Outlines: (June 11, 1996) Instructor:

Similar documents
NMR and MRI : an introduction

EL-GY 6813/BE-GY 6203 Medical Imaging, Fall 2016 Final Exam

The NMR Inverse Imaging Problem

M R I Physics Course. Jerry Allison Ph.D., Chris Wright B.S., Tom Lavin B.S., Nathan Yanasak Ph.D. Department of Radiology Medical College of Georgia

Introduction to MRI. Spin & Magnetic Moments. Relaxation (T1, T2) Spin Echoes. 2DFT Imaging. K-space & Spatial Resolution.

MRI Physics II: Gradients, Imaging. Douglas C. Noll, Ph.D. Dept. of Biomedical Engineering University of Michigan, Ann Arbor

NMR/MRI examination (8N080 / 3F240)

Introduction to MRI Acquisition

Contrast Mechanisms in MRI. Michael Jay Schillaci

MRI Physics I: Spins, Excitation, Relaxation

On Signal to Noise Ratio Tradeoffs in fmri

Magnetic Resonance Imaging. Pål Erik Goa Associate Professor in Medical Imaging Dept. of Physics

Introduction to Biomedical Imaging

Principles of MRI. Vinyl Record. Last time: Today: Homework Due tonight! EE225E / BIO265. Transforms a temporal signal to a spatial signal

K-space. Spin-Warp Pulse Sequence. At each point in time, the received signal is the Fourier transform of the object s(t) = M( k x

Basic MRI physics and Functional MRI

Introductory MRI Physics

Magnetic resonance imaging MRI

Spatial encoding in Magnetic Resonance Imaging. Jean-Marie BONNY

Spatial encoding in Magnetic Resonance Imaging. Jean-Marie BONNY

7.3.A. The expression for signal recovery is similar to that derived under exercise 7.2 and is given by:

EE225E/BIOE265 Spring 2013 Principles of MRI. Assignment 9 Solutions. Due April 29th, 2013

Fundamental MRI Principles Module Two

MRI in Review: Simple Steps to Cutting Edge Part I

Part III: Sequences and Contrast

Fundamentals of MR Imaging

Apodization. Gibbs Artifact. Bioengineering 280A Principles of Biomedical Imaging. Fall Quarter 2013 MRI Lecture 5. rect(k x )

Rochester Institute of Technology Rochester, New York. COLLEGE of Science Department of Chemistry. NEW (or REVISED) COURSE:

Introduction to the Physics of NMR, MRI, BOLD fmri

The Basics of Magnetic Resonance Imaging

SSSC Discovery Series NMR2 Multidimensional NMR Spectroscopy

Fundamental MRI Principles Module 2 N. Nuclear Magnetic Resonance. X-ray. MRI Hydrogen Protons. Page 1. Electrons

Field trip: Tuesday, Feb 5th

BASIC MRI PHYSICS SPIN GYMNASTICS Don Plewes PhD, Walter Kucharczyk MD

Chapter 14:Physics of Magnetic Resonance

Tissue Characteristics Module Three

Nuclear Magnetic Resonance Imaging

BME I5000: Biomedical Imaging

RADIOLOGIV TECHNOLOGY 4912 COMPREHENSEIVE REVIEW/MRI WORSHEET #1- PATIENT CARE AND SAFETY/PHYSICAL PRINCIPLES

Spin Echo Imaging Sequence

Introduction to Magnetic Resonance Imaging (MRI) Pietro Gori

MRS: IN VIVO SPECTROSCOPIC IMAGING MAIN POINTS

Cambridge University Press MRI from A to Z: A Definitive Guide for Medical Professionals Gary Liney Excerpt More information

MRI in Practice. Catherine Westbrook MSc, DCRR, CTC Senior Lecturer Anglia Polytechnic University Cambridge UK. John Talbot MSc, DCRR

Basic p rinciples COPYRIGHTED MATERIAL. Introduction. Atomic s tructure

Relaxation times in nuclear magnetic resonance

BMB 601 MRI. Ari Borthakur, PhD. Assistant Professor, Department of Radiology Associate Director, Center for Magnetic Resonance & Optical Imaging

BNG/ECE 487 FINAL (W16)

Principles of Magnetic Resonance Imaging

Sketch of the MRI Device

Physics of MR Image Acquisition

Magnetic Resonance Imaging

ROCHESTER INSTITUTE OF TECHNOLOGY COURSE OUTLINE FORM COLLEGE OF SCIENCE. Chester F. Carlson Center for Imaging Science

The physics US and MRI. Prof. Peter Bogner

Basic Pulse Sequences II - Spin Echoes. TE=12ms TE=47ms TE=106ms TE=153ms UCLA. Radiology

Chapter 1 Introduction

Diffusion Tensor Imaging (DTI): An overview of key concepts

Basis of MRI Contrast

Nuclear Magnetic Resonance Imaging

FREQUENCY SELECTIVE EXCITATION

The physics of medical imaging US, CT, MRI. Prof. Peter Bogner

Medical Imaging Physics Spring Quarter Week 9-1

Technical University of Denmark

MRI at a Glance. Blackwell Science CATHERINE WESTBROOK. MSC DCRR CTC Director of Training and Education Lodestone Patient Care Ltd

Low Field MRI of Laser Polarized Noble Gases. Yuan Zheng, 4 th year seminar, Feb, 2013

Lab 2: Magnetic Resonance Imaging

Suppression of Static Magnetic Field in Diffusion Measurements of Heterogeneous Materials

Protein NMR. Part III. (let s start by reviewing some of the things we have learned already)

Quantitative Susceptibility Mapping and Susceptibility Tensor Imaging. Magnetization and Susceptibility

G Medical Imaging. Outline 4/13/2012. Physics of Magnetic Resonance Imaging

HST.583 Functional Magnetic Resonance Imaging: Data Acquisition and Analysis Fall 2008

2.1.1 A Brief History of NMR The conception of NMR sprouted after the Pauli s prediction of nuclear spin in

Rad Tech 4912 MRI Registry Review. Outline of the Registry Exam: Certification Fees

Principles of Nuclear Magnetic Resonance Microscopy

Technical University of Denmark

MR Advance Techniques. Flow Phenomena. Class I

EE225E/BIOE265 Spring 2016 Principles of MRI. Assignment 4. Due Friday Feb 19st, 2016, Self Grading Due Monday Feb 22nd, 2016

Background II. Signal-to-Noise Ratio (SNR) Pulse Sequences Sampling and Trajectories Parallel Imaging. B.Hargreaves - RAD 229.

NMR Spectroscopy: A Quantum Phenomena

Magnetic Resonance Imaging (MRI)

Lecture 12 February 11, 2016

NMR, the vector model and the relaxation

Midterm Review. EE369B Concepts Simulations with Bloch Matrices, EPG Gradient-Echo Methods. B.Hargreaves - RAD 229

Chapter 24 MRA and Flow quantification. Yongquan Ye, Ph.D. Assist. Prof. Radiology, SOM Wayne State University

Exam 8N080 - Introduction to MRI

10.4 Continuous Wave NMR Instrumentation

Basic Pulse Sequences I Saturation & Inversion Recovery UCLA. Radiology

NMR course at the FMP: NMR of organic compounds and small biomolecules - II -

Introduction to functional MRI in humans. Michael Hallquist University of Pittsburgh

RAD229: Midterm Exam 2015/2016 October 19, Minutes. Please do not proceed to the next page until the exam begins.

Navigator Echoes. BioE 594 Advanced Topics in MRI Mauli. M. Modi. BioE /18/ What are Navigator Echoes?

Biomedical Imaging Magnetic Resonance Imaging

Lecture #7 In Vivo Water

22.56J Noninvasive Imaging in Biology and Medicine Instructor: Prof. Alan Jasanoff Fall 2005, TTh 1-2:30

Me myself and MRI: adventures in not understanding nuclear physics.

Magnetization Gradients, k-space and Molecular Diffusion. Magnetic field gradients, magnetization gratings and k-space

Magnetic Resonance Imaging in a Nutshell

Introduction to Magnetic Resonance Imaging

Bioengineering 278" Magnetic Resonance Imaging" Winter 2010" Lecture 1! Topics:! Review of NMR basics! Hardware Overview! Quadrature Detection!

Physics and Brain Imaging

Transcription:

Magnetic Resonance Imaging (June 11, 1996) Instructor: Tai-huang Huang Institute of Biomedical Sciences Academia Sinica Tel. (02) 2652-3036; Fax. (02) 2788-7641 E. mail: bmthh@ibms.sinica.edu.tw Reference: 1. Stark, D.D. and Bradley, W.G. eds. (1996) Magnetic Resonance Imaging 2 nd ed. Mosby Year Book. 2. Edelman, R.R. and Hesselink, J.R. eds. (1990) Clinical Magnetic Resonance Imaging Saunders Co. 3. Ernst, E.R., Bodenhausen, G. and Wokaun, A. (1987) Clarendon Press, Oxford. Principles of Nuclear Magnetic Resonance in One and Two Dimensions Outlines: I. Principles on Nuclear Magnetic Resonance Imaging (MRI): a. Basic NMR Theory: Larmor Equation, Chemical shift, Relaxation phenomenon. b. Basic Theory of Magnetic Resonance Imaging: Effect of magnetic gradient field, Slice selection, 2D Spin-warp imaging method, phase encoding, frequency encoding, Nyquist theorem, sensitivity, artifacts, fast imaging, angiography, chemical shift imaging. II. MRI Instrumentation Magnet, Gradient system, RF system, RF coil and Computer system. III. Applications

I. 2. Imaging Methods: a. Spatial Localization of the MR Signal In a homogeneous field, the spatial information is lost unless one can collimate the RF-Field as one can with light, but this is not possible. Image: Detection of magnetization (proton, water) as a function of x,y and z. M(x.y.z) b. Effect of magnetic field gradient: v B(x) = B 0 + G( x, y, z) R( x, y, z) f(x,y,z) = rb 0 + r ( G R) v v v (still a Larmor equation) The spatial information is stored in the frequency Intensity at certain frequency is correlated to the proton density at a particular spatial location Multidimensional NMR spectrum differs from real proton image only by a constant scalar fator

Proton Density: The number of MR visible protons in a unit volume of tissue ( ). is expressed as a percentage of the proton density of water. Vary very little among various tissues. MRI is a versatile, multi-parameter technique. Different nuclei (Primarily proton, in fact water). Different chemical shift (Chemical shift imaging).

T 1 and T 2 depends on: (1) Molecular motion (correlation time 2) (2) Magnetic field strength (3) Type of nucleus T 1 : Decay alone Z-axis. The time it takes to relax back to Z-axis after perturbation. T 2 : The time it takes to lose phase coherence on X-Y plane. The time it takes to lose signal on detection. (Magnetization recovers faster for shorted T 1 sample) (Magnetization Losses faster for shorter T 2 sample)

What will happen if we vary T r or T D? T R : Pulse repetition time. T d : Time between end of the pulse and the start of detection.

The shorter the TR, the smaller the signal At fixed TR, area with shorter T1 will have stronger signal (T1 weighted Image) The Longer the Td, the weaker the signal At fixed Td, area with shorted T2 will have weaker signal (T2-weighted)

Different imaging modality.

c. Spin-Warp Imaging Methods (i) (ii) (iii) Slice selection: one gradient is applied with the RF pulse to choose a slice (Z-direction) Frequency encoding: a second gradient is applied during detection period to locate the MR signal along one in-lane dimension. (x-direction) Phase encoding: A third gradient is applied at fixed strength (or duration) between the slice selection and detection period to locate the other in-plane dimension. The strength (or duration) or the third gradient increases at constant amount for a total of N repetitive experiments so that the collective phase changes can be transformed to obtain spatial I formation of this dimension. (y-direction)

(i) Slice selection (Z-direction) Slice position: Determined by the center frequency of the pulse and the gradient strength f(z) = r(b 0 +ZG)/2p 2πf Z = ( B )/ G...(5) 0 γ Slice thickness: Determined by both the pulse width and the gradient strength:? f = 1/t =??Z G/2p Z=2p/?tG (6) Z 1/t, Z 1/G Short pulse excite thick slice at fixed G Strong gradient give thinner (ii) Frequency Encoding: (x-direction) G x =0 a and b resonate at same frequency slice at fixed G x 0 a and b resonate at different requency

(iii) Phase encoding (y-direction) In the presence of G y (constant amplitude and duration for each repetition), spins at different y location will be resonating at different frequencies. Thus will accumulate different phase angle? y (t):? r (t)=?g y t Let k x =rg y t, k x =rg y t Then the NMR signal S(x,y,z) : S(x,y,z)= N(x,y)exp[-I(kxx+ kxy)]dxdy The above scheme can be extended to three dimension such that S(x,y,z,t)= N(x,y,z)exp[-I(k x x+ k x y+ k z z)]dxdydz (3-D FT imaging)

(i) (ii) (iii) (iv) (v) (vi) Use G z to select a slice perpendicular to z-direction Use G x is frequency encode magnetization along x-direction (same f at same x) Use G y to phase encode aling y-direction (same y same phase) Repeat the experiment with different G y 2-D Furier transform with respect to both x & y to get 2-D image of the slice Change G z (or f0) to select different slice to obtain 3-D image (d) Signal overaging: NMR signal is usually weak. To increase signal to noise ratio (S/N) it is often necessary to repeat the experiment n time and add the signal together. S/N will increase by: n n S n but N S/N Example: If S/N=0.5 for one scan, then for n=100 S/N = 0.5 x 100 = 5 (e) Imaging time for each slice: t = (TR) x n x (number of lines)=1.0 x 4 x 128 = 512 seconds ~ 8.4 minutes Repetition time ~ 1.05 Number of averaging scans

Fig. 1. Functional magnetic resonance (fmri) images in cat primary visual cortex during stimulation of the animal with moving gratings of two different orientations, 45 and 135. (a) Imaging slice showing the cat brain in sagittal (sag) view. (b) Image obtained from the oblique (obl) slice marked in red in (a), using T2* bloodoxygen-level dependent (BOLD) weighted fmri acquisition scheme (nominal resolution, 156 m2). The dotted yellow line highlighted by a green arrow marks the space between the two hemispheres of the brain, the inter-hemispheric fissure, where the large blood vessel of the sagittal sinus is located. Images obtained after stimulation with a grating at 45 or at 135 are shown in (c) and (d), respectively. The colored pixels in (c) and (d) depict the regions of increased conventional T2* BOLD signals. Robust and homogenous activities were observed in the lateral gyri of both hemispheres. Note, however, that regardless of the stimulus orientation presented, the region of activity extended several millimeters in the anterior posterior and medial lateral directions, with the highest BOLD activity originating from the sinus sagittalis. Consequently, the maps obtained for the different orientations

Figure 2. Group conjunction maps showing the consistency with which specific structures were activated across listeners. Conjunction maps of individual listeners, containing the voxels that were activated significantly (P < 0.001) in all scanning sessions for that listener, were normalized into a common space and summed together across listeners (see "spatial normalization" in supporting online text). Voxels that were consistently activated by at least four of the eight listeners are projected onto the group's mean normalized T1 image. (A) Areas sensitive to the two task regressors (Table 1). (B) The only areas whose activity patterns were significantly and consistently correlated with the tonality regressors both within and across listeners were the rostral portion of the ventromedial superior frontal gyrus and the right orbitofrontal gyrus.

MRI QUIZ Name: (June 11, 1996) Score: (Notice: All MRI is assumed to be detected in 1 H channel with =4257 Hz/G) I. True (O) or false (X): (4 points each) ( ) 1. All nuclei possess nuclear spin, therefore are all NMR observable. ( ) 2. All isotope of the same element resonate at the same frequency. ( ) 3. For a given nucleus, the higher the static field the higher the resonance frequency. ( ) 4. T 1 is also called transverse relaxation time. ( ) 5. The more mobile tissue has longer T 2. ( ) 6. From the decay rate of an FID one can measure T 2. ( ) 7. The relaxation of magnetization in the Z-direction is called a T 1 process. ( ) 8. A T 2 -weighted image is obtained with long TR an long TE. ( ) 9. When we apply a G x gradient to the NMR sample in a uniform static magnetic field then all water protons in the X-direction will resonate at different frequency. ( ) 10. A short pulse will allow the selection of a thicker slice in a fixed gradient. ( ) 11. A stronger gradient allows the selection of thinner slice with a fixed pulse length. ( ) 12. During the detecting period a gradient is applied in a certain dimension. This gradient is called phase encoding gradient. ( ) 13. Aliasing is an artifact resulted from improper receiver filter setting. ( ) 14. A T 1 -weighted image is obtained with short TR and short TE. ( ) 15. In a 2D spin-warp experiment the phase encoding gradient is fixed at a constant value. II. Multiple choices (only one is correct): (4 points each) ( ) 1. Which of the following factors has no effect on NMR resonance frequency: (a) magnetic field strength; (b) chemical environment; (c) magnetic field gradient (d) RF-field strength. ( ) 2. If we average the signal 4 times the signal to noise ratio of the image will increase by a factor of: (a) 4; (b) 2; (c) 1/2; (d) 1/4. ( ) 3. To detect an image of FOV=10cm in a gradient of 1 G/cm the bandwidth of the receiver must be: (a) 4257 Hz; (b) 42570 Hz; (c) 4257 khz; (d) 10Hz. ( ) 4. To obtain a T 1 -weighted image in a spin-warp experiment one must set: (a) Both TR and TE must be long; (b) TR~T 1 and TE very long; (c) TR long and TE~T 1 ; (d) Both TR and TE very long. ( ) 5. In a T 2 -weighted image which of the following is true: (a) Signal of tissue with short T 2 will be attenuated; (b) Signal of tissue with short T 2 will be enhanced; (c) Signal of tissue with short T 1 will be attenuated;

must be: (a) 10 us; (b) 14.8 ms; (c) 67.5 us; (d) 10 ms. ( ) 7. Which of the following statement concerns MRI magnet is not true:: (a) The higher the magnetic field the better the image quality one can expect. (b) Superconducting magnet has highest field homogeneity. (c) Permanent magnet is the most stable magnet. (d) The higher the field one use the higher the transmitter power one need. ( ) 8. Which of the following statement concerns MRI instrument is not true: (a) molecular motion; (b) magnetic field strength; (c) sample size; (d) temperature. ( ) 9. Which of the following factor is the least important in affecting MRI sensitivity: (a) Magnetic strength; (b) receiver preamp noise figure; (c) Coil Q factor; (d) transmitter power. ( ) 10. Calculate the pixel area of an image of 128 x 128 with FOV 10cm x 10cm: (a) 100 cm 2 ; (b) 16384 cm 2 ; (c) 1280 cm 2 ; (d) 6.1 x 10-3 cm 2.