (Preview of TG117 Report) Debra H. Brinkmann Mayo Clinic, Rochester MN Acknowledgements

More information

10. Phase Cycling and Pulsed Field Gradients Introduction to Phase Cycling - Quadrature images

10. Phase Cycling and Pulsed Field Gradients Introduction to Phase Cycling - Quadrature images 10. Phase Cycling and Pulsed Field Gradients 10.1 Introduction to Phase Cycling - Quadrature images The selection of coherence transfer pathways (CTP) by phase cycling or PFGs is the tool that allows the

More information

Medical Imaging. X-rays, CT/CAT scans, Ultrasound, Magnetic Resonance Imaging

Medical Imaging. X-rays, CT/CAT scans, Ultrasound, Magnetic Resonance Imaging Medical Imaging X-rays, CT/CAT scans, Ultrasound, Magnetic Resonance Imaging From: Physics for the IB Diploma Coursebook 6th Edition by Tsokos, Hoeben and Headlee And Higher Level Physics 2 nd Edition

More information

System/Imaging Imperfections

System/Imaging Imperfections System/Imaging Imperfections B0 variations: Shim, Susceptibility B1 variations: Transmit, Receive Gradient Imperfections: Non-linearities Delays and Eddy currents Concomitant terms 1 B0 Variations - Off-Resonance

More information

TimTX TrueShape. The parallel transmit architecture of the future. Answers for life.

TimTX TrueShape.  The parallel transmit architecture of the future. Answers for life. www.siemens.com/trueshape TimTX TrueShape The parallel transmit architecture of the future. The product/feature (mentioned herein) is not commercially available. Due to regulatory reasons its future availability

More information

Lab 8 6.S02 Spring 2013 MRI Projection Imaging

Lab 8 6.S02 Spring 2013 MRI Projection Imaging 1. Spin Echos 1.1 Find f0, TX amplitudes, and shim settings In order to acquire spin echos, we first need to find the appropriate scanner settings using the FID GUI. This was all done last week, but these

More information

Automatic Selection of Mask and Arterial Phase Images for Temporally-Resolved MR Digital Subtraction Angiography

Automatic Selection of Mask and Arterial Phase Images for Temporally-Resolved MR Digital Subtraction Angiography Automatic Selection of Mask and Arterial Phase Images for Temporally-Resolved MR Digital Subtraction Angiography 21 May 2002, ISMRM 2002 Junhwan Kim, Martin R. Prince, Ramin Zabih,, Jeff Bezanson, Richard

More information

functional MRI: A primer

functional MRI: A primer Activation Leads to: functional MRI: A primer CBF Increased +ΔR CBV Increased +ΔR (C+) O Utilization Increased slightly? Venous [O ] Increased -ΔR* Glucose Utilization Increased? Lactate BOLD R=/T R=/T

More information

Noninvasive Blood Flow Mapping with Arterial Spin Labeling (ASL) Paul Kyu Han and Sung-Hong Park

Noninvasive Blood Flow Mapping with Arterial Spin Labeling (ASL) Paul Kyu Han and Sung-Hong Park Noninvasive Blood Flow Mapping with Arterial Spin Labeling (ASL) Paul Kyu Han and Sung-Hong Park Department of Bio and Brain Engineering, Korea Advanced Institute of Science and Technology (KAIST), Daejeon,

More information

MARP. MR Accreditation Program Quality Control Beyond Just the Scans and Measurements July 2005

MARP. MR Accreditation Program Quality Control Beyond Just the Scans and Measurements July 2005 ACR MRI accreditation program MR Accreditation Program Quality Control Beyond Just the Scans and Measurements July 2005 Carl R. Keener, Ph.D., DABMP, DABR keener@marpinc.com MARP Medical & Radiation Physics,

More information

Liver imaging beyond expectations with Ingenia

Liver imaging beyond expectations with Ingenia Publication for the Philips MRI Community Issue 47 2012/3 Liver imaging beyond expectations with Ingenia Contributed by John Penatzer, RT, MR clinical product specialist, Cleveland, OH, USA Publication

More information

MRI at a Glance. Catherine Westbrook. Blackwell Science

MRI at a Glance. Catherine Westbrook. Blackwell Science MRI at a Glance Catherine Westbrook Blackwell Science MRI at a Glance MRI at a Glance CATHERINE WESTBROOK MSC DCRR CTC Director of Training and Education Lodestone Patient Care Ltd Blackwell Science 2002

More information

PET/CT Instrumentation Basics

PET/CT Instrumentation Basics / Instrumentation Basics 1. Motivations for / imaging 2. What is a / Scanner 3. Typical Protocols 4. Attenuation Correction 5. Problems and Challenges with / 6. Examples Motivations for / Imaging Desire

More information

Numerical Evaluation of an 8-element Phased Array Torso Coil for Magnetic Resonance Imaging

Numerical Evaluation of an 8-element Phased Array Torso Coil for Magnetic Resonance Imaging Numerical Evaluation of an 8-element Phased Array Torso Coil for Magnetic Resonance Imaging Feng Liu, Joe Li, Ian Gregg, Nick Shuley and Stuart Crozier School of Information Technology and Electrical Engineering,

More information

Application Guide & Release Notes

Application Guide & Release Notes Application Guide & Release Notes Inner-volume-imaging (IVI) EPI C2P Release 002a 1 September 2015 TMII Translational and Molecular Imaging Institute Conditions of Use This package is provided to support

More information

12/21/2016. Siemens Medical Systems Research Agreement Philips Healthcare Research Agreement AAN and ASN Committees

12/21/2016. Siemens Medical Systems Research Agreement Philips Healthcare Research Agreement AAN and ASN Committees Joseph V. Fritz, PhD Nandor Pintor, MD Dent Neurologic Institute ASN 2017 Friday, January 20, 2017 Siemens Medical Systems Research Agreement Philips Healthcare Research Agreement AAN and ASN Committees

More information

LCP Pilon Plate 2.7/3.5

LCP Pilon Plate 2.7/3.5 LCP Pilon Plate 2.7/3.5 Surgical Technique This publication is not intended for distribution in the USA. Instruments and implants approved by the AO Foundation. Table of contents Indications 2 Implants

More information

DURING the past 15 years the use of digitized

DURING the past 15 years the use of digitized DIGITAL IMAGING BASICS Properties of Digital Images in Radiology DURING the past 15 years the use of digitized images in radiology has proliferated. It is reasonable to expect that within a few years virtually

More information

EE225E/BIOE265 Spring 2011 Principles of MRI. Assignment 6 Solutions. (y 0 + vt) dt. 2 y 0T + 3 )

EE225E/BIOE265 Spring 2011 Principles of MRI. Assignment 6 Solutions. (y 0 + vt) dt. 2 y 0T + 3 ) EE225E/BIOE265 Spring 211 Principles of MRI Miki Lustig Handout Assignment 6 Solutions 1. Nishimura 6.7 (Thanks Galen!) a) After the 9 y pulse, the spin is in the ˆx direction (using left-handed rotations).

More information

SmartExam helps to banish most repeat knee studies at Desert Medical Imaging

SmartExam helps to banish most repeat knee studies at Desert Medical Imaging I s s u e 3 2 - J u l y 2 0 0 7 F i e l d Strength Publication for the Philips MRI Community SmartExam helps to banish most repeat knee studies at Desert Medical Imaging Total scan automation boosts efficiency,

More information

The SENSE Ghost: Field-of-View Restrictions for SENSE Imaging

The SENSE Ghost: Field-of-View Restrictions for SENSE Imaging JOURNAL OF MAGNETIC RESONANCE IMAGING 20:1046 1051 (2004) Technical Note The SENSE Ghost: Field-of-View Restrictions for SENSE Imaging James W. Goldfarb, PhD* Purpose: To describe a known (but undocumented)

More information

The development of the RF-pulse for the low level SAR used by the MRI.

The development of the RF-pulse for the low level SAR used by the MRI. The development of the RF-pulse for the low level SAR used by the MRI. Kojiro Yamaguchi a*, Eizo Umezawa a, Sachiko Ueoku b, Kazuhiro Katada c a Faculty of radiological technology, School of Health Science,

More information

MRI imaging in neuroscience Dr. Thom Oostendorp Lab class: 2 hrs

MRI imaging in neuroscience Dr. Thom Oostendorp Lab class: 2 hrs MRI imaging in neuroscience Dr. Thom Oostendorp Lab class: 2 hrs 1 Introduction In tomographic imaging techniques, such as MRI, a certain tissue property within a slice is imaged. For each voxel (volume

More information

Introduction. Sam R. Kottamasu Lawrence R. Kuhns

Introduction. Sam R. Kottamasu Lawrence R. Kuhns Pediatr Radiol (1997) 27: 119 123 Springer-Verlag 1997 Sam R. Kottamasu Lawrence R. Kuhns Musculoskeletal computed radiography in children: scatter reduction and improvement in bony trabecular sharpness

More information

Radio Frequency Field

Radio Frequency Field Radio Frequency Field Radio Frequency Coils and RF Power Distribution RF Coil Maps Distribution of RF Power GE 750W RF maps courtesy of Tobias Gilk Siemens Prisma (courtesy Siemens) Radio Frequency Field

More information

MAGNETIC RESONANCE IMAGING

MAGNETIC RESONANCE IMAGING CSEE 4620 Homework 3 Fall 2018 MAGNETIC RESONANCE IMAGING 1. THE PRIMARY MAGNET Magnetic resonance imaging requires a very strong static magnetic field to align the nuclei. Modern MRI scanners require

More information

Human Subjects in fmri Research

Human Subjects in fmri Research HST.583: Functional Magnetic Resonance Imaging: Data Acquisition and Analysis Harvard-MIT Division of Health Sciences and Technology Course Instructor: Dr. Randy Gollub. Human Subjects in fmri Research

More information

Multi-channel SQUID-based Ultra-Low Field Magnetic Resonance Imaging in Unshielded Environment

Multi-channel SQUID-based Ultra-Low Field Magnetic Resonance Imaging in Unshielded Environment Multi-channel SQUID-based Ultra-Low Field Magnetic Resonance Imaging in Unshielded Environment Andrei Matlashov, Per Magnelind, Shaun Newman, Henrik Sandin, Algis Urbaitis, Petr Volegov, Michelle Espy

More information

Silicone-Specific Imaging Using an Inversion- Recovery-Prepared Fast Three-Point Dixon Technique

Silicone-Specific Imaging Using an Inversion- Recovery-Prepared Fast Three-Point Dixon Technique JOURNAL OF MAGNETIC RESONANCE IMAGING 19:298 302 (2004) Original Research Silicone-Specific Imaging Using an Inversion- Recovery-Prepared Fast Three-Point Dixon Technique Jingfei Ma, PhD, 1 * Haesun Choi,

More information

Field Simulation Software to Improve Magnetic Resonance Imaging

Field Simulation Software to Improve Magnetic Resonance Imaging Field Simulation Software to Improve Magnetic Resonance Imaging a joint project with the NRI in South Korea CST Usergroup Meeting 2010 Darmstadt Institute for Biometry and Medicine Informatics J. Mallow,

More information

Steady-state sequences: Spoiled and balanced methods

Steady-state sequences: Spoiled and balanced methods Steady-state sequences: Spoiled and balanced methods Karla L Miller, FMRIB Centre, University of Oxford What is steady-state imaging? In the context of MRI pulse sequences, the term steady state typically

More information

Diffusion and Functional MRI of the Spinal Cord Methods and Clinical Applications

Diffusion and Functional MRI of the Spinal Cord Methods and Clinical Applications Diffusion and Functional MRI of the Spinal Cord Methods and Clinical Applications Susceptibility artifacts in DTI of the spinal cord J. Cohen-Adad Q-space imaging and axon diameter measurements Functional

More information

A Progressive Gradient Moment Nulling Design Technique

A Progressive Gradient Moment Nulling Design Technique MAGNETIC RESONANCE IN MEDICINE 19, 175-179 (1991) A Progressive Gradient Moment Nulling Design Technique JAMES G. PIPE AND THOMAS L. CHENEVERT niversity of Michigan Medical Center, 1500 East Medical Center

More information

Chapter 2. The Physics of Magnetic Resonance Imaging

Chapter 2. The Physics of Magnetic Resonance Imaging Chapter 2. The Physics of Magnetic Resonance Imaging 2.1. Introduction The origins of the Nuclear Magnetic Resonance (NMR) signal and how it is manipulated to form images are the subjects of this chapter.

More information

Half-Pulse Excitation Pulse Design and the Artifact Evaluation

Half-Pulse Excitation Pulse Design and the Artifact Evaluation Half-Pulse Excitation Pulse Design and the Artifact Evaluation Phillip Cho. INRODUCION A conventional excitation scheme consists of a slice-selective RF excitation followed by a gradient-refocusing interval

More information

IR/SR TrueFISP. Works-in-Progress package Version 1.2. For the SIEMENS Magnetom. Installation and User s Guide NUMARIS/4VA21B.

IR/SR TrueFISP. Works-in-Progress package Version 1.2. For the SIEMENS Magnetom. Installation and User s Guide NUMARIS/4VA21B. Works-in-Progress package Version 1.2 For the Installation and User s Guide NUMARIS/4VA21B January 22, 2003 Section of Medical Physics, University Hospital Freiburg, Germany Contact: Klaus Scheffler PhD

More information

SIGNA Explorer Lift revives our MR

SIGNA Explorer Lift revives our MR Seiji Shiotani, MD, PhD Seirei Fuji Hospital in Fuji City, Shizuoka, Japan Masayoshi Sugimura Seirei Fuji Hospital in Fuji City, Shizuoka, Japan SIGN Explorer Lift revives our MR The clinical usefulness

More information

Variable Angle LCP Mesh Plate 2.4/2.7. Part of the Variable Angle LCP Forefoot/Midfoot System 2.4/2.7.

Variable Angle LCP Mesh Plate 2.4/2.7. Part of the Variable Angle LCP Forefoot/Midfoot System 2.4/2.7. Variable Angle LCP Mesh Plate 2.4/2.7. Part of the Variable Angle LCP Forefoot/Midfoot System 2.4/2.7. Surgical Technique This publication is not intended for distribution in the USA. Instruments and implants

More information

High-Resolution Ultrashort Echo Time (UTE) Imaging on Human Knee With AWSOS Sequence at 3.0 T

High-Resolution Ultrashort Echo Time (UTE) Imaging on Human Knee With AWSOS Sequence at 3.0 T CME JOURNAL OF MAGNETIC RESONANCE IMAGING 35:204 210 (2012) Technical Note High-Resolution Ultrashort Echo Time (UTE) Imaging on Human Knee With AWSOS Sequence at 3.0 T Yongxian Qian, PhD, 1 * Ashley A.

More information

Digital Imaging CT & MR

Digital Imaging CT & MR Digital Imaging CT & MR January 22, 2008 Digital Radiography, CT and MRI generate images in a digital format What is a Digital Image? A digital image is made up of picture elements, pixels row by column

More information

SIGNA Pioneer: Ultra High Efficiency Gradient System Advancing the gradient technology curve

SIGNA Pioneer: Ultra High Efficiency Gradient System Advancing the gradient technology curve GE Healthcare SIGNA Pioneer: Ultra High Efficiency Gradient System Advancing the gradient technology curve NEW TECHNOLOGY 40W Watts spec is irrelevant. 4W LED bulb delivers same brightness as 40W incandescent

More information

EE469B: Assignment 1 Solutions

EE469B: Assignment 1 Solutions EE469B Fall 26-7 RF Pulse Design for MRI EE469B: Assignment Solutions Due Thursday Oct 6 Introduction This assignment concerns typical Fourier transform designs of excitation pulses. This includes designing

More information

Magnetic Resonance Imaging and Radio Frequency. Part 1. Produced on behalf of Mid Sussex Amateur Radio Society by M5BTB

Magnetic Resonance Imaging and Radio Frequency. Part 1. Produced on behalf of Mid Sussex Amateur Radio Society by M5BTB Magnetic Resonance Imaging and Radio Frequency Part 1 Produced on behalf of Mid Sussex Amateur Radio Society by M5BTB Why Now? During 2011 my physical health was deteriorating, and a brain tumour was diagnosed

More information

While digital techniques have the potential to reduce patient doses, they also have the potential to significantly increase them.

While digital techniques have the potential to reduce patient doses, they also have the potential to significantly increase them. In press 2004 1 2 Guest Editorial (F. Mettler, H. Ringertz and E. Vano) Guest Editorial (F. Mettler, H. Ringertz and E. Vano) Digital radiology An appropriate analogy that is easy for most people to understand

More information

EE225E/BIOE265 Spring 2012 Principles of MRI. Assignment 7. Due March 16, 2012

EE225E/BIOE265 Spring 2012 Principles of MRI. Assignment 7. Due March 16, 2012 EE225E/BIOE265 Spring 2012 Principles of MRI Miki Lustig Assignment 7 Due March 16, 2012 1. From Midterm I 2010: You ve just programmed up your first 2DFT pulse sequence, and are trying it out on the scanner.

More information

Optimized CT metal artifact reduction using the Metal Deletion Technique (MDT)

Optimized CT metal artifact reduction using the Metal Deletion Technique (MDT) Optimized CT metal artifact reduction using the Metal Deletion Technique (MDT) F Edward Boas, Roland Bammer, and Dominik Fleischmann Extended abstract for RSNA 2012 Purpose CT metal streak artifacts are

More information

Image quality evaluation of turbo-spin echo diffusion weighted image (TSE-DWI) : A phantom study

Image quality evaluation of turbo-spin echo diffusion weighted image (TSE-DWI) : A phantom study Image quality evaluation of turbo-spin echo diffusion weighted image (TSE-DWI) : A phantom study Poster No.: C-0631 Congress: ECR 2016 Type: Scientific Exhibit Authors: T. Yoshida, A. Urikura, K. Shirata,

More information

MRI with the VNS Therapy System October 2017

MRI with the VNS Therapy System October 2017 MRI with the VNS Therapy System October 2017 The information contained in this document is one part of the full labeling for the implanted portions of the VNS Therapy System. It is not intended to serve

More information

Enhancing Gray-to-White Matter Contrast in 3T T1 Spin-Echo Brain Scans by Optimizing Flip Angle

Enhancing Gray-to-White Matter Contrast in 3T T1 Spin-Echo Brain Scans by Optimizing Flip Angle AJNR Am J Neuroradiol 26:2000 2004, September 2005 Enhancing Gray-to-White Matter Contrast in 3T T1 Spin-Echo Brain Scans by Optimizing Flip Angle Bernd L. Schmitz, Georg Grön, Florian Brausewetter, Martin

More information

Echo-Planar Imaging for a 9.4 Tesla Vertical-Bore Superconducting Magnet Using an Unshielded Gradient Coil

Echo-Planar Imaging for a 9.4 Tesla Vertical-Bore Superconducting Magnet Using an Unshielded Gradient Coil Magn Reson Med Sci, Vol. XX, No. X, pp. XXX XXX, 2015 2016 Japanese Society for Magnetic Resonance in Medicine TECHNICAL NOTE by J-STAGE doi:10.2463/mrms.tn.2015-0123 Echo-Planar Imaging for a 9.4 Tesla

More information

SECTION I - CHAPTER 2 DIGITAL IMAGING PROCESSING CONCEPTS

SECTION I - CHAPTER 2 DIGITAL IMAGING PROCESSING CONCEPTS RADT 3463 - COMPUTERIZED IMAGING Section I: Chapter 2 RADT 3463 Computerized Imaging 1 SECTION I - CHAPTER 2 DIGITAL IMAGING PROCESSING CONCEPTS RADT 3463 COMPUTERIZED IMAGING Section I: Chapter 2 RADT

More information

MRI MRI REGISTRY REVIEW PHYSICAL PRINCIPLES OF IMAGE FORMATION ARTIFACTS SUPERCONDUCTIVE MAGNET ANAIBI MOLINA(R) (RT) (MR) (CT) T2 DEPHASING

MRI MRI REGISTRY REVIEW PHYSICAL PRINCIPLES OF IMAGE FORMATION ARTIFACTS SUPERCONDUCTIVE MAGNET ANAIBI MOLINA(R) (RT) (MR) (CT) T2 DEPHASING MRI ANAIBI MOLINA(R) (RT) (MR) (CT) T2 DEPHASING SUPERCONDUCTIVE MAGNET FREE INDUCTION DECAY ARTIFACTS MRI REGISTRY REVIEW PHYSICAL PRINCIPLES OF IMAGE FORMATION Mri Registry Review Physical Principles

More information

Potential Risks of MRI in Device Patients

Potential Risks of MRI in Device Patients Outline Potential Risks of MRI in Device Patients Redha Boubertakh r.boubertakh@qmul.ac.uk MRI and cardiac implantable electronic devices (CIED) Components of an MRI scanner MRI implant and device safety

More information

25 CP Generalize Concepts in Abstract Multi-dimensional Image Model Component Semantics Page 1

25 CP Generalize Concepts in Abstract Multi-dimensional Image Model Component Semantics Page 1 25 CP-1390 - Generalize Concepts in Abstract Multi-dimensional Image Model Component Semantics Page 1 1 STATUS Letter Ballot 2 Date of Last Update 2014/09/08 3 Person Assigned David Clunie 4 mailto:dclunie@dclunie.com

More information

NEMA Standards Publication MS (R2014) Determination of Signal-to-Noise Ratio (SNR) in Diagnostic Magnetic Resonance Imaging

NEMA Standards Publication MS (R2014) Determination of Signal-to-Noise Ratio (SNR) in Diagnostic Magnetic Resonance Imaging NEMA Standards Publication MS 1-2008 (R2014) Determination of Signal-to-Noise Ratio (SNR) in Diagnostic Magnetic Resonance Imaging Published by: National Electrical Manufacturers Association 1300 North

More information

Inherent Insensitivity to RF Inhomogeneity in FLASH Imaging

Inherent Insensitivity to RF Inhomogeneity in FLASH Imaging Inherent Insensitivity to RF Inhomogeneity in FLASH Imaging Danli Wang, Keith Heberlein, Stephen LaConte, and Xiaoping Hu* Magnetic Resonance in Medicine 52:927 931 (2004) Radiofrequency (RF) field inhomogeneity

More information

PHY3902 PHY3904. Nuclear magnetic resonance Laboratory Protocol

PHY3902 PHY3904. Nuclear magnetic resonance Laboratory Protocol PHY3902 PHY3904 Nuclear magnetic resonance Laboratory Protocol PHY3902 PHY3904 Nuclear magnetic resonance Laboratory Protocol GETTING STARTED You might be tempted now to put a sample in the probe and try

More information

Challenges of Field Inhomogeneities and a Method for Compensation. Angela Lynn Styczynski Snyder. Michael Garwood, Ph.D., Adviser

Challenges of Field Inhomogeneities and a Method for Compensation. Angela Lynn Styczynski Snyder. Michael Garwood, Ph.D., Adviser Challenges of Field Inhomogeneities and a Method for Compensation A DISSERTATION SUBMITTED TO THE FACULTY OF THE GRADUATE SCHOOL OF THE UNIVERSITY OF MINNESOTA BY Angela Lynn Styczynski Snyder IN PARTIAL

More information