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and a relaxed fixed point iteration scheme is introduced to alter the coil windings iteratively and lower the hot spot temperature. The<br />

new coil windings display a considerable improvement in hot spot temperature, at no cost to coil performance, when compared to<br />

equivalent minimum power x-gradient coils. The model can be adapted easily for other geometries, thermal properties, cooling<br />

mechanisms and non-linear constraints.<br />

14:00 3945. A Temperature Distribution Model for Gradient Coils<br />

Peter T. While 1 , Larry K. Forbes 1 , Stuart Crozier 2<br />

1 School of Maths and Physics, University of Tasmania, Hobart, TAS, Australia; 2 School of Information<br />

Technology and Electrical Engineering, University of Queensland, Brisbane, QLD, Australia<br />

Excessive heating of gradient coils is a considerable concern. An analytic model is presented for calculating theoretically the spatial<br />

temperature distribution for cylindrical gradient coils. The model includes Ohmic heating due to current density in resistive material,<br />

thermal conduction through a copper layer and an epoxy former, and radial heat loss to the environment. A great number of coil<br />

parameters can be varied, including geometry, electrical and thermal properties, and results are shown for a standard x-gradient coil<br />

under three different types of cooling. In addition, temperature rise-times are predicted using a time-dependent solution for hot spot<br />

temperature.<br />

14:30 3946. Safety Considerations for a PatLoc Gradient Insert Coil for Human Head Imaging<br />

Chris A. Cocosco 1 , Andrew J. Dewdney 2 , P Dietz 2 , M Semmler 2 , Anna M. Welz 1 , Daniel<br />

Gallichan 1 , Hans Weber 1 , Gerrit Schultz 1 , Juergen Hennig 1 , Maxim Zaitsev 1<br />

1 Dept of Diagnostic Radiology, Medical Physics, University Hospital Freiburg, Freiburg, B.W., Germany;<br />

2 Siemens Healthcare, Erlangen, Germany<br />

We present the design considerations and evaluation measurements for the safety of a PatLoc (Parallel Acquisition Technique using<br />

Localized Gradients) gradient insert coil designed for human head imaging on a 3T MRI system. This novel concept has the potential<br />

to allow higher gradient switching rates while not exceeding the Peripheral Nerve Stimulation (PNS) limits. Based on the presented<br />

experimental measurements and simulations, we consider imaging human volunteers with this system to be safe.<br />

15:00 3947. First Results for Diffusion-Weighted Imaging with a 4th Channel Gradient Insert<br />

Rebecca E. Feldman 1 , Jamu Alford 2 , Timothy Scholl 2 , Blaine A. Chronik 2<br />

1 Medical Biophysics, University of Western Ontario, London, Ontario, Canada; 2 Physics and Astronomy,<br />

University of Western Ontario, London, Ontario, Canada<br />

Gradients in diffusion-weighted imaging play two distinct roles. A gradient with a linear range sufficient to cover the sample is<br />

required for imaging. For the diffusion-weighting, the gradient is only required to be strong. A fourth gradient was inserted into the<br />

bore for the purposes of diffusion-weighting only. The inserted gradient was pulsed twice, before and after the 180 degree RF pulse,<br />

and the image acquisition was done using the whole body gradients. Using the insert b-values greater than 1000 s/mm2 were obtained<br />

a time frame that would permit only a b-value of 100 using the whole-body gradients.<br />

Hybrid Systems: MR+<br />

Hall B Monday 14:00-16:00 Computer 53<br />

14:00 3948. A Depth-Encoding Detector Module for an MR-Compatible PET Insert<br />

Yibao Wu 1 , Yongfeng Yang 1 , Bo J. Peng 1 , Simon R. Cherry 1<br />

1 Department of Biomedical Engineering, University of California, Davis, Davis, CA, United States<br />

The next generation of MR-compatible PET insert is under development for small-animal imaging providing greater than an order of<br />

magnitude increase in sensitivity by utilizing 20 mm thick scintillator crystal elements with excellent stopping power. A detector<br />

module based on avalanche photodiode read out with depth-of-interaction encoding was designed and evaluated to overcome the<br />

resolution-degrading parallax errors associated with such thick detectors. Detectors for the new PET insert were characterized in terms<br />

of crystal identification and energy spectra. Data were acquired outside a 7T MR scanner, inside the MR scanner, with and without<br />

sequences running. An MR phantom also was measured with the PET detector module inside the MR system. No significant<br />

interference between the PET detector module and the MR system were observed. The design of the new PET insert based on these<br />

detectors is presented.<br />

14:30 3949. Design of a Dynamically-Controlled Resistive Shield for a Combined PET and<br />

Superconducting MRI System for Small Animal Imaging<br />

Geron Andre Bindseil 1 , Timothy J. Scholl 1 , William B. Handler 1 , Chad T. Harris 1 , Blaine<br />

A. Chronik 1<br />

1 Department of Physics and Astronomy, University of Western Ontario, London, Ontario, Canada<br />

Combining conventional PET and MRI faces numerous technical challenges, particularly the sensitivity of photomultiplier tube-based<br />

(PMT) PET detectors to magnetic fields. The authors describe an approach to PET/MRI in which a resistive electromagnet shield is<br />

used to null the field at the PMTs of a conventional PET system in the vicinity of a superconducting MRI system. The electromagnetic<br />

characteristics of the shield coil are presented. This approach benefits from allowing the use of commercially available PET systems,<br />

which include state-of-the-art timing & energy resolution, high sensitivity, and highly optimized event processing hardware.

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