Microwave Imaging - University of...
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University of ManitobaDepartment of Electrical & Computer Engineering
ECE 4600 Group Design Project
Progress Report
Microwave Imaging
byGroup 12
Steven Brown Bryce O’DonnelTrevor Ingelbeen Steve Demedash
Brett Trombo Devon Hudson
Academic Supervisor(s)
Dr. Joe LoVetri
Industry Supervisors
Ian Jeffrey – 151 Industries
Colin Gilmore – 151 Industries
Paul Card – 151 Industries
Date of Submission
January 12, 2015Copyright © 2015 Steven Brown, Bryce O’Donnel, Trevor Ingelbeen, Steve Demedash,
Brett Trombo, Devon Hudson
Microwave Imaging Methods for Breast Cancer Research TABLE OF CONTENTS
Table of Contents
1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 1
2 Project Progress and Future Work . . . . . . . . . . . . . . . . . . . . . . . . . . . . 1
2.1 Field Coil . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 1
2.2 Antennas . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 3
2.3 Software . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 5
3 Conclusions . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 7
Appendix A Updated Gantt Chart . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 8
Appendix B Updated Budget . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 10
Appendix C System Diagram . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 11
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Microwave Imaging Methods for Breast Cancer Research 1 Introduction
1 Introduction
The Electromagnetic Imaging Lab (EIL) at the University of Manitoba is researching breast imaging
systems for the purpose of non-invasive breast cancer detection. The imaging systems researched
in the EIL use microwave imaging (MWI) technology to detect breast cancer as an alternative to
MRI and mammogram technology.
The first MWI system contains a field coil capable of producing 0.2 Tesla magnetic field and
Group 12 is designing the hardware for this project. The material costs of this project have driven
a scope change therefore this project is no longer progressing according to the original plan.
The second MWI system requires a dual polarized antenna array to produce a 3D image
of the healthy and cancerous tissue within a patient’s breast. During the design phase of the
dual polarized antenna, Group 12 encountered significant project scope change and is no longer
progressing according to the original plan.
Lastly, the EIL requires control and monitoring software for its devices. Group 12 is developing
new software for the devices mentioned above as well as improving existing software within the EIL.
The software project is progressing as originally planned.
2 Project Progress and Future Work
The progress for group 12 from the past four months and planned future work is described below
for each of the three project components, with our new tasks outlined in Appendix A. To view a
system block diagram refer to Appendix C.
2.1 Field Coil
In the past four months, Group 12 has divided the magnetic field coil design into three sections:
field coil, cooling system and power supply. Bryce and Trevor simulated the magnetic field with
Matlab to design the coil size and electric current required to produce the magnetic field. The
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Microwave Imaging Methods for Breast Cancer Research 2 Project Progress and Future Work
simulation determined that a magnetic field of 0.2T could be achieved by feeding 500 Amps of DC
current though a field coil. Bryce, Joe LoVetri and Dan Card determined that from an economic
standpoint, using copper refrigeration tubing was the best material for the copper conductor and
cooling system. Refrigeration copper is malleable, readily available, and can be manually coiled
without outsourcing to a manufacturer. The cost of the copper conductor required for this project
created a scope change for project. Group 12 and its supervisor removed the manufacturing of the
entire field coil from the project scope. Instead Group 12 will now produce a 1/16th scaled proof
of concept test and if time and money permits, the remainder 15/16th of the project will be built.
The cooling system design was completed in parallel with the field coil design by Bryce and
Trevor. Originally the cooling system was proposed to be completed after the coil design but due
to the high importance of the cooling system it was incorporated into the field coil design. The
high amperage required to produce the specified magnetic field will generate a large amount of
heat. The heat will affect the resistivity of the coil and potentially damage the coils insulation.
The cooling system maintains a safe operating temperature by circulating a coolant through the
hollow interior of the field coil conductor.
The power supply will provide the field coil with 500A which will produce the magnetic field.
Trevor designed the power source using lithium batteries because Group 12 had access to these
batteries. Trevor and Bryce designed the power source to have a freewheeling diode to allow a
gradual current decay across the inductive coil when the device is turned off. A properly rated
controllable switch was also used in the power supply so that the GUI control software can turn
the source on or off.
In the next two months, Trevor and Bryce will assemble the individual components required to
build and test the entire field coil, power supply and cooling system. A complete list of parts and
their expected delivery date is located in the budget section of Appendix B. The first component
that Trevor and Bryce will assemble is the power supply. Jumper cables, capable of withstanding
500A DC are required to connect the field coil, freewheeling diode and switch to the batteries.
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Microwave Imaging Methods for Breast Cancer Research 2 Project Progress and Future Work
Custom jumper cables will be built by Trevor and Bryce because they are less expensive than pur-
chasing them from a supplier. Next, the batteries, freewheeling diode and switch will be installed,
completing the assembly of the power supply. Prior to installing the switch, the interface between
the GUI and switch will be assembled and tested by Trevor, Devon and Bryce. The GUI will control
the on/off status of the magnetic field. During the assembly of the power supply, quality control
measures will be implemented to determine the circuit properties and verify the functionality of
the control switch.
The next component that Trevor and Bryce will build is the interface between the power supply
and field coil. The preferred method to electrically connect the field coil and power supply will
require a soldered connection arm between the field coil and the cables from the power supply.
If the soldered connection arm fails, a ground clamp will be used to connect the field coil to the
power supply cable cables. Next, the cooling system will be assembled by Trevor and Bryce. The
plumbing from the pump outlet to field coil will be assembled and tested to verify the flow rate of
the cooling system.
Finally, Trevor and Bryce will assemble the entire field coil system which consists of the field
coil, power supply, and cooling system as shown in our updated Gantt Chart in Appendix A. All
electrical connections will be terminated and the entire system will be tested to verify that the
system is operating as intended. If required, troubleshooting will occur at this point.
2.2 Antennas
The antenna portion of the project can be separated into three areas, the cavity resonator, the
printed circuit board (PCB), and the control system. Thus far Group 12 has researched and
preformed various simulations of time electric (TE10) mode resonating cavities. From these sim-
ulations, Brett and Steven Brown were able to create the polarization of an antenna in both
orientations. The number of slots are not increasing in the antenna cavity as proposed due to
the orthogonal orientation of the cavities. Brett and Steven Brown explored higher order modes
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Microwave Imaging Methods for Breast Cancer Research 2 Project Progress and Future Work
of waveguides, which does increase the physical size and complexity of the feed arrangement. Al-
though more challenging, we have determined that a waveguide using higher order modes is better
as it allowed both polarizations of antenna slots to be on one resonating waveguide cavity.
Brett and Steven Brown have designed multiple resonating waveguide cavities using high fre-
quency simulation software (HFSS). The HFSS simulations show a simulated TE11 resonating
cavity with the reflection coefficient or return loss. The1 HFSS simulations have calculated the
gain loss coefficient to -11.31dB, which exceeds our project specifications. Brett and Steven Brown
are currently optimizing the antenna design by adjusting the input feed position and slot length
with a method called optometrics. This is a process in which the model is simulated in the HFSS
CAD Tool and the position of various variables are adjusted. The position and length of the coax-
ial feed that satisfies the most requirements are saved for the user. Brett and Steven Brown have
decided to minimize the return loss of the resonating cavity to ensure that the maximum radiation
would propagate from the resonating cavity as well as, maximize the surface current density on the
PCB ground plane.
Brett and Steven Brown are actively working on slot schemes (positioning of slots in the PCB)
that cut the surface current density to maximize the radiation in the desired polarization. By
selecting to cut the slots on one resonating cavity as opposed to making two, saves space in the
antenna chamber because the resonating cavities with one polarization take up horizontal and ver-
tical space. The TE11 resonating cavity occupies mainly one orientation which we can select. A
singular resonating cavity also enables us to modify the existing slot selection system by simply
running through all combinations of receiver and transmitter in one orientation followed by the
other orientation. For the remainder of the course, Group 12 will concentrate on three antenna
system components: the cavity resonator, PCB, and control system. The TE11 mode resonating
cavity must adapt the design to the specific application. Manufacturing, mounting, and mechanical
limitations must now be balanced with the best theoretical design. After final mechanical dimen-
sions are selected the appropriate slot schemes will be selected and simulated to verify the new
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dimensions. The best slot scheme from the simulations will be used for manufacturing.
There three major system components that still have to be manufactured as seen on the updated
Gantt Chart in Appendix A. After the resonating cavity design is finalized, the PCB design can
be sized to meet physical constraints of the antenna chamber. Once the PCB size is determined
it will be manufactured by an external vendor. The cavity resonator is purchased at the required
dimensions and the one side is removed then replaced with the PCB at the University of Manitoba.
The existing control system in the EIL is retrofitted to work with the new design.
Next testing will be conducted on the input impedance, radiated power, and slot control of
the antenna. Input impedance will be measured using a network analyzer and verified with the
expected design results. If time permits the antenna will be tested in an antenna lab to determine
radiation pattern and radiated power. The fall-back method will be to test the antennas in the
prototype application system and results measured by the control system. Integration with the
software control system will be the last testing procedure after the main components have been
tested individually.
2.3 Software
In the past four months, Group 12 has worked on the integration of the existing data acquisition and
control software currently used by the EIL into a single software package. Individual VNA and LIA
devices within the EIL are controlled by multiple versions of the control software. By consolidating
these versions, a single version will exist that is capable of running a variety of different devices,
allowing the user to select which device is to be used.
To begin, Devon and Steve Demedash modified the existing versions of the separate software
by removing extraneous comments and lines of code from the existing code. Devon and Steve
Demedash removed large blocks of code that constituted individual sub-processes from the main
loop, and created separate functions which increased the modularity and readability of the software.
When consolidating multiple versions of the algorithm Devon and Steve Demedash maintained
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functionality without reducing algorithm speed. However, consolidating the software versions added
more decision-making steps to the main process, introducing significant lag. To maintain algorithm
speed, and further reduce the code size, Devon and Steve Demedash designed a Finite State Machine
for quick branching when device specific portions of code were encountered.
In the next two months, Devon and Steve Demedash will follow the tasks outlined in the Gantt
Chart located in Appendix A. They will test the software to ensure it is operating as intended.
There are multiple hardware setups to be tested, this testing phase may be quick and present
positive results from the outset. Alternatively it could last much longer than anticipated, and may
take until the end of the semester to complete.
After the testing phase, they will either need to reevaluate the completed software updates, or
proceed with graphical user interface updates, and algorithm optimization. We introduced these
as an optional task, to be completed if time permits.
To update the graphical user interface, Devon and Steve Demedash will propose a new layout
that does not take away any functionality that already exists. The majority of the user interface
involves the selection of devices through which the user may configure the system for the devices
used, and type of scan to be done. This layout is cumbersome, so moving the device selection panel
over to a temporary tab or window would create a cleaner, more straight-forward interface. The
method by which the antennas are selected also needs to be re-examined. Currently, this portion
of the interface is small, and as such, it is difficult to select the desired antenna positioning.
Optimizing the imaging algorithm involves two things. First, the time it takes to measure
the data between antennas is the longest running time of the program, so they have the most to
gain by focusing our attention on this area of the code. Secondly, the software currently sends out
data to an excel file that is then loaded into Matlab where graphs and plots are generated. This
transfer over to Matlab takes time and it would be nice to have this in the same program that
performs the measurements. To do this Devon and Steve Demedash will need to get familiar with
the preexisting Matlab code and create graphical elements in the imaging software that allow the
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Microwave Imaging Methods for Breast Cancer Research 3 Conclusions
program to display the relevant graphs after taking the measurements has been completed.
3 Conclusions
Overall Group 12 has made significant progress in all areas of the project. Numerous setbacks in
specific project areas has led to a change in scope for both the field coil and antenna portion of the
project. Due to the sensitive nature of electromagnet devices more time was allotted to the design
stages of the product to ensure of functionality of the final product. The field coil section will
complete 1/16th of the original scope of the project due to expensive manufacturing and material
cost. The antenna portion is now designing a TE11 resonating cavity to meet all of the project
specification, while software is completing proposed tasks on schedule. With these new changes we
intend on completing tasks as assigned in our revised project schedule found on our updated Gantt
chart.
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Microwave Imaging Methods for Breast Cancer Research
Appendix A
Updated Gantt Chart
Fig. A.1: Revised Gantt Chart for Microwave Imaging Project (1 of 2)
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Microwave Imaging Methods for Breast Cancer Research
Fig. A.2: Revised Gantt Chart for Microwave Imaging Project (2 of 2)
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Appendix B
Updated Budget
The budget for the our Microwave imaging project is $1346.48 and is covered but the Dept. of
Electrical and Computer Engineering with the remainder of the fund provided EIL.
Fig. B.1: Up to Date Budget of the Project
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