ADC PRE-PATIENT COLLIMATION POST-PATIENT COLLIMATION.

Slides:



Advertisements
Similar presentations
Instruments for Radiation Detection and Measurement Lab # 4.
Advertisements

DIGITAL RADIOGRAPHY.
Technical Aspects: the machine the image
Introduction to x-rays
COMPUTED TOMOGRAPHY INSTRUMENTATION AND OPERATION
COMPUTED TOMOGRAPHY INSTRUMENTATION AND OPERATION
RAD 350 Chapter 16 Digital Radiography Many types/names for the digital imaging processes and devices.
X-Ray Interaction with Matter & Human Biology
Chapter 6 Control of Secondary and Scattered Radiation.
Computed Tomography Stewart C. Bushong
Computed Tomography II
Digital Radiographic Imaging 101
Fysisk institutt - Rikshospitalet 1. 2 Overview Gamma camera Positron emission technology (PET) Computer tomography (CT) Proton therapy Electrical impedance.
Nuclear Medicine Spring 2009 FINAL. 2 NM Team Nuclear medicine MD Nuclear medicine MD Physicist Physicist Pharmacist Pharmacist Technologist Technologist.
BME 560 Medical Imaging: X-ray, CT, and Nuclear Methods X-ray Instrumentation Part 1.
BME 560 Medical Imaging: X-ray, CT, and Nuclear Methods
Types of Radiation Interactions All or Nothing Many Small There is a finite probability per unit length that the radiation is absorbed. If not, there is.
Computed Tomography RAD309
Computed Tomography. Introduced in 70’s Principle: Internal structures of an object can be reconstructed from multiple projections of the object.
Main detector types Multi Pixel Photon Counter (MPPC) and Charge Coupled Devices (CCDs) How does it work? 1. Photon hits a pixel producing electron hole.
Seeram Chapter 5: Data Acquisition in CT
Techniques for detecting X-rays and gamma-rays Pair production Creation of elementary particle and its antiparticle from a photon. Occurs only if enough.
Instruments for Radiation Detection and Measurement
Direct Digital Radiography or Direct Capture Radiography Bushong Ch. 27.
X-Ray Production & Emission
X-Ray Production & Emission
X-rays Ouch!.
Instruments for Radiation Detection and Measurement Lab # 3 (1)
Reference Reading Chapter 2: pp  X-rays are produced within the dental x-ray machine  The x-ray machine can be divided into 3 study areas.
5.4.1 X-Rays. (a) describe the nature of X-rays Stowmarket Physics X-rays - nature Forms of electromagnetic radiation Short wavelength High frequency.
Resident Physics Lectures Christensen, Chapter 6Filters George David Associate Professor Department of Radiology Medical College of Georgia.
Alhanouf Alshedi CT Physics and Instrumentation RAD
Chapter 6: Digital Radiographic Imaging
A-LEVEL PHYSICS 15/09/ :49 Medical Physics.
HABIS X-RAY PRODUCTION AND EXPOSURE FACTORS X-RAY PRODUCTION AND EXPOSURE FACTORS PREPARED BY PREPARED BY Dr fahad albadr radiology chairman radiology.
DIGITAL PROJECTION RADIOGRAPHY COMPUTED RADIOGRAPHY
INVERSE SQUARE LAW. The picture above demonstrates the typical x-ray tube used to produce a point source of x-rays. Then as radiation exits the tube it.
CT Physics Lecture 3.
Computed Tomography Physics, Instrumentation, and Imaging
Characteristic Radiation in Tungsten Targets Shel l # of electrons Binding energy L Char M Char N Char O Char P Char Eff X-ray Energy.
CT Instrumentation and X-ray system
Factors affecting CT image RAD
Digital Radiography and PACS By Professor Stelmark.
Elements of DR Imaging Systems
▪ History ▪ Equipment ▪ Image Production/Manipulation.
Module C Computed Tomography Physics, Instrumentation, and Imaging.
LEC (1) Design/layout by E Bashir, CAMS, King Saud University, Ref: Seeram, Karthikeyan, internet.
Radiographic Equipment
CT Chapter 4: Principles of Computed Tomography. Radiography vs. CT Both based on differential attenuation of x-rays passing through body Radiography.
Medical applications of particle physics General characteristics of detectors (5 th Chapter) ASLI YILDIRIM.
X-rays is a form of electromagnetic radiation having a wavelength in the range of 0.01 to 10 nanometers, corresponding to frequencies in the range 30.
CAT scanners and gamma cameras Unit 16 Waves. Learning objectives Describe how CAT scanners can produce a much more detailed image than conventional X-rays.
Chapter V Radiation Detectors.
Fluroscopy and II’s. Fluroscopy Taking real time x-ray images Requires very sensitive detector to limit the radiation needed Image Intensifier (II) is.
Interaction of x-ray photons (and gamma ray photons) with matter.
Nuclear Medicine Instrumentation 242 NMT 1 Dr. Abdo Mansour Assistant Professor of radiology
DIGITAL RADIOGRAPHY.
Direct Digital Radiography or Direct Capture Radiography
Acronyms. A SEQUENCE OF COMPUTER OPERATIONS FOR ACCOMPLISHING A SPECIFIC TASK Algorithm.
Analog X-ray Imaging Recommended Book: Walter Huda, REVIEW OF RADIOLOGIC PHYSICS By: Maisa Alhassoun
Computed Tomography Computed Tomography is the most significant development in radiology in the past 40 years. MRI and Ultrasound are also significant.
Optimizing The Image RVT: Chapter 7
Radiation Protection RTMR 284 CHAPTER 20 PART II.
Comparison of Film v. Digital Image Display
Computed Tomography Data Acquisition
Resident Physics Lectures (year 1)
X-RAY PRODUCTION AND EXPOSURE FACTORS
X-Radiation.
Resident Physics Lectures (year 1)
COMPUTED RADIOGRAPHY -Dr.SHEFALI MESHRAM
Presentation transcript:

ADC PRE-PATIENT COLLIMATION POST-PATIENT COLLIMATION

 The Restriction of X-Radiation to the Area being Examined or Treated by Confining the Beam with Metal Diaphragms or Shutters made of Lead which Completely Absorb the Photons; With High Radiation - Absorption Power.  In addition to Protecting the Patient and Others From Scatter Radiation.  Beam Collimation Reduces Radiographic Density.  Collimator Reduces Scatter Radiation that Reaches the Detector Array.  Improving the Image Contrast.  Determines the Slice Thickness.  In CT Imaging, Two Collimators are used.  One Collimator is Mounted on the X-Ray Tube Housing or Adjacent to it.  This is Called Prepatient Collimator that Determines Patient Dose.  Second Collimator is Called Predetector Collimator.

 Remove the Soft, Low - Energy X - Rays, which Contribute Strongly to the Patient Dose and Scatter Radiation but Less to the Detected Signal.  Make the Beam Harder and More Monoenergetic.  The Inherent Filtration of the X - ray - Tube, Typically 3 mm Aluminum Equivalent Thickness, is the First Filter.  In addition, Flat or Shaped Filters Made of Copper or Aluminum, are placed between the X - Ray Source and the Patient.

 CT Imaging system have Multiple Detectors in an Array that Numbers Up to Tens of Thousands.  The Detector is the System for Quantitative Recording of the Incident Ionizing Radiation. It Acts in Two Steps; The Reception of the Incident X - Ray Photon, and The Transformation of the X - Ray Photon into a Corresponding Electrical Signal, that is then Amplified and Converted from an Analog to a Digital Form.  Previously Gas – Filled Detectors were used: Ionization Chambers, mostly Filled with the Noble Gas Xenon Under High Pressure. Gas Detectors have become Obsolete Due to their Limited Detection Efficiency and the Difficulty in Manufacturing them for Multi - Row Design, but now, all are Scintillation, Solid State Detectors.  Early Scintillation Detector Arrays contained Scintillation Crystal in Photodiode such as Cesium Iodide or Cadmium Tungstate, and Ceramic Materials such as Gadolinium Oxysulfide. Photodiodes Convert the Light into an Electronic Signal.  The Combination of a Scintillation Crystals and the Light Detectors is Called a Scintillation Detectors.