Chapter 5 Mark D. Herbst, M.D., Ph.D.. The MR Imaging Process Two major functions –Acquisition of RF signals –Reconstruction of images.

Slides:



Advertisements
Similar presentations
Durgesh Kumar Dwivedi Department of NMR & MRI AIIMS, New Delhi, India
Advertisements

Contrast T1 weighted – (MPRAGE-anatomical) T2 weighted – (fmri)
Magnetic Resonance Imaging
Imaging Sequences part I
Chapter 7: Gradient Echo Imaging Methods
Introduction to MRI Magnetic Resonance Imaging
PULSE SEQUENCES Emphasizing the differences among spin density, T1, and T2 relaxation time constants of the tissues is the key to the exquisite contrast.
Proton Spin In absence of a magnetic field, protons spin at random
M R I Pulse Sequences Jerry Allison Ph.D..
BE 581 Lecture 3- Intro to MRI.
Magnetic Resonance Imaging - MRI
MR Sequences and Techniques
Statistical Parametric Mapping
Fund BioImag : MRI contrast mechanisms 1.What is the mechanism of T 2 * weighted MRI ? BOLD fMRI 2.How are spin echoes generated ? 3.What are.
Parameters and Trade-offs
Magnetic Resonance Imaging
Topics spatial encoding - part 2. Slice Selection  z y x 0 imaging plane    z gradient.
Chapter 9 Basic MRI I Mark D. Herbst, MD, PhD. Notice This lecture contained many drawings on the whiteboard, so get these from one of the other students.
Fast spin echo 단국대학교 영상의학과 유 동 수.
Terry M. Button, Ph.D. Principals of Magnetic Resonance Image Formation.
Chapter 10 Lecture Mark D. Herbst, M.D., Ph.D..
Relaxation Exponential time constants T1 T2 T2*
FMRI: Biological Basis and Experiment Design Lecture 9: Pulse sequences, Take 3 Slice selection homework review Pulse sequence/k- space trajectory matching.
FMRI: Biological Basis and Experiment Design Lecture 7: Gradients and k-space FFT examples –Sampling and aliasing Gradient Gradient echo K-space
FMRI: Biological Basis and Experiment Design Lecture 8: Pulse sequences, Take 2 Gradient echo review K-space review Slice selection K-space navigation.
Compressed Sensing for Chemical Shift-Based Water-Fat Separation Doneva M., Bornert P., Eggers H., Mertins A., Pauly J., and Lustig M., Magnetic Resonance.
Tissue Contrast intrinsic factors –relative quantity of protons tissue proton density –relaxation properties of tissues T1 & T2 relaxation secondary factors.
대구가톨릭대학병원 영상의학과 이 영 환 M M R R Basic Physics. MR Signal T1-, T2-weighted TR, TE MR Signal T1-, T2-weighted TR, TE.
Principles of MRI Physics and Engineering
Principles of Magnetic Resonance
Imaging Sequences part II
Medical Imaging Systems: MRI Image Formation
Chapter 4 Mark D. Herbst, M.D., Ph.D.. Magnetization MRI depends on magnetization of tissues Temporary magnetization occurs when the hydrogen nuclei are.
Pulse sequences.
Pulse Sequences Types of Pulse Sequences: Functional Techniques
Chapter 6 Lecture Spin Echo Imaging Methods Mark D. Herbst, MD, PhD Two Main Types of MR methods –Spin Echo –uses RF pulse to get an echo –Gradient Echo.
RT 4912 Review (A) Rex T. Christensen MHA RT (R) (MR) (CT) (ARRT) CIIP.
Contrast Mechanism and Pulse Sequences Allen W. Song Brain Imaging and Analysis Center Duke University.
Rad T 265 MRI Lecture. No Magnetic Field = No Net Magnetization Protons align with a magnetic field…
G Practical MRI 1 Basic pulse sequences.
Contrast Mechanism and Pulse Sequences
Chapter 10 Lecture Mark D. Herbst, M.D., Ph.D.. Image Detail and Noise Two image characteristics that reduce the visibility of anatomy/pathology –Blurring.
MRI Physics Dr Mohamed El Safwany, MD.. MRI Magnetic Resonance Imaging Magnetic Resonance Imaging.
BIOE 220/RAD 220 REVIEW SESSION 6 March 5, What We’ll Cover Today General questions? Spinal cord anatomy review Fat in images T2* vs T2 decay Review.
FMRI – Week 4 – Contrast Scott Huettel, Duke University MR Contrast FMRI Graduate Course (NBIO 381, PSY 362) Dr. Scott Huettel, Course Director.
Protons (hydrogen nuclei act like little magnets) MRI Collective Magnetic Moment of Protons (M 0 ) Each pixel is a glass of protons B 0 = 3T (not to scale)
MRI Physics: Pulse Sequences
Basic MRI Chapter 1 Lecture. Introduction MRI uses radio waves and a magnetic field to make images MRI uses radio waves and a magnetic field to make images.
V.G.Wimalasena Principal School of Radiography
2002 symposium1 Craig Goodrich 2002 MIRL Symposium.
MR Image Formation FMRI Graduate Course (NBIO 381, PSY 362)
MRI: Contrast Mechanisms and Pulse Sequences
Magnetic Resonance Learning Objectives
Principles of MRI Physics and Engineering Allen W. Song Brain Imaging and Analysis Center Duke University.
FMRI data acquisition.
Fig. 1. Pulse sequence diagram of balanced steady-state free precession. Sum of all gradients in each of three directions (slice-selection, phase-encoding,
MRI Physics in a Nutshell Christian Schwarzbauer
بسم الله الرحمن الرحيم.
Where Mt is the magnetization at time = t, the time after the 90o pulse, Mmax is the maximum magnetization at full recovery. At a time = one T1, the signal.
Magnetic Resonance Imaging: Physical Principles
Bioengineering 280A Principles of Biomedical Imaging Fall Quarter 2005 MRI Lecture 5 Thomas Liu, BE280A, UCSD, Fall 2005.
MRI Pulse Sequences: IR, EPI, PC, 2D and 3D
Chapter 11 Lecture Mark D. Herbst, M.D., Ph.D..
Basic MRI I Mark D. Herbst, MD, PhD
Basic MRI I Dr. Mark D. Herbst
Magnetic Resonance Imaging
Basic MRI I Dr. Mark D. Herbst
(4)ELECTRONIC SUPPORT SYSTEM
The echo time (TE) The echo time (TE) refers to the time between the application of the radiofrequency excitation pulse and the peak of the signal induced.
MRI: 造影原理.
Presentation transcript:

Chapter 5 Mark D. Herbst, M.D., Ph.D.

The MR Imaging Process Two major functions –Acquisition of RF signals –Reconstruction of images

k-space Where acquired signals are stored in the computer –Filled one line at a time –Must be filled completely before reconstruction –The number of lines = the resolution in the phase direction –The number of dots per line = the resolution in the frequency direction

To get a 256 x 256 image Need 256 lines in k-space Each line must have 256 dots per line Each line takes time to get, and that time is TR in conventional single echo spin echo imaging, so this would take 256 TRs.

To get a 192 x 256 image Need 192 lines in k-space Each line must have 256 dots per line Each line takes time to get, and that time is TR in conventional single echo spin echo imaging, so this would take 192 TRs.

Acquisition Usually one line of k-space for each repetition of the imaging sequence = each repetition time = each TR Fast methods produce multiple lines for each TR

Definition of TR Repetition time Time between 90 degree pulses in a spin echo technique

Imaging Protocol Various methods—spin echo, gradient echo, inversion recovery Various image types-T1-weighted images (T1WI), T2WI, T2*WI, STIR, FLAIR, MRA Spatial characteristics—slice thickness, number of slices, pixel size, voxel size Detail/noise—matrix, pixel, and voxel size Selective signal suppression Artifact reduction techniques

The Imaging Cycle Two distinct phases –Longitudinal relaxation – T1 weighting –Transverse relaxation – T2 weighting –Amount of T1 or T2 weighting depends on TR and TE –Echo event is produced by an RF pulse followed by either an RF pulse or a gradient pulse

T1 contrast

PD contrast

T2 contrast

T1, PD, and T2 contast all contribute to the final brightness of the pixel on the MR image