Ultrasound Generation using Implanted Metallic Surfaces as Electromagnetic Acoustic Transducers By Yarub Alazzawi Chunqui Qian and Shantanu Chakrabartty alazzawi shantanuwustledu ID: 484460
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Slide1
Feasibility of Non-Contact Ultrasound Generation using Implanted Metallic Surfaces as Electromagnetic Acoustic Transducers
By:
Yarub
Alazzawi,
Chunqui
Qian, and Shantanu
Chakrabartty
alazzawi, shantanu@wustl.eduSlide2
Abstract—In this paper we investigate the feasibility of using an in-vivo metallic implant like a stent for generation of acoustic waves which can then be used for imaging areas inside or near the surface of the implant.
The proposed method relies
on time-varying
eddy-current loops that are excited on the metallic surface of the stent using an external RF coil.
In
this paper
we have designed a phantom set up to characterize
the acoustic
wave generation process and we demonstrate that
the acoustic
waves can be measured, imaged and harvested
remotely using
a piezoelectric probe.Slide3
Stents are routinely used in the surgical treatment of vascular stenosis where the metallic mesh in the stent provides mechanical support to the tissue walls and to facilitate the flow of vital fluids like blood or bile (as shown in Fig.1).
Fig. 1. Application of metallic stents and technologies used for
monitoring stent
potency [source: google images]
Post-surgery, the implanted stents are routinely monitored for occlusions which could potentially lead to restenosis and hence require surgical intervention.
A popular method
for post-operative
imaging of stents include x-ray
which
do not
provide
insight to the mechanics or growth
of occlusions
and the procedure neither provides any
information regarding
the fluid-flow through the stent. Direct magnetic
resonance imaging
(MRI) of stents are limited by the
generation of
eddy-currents which shield the spin signals emanating
from within
the
stent.Slide4
In-vivo metallic implant to generate acoustic waves.Objective
Non-contact imaging areas inside or near the implant
.
Remotely harvest acoustic waves.
In this paper, we explore an alternate approach
where the
metallic surface of the stent could be used for
in-vivo generation
of acoustic waves, which can then be used
for characterizing
stent potency
.Slide5
At the core of the proposed technique is the use of electromagnetic acoustic transducers (EMAT) which have been routinely used for non-destructive evaluation (NDE) of conductive structures like aircraft skins and metallic pipes.
The principle of EMAT is shown in Fig. 2 where an RF
coil generates
a time-varying electromagnetic (EM) field.
When a
metallic structure is exposed to this
field,
eddy-current loops are generated on the surface of
the structure
. The direction of the current is such that it
opposes the
change in the EM field and the result is loss of energy
due to
Joule
heating.
However, when the structure is
simultaneously subjected
to a constant magnetic field, the eddy-current loops experience a Lorentzian force that mechanically excite the metallic structure. The result is the generation of pressure waves, and the frequency of the acoustic wave is determined by the frequency of the EM field and by the mechanical properties of the structure.
Fig. 2. Operational principle of EMATSlide6Slide7
In this paper we have designed a phantom set up, as shown in Fig. 3, to characterize the acoustic wave generation process and we demonstrate that the acoustic waves can be measured, imaged and harvested remotely using a piezoelectric probe.
Experimental Setup
Fig.3 (
a)Schematic of the phantom experimental setup; (b)Photograph of the experimental setupSlide8
Experimental Setup
Water tank to emulate in-vivo conditions
Aluminum strip suspended in water to emulate metallic substrate
1.7 T permanent magnet suspended above water tank using a pulley
RF coil
(coated copper wires) connected to (10V, 500mA) HP function generator
Piezoelectric probe attached to the bottom of the water tank and connected to the oscilloscope to measure the acoustic signal generated by EMAT Slide9
Amplitude of Acoustic Wave
Real part of the amplitude of the acoustic wave:
Parameter
Description
RF electromagnetic field
Static magnetic field
Permeability of the vacuum
Bulk density of the metal
Acoustic wave velocity
Skin depth
Parameter
Description
RF electromagnetic field
Static magnetic field
Permeability of the vacuum
Bulk density of the metal
Acoustic wave velocity
Skin depth
Fig
. 4 Amplitude
of the acoustic wave generated using EMAT for
different metalsSlide10
Measurement Results
Fig.
5 Measured
signal power when the height of the magnet is varied and the implantation depth is set to 0mm.
0 mm implanting depth (the
aluminum substrate
was freely
floating on the water surface.
)
Variable magnet height (d)
20 mm water depth
5 mm RF-coil height
Fig.
5
shows the
result of the experiment and clearly shows an
inverse relationship
between the recorded signal and distance (d
).
This can
be attributed to the EM losses inside water which results
in smaller
magnitude of eddy-current loops.Slide11Fig. 6. Measured signal power when the height of the magnet is varied
and the implantation depth is set to 3mm.
3 mm implanting depth
Variable magnet height (d)
20 mm water depth
5 mm RF-coil height
Measurement Results
The power
received by the piezoelectric probe is lower for the
case when
the aluminum substrate was immersed in the
water, as shown in Fig. 6.Slide12
Measurement Results
Fig
. 7 System
frequency response measured using the EMAT setup
0 mm implanting depth
Variable RF analog signal frequency(Hz)
20 mm water depth
5 mm RF-coil height
10 mm distance between the RF coil and the
Magnet
Fig. 7 clearly
shows the existence multiple system poles which
leads to
different frequency windows where the EMAT method
is more
effective. These system poles and frequency windows
are determined
by several
mechanical and electrical factors.Slide13
The important point is that for both the experiments, the probe was able to harvest more than 100nW of power (when accounting for coupling losses) even when it was placed 2cm away from the surface of the aluminum plate. Thus, the proposed method could in principle be used for designing an in-vivo acoustic beacon or an ultrasonic telemetry system that is powered remotely using the EMAT technique.Slide14
Conclusions & Future Work
Conclusions
Feasibility of non-contact ultrasound generation using in-vivo EMAT based approach
Possibility of non-contact imaging and energy harvesting
Electrical and mechanical factors affect the process efficiency.
Future work
Optimizing EMAT technique for in-vivo studies using multi-physics modeling and analysis of EM and acoustic phenomena in biological tissue Slide15
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