Xin Chen1, Shinji Mitsui2, Yoshinori Hamamura1, and Michael Steckner1
1Canon Medical Research USA, Inc., Mayfield Village, OH, United States, 2Canon Medical Systems Corporation, Otawara-shi, Japan
Synopsis
Pulse energy SAR measurement method (NEMA standard MS-8)
uses current sensing flux loops to measure coil power loss, which varies in
different imaging conditions. Modeling results suggest that using multiple flux
loops distributed around Tx coil, as presently defined by the standard, may not
give accurate results. For whole body birdcage coil loaded with a human
subject, single flux loop spaced from endring and positioned at 3 or 9 o’clock
may give more accurate results.
Introduction
Two widely used Whole Body (WB) SAR assessment methods (pulse
energy method and calorimetry method) are described in NEMA standard MS-81, but
only the pulse energy method can be used with a human subject. The critical
aspect is current sensing flux loops placement near the Tx coil to measure coil
power loss, which varies in different imaging conditions. RF power deposition
in the subject Psub is calculated as:
Psub = Pin – PCPL_loaded [1]
where Pin is Tx coil “net” input power, i.e. forward power minus reflected power, and PCPL_loaded is
coil power loss with the presence of test subject. Furthermore,
PCPL_loaded
= PCPL_unloaded x (Vsub/Vunloaded)2 [2]
where Vsub and Vunloaded are B1 field
induced voltage in the flux loop measured with the test subject and a lossless
phantom respectively, and PCPL_unloaded is the Tx coil net input
power measured with the lossless phantom. The standard recommends using a
sufficient number of flux loops distributed evenly to get a balanced sample of
the coil currents. In this case, the sum of the squared voltage values from all
flux loops need to be calculated in Equation [2], assuming all flux loops have same
sensitivity:
Vsub2 (with test subject) or Vunloaded2 (with the lossless phantom)= ∑ Vflux loop2 [3]
We
use numerical EM modeling to show that using multiple flux loops evenly
distributed around the birdcage coil and spaced from endring may not give
accurate results. Instead, single flux loop at a strategically selected location
can give more accurate results.Methods
Numerical FDTD EM modeling was performed with a
generic 3T WB Tx coil (16-rung
high-pass birdcage, diameter 750mm, length 650mm. RF shield diameter 790mm,
length 850mm.2,3)
with Sim4Life (v4.4, ZMT, Zurich, Switzerland). The coil was tuned to 128MHz
for 3T MRI and driven with two voltage sources located on one end ring. Sixteen
square flux loops (Figure 1) were positioned near the coil endring (Figure 2),
per MS-8. The flux loops form a circular loop with 730mm diameter. Visible Man4 was modeled with three imaging conditions (head, abdomen, and foot), and the
following computed: power deposition in the subject, coil input power and
induced voltage in all flux loops recorded by 50 Ohm resistors.Results
Table 1 shows the differences between the RF power
deposition in Visible Man and the value calculated based on MS-8, using all 16 flux loops and Equations [1]-[3]. RF power deposition in Visible Man is also compared with
values calculated with each individual flux loop’s voltage using Equation [1], assuming
each flux loop provides a separate measurement (Figure 3).Discussion
Table 1 shows that based on MS-8, pulse energy measurement
with a number of flux loops spaced from birdcage coil’s endring and evenly distributed
around the coil (all with same sensitivity) did not give accurate power
deposition in Visible Man for the three imaging landmarks investigated. The
error ranges from 14.7% underestimate for abdomen and 41.0% overestimate for
head. We did not model flux loops placed between coil rungs in the center axial
slice. Experiment setup like the modeling presented here with all flux loops
outside coil imaging volume is more advantageous at reducing cable (used to transmit flux
loop voltage signal) exposure to Tx coil fields and resultant inference with
the measurement. It can also help reduce potential interaction between human
subject (especially big subjects) and flux loops if the loops are placed at
positions 4, 5, 13, and 14 in Figures 2 and 3 (i.e. 3 and 9 o’clock). For the three landmarks
investigated, although gray curves in Figure 3 had different patterns, flux
loops placed at side of the bore (e.g. 3 and 9 o’clock locations) generally
give better results than other locations.Conclusion
We used numerical EM modeling to investigate the impact of
current sensing flux loop’s location on pulse energy SAR measurement accuracy. Results
obtained with a human model at three imaging landmark positions suggest that a
single flux loop placed at 3 or 9 o’clock and spaced from WB birdcage coil’s
endring may give more accurate results.Acknowledgements
References
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