BIOE 220/RAD 220 REVIEW SESSION 6 March 5, 2012. What We’ll Cover Today General questions? Spinal cord anatomy review Fat in images T2* vs T2 decay Review.

Slides:



Advertisements
Similar presentations
Pulse Timing parameters & Weighting
Advertisements

Principles of the MRI Signal Contrast Mechanisms MR Image Formation John VanMeter, Ph.D. Center for Functional and Molecular Imaging Georgetown University.
Imaging Sequences part I
Chapter 7: Gradient Echo Imaging Methods
Proton Spin In absence of a magnetic field, protons spin at random
MRI Phillip W Patton, Ph.D..
BE 581 Lecture 3- Intro to MRI.
PHYSICS OF MAGNETIC RESONANCE
MR Sequences and Techniques
Statistical Parametric Mapping
Parameters and Trade-offs
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.
Noll An Overview of Echo Planar Imaging (EPI) Douglas C. Noll, Ph.D. Depts. of Biomedical Engineering and Radiology University of Michigan, Ann Arbor.
Noll Spin-Warp Imaging For each RF pulse:For each RF pulse: –Frequency encoding is performed in one direction –A single phase encoding value is obtained.
Psy 8960, Fall ‘06 EPI, Part 11 Pulse sequences Nyquist ghost Chemical shift –FLASH –EPI.
Relaxation Exponential time constants T1 T2 T2*
FMRI: Biological Basis and Experiment Design Lecture 10: The Dreaded Drop-out Spin echo review Field maps Through-slice dephasing © Melissa Tillery
EPI – Echo Planar Imaging Joakim Rydell
Basics of Magnetic Resonance Imaging
FMRI: Biological Basis and Experiment Design Lecture 9: Pulse sequences, Take 3 Slice selection homework review Pulse sequence/k- space trajectory matching.
Steady-state magnetization
Psy 8960, Fall ‘06 Fourier transforms1 –1D: square wave –2D: k x and k y Spatial encoding with gradients Common artifacts Phase map of pineapple slice.
FMRI: Biological Basis and Experiment Design Lecture 7: Gradients and k-space FFT examples –Sampling and aliasing Gradient Gradient echo K-space
Psy 8960, Fall ‘06 EPI, Part 2: variants1 Segmentation Partial Fourier Spin echo vs. gradient echo Inversion recovery Long vs. short TE.
Magnetic Resonance Imaging 4
Gradient echo pulse sequences
Advanced pulse sequences
Principles of Magnetic Resonance
Imaging Sequences part II
Gradients (Continued), Signal Acquisition and K-Space Sampling
2012 spring fMRI: theory & practice
Medical Imaging Systems: MRI Image Formation
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.
Basics of MRI.
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.
Quiz In a 2D spin warp or FT MR scan, aliasing should only occur
Rad T 265 MRI Lecture. No Magnetic Field = No Net Magnetization Protons align with a magnetic field…
G Practical MRI 1 Basic pulse sequences.
G Practical MRI 1 Gradients.
BIOE 220/RAD 220 REVIEW SESSION 8 March 19, 2012.
Contrast Mechanism and Pulse Sequences
Statistical Parametric Mapping
BIOE 220/RAD 220 REVIEW SESSION 7 March 13, 2012.
Magnetic Resonance Imaging
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
V.G.Wimalasena Principal School of Radiography
BIOE 220/RAD 220 REVIEW SESSION 3 February 6, 2011.
MRI: Contrast Mechanisms and Pulse Sequences
Spinning Nucleus Produces Magnetic Moment
Principles of MRI Physics and Engineering Allen W. Song Brain Imaging and Analysis Center Duke University.
DTI Acquisition Guide Donald Brien February 2016.
Chapter 5 Mark D. Herbst, M.D., Ph.D.. The MR Imaging Process Two major functions –Acquisition of RF signals –Reconstruction of images.
10 spring fMRI: theory & practice
FMRI data acquisition.
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.
An Optimal Design Method for MRI Teardrop Gradient Waveforms
MRI Pulse Sequences: IR, EPI, PC, 2D and 3D
Basic MRI I Dr. Mark D. Herbst
MRI ARTEFACTS PG Student : Dr Aditi Shah PG Guide: Dr Rajendra Chavan
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.
Presentation transcript:

BIOE 220/RAD 220 REVIEW SESSION 6 March 5, 2012

What We’ll Cover Today General questions? Spinal cord anatomy review Fat in images T2* vs T2 decay Review of sequences Questions on the hw?

Nasal and Oral cavities Nasal Cavity Nasopharynx Uvula/Soft Palate Oropharynx Epiglottis Tongue

Parotid glands Parotid Gland Stensen’s Duct

Salivary glands Sublingual gland Submandibular gland Submandibular duct

Thyroid

Spinal Vertebrae Breakfast at 7 Lunch at 12 Dinner at 5 Cervical roots: C1-C8 (all above their vertebrae except 8) Thoracic: T1-T12, Lumbar: L1-L5, Sacral: S1-S5

Cervical Spine Anterior Posterior

Cervical spine

Thoracic Spine

Lumbar Spine

How does fat look in MRI? Without fat suppression, fat always appears bright Why? Short T1, normalT2 but high PD Fat precesses at a different frequency (3.5 ppm shift – how fast?) so it appears shifted in images This effect can be minimized by maximizing the strength of readout gradients (why?) How can we remove fat from the signal? Take advantage of difference in precession frequency Chemical saturation: Hit fat with selective 90º pulse, spoil the transverse signal, then do a normal measurement afterwards Short TI Inversion recover: After a 180º pulse, wait for the fat to recover to 0 (shorter T1), then measure the other signals

T2 vs T2* decay When do we see T2* decay, when do we see T2 decay? T2* decay is observed after a 90º pulse if no other preparation is done (GRE sequence) T2 decay is observed if a 180º refocusing pulses is used to “unroll” any off-resonance defocusing (SE sequence) After the 180º pulse, must wait the same amount of time as we waited before the pulse until things have refocused

What sequences have we learned about? Simplest: GRE 2DFT Excite with 90º pulse, then read out K-space trajectory will be lines in the frequency encode direction, stepped in the phase encode direction between every TR Spin echo 2DFT Same as before, except now we add a 180º refocusing pulse after the 90º so that we’ll obtain T2 weighting instead of T2* 180º pulse occurs at TE/2 Spatial saturation Add a 90º pulse to excite a slab and then spoil it, before regular sequence This nulls the signal in the slab, so that only fresh spins flowing in will be visible

What sequences have we learned about? Fat suppression: Chem Sat Use a 90º selective pulse on the fat signal and spoil it, before regular sequence Ideally nulls the fat signal without effecting rest of image Fat suppression: STIR Use a 180º pulse to flip everything, then wait until the fat passes through 0 to do our readout Diffusion weighting Use strong bipolar (sums to zero) gradient, so that spins will dephase based on their movement during gradient Flow encoding Similar to diffusion weighting, except that we’re interested in much higher velocities (of bulk spins)

What sequences have we learned about? Fast spin echo Perform multiple 180º - readout – 180º - readout in a single TR Allows faster acquisition of SE image, but fat appears brighter EPI Instead of recording line by line, traverse 2DFT grid very quickly in single sequence Fast, but very susceptible to artifacts Spiral Instead of collecting k-space in grid like 2DFT, traverse k-space in a spiral, to be more efficient with gradients Efficient/fast, but susceptible to artifacts and leads to spatially variant resolution/blurring