Changes in the specific absorption rate (SAR) of radiofrequency energy in patients with retained cardiac leads during MRI at 1.5T and 3T
Corresponding Author
Laleh Golestanirad
Athinoula A. Martinos Center for Biomedical Imaging, Department of Radiology, Massachusetts General Hospital, Harvard Medical School, Charlestown, Massachusetts
Department of Radiology, Northwestern University, Feinberg School of Medicine, Chicago, Illinois
Correspondence
Laleh Golestani Rad, AA Martinos Center, Massachusetts General Hospital, Harvard Medical School, Building 75, Third Ave, Charlestown, MA 02129 Email: [email protected] or Department of Radiology, Feinberg School of Medicine, 737 N Michigan Ave. Suite 1600, Chicago IL 60611.
Email: [email protected]
Search for more papers by this authorAmir Ali Rahsepar
Department of Radiology, Northwestern University, Feinberg School of Medicine, Chicago, Illinois
Search for more papers by this authorJohn E Kirsch
Athinoula A. Martinos Center for Biomedical Imaging, Department of Radiology, Massachusetts General Hospital, Harvard Medical School, Charlestown, Massachusetts
Search for more papers by this authorKenichiro Suwa
Department of Radiology, Northwestern University, Feinberg School of Medicine, Chicago, Illinois
Search for more papers by this authorJeremy C. Collins
Department of Radiology, Northwestern University, Feinberg School of Medicine, Chicago, Illinois
Search for more papers by this authorLeonardo M. Angelone
Division of Biomedical Physics, Office of Science and Engineering Laboratories, Center for Devices and Radiological Health, U.S. Food and Drug Administration, Silver Spring, Maryland
Search for more papers by this authorBoris Keil
Department of Life Science Engineering, Institute of Medical Physics and Radiation Protection, Giessen, Germany
Search for more papers by this authorRod S. Passman
Division of Cardiology, Department of Medicine, Northwestern University, Feinberg School of Medicine, Chicago, Illinois
Search for more papers by this authorGiorgio Bonmassar
Athinoula A. Martinos Center for Biomedical Imaging, Department of Radiology, Massachusetts General Hospital, Harvard Medical School, Charlestown, Massachusetts
Search for more papers by this authorPeter Serano
Division of Biomedical Physics, Office of Science and Engineering Laboratories, Center for Devices and Radiological Health, U.S. Food and Drug Administration, Silver Spring, Maryland
Search for more papers by this authorJames C. Carr
Department of Radiology, Northwestern University, Feinberg School of Medicine, Chicago, Illinois
Search for more papers by this authorLawrence L. Wald
Athinoula A. Martinos Center for Biomedical Imaging, Department of Radiology, Massachusetts General Hospital, Harvard Medical School, Charlestown, Massachusetts
Search for more papers by this authorCorresponding Author
Laleh Golestanirad
Athinoula A. Martinos Center for Biomedical Imaging, Department of Radiology, Massachusetts General Hospital, Harvard Medical School, Charlestown, Massachusetts
Department of Radiology, Northwestern University, Feinberg School of Medicine, Chicago, Illinois
Correspondence
Laleh Golestani Rad, AA Martinos Center, Massachusetts General Hospital, Harvard Medical School, Building 75, Third Ave, Charlestown, MA 02129 Email: [email protected] or Department of Radiology, Feinberg School of Medicine, 737 N Michigan Ave. Suite 1600, Chicago IL 60611.
Email: [email protected]
Search for more papers by this authorAmir Ali Rahsepar
Department of Radiology, Northwestern University, Feinberg School of Medicine, Chicago, Illinois
Search for more papers by this authorJohn E Kirsch
Athinoula A. Martinos Center for Biomedical Imaging, Department of Radiology, Massachusetts General Hospital, Harvard Medical School, Charlestown, Massachusetts
Search for more papers by this authorKenichiro Suwa
Department of Radiology, Northwestern University, Feinberg School of Medicine, Chicago, Illinois
Search for more papers by this authorJeremy C. Collins
Department of Radiology, Northwestern University, Feinberg School of Medicine, Chicago, Illinois
Search for more papers by this authorLeonardo M. Angelone
Division of Biomedical Physics, Office of Science and Engineering Laboratories, Center for Devices and Radiological Health, U.S. Food and Drug Administration, Silver Spring, Maryland
Search for more papers by this authorBoris Keil
Department of Life Science Engineering, Institute of Medical Physics and Radiation Protection, Giessen, Germany
Search for more papers by this authorRod S. Passman
Division of Cardiology, Department of Medicine, Northwestern University, Feinberg School of Medicine, Chicago, Illinois
Search for more papers by this authorGiorgio Bonmassar
Athinoula A. Martinos Center for Biomedical Imaging, Department of Radiology, Massachusetts General Hospital, Harvard Medical School, Charlestown, Massachusetts
Search for more papers by this authorPeter Serano
Division of Biomedical Physics, Office of Science and Engineering Laboratories, Center for Devices and Radiological Health, U.S. Food and Drug Administration, Silver Spring, Maryland
Search for more papers by this authorJames C. Carr
Department of Radiology, Northwestern University, Feinberg School of Medicine, Chicago, Illinois
Search for more papers by this authorLawrence L. Wald
Athinoula A. Martinos Center for Biomedical Imaging, Department of Radiology, Massachusetts General Hospital, Harvard Medical School, Charlestown, Massachusetts
Search for more papers by this authorFunding information: National Institutes of Health, Grant/Award Numbers: K99EB021320, R01EB00684, R01MH111875, and R03 EB024705
Abstract
Purpose
To evaluate the local specific absorption rate (SAR) and heating around retained cardiac leads during MRI at 64 MHz (1.5T) and 127 MHz (3T) as a function of RF coil type and imaging landmark.
Methods
Numerical models of retained cardiac leads were built from CT and X-ray images of 6 patients with retained cardiac leads. Electromagnetic simulations and bio-heat modeling were performed with MRI RF body and head coils tuned to 64 MHz and 127 MHz and positioned at 9 different imaging landmarks covering an area from the head to the lower limbs.
Results
For all patients and at both 1.5T and 3T, local transmit head coils produced negligible temperature rise (
) for
. For body imaging with quadrature-driven coils at 1.5T,
during a 10-min scan remained < 3°C at all imaging landmarks for
and <6°C for
. For body imaging at 3T,
during a 10-min scan remained < 6°C at all imaging landmarks for
. For shorter pulse sequences up to 2 min,
remained < 6°C for
.
Conclusion
For the models based on 6 patients studied, simulations suggest that MRI could be performed safely using a local head coil at both 1.5T and 3T, and with a body coil at 1.5T with pulses that produced
. MRI at 3T could be performed safely in these patients using pulses with
.
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