Treatment Machines for External Beam Radiotherapy

Slides:



Advertisements
Similar presentations
Introduction to RF for Accelerators
Advertisements

PowerPoint ® Presentation Chapter 4 System Components and Configurations Components Electricity Sources System Configurations.
Beam Therapy Equipment 2 Linear Accelerator Head.
CHAPTER 3 MICROWAVE ‘O’ TYPE TUBES
Microwave Tubes.
CHAPTER 4 HELIX TRAVELING-WAVE TUBES(TWT’S)
Areal RF Station A. Vardanyan RF System The AREAL RF system will consist of 3 RF stations: Each RF station has a 1 klystron, and HV modulator,
Areal RF Station A. Vardanyan RF System The AREAL RF system will consist of 3 RF stations: Each RF station has a 1 klystron, and HV modulator,
CHAPTER 5 CROSSED-FIELD TUBES (M-TYPE TUBES)
POTENTIAL GRADIENT & CATHODE RAY TUBE
RF-Gun cavity for high charge electron generation Takuya Natsui.
Dental X-ray Machine 118 Radiology.
Physics of Radiation Therapy
ACVR Artifacts Artifacts of Diagnostic Radiology
Bunch shape monitor for Linac-4 A.V.Feschenko Institute For Nuclear Research (INR), Moscow , Russia.
Resident Physics Lectures
Department of Radiation Physics
BME 560 Medical Imaging: X-ray, CT, and Nuclear Methods X-ray Instrumentation Part 1.
University of Idaho Research Colloquium Microwave Electron Linear Accelerators for Cancer Therapy and Non-Destructive Testing: History, Application & Theory.
Beam Therapy Equipment 3 Patient Treatment and Accessories.
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.
Accelerators We’ve seen a number of examples of technology transfer in particle detector development from HEP (basic science) to industry (medical, …)
Beam Therapy Equipment
- Kim Couthinho -Theon Couthinho - Neil Crasto - Frigen Dabre - Zelem Dabre.
Week one Chapters one and two
1 Waveguides This is the conduit that links the transmitter to the duplexer and antenna It is a hollow conducting tube along which the microwave energy.
Conventional Tubes Conventional Device tubes cannot be used for frequencies above 100MHz 1. Interelectrode capacitance 2. Lead Inductance effect 3. Transit.
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.
Physics of Particle Accelerators Kalanand Mishra Department of Physics University of Cincinnati.
Radiation Protection in Radiotherapy
ECE 662 – Microwave Electronics Cross-Field Devices: Magnetrons April 7, 14, 2005.
Particle Accelerators
1 C-Band Linac Development Satoshi Ohsawa 2004.Feb.19LCPAC.
Visits to Chinese accelerator companies Peter Pearce (April 2004) Two companies were visited. Beijing Medical Equipment Institute at Chongping and Beijing.
Electrostatic Deflection and Focus Control.  The cathode ray tube consists essentially of an "electron gun" for producing a beam of rapidly moving electrons.
CT Instrumentation and X-ray system
Medical Accelerator F. Foppiano, M.G. Pia, M. Piergentili
Linear accelerator in medicine  XR Tubes  Particles Accelerators  Betatron  Cyclotron  Synchrocyclotron  Synchrotron  Linear accelerator.
Non Traditional Machining Processes MIME Presented by, µAbhijit Thanedar µNaga Jyothi Sanku µPritam Deshpande µVijayalayan Krishnan µVishwajeet.
Travelling Wave Tube For Broadband amplifier helix TWTs (proposed by Pierce and others in 1946 ) are widely used For High average power purposes the.
Electron beam machining (EBM) – MM461 Dr. Dermot Brabazon Sch. Of Mech. and Manu. Eng. Dublin City University.
The electron.  An indivisible quantity of charge that orbits the nucleus of the atom.
ELECTRON BEAM WELDING The electron beam gun has a tungsten filament which is heated, freeing electrons. The electrons are accelerated from the source with.
Linacs for Cargo Screening Dr Graeme Burt Lancaster University, Cockcroft Institute CERN High gradient Day 2015.
Book Reference : Pages To understand that the path of a charged particle in a magnetic field is circular 2.To equate the force due to the magnetic.
Microwave Devices.
1 LONGITUDINAL DYNAMICS Slides of Frank Tecker CERN, BE-OP Presented by Piotr Skowronski CERN, BE-ABP Part One.
Medical Equipment Technology Department 1 Introduction to Biomed. Imaging Systems Lecture No.5-6 Dr. Yousif Mohamed Y. Abdallah.
Bremsstrahlung Example of conservation of energy Radiative energy loss by fast electron when slowed near nucleus Results in spectrum of energies from many.
Electrons Thermionic Emission
© 2013 MITSUBISHI HEAVY INDUSTRIES, LTD. All Rights Reserved. An example of Technical Innovation Cascade Dynamic Tracking Radiation Therapy System US-Japan.
Applications of electron linear accelerators for radiotherapy
HEBT Design Considerations Jingyu Tang, Xiangqi Wang, Hao Hao, Jiajia Tian IHEP, USTC International Review Meeting on Accelerator Physics Design of C-ADS,
X-ray tube.
Diagnostic Radiology II X-ray Tubes. Anode angle Anode angle defined as the angle of the target surface with respect to the central ray in the x-ray field.
Areal RF Station A. Vardanyan
Chapter 4 Clinical Radiation Generators
Visit for more Learning Resources
Development of X-band 50MW klystron in BVERI
X-RAY PRODUCTION AND EXPOSURE FACTORS
Ch 4. Clinical Radiation Generators
X-Radiation.
Source Technologies and Magnets
Electron-Beam Machining
Resident Physics Lectures
Principles and Practice of Radiation Therapy
B.Sc.II, Paper VIII ( IIISemester)
Machine Sources of Radiation
Electron mode A B C D > 4 GeV e- θ g e- DR α PS
Presentation transcript:

Treatment Machines for External Beam Radiotherapy By Dr: Nahla Nagy Assistant Professor Radiological Science

Components of modern linacs IAEA LINACS Components of modern linacs  Linacs are usually mounted isocentrically and the operational systems are distributed distinct sections of the machine: over five major and • Gantry Gantry stand and support Modulator cabinet Patient support assembly Control console

LINACS 5.5.3 Components of modern linacs  IAEA LINACS 5.5.3 Components of modern linacs  The main beam forming components of a modern medical linac (1) (2) (3) (4) (5) (6) are usually grouped into six classes: Injection system Radiofrequency power generation system Accelerating waveguide Auxiliary system Beam transport system collimation and monitoring system

LINACS 5.5.4 Configuration of modern linacs  In IAEA LINACS 5.5.4 Configuration of modern linacs  In • the simplest and most practical configuration: Electron source and the x-ray target form part of the accelerating waveguide Since the target is embedded into the waveguide, this linac type cannot produce electron beams.

LINACS 5.5.4 Configuration of modern linacs  IAEA LINACS 5.5.4 Configuration of modern linacs  Accelerating waveguides for intermediate (8 – 15 MV) and high (15 – 30 MV) energy linacs are located: • Either in the gantry parallel to the gantry axis of rotation Or in the gantry stand. In both cases, a beam transport system is used to transport the electron beam from the accelerating target. waveguide to the x-ray The radiofrequency power source in mounted in the gantry stand both configurations is

 Configurations for intermediate and high energy linacs IAEA Waveguide in the gantry Waveguide in the gantry stand RF power source in gantry stand RF power source in gantry stand

LINACS Injection system   IAEA LINACS Injection system  The linac injection system is the source of electrons, a simple electrostatic accelerator referred to as the electron gun. Both electron gun types contain: • Heated filament cathode Perforated grounded anode Triode gun also incorporates a grid 

IAEA  Two types of electron gun producing electrons in linac:

Radiofrequency power generation system IAEA LINACS Radiofrequency power generation system The radiofrequency power generation system produces the microwave radiation used in the accelerating waveguide to accelerate electrons to the desired kinetic energy and consists  of • two major components: RF power source (magnetron or klystron) Pulsed modulator •

 Accelerating waveguide is obtained from a cylindrical IAEA  Accelerating waveguide is obtained from a cylindrical uniform waveguide by adding a series of disks (irises) with circular holes at the centre, placed at equal distances of cavities. along the tube to form a series

   The role of the disks (irises) is to slow the phase velocity of IAEA  The role of the disks (irises) is to slow the phase velocity of the RF wave to a velocity below the speed of light in vacuum to allow acceleration of electrons.  The free accelerating waveguide is evacuated (106 tor) to propagation of electrons. cavities serve two purposes: allow  • To couple and distribute microwave power between adjacent cavities. To provide a suitable electric field pattern for electron acceleration. •

 Two types of accelerating waveguide are in use: IAEA • Traveling wave structure Standing wave structure

LINACS Auxiliary system  IAEA LINACS Auxiliary system  Auxiliary service consists of four systems that are not directly involved with electron acceleration: • Vacuum pumping system producing high vacuum in the accelerating waveguide. • Water cooling system for cooling the accelerating waveguide, target, circulator and RF generator. • Air pressure system for pneumatic movement of the target and beam shaping components. other • Shielding against leakage radiation produced by target, beam transport system and RF generator.

Electron beam transport IAEA LINACS Electron beam transport  In medium-energy and high-energy linacs an electron beam transport system is used to transport from the accelerating waveguide to: electrons • X-ray target in x-ray beam therapy Beam exit window in electron beam therapy  Beam transport system consists of: • Drift tubes Bending magnets Steering coild Focusing coils Energy slits

LINACS 5.5.11 Linac treatment head   IAEA LINACS 5.5.11 Linac treatment head  Electrons forming the electron pencil beam: • Originate in the electron gun. Are accelerated in the accelerating waveguide to the desired kinetic energy. Are brought through the beam transport system into the linac treatment head. •  The clinical x-ray beams or clinical electron beams are produced in the linac treatment head.

Production of clinical x-ray beams IAEA LINACS Production of clinical x-ray beams  Typical linac. electron pulses arriving on the x-ray target of a Typical values: Pulse height: 50 mA Pulse duration: 2 s Repetition rate: 100 pps Period: 104 s  The target is insulated from ground, acts as a Faraday cup, and allows measurement of the electron charge striking the target.

LINACS Beam collimation   IAEA LINACS Beam collimation  In modern linacs the x-ray beam collimation is achieved with three collimation devices: • Primary collimator. Secondary adjustable beam defining collimator (independent Multileaf collimator (MLC). jaws).  The electron beam collimation is achieved with: • Primary collimator. Secondary collimator. Electron applicator (cone). Multileaf collimator (under development).

Production of clinical electron IAEA LINACS Production of clinical electron beam  To activate the electron mode the x-ray target and flattening filter are removed from the electron pencil beam. Two techniques for producing clinical electron beams from the pencil electron beam:  • Pencil beam scattering with a scattering foil (thin foil of lead). Pencil beam scanning with two computer controlled magnets. •

Thank you for your attention