Advanced Biomedical Imaging Dr. Azza Helal A. Prof. of Medical Physics Faculty of Medicine Alexandria University Lecture 6 Basic physical principles of.

Slides:



Advertisements
Similar presentations
PRINCIPLES OF CT.
Advertisements

IMAGE GENERATION IN CT.
Computers and Computed Tomography
Image Reconstruction.
Computed Tomography
Advanced Biomedical Imaging Lecture 4 Dr. Azza Helal A. Prof. of Medical Physics Faculty of Medicine Alexandria University.
COMPUTED TOMOGRAPHY HISTORICAL PERSPECTIVE. OUTLINE TOMOGRAPHY – DEFINITION WHY CT – LIMITATIONS OF RADIOGRAPHY AND TOMOGRAPHY CT- BASIC PHYSICAL PRINCIPLE.
Ionizing Radiation – X-Ray Imaging Gerald R. Aben, MD, FACR Department of Radiology College of Osteopathic Medicine.
A Technical Seminar On X-RAY AND CT SCAN.
Computed Tomography Basic principles V.G.Wimalasena Principal
Historical Development
Computed Tomography II
SCANCOMEDICAL Computed Tomography SCANCO User Meeting 2005 Dr. Bruno Koller SCANCO Medical AG
COMUTED TOMOGRAHY Dr. Amr A. Abd-Elghany 1.
Advanced Biomedical Imaging
CT Physics V.G.Wimalasena Principal School of radiography.
Computed Tomography III
Computed Tomography RAD309
General introduction- fundamental principles X ray & CT Radiology Dept. 1st Hospi. of Peking University 唐光健 Radiology Dept. 1st Hospi. of Peking University.
Computed Tomography. Introduced in 70’s Principle: Internal structures of an object can be reconstructed from multiple projections of the object.
tomos = slice, graphein = to write
X-Rays and CT Scans.
Chapter 2 Stewart C. Bushong
CT scanning (f) Candidates should be able to show an understanding of the principles of CT scanning. (g) Candidates should be able to show an understanding.
Lean Body Mass Assessment: Interpretations of Computed Tomography
Computed Tomography
Advanced Biomedical Imaging Dr. Azza Helal A. Prof. of Medical Physics Faculty of Medicine Alexandria University Lecture 2 Overview & comparison of different.
Conventional and Computed Tomography
…….CT Physics - Continued V.G.WimalasenaPrincipal School of radiography.
Advanced Biomedical Imaging Dr. Azza Helal A. Prof. of Medical Physics Faculty of Medicine Alexandria University.
LEC ( 2 ) RAD 323. Reconstruction techniques dates back to (1917), when scientist (Radon) developed mathematical solutions to the problem of reconstructing.
COMPUTED TOMOGRAPHY (I) RAD 365 CT - Scan
Basic principles Geometry and historical development
COMPUTED TOMOGRAPHY I – RAD 365 CT - Scan
Without reference, identify principles relating to Computed Tomography Clinical Applications with at least 70 percent accuracy.
Alhanouf Alshedi CT Physics and Instrumentation RAD
X-Ray Medical Imaging Physics – IB Objectives
Medical Image Analysis Medical Imaging Modalities: X-Ray Imaging Figures come from the textbook: Medical Image Analysis, Second Edition, by Atam P. Dhawan,
Computer Tomography By Moustafa M. Mohamed. Introduction to Medical Imaging Uses of medical imaging Obtain information about internal body organs or the.
SPECIAL IMAGING/ADVANCED IMAGING INTRODUCTION TO DIGITAL RADIOGRAPHY
An experiment in computed tomography
Schematic Representation o f the Scanning Geometry of a CT System
Computed Tomography Q & A
PRINCIPLE AND BASIC PHYSICS OF COMPUTED TOMOGRAPHY
Seeram Chapter 9: Image Manipulation in CT
Computed Tomography Physics, Instrumentation, and Imaging
Module A Computed Tomography Physics, Instrumentation, and Imaging.
X-rays. Electromagnetic Spectrum to 10 nm 400 to 700 nm to nm 10 to 400 nm 700 to 10 4 nm X-ray radiation was discovered by Roentgen.
CT and MRI. Computed Tomography 1972 __________________ X-ray tube in a tube Rows of _________ opposite x-ray tube Produces ___________________.
Principles and Practice of Radiation Therapy
CT IMAGE RECONSTRUCTION  Hounsfield envisioned dividing a slice into a matrix of 3-dimensional rectangular boxes (voxels) of material (tissue). Conventionally,
The production of X-Rays X-Rays are produced whenever charged particles are slowed down or stopped. X-rays are generated via interactions of the accelerated.
Image Display. But first a review Remember the 3 main steps 1. Data Acquisition 2. Image Reconstruction 3. Image Display.
Part No...., Module No....Lesson No
Part No...., Module No....Lesson No
Revision Imaging Procedure 3 Dr Mohamed El Safwany, MD.
CT Chapter 4: Principles of Computed Tomography. Radiography vs. CT Both based on differential attenuation of x-rays passing through body Radiography.
Advanced Biomedical Imaging Dr. Azza Helal A. Prof. of Medical Physics Faculty of Medicine Alexandria University.
Introducing cross- sectional imaging Dr.Ahmed S. Tawfeek FIBMS(Rad.)
Computed Tomography Computed Tomography is the most significant development in radiology in the past 40 years. MRI and Ultrasound are also significant.
Introduction to Medical Imaging Week 2: X-ray and CT
Computed tomography. Formation of a CT image Data acquisitionImage reconstruction Image display, manipulation Storage, communication And recording.
Basic Principles of CT Scanning. CT CT - Computed Tomography CAT Scan - Computerized Axial Tomography.
Computed Tomography Basics
Learning Objectives By the end of this lesson you should…
CT BASICS AND CT BRAIN.
INTRODUCTION to RADIOLOGY
Basic principles Geometry and historical development
Basic Principles of CT Chapter 1.
Computed Tomography (CT)
Presentation transcript:

Advanced Biomedical Imaging Dr. Azza Helal A. Prof. of Medical Physics Faculty of Medicine Alexandria University Lecture 6 Basic physical principles of computed tomography & Image formation

Points to be covered  Linear Tomography  Components of computed tomography unit  Basic data acquisition  CT scanner generations  Principle of CT imaging  CT number & its clinical application  Windowing.

Method of imaging single slice of object parallel to film and placed at a specific point (fulcrum) which is adjusted to height of anatomy of interest. 1. Linear Tomography: (single slice imaging)

 Tube and film moves from 1st position to the 2nd, all points in focal plane project to same position on the film  Points above or below the focal plane do not project to the same film position and are blurred.  By changing the relative motion of the film and tube the focal plane can be adjusted upward or downward  It is useful in IV urography  Body imaging tomography (Computed tomography) (CT): Reconstruction by a computer of an image of a plane or slices of an object.

5 X-ray Tube Detectors CT Table X-ray Beam Table, scanning gantry (x-ray source & detector array) x-ray generator, computer and viewing consoles. 2. Components of CT unit

3. Basic data acquisition

 Probing patient from different directions during 360 rotations with x-ray beam of known intensity (I 0 ) & measuring it after it has passed the pt (I) using detectors.  Detector (Scintillator / ionization chambers) measures exiting x-ray beam (I) & converts it into a proportional signal current.  From I & I 0, (U) is calculated (reflect intensity of photon beam attenuated) I=I 0 e -ux

 u is different for different tissue density.  Image is developed from multiple measurements of x-ray u detected from exterior of the patient.  By solving a system of linear equations for several projections, value of u can be computed.

4. CT scanner generations  1st: single beam & detector. Translate - rotate  2nd : narrow fan beam / detector array.  3rd: wide fan beam / detectors array, both rotate  4th: x ray tube alone rotates / stationary detectors.  5th : multiple x ray tubes & multiple stationary detectors to scan multiple slices simultaneously. 4. CT scanner generations

1st 2nd 3rd 4th 4. CT scanner generations

To allow the computer to present this information with a large scale, a reference material is used (water). Why? its µ is close to those of soft tissues. CT number is calculated as a relative comparison of x-ray attenuation of a voxel of tissue to equal volume of water. CT number of each voxel (average of individual CT no of the contents of corresponding voxel) is computed & stored in computer memory. 5. Principle of CT imaging

Hounsfield Units

 large amount of data presented as grey scale (whiteness is α average µ of contents /voxel).  Tissues appear as shades of gray from black & white.  Tissues with high u (bone) appear white  Tissues with low u (air) appears black.  bone= 1000 water= 0 air= .. The Hounsfield scale

CT number (reflect density) Air = -1000, Lung -550 to -950 Fat=-80 to -100 Water = 0 White matter = 20-30, Gray matter = soft tissue +40 to +60 depends on KV Acute Hge = 70 to 100 HU Calcification = 200 to 300 HU Bone +500 to Contrast agent +3000

CT Numbers or Hounsfield Units CT tissue characterization

 Selective display of a restricted range of gray scale of selected tissues (tissues of interest).  Tissues with CT no outside this window un displayed. Manipulated by selection of : window center. window width Windowing

Window level is CT number selected for centre of the range of numbers displayed on the image. Window width is total range of values selected. Width determines contrast. A narrow window enhances inherent contrast. Window level determines the brightness

W = 80 C = 50 W = 80 C = 20 W = 200 C = 30 W = 80 C = 30 W = 50 C = 30 Centre average gray <centre lighter gray >centre darker gray

In routine work Brain is visualized at level 30 and width 80. Soft tissue is visualized at level 40 and width 250. Bones are visualized at level 1000 & width Lungs are visualized at level -600 & width As CT no reflects u and so different tissues densities, So it is used to characterize normal tissues & pathologies as calcification & lesion diameter.

Questions 1.Define; window level & width? 2.What are the detectors used in CT unit? 3.What is the CT number of bone, air and water? 4.What is the difference between u and CT number of the tissue?