Diego F. Martinez1, Kieffer J. Davieau1,2, Eric J. Lessard1,2, William B. Handler1, and Blaine A. Chronik1,2
1The xMR Labs, Physics and Astronomy, Western University, London, ON, Canada, 2Medical Biophysics, Western University, London, ON, Canada
Synopsis
Developments in MR systems are allowing for siting which
does not follow the typical “4 zone” architecture, removing barriers for MR
implementation. A consequence of this is that these systems are nearer to
elements of a building or hospital that may cause field distortions and cannot
be resolved by shimming. This work quantifies the field distortions due to two
typical elevators along a hallway and compares the distortion to a fit using a
magnetic dipole approximation, verifying a 1/r3 field behaviour. This
demonstrates the need for MR system placement guidelines which mitigate
potential field stability concerns due to building elements.
Introduction
Developments in
modern MR systems are allowing for more widely accessible systems that blur the
lines of the typical “4 zone” MR room approach. This simplification can reduce
costs associated with the set up of systems but comes at the expense of placing
these sensitive systems nearer to objects which cause field distortions, potentially
introducing challenges for applications which require high field stability. Of concern
are the sources of field disturbance whose distortions are dynamic and cannot
simply be resolved with shimming, such as an elevator, nearby car park, or the
movement of a metal patient gurney. Studies to date on the magnetic fields
generated by this class of objects focus more on applications for localization
based on these distortions and their analysis is based on data collected using
magnetometers with low precision1. In this paper, the field distortions due
to typical elevators were investigated to gain insight into the potential
effects on main magnetic fields of moving metal objects near an MR scanner.Methods
Field information was collected using a 3-axis fluxgate probe with
calibration range 0-100 µT (Metrolab THM1186). The sampling
rate of the probe was set to 100 points per second, and a 50-point rolling
average was performed to reduce the noise in the measurements, also providing a
standard deviation. Two elevators (Elevator A and Elevator B) were used in this
study. A schematic of the probe locations measured is shown in the experimental
setup Figure 1. A time series was
acquired while the elevator was taken to each floor in order, producing a record
of the field changes relative to the initiation of data collection (initial
condition was door open while on the same floor as the probe). This process was
repeated for all 6 positions on all the accessible floors for both elevators. The
analysis of magnetic field time series was conducted in Python, with the
maximum field change determined at each of the sampling locations. The maximum
field change as a function of distance was fitted to a 1/r3 function
to match a gross approximation of the elevators as magnetic dipoles2.Results
Figure 2 shows an annotated sample
time series, highlighting the change of floors as the elevator cycles, as well
as the confidence intervals due to the rolling average taken. The 1/r3
fit is shown in Figure 3 for the six
positions on a particular floor for elevator A as an example. In Figure 4, all the data for both elevators,
A and B, on all floors are shown with a fit, and in Figure 5 an order of magnitude comparison is shown for general
distances from the elevator, with elevator B generally having lower field
values at similar distances.Discussion
The expected fit showing the 1/r3 behaviour was verified,
suggesting that in terms of modelling and predicting the effects that a system
could be exposed to, a magnetic dipole approximation is appropriate. The
limitations of this are evidently displayed in Figure 4 where the spread of the 50 point average leads to large
error bars, particularly near the elevator door in B. Thus, it is recommended
that for any modelling, the nearest predictions using a dipole approximation
occur past 5m from the elevator door. In general, the effect on field was in
the order of 1000 nT at ~5 m, 100 nT at ~10 m, and 10 nT at ~20 m.
From this, it is unlikely that an elevator will significantly distort the
static field of an MR system if located more that 10 m away. Typically, it is
only the field oriented in the axis of the magnet that will affect imaging, and
the current through the superconducting coils will flow to compensate for a
changing magnetic flux. These factors represent a reduction in the effect of
the distorting field of about an order of magnitude, with further work to be
done quantifying these relationships.
The elevators
studied in this experiment both used a counterweight system. To expand the
work, other elevator types such as freight and hydraulic systems could be
tested. As well, other elements which can contribute to magnetic distortions
exist in medical environments, and another step is to expand these measurements
to other common sources of distortion in order to present a full picture of how
the main magnetic field is affected. Modern approaches to field stability normally
attempt to measure and compensate for or prevent distortion, such as using
passive superconducting coils and passive steel room shielding. Developing guidelines
for MR placement that account for some of these other factors could help to simplify
the siting of an MR system.Conclusion
In this
work, we have conducted a study quantifying the effect that a typical elevator
has on magnetic field in the vicinity. Through this study, these effects can be
better quantified when determining the location of an MR system, particularly
in relation to the moving elements in a building.Acknowledgements
The authors would like to acknowledge support form NSERC and the Ontario
Research Fund.References
1. Shu Y, Bo C, Shen G, et al. Magicol: Indoor localization using
pervasive magnetic field and opportunistic WiFi sensing. IEEE Journal on
Selected Areas in Communications. 2015;33(7), 1443-1457.
2. Jackson J. D. Classical Electrodynamics, 1999.