X-Ray Production & Emission

Slides:



Advertisements
Similar presentations
X-RAY PRODUCTION BREMSTRAHLUNG RADIATION CHARACTERISTIC RADIATION.
Advertisements

X-ray Production.
Chapter 11 Prime Factors.
The X-Ray Tube Bushong Ch 7.
X-Ray Interaction with Matter & Human Biology
Physics of X-rays By Dr. Amr A. Abd-Elghany.
X-ray tube and detection of X-rays Lecture 5. Reminder: The rough schematics of an X-ray tube filament cathod target anode photon flux e-e- electron kinetic.
ACVR Artifacts Artifacts of Diagnostic Radiology
Analyzing the Image Density. Density Overall blackening of the image.
X-radiation. X-rays are part of the electromagnetic spectrum. X-radiation (composed of X-rays) is a form of electromagnetic radiation. X- rays have a.
Radiation Physics II.
Medical Imaging X-Rays I.
PRODUCTION OF X-RAY & X-RAY SPECTRUM
BME 560 Medical Imaging: X-ray, CT, and Nuclear Methods X-ray Instrumentation Part 1.
The Origins of X-Rays. The X-Ray Spectrum The X-Ray Spectrum (Changes in Voltage) The characteristic lines are a result of electrons ejecting orbital.
8.1 PRODUCTION AND CHARACTERISTICS OF X-RAYS
Factors affecting the X-Ray output
X-Ray Production & Emission
RAD 354 Chapt 7 X-ray Production The primary purpose of an x-ray tube is to accelerate electrons across the tube and suddenly stop them in the target to.
Elsevier items and derived items © 2009 by Mosby, Inc., an affiliate of Elsevier Inc. X-Ray Production Chapter 8.
The X-ray Imaging System
Resident Physics Lectures Christensen, Chapter 6Filters George David Associate Professor Department of Radiology Medical College of Georgia.
Topic 29: Remote Sensing 29.1 Production and use of X-rays 29.2 Production and uses of ultrasound 29.3 Use of magnetic resonance as an imaging technique.
Week one Chapters one and two
Ch. 2 – Anatomy of the X-ray Machine
HABIS X-RAY PRODUCTION AND EXPOSURE FACTORS X-RAY PRODUCTION AND EXPOSURE FACTORS PREPARED BY PREPARED BY Dr fahad albadr radiology chairman radiology.
Resident Physics Lectures
Mammography Questions and Answers
RTEC A - WEEK 3 GENERAL SCIENCE REVIEW & X-RAY PRODUCTION IN THE TUBE.
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.
Chapter 2 The X-ray Beam.
RAD 254 Chapter 15 Radiographic Technique 4 primary exposure factors are: kVp, mA, time, distance.
Factors affecting CT image RAD
Exposure Factors or Prime Factors
Physics of Radiography X-ray production and Spectra.
X-ray emission spectra
Photon Tissue Interactions
What is being tested? (kVp, mA, mAs, mR?) What is the purpose of the HVL test? If an x-ray tube does not pass the HVL test what is done to correct the.
Radiation Quality Chapter 4. X-ray Intensity Intensity: the amount of energy present per unit time per unit area perpendicular to the beam direction at.
Elsevier items and derived items © 2009 by Mosby, Inc., an affiliate of Elsevier Inc. X-Ray Emission Chapter 9.
PRINCIPLES OF TECHNIQUE AND EXPOSURE
RAD 354 Chapt. 8 X-ray emission
X-rays discovered in 1895 by Wilhem Roentgen Roentgenology – Branch of medicine dealing with x-ray or gamma rays in diagnosis and treatment. Radiology.
RAD 354 Chap. 13 Radiographic Technique
Interactions of EM Radiation with Matter
Attenuation As x-rays pays through matter, the exit beam will contain less photons than the entrance beam. This reduction in the quantity of photons is.
Medical Equipment Technology Department 1 Introduction to Biomed. Imaging Systems Lecture No.5-6 Dr. Yousif Mohamed Y. Abdallah.
Quiz Review…….. 1 st Quiz-Class Average 88% 2 nd Quiz-Class Average 75% What happened? Suggestions from class Suggestions from instructor 1.
Resident Physics Lectures Christensen, Chapter 2C Production of X-Rays George David Associate Professor Department of Radiology Medical College of Georgia.
RTT 425 Radiation Therapy Physics Radiation Quality, Chapter 4 From Stanton and Stinson: Applied physics for Radiation Oncology.
Tube Exposure Factors Math Technique Contrast and Density
Alhanouf Alshedi Basic Interactions of Radiation with Matter 2 ed Lecture.
Sergeo Guilbaud School of Radiologic Sciences
RTEC A - WEEK 4 GENERAL SCIENCE REVIEW & X-RAY PRODUCTION IN THE TUBE
X-ray tube.
An early x-ray by Wilhem Rontgen
Chapter 9 Concepts you already know!!! INTENSITY = ROENTGENS AKA EXPOSURE l mAs and mR proportional? l kVp and mRproportional? l Distance and mRproportional?
Exposure Factors or Prime Factors
Resident Physics Lectures (year 1)
X-RAY PRODUCTION AND EXPOSURE FACTORS
Part No...., Module No....Lesson No
X-Radiation.
Stacy Kopso, M.Ed., RT(R)(M)
Characteristic Radiation in Tungsten Targets Shell # of electrons Binding energy L Char M N O P Eff X-ray Energy K
Resident Physics Lectures (Year 1)
Resident Physics Lectures (year 1)
CHAPTER 7 X-RAY PRODUCTION.
Welcome! Emission Spectra Emission Spectra.
Resident Physics Lectures (Year 1)
Generation of X-rays Q&A
Presentation transcript:

X-Ray Production & Emission

Objectives: Review x-ray production requirements X-ray tube interactions X-ray emission spectrum

Principle Parts of the X-ray Imaging System Operating Console High-voltage generator X-ray tube The system is designed to provide a large number of e- with high kinetic energy focused to a small target

E- traveling from cathode to anode Projectile e- interacts with the orbital e- of the target atom. This interaction results in the conversion of e- _______ energy into ________ energy and ________ energy.

Tube Interactions 3 possible tube interactions Tube interactions are generated from _____ slamming into ________? Heat (99%), EM energy as infrared radiation (heat) & x-rays (1%) X-rays = Characteristic (20%) or Bremsstrahlung (80%)

Heat Most kinetic energy of projectile e- is converted into heat – 99% Projectile e- interact with the outer-shell e- of the target atoms but do not transfer enough energy to the outer-shell e- to ionize

Heat is an excitation rather than an ionization

Heat production Production of heat in the anode increases directly with increasing x-ray tube current & kVp Doubling the x-ray tube current doubles the heat produced Increasing kVp will also increase heat production

Characteristic Radiation – 2 steps Projectile e- with high enough energy to totally remove an inner-shell electron of the tungsten target Characteristic x-rays are produced when outer-shell e- fills an inner-shell void All tube interactions result in a loss of kinetic energy from the projectile e-

It is called characteristic because it is characteristic of the target element in the energy of the photon produced

Only K-characteristic x-rays of tungsten are useful for imaging

Bremsstrahlung Radiation Heat & Characteristic produces EM energy by e- interacting with tungsten atoms e- of the target material Bremsstrahlung is produced by e- interacting with the nucleus of a target tungsten atom

Bremsstrahlung Radiation A projectile e- that completely avoids the orbital e- as it passes through a target atom may pass close enough to the nucleus of the atom to convert some of the projectile e- kinetic energy to EM energy Because of the electrostatic force?

Bremsstrahlung is a german word meaning slowed-down radiation

X-ray energy Characteristic x-rays have very specific energies. K-characteristic x-rays require a tube potential of a least 70 kVp Bremsstrahlung x-rays that are produced can have any energy level up to the set kVp value. Brems can be produced at any projectile e- value

Discrete spectrum Contains only specific values

Continuous Spectrum Contains all possible values

Characteristic X-ray Spectrum Characteristic has discrete energies based on the e- binding energies of tungsten Characteristic x-ray photons can have 1 of 15 different energies and no others

Characteristic x-ray emission spectrum

Bremsstrahlung X-ray Spectrum Brems x-rays have a range of energies and form a continuous emission spectrum

Factors Affecting the x-ray emission spectrum Tube current, Tube voltage, Added filtration, Target material, Voltage waveform The general shape of an emission spectrum is always the same, but the position along the energy axis can change

Quality The farther to the right the higher the effective energy or quality

Quantity The more values in the curve, the higher the x-ray intensity or quantity

mAs A change in mA or s or both results in the amplitude change of the x-ray emission spectrum at all energies The shape of the curve will remain the same

mA increase from 200 to 400

kVp A change in voltage peak affects both the amplitude and the position of the x-ray emission spectrum

Filtration Adding filtration is called hardening the x-ray beam because of the increase in average energy Characteristic spectrum is not affected & the maximum energy of x-ray emission is not affected

Filtration Adding filtration to the useful beam reduces the x-ray beam intensity while increasing the average energy Added filtration is an increase in the average energy of the x-ray beam (higher quality) with a reduction in x-ray quantity Lowering the amplitude and shifting to the right

What kVp does this graph indicate?

Target Material The atomic number of the target affects both the quantity and quality of x-rays Increasing the target atomic number increases the efficiency of x-ray production and the energy of characteristic and bremsstrahlung x-rays

Target material

Voltage Waveform 5 voltage waveforms: half-wave rectification, full-wave rectification, 3-phase/6-pulse, 3-phase/12-pulse, and high-frequency. Maintaining high voltage potential

Voltage generators

X-ray Quantity or Intensity What units of measurement is used for radiation exposure or exposure in air? Milliampere-seconds (mAs) – x-ray quantity is proportional to mAs Kilovolt Peak (kVp) – If kVp were doubled the x-ray intensity would increase by a factor of four or kVp2

X-ray Quantity or Intensity Distance – x-ray intensity varies inversely with the square of the distance from the x-ray target When SID is increased, mAs must be increased by SID2 to maintain constant OD

Filtration 1 to 3 mm of aluminum (Al) added to the primary beam to reduce the number of low-energy x-rays that reach the patient, reducing patient dose Filtration reduces the quantity of x-rays in the low-energy range

Reducing low-energy photons

X-ray Quality or Penetrability As the energy of an x-ray beam is increased, the penetrability is also increased High-energy photons are able to penetrate tissue farther than low-energy photons High-quality = high-penetrability Low-quality = low-penetrability

HVL = Half-Value Layer What is the HVL HVL is affected by the kVp and added filtration in the useful beam Photon quality is also influenced by kVp & filtration HVL is affected by kVp

HVL In radiography, the quality of the x-rays is measured by the HVL The HVL is a characteristic of the useful x-ray beam A diagnostic x-ray beam usually has an HVL of 3 to 5 mm Al

HVL 3 to 5 mm Al = to 3 to 6 cm of soft tissue HVL is determined experimentally and a design specification of the equipment

X-ray Quality Kilovolt Peak (kVp) = increasing the kVp increased photon quality and the HVL

Types of Filtration Diagnostic x-ray beams have two filtration components – inherent filtration and added filtration Inherent filtration – The glass enclosure of the tube (the window) – approximately 0.5 mm Al equivalent

Added Filtration 1 or 2 mm sheet of aluminum between the tube housing and the collimator The collimator contributes an additional 1mm Al equivalent added filtration

Compensating filter A filter usually made of Al, but plastic can be used to maintain OD when patient anatomy varies greatly in thickness Are useful in maintaining image quality. They are not radiation protection devices

Wedge filter

Compensating Filter What is an aspect of the tube design that works as a compensating filter? What causes this?

Avez-vous des questions? ¿Tiene alguna pregunta?