<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">JBiSE</journal-id><journal-title-group><journal-title>Journal of Biomedical Science and Engineering</journal-title></journal-title-group><issn pub-type="epub">1937-6871</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jbise.2017.105B011</article-id><article-id pub-id-type="publisher-id">JBiSE-76950</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Biomedical&amp;Life Sciences</subject></subj-group></article-categories><title-group><article-title>
 
 
  The Forward and Inverse Problem Based on Magneto-Acoustic Tomography with Current Injection
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Hui</surname><given-names>Xia</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Guoqiang</surname><given-names>Liu</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Xin</surname><given-names>Huang</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Liang</surname><given-names>Guo</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Yanjiu</surname><given-names>Yang</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Minhua</surname><given-names>Lu</given-names></name><xref ref-type="aff" rid="aff3"><sup>3</sup></xref></contrib></contrib-group><aff id="aff3"><addr-line>Guangdong Key Laboratory for Biomedical Measurements and Ultrasound Imaging, Shenzhen, China</addr-line></aff><aff id="aff1"><addr-line>Department of Engineering Electromagnetics, Applications Institute of Electrical Engineering, Chinese Academy of Sciences, Beijing, China</addr-line></aff><aff id="aff2"><addr-line>University of Chinese Academy of Sciences, Beijing, China</addr-line></aff><pub-date pub-type="epub"><day>10</day><month>05</month><year>2017</year></pub-date><volume>10</volume><issue>05</issue><fpage>97</fpage><lpage>105</lpage><history><date date-type="received"><day>April</day>	<month>6,</month>	<year>2017</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>June</month>	<year>13,</year>	</date><date date-type="accepted"><day>June</day>	<month>16,</month>	<year>2017</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
   
   The Magneto-acoustic Tomography with Current Injection (MAT-CI) is a new biological electrical impedance imaging technique that combines Electrical Impedance Tomography (EIT) with Ultrasonic Imaging (UI), which possesses the non-invasive and high-contrast of the EIT and the high-resolution of the UI. The MAT-CI is expected to acquire high quality image and embraces a wide application. Its principle is to put the conductive sample in the Static Magnetic Field(SMF) and inject a time-varying current, during which the SMF and the current interact and generate the Lorentz Force that inspire ultrasonic signal received by the ultrasonic transducers positioned around the sample. And then according to related reconstruction algorithm and ultrasonic signal, electrical conductivity image is obtained. In this paper, a forward problem mathematical model of the MAT-CI has been set up to deduce the theoretical equation of the electromagnetic field and solve the sound source distribution by Green’s function. Secondly, a sound field restoration by Wiener filtering and reconstruction of current density by time-rotating method have deduced the Laplace’s equation that caters to the current density to further acquire the electrical conductivity distribution image of the sample through iteration method. In the end, double-loop coils experiments have been conducted to verify its feasibility. 
  
 
</p></abstract><kwd-group><kwd>Magneto-Acoustic Tomography With Current Injection</kwd><kwd> Axial Symmetry Model</kwd><kwd> the Forward and Inverse Problem of Electromagnetic Field</kwd><kwd>  Reconstruction Image</kwd><kwd> Reconstruction Electrical Conductivity Image</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>At present, structure imaging is relatively mature in medical imaging for clinical use. However, it is limited to the imaging of the form and structure of the tissue and fails to detect and diagnose tissue lesion in an early stage. A research has shown that a MAT-CI that combined the form and the function of the tissue is expected to fulfill the early warning and diagnosis of a disease. As a new type of imaging method that based on magneto-acoustic coupling, the MAT-CI possesses all the advantages of magneto acoustic coupling and resolves the problem of producing a step signal in magneto acoustic tomography with magnetic induction [<xref ref-type="bibr" rid="scirp.76950-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.76950-ref2">2</xref>]. The efficiency of energy conversion can be improved by the MAT-CI. Meanwhile exciting coil is not used in the MAT-CI, which leads to negative influence of the altering magnetic field to the current of the specimen and interference of the altering magnetic field to the detection equipments such as ultrasonic transducer.</p><p>Towe B C is the first researcher who has conducted the research on the MAT- CI, who put forward a bioelectric currents detecting method through electromagnetic coupling and prove the feasibility of this method through experiment [<xref ref-type="bibr" rid="scirp.76950-ref3">3</xref>]. It was not until 2010 that the Chinese Academy of Medical Sciences and the Institute of Electrical Engineering of the Chinese Academy of Sciences conducted researches on the MAT-CI [<xref ref-type="bibr" rid="scirp.76950-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.76950-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.76950-ref6">6</xref>]. This paper conducts systematic research on the theory system of the MAT-CI, focuses on the axial symmetry model, verifies the feasibility in the field of electrical impedance tomography through experimentation and simulation.</p></sec><sec id="s2"><title>2. Research on the Forward Problem of Electromagnetic Field</title><sec id="s2_1"><title>2.1. Theoretical Analysis on Forward Problem</title><p>Assuming the imaging sample’s electrical conductivity is <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76950x2.png" xlink:type="simple"/></inline-formula> , the sample is put in the static electric field of which the field density is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76950x3.png" xlink:type="simple"/></inline-formula>, the current density in the sample after the injunction of the current is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76950x4.png" xlink:type="simple"/></inline-formula>, the electric field intensity in the sample is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76950x5.png" xlink:type="simple"/></inline-formula>.</p><p>According to Maxwell’s equations, introduce the magnetic vector potential <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76950x6.png" xlink:type="simple"/></inline-formula> while meet Cullen specification, namely <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76950x7.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.76950-formula22"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/76950x8.png"  xlink:type="simple"/></disp-formula><p>From Maxwell’s equation</p><disp-formula id="scirp.76950-formula23"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/76950x9.png"  xlink:type="simple"/></disp-formula><p>Assuming that the permeability of the sample and air are<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76950x10.png" xlink:type="simple"/></inline-formula>, and simplifying it with the vector equation <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76950x11.png" xlink:type="simple"/></inline-formula> and Cullen specification<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76950x12.png" xlink:type="simple"/></inline-formula>, it is concluded from (1) and (2):</p><disp-formula id="scirp.76950-formula24"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/76950x13.png"  xlink:type="simple"/></disp-formula><p>Injecting the electric current on the boundary of the sample, and the current density is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76950x14.png" xlink:type="simple"/></inline-formula>. Using the electric insulation boundary, and the condition of the boundary is</p><disp-formula id="scirp.76950-formula25"><graphic  xlink:href="http://html.scirp.org/file/76950x15.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76950x16.png" xlink:type="simple"/></inline-formula> is the normal direction of the outer boundary, where the sample is injected by electric current. With the Equation (3) and boundary condition, magnetic vector potential <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76950x17.png" xlink:type="simple"/></inline-formula> can be obtained and the current density of the specimen can be calculated</p><disp-formula id="scirp.76950-formula26"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/76950x18.png"  xlink:type="simple"/></disp-formula></sec><sec id="s2_2"><title>2.2. Simulation Analysis on Forward Problem</title><p>It is shown in <xref ref-type="fig" rid="fig1"><xref ref-type="fig" rid="fig">Figure </xref>1</xref> that a hollow cylinder in axial symmetry models is simulated. The electrical conductivity distribution on the inner wall of the cylinder is abnormal. For axial symmetry models, its electrical conductivity distribution of the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76950x19.png" xlink:type="simple"/></inline-formula> section is same. Therefore, in simulation calculation, the parameter distribution of the meridian plane of the dylinder just is researched.</p><p>Assuming that the density of the cylinder is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76950x20.png" xlink:type="simple"/></inline-formula>, the spread speed of the original sound field is <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76950x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76950x21.png" xlink:type="simple"/></inline-formula> in it, and the outer radius is <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76950x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76950x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76950x22.png" xlink:type="simple"/></inline-formula> while the inner radius is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76950x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76950x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76950x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76950x23.png" xlink:type="simple"/></inline-formula>. In the coordinates of <xref ref-type="fig" rid="fig1"><xref ref-type="fig" rid="fig">Figure </xref>1</xref>, the electrical conductivity in the section meets:</p><disp-formula id="scirp.76950-formula27"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/76950x24.png"  xlink:type="simple"/></disp-formula><p>Lorentz force divergence in this sample</p><disp-formula id="scirp.76950-formula28"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/76950x25.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76950x26.png" xlink:type="simple"/></inline-formula> is the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76950x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76950x27.png" xlink:type="simple"/></inline-formula> component of current density. The matching Lorentz force divergence is</p><fig-group id="fig1"><label><xref ref-type="fig" rid="fig1"><xref ref-type="fig" rid="fig">Figure </xref>1</xref></label><caption><title> Axial symmetry model and electrical conductivity distribution on meridian plane.</title></caption><fig id ="fig1_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/76950x29.png"/></fig><fig id ="fig1_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/76950x28.png"/></fig></fig-group><disp-formula id="scirp.76950-formula29"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/76950x30.png"  xlink:type="simple"/></disp-formula><p>From Equation (4) and (5), Lorentz force divergence on meridian plane of the axial symmetry model can be obtained, as shown in <xref ref-type="fig" rid="fig2"><xref ref-type="fig" rid="fig">Figure </xref>2</xref>. From the <xref ref-type="fig" rid="fig2"><xref ref-type="fig" rid="fig">Figure </xref>2</xref>, it is shown that under the effect of the magneto-static field, the current density and Lorentz force are strong when the electrical conductivity is strong which could motivate stronger Lorentz force divergence sound source. Therefore, there is a corresponding relation between strength of sound source and electrical conductivity distribution.</p></sec></sec><sec id="s3"><title>3. The Inverse Problem of Electromagnetic Field</title><sec id="s3_1"><title>3.1. Inverse Problem Theory Analysis</title><p>In the research of inverse problem on the axisymmetric model, as the current density in the samples is only on the circumferential component<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76950x31.png" xlink:type="simple"/></inline-formula>, and the distribution of the current density of the samples on each meridian plane is the same, the study about the electromagnetic field on a certain meridian plane is available. Thus</p><disp-formula id="scirp.76950-formula30"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/76950x32.png"  xlink:type="simple"/></disp-formula><p>If <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76950x33.png" xlink:type="simple"/></inline-formula></p><p>Then the current density of the samples will be</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76950x34.png" xlink:type="simple"/></inline-formula> （9)</p><p>The distribution of current density on the meridian plane would be available through the Formula (9). And the distribution of electrical conductivity on the meridian plane of the axisymmetric filed model could be obtained by an iterative method with the result of current density.</p></sec><sec id="s3_2"><title>3.2. The Simulation Analysis of Inverse Problem</title><p>Using the axisymmetric model in <xref ref-type="fig" rid="fig1"><xref ref-type="fig" rid="fig">Figure </xref>1</xref> and collecting acoustic pressure signal, which the number of is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76950x35.png" xlink:type="simple"/></inline-formula>, around the interface, the sound sources, Lorentz force divergence can be rebuilt for the sample by the time reversal way. The <xref ref-type="fig" rid="fig3"><xref ref-type="fig" rid="fig">Figure </xref>3</xref> is the distribution of Lorentz force divergence about the samples by the time reversal way with the use of sound pressure in the original sound field. Comparing to the <xref ref-type="fig" rid="fig">Figure </xref> 2 in the forward problem, they have the similar distribution.</p><p>Reconstruction electrical conductivity distribution is shown in <xref ref-type="fig" rid="fig">Figure </xref>4, and consistent with <xref ref-type="fig" rid="fig1"><xref ref-type="fig" rid="fig">Figure </xref>1</xref>(b) the original conductivity images, which verifies the feasibility of reconstruction methods.</p><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2"><xref ref-type="fig" rid="fig">Figure </xref>2</xref></label><caption><title> Lorentz force divergence on forward problem calculation</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/76950x36.png"/></fig><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3"><xref ref-type="fig" rid="fig">Figure </xref>3</xref></label><caption><title> Lorentz force divergence reconstructed by the sound pressure</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/76950x37.png"/></fig></sec></sec><sec id="s4"><title>4. Experiment Study</title><p>The experiment principle is shown in <xref ref-type="fig" rid="fig">Figure </xref>5, the plate that double-ring model in is vertical to the static magnetic field. In order to avoid the reflection between inner ring and outer ring, the plane that fits the inner ring and outer ring, however, the separation between is 2 mm for the probe of ultrasonic transducer is 10 mm. Thus, the double-ring model can be regarded in the same plate when imaging. <xref ref-type="fig" rid="fig">Figure </xref>5(b) is the top view of double-ring model while point A and B is the injection point electrode, with frequency of 1 KHZ, duty ratio is 0.1%, am- plitude of pulse current is 50 V.</p><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig">Figure </xref>4</label><caption><title> The reconstruction electrical conductivity of sampl</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/76950x38.png"/></fig><fig-group id="fig5"><label><xref ref-type="fig" rid="fig">Figure </xref>5</label><caption><title> Experiment principle of MAT-CI and double-ring model</title></caption><fig id ="fig5_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/76950x39.png"/></fig></fig-group><p>Magnetic acoustic signal received by ultrasonic transducer as shown in <xref ref-type="fig" rid="fig">Figure </xref>6, among which CH1 represents waveform of synchronizing signal, CH2 re- presents waveform of excited signal, CH3 represents waveform of magnetic acoustic signal. Each of the vertical axes of CH3 is 5mV while excited signal seen as reference signal. Four peaks in the right side are seen, in accordance with the four positions of electrical conductivity.</p><p>Two sets of coaxial double-loop coils are adopted in experiment, the outer diameters of the two sets of coaxial double-loop coils keep the same,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76950x40.png" xlink:type="simple"/></inline-formula>. The inner diameters are <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76950x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76950x41.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76950x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76950x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76950x42.png" xlink:type="simple"/></inline-formula>. <xref ref-type="fig" rid="fig">Figure </xref>7 and <xref ref-type="fig" rid="fig">Figure </xref>8 are images of electrical conductivity of double coils. From <xref ref-type="fig" rid="fig">Figure </xref>7, when the distance between the borders of 2 coils comes to 10 mm, the reinstituted image of Lorentz Force divergence and the image of electrical conductivity coincide the spread of electrical conductivity of sample.</p><p>From <xref ref-type="fig" rid="fig">Figure </xref>8, when the distance between 2 coils becomes 5 mm, the reconstruction image can be reflected the distance clearly, illustrating that MAT-CI</p><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig">Figure </xref>6</label><caption><title> Waveform of magnetic acoustic signal of double-ring model collected by ultrasonic transduce</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/76950x43.png"/></fig><fig id="fig7"  position="float"><label><xref ref-type="fig" rid="fig">Figure </xref>7</label><caption><title> The image of electrical conductivity of reconstructed double-loop coils. (inner diameter: 10 mm</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/76950x44.png"/></fig><p>experiment system and reconstruction arithmetic can make the resolution of MAT-CI to 5 mm.</p></sec><sec id="s5"><title>5. Conclusion</title><p>In this paper, it is conducted systematic research on the theory system of the MAT-CI, focused on the axial symmetry model, and verified the feasibility in the field of electrical impedance tomography through experimentation and simula-</p><fig id="fig8"  position="float"><label><xref ref-type="fig" rid="fig">Figure </xref>8</label><caption><title> The image of electrical conductivity of reconstruction double- loop coils. (inner diameter: 20 mm</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/76950x45.png"/></fig><p>tion. Meanwhile, by making use of double-loop model to conduct an experiment proving when distance of electrical conductivity becomes 5 mm, the reconstruction image of sample is obtained clearly. It is proved the prospect of MAT-CI in medical area.</p></sec><sec id="s6"><title>Acknowledgements</title><p>This work was supported by the National Natural Science Foundation of China under Grant Nos 51137004, 61427806 and 61271424, and also supported by Instrument development project of Chinese Academy of Sciences Nos YZ201507. Corresponding author E-mail: gqliu@mail.iee.ac.cn.</p></sec><sec id="s7"><title>Cite this paper</title><p>Xia, H., Liu, G.Q., Huang, X., Guo, L., Yang, Y.J. and Lu, M.H. (2017) The Forward and Inverse Problem Based on Magneto-Acoustic Tomography with Current Injection. J. 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