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FEM Based design and simulation tool for MRI birdcage coils Including eigenfrequency analysis

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(1)

Introduction Motivation Methods Experimental Results Conclusion

FEM Based Design and Simulation Tool for

MRI Birdcage Coils Including Eigenfrequency

Analysis

Necip Gurler and Yusuf Ziya Ider Electrical and Electronics Engineering Department

(2)

Outline

1 Introduction RF coils in MRI RF birdcage coils

Design and simulation of RF birdcage coils 2 Motivation

Review of previous studies Problem definition

Our work 3 Methods

FEM Models of Birdcage Coils Frequency Domain Analysis Eigenfrequency Analysis Software Tool

4 Experimental Results 5 Conclusion

(3)

Introduction Motivation Methods Experimental Results Conclusion RF coils in MRI RF birdcage coils

Design and simulation of RF birdcage coils

Outline

1 Introduction RF coils in MRI RF birdcage coils

Design and simulation of RF birdcage coils

2 Motivation

Review of previous studies Problem definition

Our work 3 Methods

FEM Models of Birdcage Coils Frequency Domain Analysis

(4)

Outline

1 Introduction RF coils in MRI

RF birdcage coils

Design and simulation of RF birdcage coils 2 Motivation

Review of previous studies Problem definition

Our work 3 Methods

FEM Models of Birdcage Coils Frequency Domain Analysis Eigenfrequency Analysis Software Tool

4 Experimental Results 5 Conclusion

(5)

Introduction Motivation Methods Experimental Results Conclusion RF coils in MRI RF birdcage coils

Design and simulation of RF birdcage coils

What Do the RF Coils Serve in MRI?

generate RF magnetic field (B1field) at the Larmor

frequency

(6)

RF Birdcage Head Coil Example

Source of figure: http://www.healthcare.philips.com

(7)

Introduction Motivation Methods Experimental Results Conclusion RF coils in MRI RF birdcage coils

Design and simulation of RF birdcage coils

Outline

1 Introduction RF coils in MRI

RF birdcage coils

Design and simulation of RF birdcage coils 2 Motivation

Review of previous studies Problem definition

Our work 3 Methods

FEM Models of Birdcage Coils Frequency Domain Analysis

(8)

RF Birdcage Coils

(9)

Introduction Motivation Methods Experimental Results Conclusion RF coils in MRI RF birdcage coils

Design and simulation of RF birdcage coils

RF Birdcage Coils

(10)

RF Birdcage Coils

based on the lumped element delay line (Hayes et al., 1985) widely used in MRI

(11)

Introduction Motivation Methods Experimental Results Conclusion RF coils in MRI RF birdcage coils

Design and simulation of RF birdcage coils

RF Birdcage Coils

based on the lumped element delay line (Hayes et al., 1985) widely used in MRI

(12)

RF Birdcage Coils

based on the lumped element delay line (Hayes et al., 1985) widely used in MRI

Advantages

very homogeneous RF magnetic field

(13)

Introduction Motivation Methods Experimental Results Conclusion RF coils in MRI RF birdcage coils

Design and simulation of RF birdcage coils

RF Birdcage Coils

based on the lumped element delay line (Hayes et al., 1985) widely used in MRI

Advantages

very homogeneous RF magnetic field high signal-to-noise ratio (SNR)

(14)

RF Birdcage Coils

based on the lumped element delay line (Hayes et al., 1985) widely used in MRI

Advantages

very homogeneous RF magnetic field high signal-to-noise ratio (SNR)

quadrature excitation and reception capability

(15)

Introduction Motivation Methods Experimental Results Conclusion RF coils in MRI RF birdcage coils

Design and simulation of RF birdcage coils

(16)

Birdcage Coils Consist of...

two circular end rings connected by N equally spaced rungs (or legs)

(17)

Introduction Motivation Methods Experimental Results Conclusion RF coils in MRI RF birdcage coils

Design and simulation of RF birdcage coils

Birdcage Coils Consist of...

two circular end rings connected by N equally spaced rungs (or legs)

(18)

Resonance Behavior of Birdcage Coils

A birdcage coil with N number of rungs and equal valued capacitors has

(19)

Introduction Motivation Methods Experimental Results Conclusion RF coils in MRI RF birdcage coils

Design and simulation of RF birdcage coils

Resonance Behavior of Birdcage Coils

A birdcage coil with N number of rungs and equal valued capacitors has

(20)

Resonance Behavior of Birdcage Coils

A birdcage coil with N number of rungs and equal valued capacitors has

N/2 resonant modes (m=1,2... N/2)

degenerate mode pairs - two modes with the same frequency

(21)

Introduction Motivation Methods Experimental Results Conclusion RF coils in MRI RF birdcage coils

Design and simulation of RF birdcage coils

Resonance Behavior of Birdcage Coils

A birdcage coil with N number of rungs and equal valued capacitors has

N/2 resonant modes (m=1,2... N/2)

degenerate mode pairs - two modes with the same frequency

(22)

Resonance Behavior of Birdcage Coils

A birdcage coil with N number of rungs and equal valued capacitors has

N/2 resonant modes (m=1,2... N/2)

degenerate mode pairs - two modes with the same frequency

end ring resonant mode (m=0)

currents only flow in the end rings - Helmholtz pair

(23)

Introduction Motivation Methods Experimental Results Conclusion RF coils in MRI RF birdcage coils

Design and simulation of RF birdcage coils

Which Resonant Mode is used in MRI?

most homogeneous B1field

(24)

Which Resonant Mode is used in MRI?

most homogeneous B1field

sinusoidal current distribution in the rungs for m=1 mode

Source of figure: M. Lupu, MAGMA, 2004, 17, 363-371

(25)

Introduction Motivation Methods Experimental Results Conclusion RF coils in MRI RF birdcage coils

Design and simulation of RF birdcage coils

Which Resonant Mode is used in MRI?

most homogeneous B1field

(26)

Outline

1 Introduction RF coils in MRI RF birdcage coils

Design and simulation of RF birdcage coils

2 Motivation

Review of previous studies Problem definition

Our work 3 Methods

FEM Models of Birdcage Coils Frequency Domain Analysis Eigenfrequency Analysis Software Tool

4 Experimental Results 5 Conclusion

(27)

Introduction Motivation Methods Experimental Results Conclusion RF coils in MRI RF birdcage coils

Design and simulation of RF birdcage coils

Designing a RF Birdcage Coil

In order to generate a homogeneous B1field at the desired

frequency;

use the correct capacitance value

calculate an initial capacitance value tuning and matching procedures

knowing resonant modes of the birdcage coil

(28)

Designing a RF Birdcage Coil

In order to generate a homogeneous B1field at the desired

frequency;

use the correct capacitance value

calculate an initial capacitance value tuning and matching procedures

knowing resonant modes of the birdcage coil

tuning and matching procedures can be done without interfering with the other modes

m=0 mode is used in open MRI systems

(29)

Introduction Motivation Methods Experimental Results Conclusion RF coils in MRI RF birdcage coils

Design and simulation of RF birdcage coils

Designing a RF Birdcage Coil

In order to generate a homogeneous B1field at the desired

frequency;

use the correct capacitance value

calculate an initial capacitance value tuning and matching procedures

knowing resonant modes of the birdcage coil

(30)

Designing a RF Birdcage Coil

In order to generate a homogeneous B1field at the desired

frequency;

use the correct capacitance value

calculate an initial capacitance value tuning and matching procedures

knowing resonant modes of the birdcage coil

tuning and matching procedures can be done without interfering with the other modes

m=0 mode is used in open MRI systems

(31)

Introduction Motivation Methods Experimental Results Conclusion RF coils in MRI RF birdcage coils

Design and simulation of RF birdcage coils

Designing a RF Birdcage Coil

In order to generate a homogeneous B1field at the desired

frequency;

use the correct capacitance value

calculate an initial capacitance value tuning and matching procedures

knowing resonant modes of the birdcage coil

(32)

Designing a RF Birdcage Coil

In order to generate a homogeneous B1field at the desired

frequency;

use the correct capacitance value

calculate an initial capacitance value tuning and matching procedures

knowing resonant modes of the birdcage coil

tuning and matching procedures can be done without interfering with the other modes

m=0 mode is used in open MRI systems

(33)

Introduction Motivation Methods Experimental Results Conclusion RF coils in MRI RF birdcage coils

Design and simulation of RF birdcage coils

Designing a RF Birdcage Coil

In order to generate a homogeneous B1field at the desired

frequency;

use the correct capacitance value

calculate an initial capacitance value tuning and matching procedures

knowing resonant modes of the birdcage coil

(34)

Designing a RF Birdcage Coil

In order to generate a homogeneous B1field at the desired

frequency;

use the correctcapacitance value

calculate an initial capacitance value tuning and matching procedures

knowing resonant modes of the birdcage coil

tuning and matching procedures can be done without interfering with the other modes

m=0 mode is used in open MRI systems

(35)

Introduction Motivation Methods Experimental Results Conclusion RF coils in MRI RF birdcage coils

Design and simulation of RF birdcage coils

Designing a RF Birdcage Coil

In order to generate a homogeneous B1field at the desired

frequency;

use the correctcapacitance value

calculate an initial capacitance value tuning and matching procedures

knowingresonant modesof the birdcage coil

(36)

Simulating a RF Birdcage Coil

Solving for the electromagnetic fields of a birdcage coil at the specified frequency.

B1field distribution inside the coil

specific absorption rate (SAR) at any object

variation of any electromagnetic field variables with respect to frequency

(37)

Introduction Motivation Methods Experimental Results Conclusion RF coils in MRI RF birdcage coils

Design and simulation of RF birdcage coils

Simulating a RF Birdcage Coil

Solving for the electromagnetic fields of a birdcage coil at the specified frequency.

B1field distribution inside the coil

specific absorption rate (SAR) at any object

variation of any electromagnetic field variables with respect to frequency

(38)

Simulating a RF Birdcage Coil

Solving for the electromagnetic fields of a birdcage coil at the specified frequency.

B1field distribution inside the coil

specific absorption rate (SAR) at any object

variation of any electromagnetic field variables with respect to frequency

(39)

Introduction Motivation Methods Experimental Results Conclusion RF coils in MRI RF birdcage coils

Design and simulation of RF birdcage coils

Simulating a RF Birdcage Coil

Solving for the electromagnetic fields of a birdcage coil at the specified frequency.

B1field distribution inside the coil

specific absorption rate (SAR) at any object

variation of any electromagnetic field variables with respect to frequency

(40)

Outline

1 Introduction RF coils in MRI RF birdcage coils

Design and simulation of RF birdcage coils 2 Motivation

Review of previous studies Problem definition

Our work

3 Methods

FEM Models of Birdcage Coils Frequency Domain Analysis Eigenfrequency Analysis Software Tool

4 Experimental Results 5 Conclusion

(41)

Introduction

Motivation

Methods Experimental Results Conclusion

Review of previous studies

Problem definition Our work

Outline

1 Introduction RF coils in MRI RF birdcage coils

Design and simulation of RF birdcage coils 2 Motivation

Review of previous studies

Problem definition Our work

3 Methods

FEM Models of Birdcage Coils Frequency Domain Analysis

(42)

Studies on Designing a Birdcage Coil

Tropp, 1989

analyzing low-pass birdcage resonator - using lumped circuit element model and perturbation theory

Jin, 1989

resonant modes calculation - lumped circuit element model Pascone et al., 1991

analyzing both low-pass and high-pass birdcage coil - using transmission line theory

Leifer, 1997

resonant modes calculation - using discrete Fourier transform Chin et al., 2002

capacitance calculation - lumped circuit element model

(43)

Introduction

Motivation

Methods Experimental Results Conclusion

Review of previous studies

Problem definition Our work

Studies on Designing a Birdcage Coil

Tropp, 1989

analyzing low-pass birdcage resonator - using lumped circuit element model and perturbation theory

Jin, 1989

resonant modes calculation - lumped circuit element model Pascone et al., 1991

analyzing both low-pass and high-pass birdcage coil - using transmission line theory

Leifer, 1997

(44)

Studies on Designing a Birdcage Coil

Tropp, 1989

analyzing low-pass birdcage resonator - using lumped circuit element model and perturbation theory

Jin, 1989 - MRIEM Software Tool

resonant modes calculation - lumped circuit element model Pascone et al., 1991

analyzing both low-pass and high-pass birdcage coil - using transmission line theory

Leifer, 1997

resonant modes calculation - using discrete Fourier transform Chin et al., 2002

capacitance calculation - lumped circuit element model

(45)

Introduction

Motivation

Methods Experimental Results Conclusion

Review of previous studies

Problem definition Our work

Lumped Circuit Element Model

end rings and rungs are modeled as inductors self and mutual inductances are calculated using handbook formulas

equivalent circuit model (LC network) is solved using Kirchoff’s voltage and current laws

(46)

Lumped Circuit Element Model

end rings and rungs are modeled as inductors self and mutual inductances are calculated using handbook formulas

equivalent circuit model (LC network) is solved using Kirchoff’s voltage and current laws

(47)

Introduction

Motivation

Methods Experimental Results Conclusion

Review of previous studies

Problem definition Our work

Lumped Circuit Element Model

end rings and rungs are modeled as inductors self and mutual inductances are calculated using handbook formulas

equivalent circuit model (LC network) is solved using Kirchoff’s voltage and current laws

(48)

Lumped Circuit Element Model

end rings and rungs are modeled as inductors self and mutual inductances are calculated using handbook formulas

equivalent circuit model (LC network) is solved using Kirchoff’s voltage and current laws

(49)

Introduction

Motivation

Methods Experimental Results Conclusion

Review of previous studies

Problem definition Our work

Lumped Circuit Element Model

Figure: Equivalent lumped circuit element models for low-pass

(50)

Outline

1 Introduction RF coils in MRI RF birdcage coils

Design and simulation of RF birdcage coils 2 Motivation

Review of previous studies

Problem definition

Our work 3 Methods

FEM Models of Birdcage Coils Frequency Domain Analysis Eigenfrequency Analysis Software Tool

4 Experimental Results 5 Conclusion

(51)

Introduction

Motivation

Methods Experimental Results Conclusion

Review of previous studies

Problem definition

Our work

Limitation of Lumped Circuit Element Model

There are some limitations of using lumped circuit element model

(52)

Limitation of Lumped Circuit Element Model

There are some limitations of using lumped circuit element model in the capacitance and resonant modes calculations:

heavily depends on the inductance calculations

(53)

Introduction

Motivation

Methods Experimental Results Conclusion

Review of previous studies

Problem definition

Our work

Limitation of Lumped Circuit Element Model

There are some limitations of using lumped circuit element model in the capacitance and resonant modes calculations:

(54)

Limitation of Lumped Circuit Element Model

There are some limitations of using lumped circuit element model in the capacitance and resonant modes calculations:

heavily depends on the inductance calculationswhich are

made under the quasi-static assumption

(55)

Introduction

Motivation

Methods Experimental Results Conclusion

Review of previous studies

Problem definition

Our work

Limitation of Lumped Circuit Element Model

There are some limitations of using lumped circuit element model in the capacitance and resonant modes calculations:

heavily depends on the inductance calculationswhich are

made under the quasi-static assumption

Example: L=0.002l  ln  2l B  +0.5 

(56)

Limitation of Lumped Circuit Element Model

There are some limitations of using lumped circuit element model in the capacitance and resonant modes calculations:

heavily depends on the inductance calculationswhich are

made under the quasi-static assumption

Example: L=0.002l  ln  2l B  +0.5  frequency

(57)

Introduction

Motivation

Methods Experimental Results Conclusion

Review of previous studies

Problem definition

Our work

Limitation of Lumped Circuit Element Model

There are some limitations of using lumped circuit element model in the capacitance and resonant modes calculations:

heavily depends on the inductance calculationswhich are

made under the quasi-static assumption

Example: L=0.002l  ln  2l B  +0.5 

(58)

Modelling a Transmission Line as a Lumped Circuit

Element

Deutsch et al., 1997

There is an important criterion

(59)

Introduction

Motivation

Methods Experimental Results Conclusion

Review of previous studies

Problem definition

Our work

Modelling a Transmission Line as a Lumped Circuit

Element

Deutsch et al., 1997

There is an important criterion - used for determining whether a

(60)

-Modelling a Transmission Line as a Lumped Circuit

Element

Deutsch et al., 1997

There is an important criterion - used for determining whether a

wire can be modeled as lumped circuit element or not -which is given as

(61)

Introduction

Motivation

Methods Experimental Results Conclusion

Review of previous studies

Problem definition

Our work

Modelling a Transmission Line as a Lumped Circuit

Element

Deutsch et al., 1997

There is an important criterion - used for determining whether a

wire can be modeled as lumped circuit element or not -which is given as

length of wire≤ λ

(62)

Outline

1 Introduction RF coils in MRI RF birdcage coils

Design and simulation of RF birdcage coils 2 Motivation

Review of previous studies Problem definition

Our work

3 Methods

FEM Models of Birdcage Coils Frequency Domain Analysis Eigenfrequency Analysis Software Tool

4 Experimental Results 5 Conclusion

(63)

Introduction

Motivation

Methods Experimental Results Conclusion

Review of previous studies Problem definition

Our work

(64)

What Have We Done in this Study?

We have first developed FEM models of low-pass and

high-pass birdcage coils in COMSOL Multiphysics.

(65)

Introduction

Motivation

Methods Experimental Results Conclusion

Review of previous studies Problem definition

Our work

What Have We Done in this Study?

We have first developed FEM models of low-pass and

high-pass birdcage coils in COMSOL Multiphysics.

(66)

What Have We Done in this Study?

We have first developed FEM models of low-pass and

high-pass birdcage coils in COMSOL Multiphysics.

Using these models;

Two FEM based simulation methods

(67)

Introduction

Motivation

Methods Experimental Results Conclusion

Review of previous studies Problem definition

Our work

What Have We Done in this Study?

We have first developed FEM models of low-pass and

high-pass birdcage coils in COMSOL Multiphysics.

Using these models;

Two FEM based simulation methods

(68)

What Have We Done in this Study?

We have first developed FEM models of low-pass and

high-pass birdcage coils in COMSOL Multiphysics.

Using these models;

Two FEM based simulation methods

Frequency Domain Analysis Eigenfrequency Analysis

(69)

Introduction

Motivation

Methods Experimental Results Conclusion

Review of previous studies Problem definition

Our work

What Have We Done in this Study?

We have first developed FEM models of low-pass and

high-pass birdcage coils in COMSOL Multiphysics.

Using these models;

Two FEM based simulation methods

Frequency Domain Analysis Eigenfrequency Analysis

(70)

What Have We Done in this Study?

We have first developed FEM models of low-pass and

high-pass birdcage coils in COMSOL Multiphysics.

Using these models;

Two FEM based simulation methods

Frequency Domain Analysis Eigenfrequency Analysis

Software Tool

FEM-FDA-EFAT

(71)

Introduction

Motivation

Methods Experimental Results Conclusion

Review of previous studies Problem definition

Our work

What Have We Done in this Study?

We have first developed FEM models of low-pass and

high-pass birdcage coils in COMSOL Multiphysics.

Using these models;

Two FEM based simulation methods

Frequency Domain Analysis Eigenfrequency Analysis

Software Tool

(72)

Outline

1 Introduction RF coils in MRI RF birdcage coils

Design and simulation of RF birdcage coils 2 Motivation

Review of previous studies Problem definition

Our work 3 Methods

FEM Models of Birdcage Coils Frequency Domain Analysis Eigenfrequency Analysis Software Tool

4 Experimental Results 5 Conclusion

(73)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils

Frequency Domain Analysis Eigenfrequency Analysis Software Tool

Outline

1 Introduction RF coils in MRI RF birdcage coils

Design and simulation of RF birdcage coils 2 Motivation

Review of previous studies Problem definition

Our work 3 Methods

FEM Models of Birdcage Coils

(74)

Geometry

(75)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils

Frequency Domain Analysis Eigenfrequency Analysis Software Tool

Geometry

low-pass and high-pass birdcage coils are geometrically modeled in the simulation environment

(76)

Geometry

low-pass and high-pass birdcage coils are geometrically modeled in the simulation environment

(77)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils

Frequency Domain Analysis Eigenfrequency Analysis Software Tool

(78)

Adding Physics

Radio Frequency Branch→Electromagnetic Waves

Interface

(79)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils

Frequency Domain Analysis Eigenfrequency Analysis Software Tool

Adding Physics

Radio Frequency Branch→Electromagnetic Waves

Interface

solves the electromagnetic wave equation for the time harmonic and eigenfrequency problem

(80)

Adding Physics

Radio Frequency Branch→Electromagnetic Waves

Interface

solves the electromagnetic wave equation for the time harmonic and eigenfrequency problem

∇ × µ−1 r (∇ ×E) −k02  ǫrjσ ωǫ0  E=0

(81)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils

Frequency Domain Analysis Eigenfrequency Analysis Software Tool

(82)

Boundary Conditions

boundaries of rungs, end rings, capacitor plates and RF

shield are assigned toPerfect Electric Conductor (PEC)

(83)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils

Frequency Domain Analysis Eigenfrequency Analysis Software Tool

Boundary Conditions

boundaries of rungs, end rings, capacitor plates and RF

shield are assigned toPerfect Electric Conductor (PEC)

(84)

Boundary Conditions

boundaries of rungs, end rings, capacitor plates and RF

shield are assigned toPerfect Electric Conductor (PEC)

n×E=0

(85)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils

Frequency Domain Analysis Eigenfrequency Analysis Software Tool

(86)

Boundary Conditions

we need to prevent reflections from the outer boundary of the solution domain

(87)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils

Frequency Domain Analysis Eigenfrequency Analysis Software Tool

Boundary Conditions

we need to prevent reflections from the outer boundary of the solution domain

(88)

Boundary Conditions

we need to prevent reflections from the outer boundary of the solution domain

scattering boundary condition→for boundaries

perfectly matched layer→for domain

(89)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils

Frequency Domain Analysis Eigenfrequency Analysis Software Tool

Boundary Conditions

we need to prevent reflections from the outer boundary of the solution domain

scattering boundary condition→for boundaries

(90)

Boundary Conditions

(91)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils

Frequency Domain Analysis Eigenfrequency Analysis Software Tool

Boundary Conditions

In frequency domain analysis,lumped port boundary

conditionis used for voltage excitation (Zport = Vport

(92)

Boundary Conditions

In frequency domain analysis,lumped port boundary

conditionis used for voltage excitation (Zport = Vport

Iport )

(93)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils

Frequency Domain Analysis Eigenfrequency Analysis Software Tool

Boundary Conditions

In frequency domain analysis,lumped port boundary

conditionis used for voltage excitation (Zport = Vport

(94)

Mesh

(95)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils

Frequency Domain Analysis Eigenfrequency Analysis Software Tool

Mesh

(96)

Mesh

(Element Size) << λ5

(97)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils

Frequency Domain Analysis

Eigenfrequency Analysis Software Tool

Outline

1 Introduction RF coils in MRI RF birdcage coils

Design and simulation of RF birdcage coils 2 Motivation

Review of previous studies Problem definition

Our work 3 Methods

FEM Models of Birdcage Coils

(98)

Simulation of a Birdcage Coil

(99)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils

Frequency Domain Analysis

Eigenfrequency Analysis Software Tool

Simulation of a Birdcage Coil

(100)

Simulation of a Birdcage Coil

solves for the electromagnetic fields in the solution domain at the desired frequency (or frequencies)

(101)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils

Frequency Domain Analysis

Eigenfrequency Analysis Software Tool

Simulation of a Birdcage Coil

solves for the electromagnetic fields in the solution domain at the desired frequency (or frequencies)

(102)

Simulation of a Birdcage Coil

solves for the electromagnetic fields in the solution domain at the desired frequency (or frequencies)

for the specified capacitance value

In Frequency Domain Analysis;

(103)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils

Frequency Domain Analysis

Eigenfrequency Analysis Software Tool

Simulation of a Birdcage Coil

solves for the electromagnetic fields in the solution domain at the desired frequency (or frequencies)

for the specified capacitance value

In Frequency Domain Analysis;

(104)

Simulation of a Birdcage Coil

solves for the electromagnetic fields in the solution domain at the desired frequency (or frequencies)

for the specified capacitance value

In Frequency Domain Analysis;

loaded (or unloaded) birdcage coils shielded (or unshielded) birdcage coils

(105)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils

Frequency Domain Analysis

Eigenfrequency Analysis Software Tool

Simulation of a Birdcage Coil

solves for the electromagnetic fields in the solution domain at the desired frequency (or frequencies)

for the specified capacitance value

In Frequency Domain Analysis;

loaded (or unloaded) birdcage coils shielded (or unshielded) birdcage coils

(106)

Simulation Results

(107)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils

Frequency Domain Analysis

Eigenfrequency Analysis Software Tool

Simulation Results

three different scenarios;

(108)

Simulation Results

three different scenarios;

unloaded and unshielded 8-leg low-pass birdcage coil

(109)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils

Frequency Domain Analysis

Eigenfrequency Analysis Software Tool

Simulation Results

three different scenarios;

unloaded and unshielded 8-leg low-pass birdcage coil unloaded and shielded 8-leg low-pass birdcage coil

(110)

Simulation Results

three different scenarios;

unloaded and unshielded 8-leg low-pass birdcage coil unloaded and shielded 8-leg low-pass birdcage coil loaded and shielded 16-leg high-pass birdcage coil

(111)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils

Frequency Domain Analysis

Eigenfrequency Analysis Software Tool

Simulation Results

three different scenarios;

unloaded and unshielded 8-leg low-pass birdcage coil unloaded and shielded 8-leg low-pass birdcage coil loaded and shielded 16-leg high-pass birdcage coil

(112)

Simulation Results

three different scenarios;

unloaded and unshielded 8-leg low-pass birdcage coil unloaded and shielded 8-leg low-pass birdcage coil loaded and shielded 16-leg high-pass birdcage coil

electromagnetic field distributions

H+ and H

(113)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils

Frequency Domain Analysis

Eigenfrequency Analysis Software Tool

Simulation Results

three different scenarios;

unloaded and unshielded 8-leg low-pass birdcage coil unloaded and shielded 8-leg low-pass birdcage coil loaded and shielded 16-leg high-pass birdcage coil

electromagnetic field distributions

H+ and H

(114)

Simulation Results

three different scenarios;

unloaded and unshielded 8-leg low-pass birdcage coil unloaded and shielded 8-leg low-pass birdcage coil loaded and shielded 16-leg high-pass birdcage coil

electromagnetic field distributions

H+ and H H+ = Hx +iHy 2 H= (HxiHy) ∗ 2 E-field

(115)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils

Frequency Domain Analysis

Eigenfrequency Analysis Software Tool

Simulation Results - 1

st

Scenario

(116)

Simulation Results - 1

st

Scenario

Unloaded and Unshielded 8-leg Low-pass BC

H+

and Hfor linear excitation

(117)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils

Frequency Domain Analysis

Eigenfrequency Analysis Software Tool

Simulation Results - 1

st

Scenario

Unloaded and Unshielded 8-leg Low-pass BC

H+and H

(118)

Simulation Results - 1

st

Scenario

Unloaded and Unshielded 8-leg Low-pass BC

H+

and Hfor quadrature excitation

(119)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils

Frequency Domain Analysis

Eigenfrequency Analysis Software Tool

Simulation Results - 1

st

Scenario

Unloaded and Unshielded 8-leg Low-pass BC

H+and H

(120)

Simulation Results - 1

st

Scenario

Unloaded and Unshielded 8-leg Low-pass BC

Electric field→for linear and quadrature excitation

(121)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils

Frequency Domain Analysis

Eigenfrequency Analysis Software Tool

Simulation Results - 1

st

Scenario

Unloaded and Unshielded 8-leg Low-pass BC

(122)

Simulation Results - 1

st

Scenario

Unloaded and Unshielded 8-leg Low-pass BC

H+uniformityfor quadrature excitation

(123)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils

Frequency Domain Analysis

Eigenfrequency Analysis Software Tool

Simulation Results - 1

st

Scenario

Unloaded and Unshielded 8-leg Low-pass BC

H+uniformity

(124)

Simulation Results - 2

nd

Scenario

Unloaded and Shielded 8-leg Low-pass BC

(125)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils

Frequency Domain Analysis

Eigenfrequency Analysis Software Tool

Simulation Results - 2

nd

Scenario

Unloaded and Shielded 8-leg Low-pass BC

H+

(126)

Simulation Results - 2

nd

Scenario

Unloaded and Shielded 8-leg Low-pass BC

H+uniformity

→for quadrature excitation

(127)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils

Frequency Domain Analysis

Eigenfrequency Analysis Software Tool

Simulation Results - 3

rd

Scenario

(128)

Simulation Results - 3

rd

Scenario

Loaded and Shielded 16-leg High-pass BC

Geometric model

(129)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils

Frequency Domain Analysis

Eigenfrequency Analysis Software Tool

Simulation Results - 3

rd

Scenario

Loaded and Shielded 16-leg High-pass BC

H+

(130)

Simulation Results - 3

rd

Scenario

Loaded and Shielded 16-leg High-pass BC

H+ for unloaded and loaded case (quadrature excitation)

(131)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils

Frequency Domain Analysis

Eigenfrequency Analysis Software Tool

Simulation Results - 3

rd

Scenario

Loaded and Shielded 16-leg High-pass BC

(132)

Simulation Results - 3

rd

Scenario

Loaded and Shielded 16-leg High-pass BC

Hfor unloaded and loaded case (quadrature excitation)

(133)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils

Frequency Domain Analysis

Eigenfrequency Analysis Software Tool

Simulation Results - 3

rd

Scenario

Loaded and Shielded 16-leg High-pass BC

(134)

Simulation Results - 3

rd

Scenario

Loaded and Shielded 16-leg High-pass BC

SAR distribution of an object

SAR= σ|E|

2

ρ σ: conductivity,ρ: density

(135)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils

Frequency Domain Analysis

Eigenfrequency Analysis Software Tool

Simulation Results - 3

rd

Scenario

Loaded and Shielded 16-leg High-pass BC

SAR distribution of an object

SAR= σ|E|

2

ρ σ: conductivity,ρ: density

(136)

Simulation Results - 3

rd

Scenario

Loaded and Shielded 16-leg High-pass BC

Normalized SAR distribution→for quadrature excitation

(137)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils Frequency Domain Analysis

Eigenfrequency Analysis Software Tool

Outline

1 Introduction RF coils in MRI RF birdcage coils

Design and simulation of RF birdcage coils 2 Motivation

Review of previous studies Problem definition

Our work 3 Methods

FEM Models of Birdcage Coils Frequency Domain Analysis

(138)

Resonant Mode Analysis of a Birdcage Coil

(139)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils Frequency Domain Analysis

Eigenfrequency Analysis

Software Tool

Resonant Mode Analysis of a Birdcage Coil

(140)

Resonant Mode Analysis of a Birdcage Coil

calculates the resonant modes of the birdcage coil and the

electromagnetic field distributions at these resonant modes

(141)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils Frequency Domain Analysis

Eigenfrequency Analysis

Software Tool

Resonant Mode Analysis of a Birdcage Coil

calculates the resonant modes of the birdcage coil and the

electromagnetic field distributions at these resonant modesfor the given capacitance value

(142)

Eigenfrequency Analysis in COMSOL Multiphysics

(143)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils Frequency Domain Analysis

Eigenfrequency Analysis

Software Tool

Eigenfrequency Analysis in COMSOL Multiphysics

(144)

Eigenfrequency Analysis in COMSOL Multiphysics

use developed FEM models of birdcage coils add eigenfrequency study

(145)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils Frequency Domain Analysis

Eigenfrequency Analysis

Software Tool

Eigenfrequency Analysis in COMSOL Multiphysics

use developed FEM models of birdcage coils add eigenfrequency study

(146)

Eigenfrequency Analysis in COMSOL Multiphysics

use developed FEM models of birdcage coils add eigenfrequency study

specify number of eigenfrequencies specify a frequency point

add eigenvalue solver

(147)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils Frequency Domain Analysis

Eigenfrequency Analysis

Software Tool

Eigenfrequency Analysis in COMSOL Multiphysics

use developed FEM models of birdcage coils add eigenfrequency study

specify number of eigenfrequencies specify a frequency point

add eigenvalue solver

(148)

Simulation Results

(149)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils Frequency Domain Analysis

Eigenfrequency Analysis

Software Tool

Simulation Results

(150)

Simulation Results

two different scenarios;

unloaded and unshielded 8-leg low-pass birdcage coil

(151)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils Frequency Domain Analysis

Eigenfrequency Analysis

Software Tool

Simulation Results

two different scenarios;

unloaded and unshielded 8-leg low-pass birdcage coil unloaded and shielded 16-leg high-pass birdcage coil

(152)

Simulation Results

two different scenarios;

unloaded and unshielded 8-leg low-pass birdcage coil unloaded and shielded 16-leg high-pass birdcage coil

observed electromagnetic variables

(153)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils Frequency Domain Analysis

Eigenfrequency Analysis

Software Tool

Simulation Results

two different scenarios;

unloaded and unshielded 8-leg low-pass birdcage coil unloaded and shielded 16-leg high-pass birdcage coil

observed electromagnetic variables

(154)

Simulation Results

two different scenarios;

unloaded and unshielded 8-leg low-pass birdcage coil unloaded and shielded 16-leg high-pass birdcage coil

observed electromagnetic variables

H+ at these resonant modes

surface current density

(155)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils Frequency Domain Analysis

Eigenfrequency Analysis

Software Tool

Simulation Results - 1

st

Scenario

(156)

Simulation Results - 1

st

Scenario

Unloaded and Unshielded 8-leg Low-pass BC

H+

→for all resonant modes

(157)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils Frequency Domain Analysis

Eigenfrequency Analysis

Software Tool

Simulation Results - 1

st

Scenario

(158)

Simulation Results - 2

nd

Scenario

Unloaded and shielded 16-leg High-pass BC

(159)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils Frequency Domain Analysis

Eigenfrequency Analysis

Software Tool

Simulation Results - 2

nd

Scenario

Unloaded and shielded 16-leg High-pass BC

H+and surface current densities

(160)

Simulation Results - 2

nd

Scenario

Unloaded and shielded 16-leg High-pass BC

H+and surface current densities

→for m=0 mode

(161)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils Frequency Domain Analysis Eigenfrequency Analysis Software Tool

Outline

1 Introduction RF coils in MRI RF birdcage coils

Design and simulation of RF birdcage coils 2 Motivation

Review of previous studies Problem definition

Our work 3 Methods

FEM Models of Birdcage Coils Frequency Domain Analysis

(162)

Software Tool for Designing and Simulating a Birdcage

Coil

(163)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils Frequency Domain Analysis Eigenfrequency Analysis

Software Tool

Software Tool for Designing and Simulating a Birdcage

Coil

(164)

Software Tool for Designing and Simulating a Birdcage

Coil

PURPOSE:

To provide convenience for the coil designers and the researchers in the field of MRI

(165)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils Frequency Domain Analysis Eigenfrequency Analysis

Software Tool

Software Tool for Designing and Simulating a Birdcage

Coil

PURPOSE:

To provide convenience for the coil designers and the

researchers in the field of MRIto use the proposed

simulation methods easily and according to the parameters they specify

(166)

Software Tool for Designing and Simulating a Birdcage

Coil

PURPOSE:

To provide convenience for the coil designers and the

researchers in the field of MRIto use the proposed

simulation methods easily and according to the parameters they specify

developed software tool

(167)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils Frequency Domain Analysis Eigenfrequency Analysis

Software Tool

Software Tool for Designing and Simulating a Birdcage

Coil

PURPOSE:

To provide convenience for the coil designers and the

researchers in the field of MRIto use the proposed

simulation methods easily and according to the parameters they specify

(168)

Properties of the sofware tool

(169)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils Frequency Domain Analysis Eigenfrequency Analysis

Software Tool

Properties of the sofware tool

developed in MATLAB

(170)

Properties of the sofware tool

developed in MATLAB

has graphical-user-interface (GUI)

(171)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils Frequency Domain Analysis Eigenfrequency Analysis

Software Tool

Properties of the sofware tool

developed in MATLAB

has graphical-user-interface (GUI)

makes all design and simulation steps according to the user-specified parameters by connecting to the COMSOL Multiphysics server

(172)

Properties of the sofware tool

developed in MATLAB

has graphical-user-interface (GUI)

makes all design and simulation steps according to the user-specified parameters by connecting to the COMSOL Multiphysics server

modeling the coil geometry

(173)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils Frequency Domain Analysis Eigenfrequency Analysis

Software Tool

Properties of the sofware tool

developed in MATLAB

has graphical-user-interface (GUI)

makes all design and simulation steps according to the user-specified parameters by connecting to the COMSOL Multiphysics server

modeling the coil geometry

(174)

Properties of the sofware tool

developed in MATLAB

has graphical-user-interface (GUI)

makes all design and simulation steps according to the user-specified parameters by connecting to the COMSOL Multiphysics server

modeling the coil geometry

adding physics and boundary condition generating mesh for the model

(175)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils Frequency Domain Analysis Eigenfrequency Analysis

Software Tool

Properties of the sofware tool

developed in MATLAB

has graphical-user-interface (GUI)

makes all design and simulation steps according to the user-specified parameters by connecting to the COMSOL Multiphysics server

modeling the coil geometry

adding physics and boundary condition generating mesh for the model

(176)

Properties of the sofware tool

developed in MATLAB

has graphical-user-interface (GUI)

makes all design and simulation steps according to the user-specified parameters by connecting to the COMSOL Multiphysics server

modeling the coil geometry

adding physics and boundary condition generating mesh for the model

adding study and solver sequence computing the solutions

(177)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils Frequency Domain Analysis Eigenfrequency Analysis

Software Tool

Properties of the sofware tool

developed in MATLAB

has graphical-user-interface (GUI)

makes all design and simulation steps according to the user-specified parameters by connecting to the COMSOL Multiphysics server

modeling the coil geometry

adding physics and boundary condition generating mesh for the model

adding study and solver sequence computing the solutions

(178)

FEM-FDA-EFAT

(179)

Introduction Motivation

Methods

Experimental Results Conclusion

FEM Models of Birdcage Coils Frequency Domain Analysis Eigenfrequency Analysis

Software Tool

(180)

Outline

1 Introduction RF coils in MRI RF birdcage coils

Design and simulation of RF birdcage coils 2 Motivation

Review of previous studies Problem definition

Our work 3 Methods

FEM Models of Birdcage Coils Frequency Domain Analysis Eigenfrequency Analysis Software Tool

4 Experimental Results 5 Conclusion

(181)

Introduction Motivation Methods

Experimental Results

Conclusion

(182)

Handmade Low-pass Birdcage Coil

8-leg low-pass birdcage coil is constructed on plexiglass tube

(183)

Introduction Motivation Methods

Experimental Results

Conclusion

(184)

Experimental Results and Comparison with Numerical

Analyses

for the resonant modes

(185)

Introduction Motivation Methods

Experimental Results

Conclusion

Experimental Results and Comparison with Numerical

Analyses

(186)

Experimental Results and Comparison with Numerical

Analyses

for the resonant modes

S11 of the coil for five different capacitance values

(187)

Introduction Motivation Methods

Experimental Results

Conclusion

Experimental Results and Comparison with Numerical

Analyses

for the resonant modes

S11 of the coil for five different capacitance values

(188)

Experimental Results and Comparison with Numerical

Analyses

for the resonant modes

S11 of the coil for five different capacitance values

compare the measured resonant modes

Jin’s software tool,MRIEM

(189)

Introduction Motivation Methods

Experimental Results

Conclusion

Experimental Results and Comparison with Numerical

Analyses

for the resonant modes

S11 of the coil for five different capacitance values

compare the measured resonant modes

Jin’s software tool,MRIEM Our software tool,FEM-EFAT

(190)

Experimental Results and Comparison with Numerical

Analyses

(191)

Introduction Motivation Methods

Experimental Results

Conclusion

Experimental Results and Comparison with Numerical

Analyses

(192)

Measured and Calculated Resonant Modes

Results for Low-pass Birdcage Coil

(193)

Introduction Motivation Methods

Experimental Results

Conclusion

Measured and Calculated Resonant Modes

Results for Low-pass Birdcage Coil

used capacitance values

(194)

Measured and Calculated Resonant Modes

Results for Low-pass Birdcage Coil

Results for 47pF

Modes Measured (MHz) MRIEM (MHz) FEM-EFAT (MHz)

m=1 60.75 67.46 59.1

m=2 85.88 90.64 87.22

m=3 93.38 102.2 101.1

m=4 102.8 - 105.4

(195)

Introduction Motivation Methods

Experimental Results

Conclusion

Measured and Calculated Resonant Modes

Results for Low-pass Birdcage Coil

Results for 10pF

Modes Measured (MHz) MRIEM (MHz) FEM-EFAT (MHz)

m=1 122.11 146.25 124.76

m=2 196.48 196.51 184.80

m=3 208.54 221.57 214.41

(196)

Measured and Calculated Resonant Modes

Results for Low-pass Birdcage Coil

Results for 3.3pF

Modes Measured (MHz) MRIEM (MHz) FEM-EFAT (MHz)

m=1 211.3 254.59 205.37

m=2 306.3 342.08 306.62

m=3 330.0 385.71 356.47

m=4 345.0 - 371.75

(197)

Introduction Motivation Methods

Experimental Results

Conclusion

Measured and Calculated Resonant Modes

Results for Low-pass Birdcage Coil

Results for 1.8pF

Modes Measured (MHz) MRIEM (MHz) FEM-EFAT (MHz)

m=1 255.2 344.71 260.62

m=2 382.0 463.19 392.18

m=3 417.0 522.26 456.8

(198)

Measured and Calculated Resonant Modes

Results for Low-pass Birdcage Coil

Results for 1pF

Modes Measured (MHz) MRIEM (MHz) FEM-EFAT (MHz)

m=1 335.7 462.48 316.85

m=2 473.1 621.42 481.6

m=3 512.3 700.68 562.24

m=4 525.9 - 586.63

(199)

Introduction Motivation Methods

Experimental Results

Conclusion

Measured and Calculated Resonant Modes

Results for Low-pass Birdcage Coil

Percentage error Error rate(%) =100× fmeasfcalc fmeas

(200)

Measured and Calculated Resonant Modes

Results for Low-pass Birdcage Coil

Percentage error rate for FEM-EFAT and MRIEM

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