Chapter XIII. PDD TAR TMR Dose Free Space

Size: px
Start display at page:

Download "Chapter XIII. PDD TAR TMR Dose Free Space"

Transcription

1 Ver 2.11 Chapter XIII PDD TAR TMR Dose Free Space Joseph F. Buono RTT Allied Health Science Nassau Community College 1 Education Drive Garden City, NY phone: oice Secretary joseph.buono@ncc.edu website: rtscanner.com page setup Title

2 Menu - Objectives - next by deault - Dose in ree space - BackScatter Factor ( BSF ) - Percentage Depth Dose ( PDD ) - Tissue Air Ratio ( TAR ) - Dose to second point ( i.e. - Cord Dose ) or SSD setup - Tissue Maximum Ratio ( TMR ) - Dose to second point ( i.e. - Cord Dose ) or SAD setup - Relationship between BSF, PDD, TAR, TMR - Conversion between PDD & TAR (also TMR) Menu

3 Objectives 1 - Deine Dose in Free Space. 2 - Deine BackScatter Factor ( BSF ). 3 - State the actors that eect BackScatter Factor ( BSF ). 4 - Deine Percantage Depth Dose ( PDD ). 5 - State the actors that eect Percentage Depth Dose ( PDD ). 6 - Deine Tissue Air Ratio ( TAR ). 7 - State the actors that eect Tissue Air Ratio ( TAR ). 8 - Deine Tissue Maximum Ratio ( TMR ). 9 - State the actors that eect Tissue Maximum Ratio ( TMR ) State the relationship between TAR, TMR and BSF State the relationship between TAR table and BSF. obj 1

4 Dose in Free Space Dose in Free Space DFS 0

5 source Dose in Free Space radiation beam ionization chamber build-up cap point in space The exposure measured in Air at the center o the chamber is: X exposure Meter reading C T,P,S N x Exposure measured in Roentgen Correction actors due to Temperature Pressure Stem error Calibration actor DFS 1

6 source Dose in Free Space The reading rom the ionization chamber gives the X exposure at the center o the beam without the perturbing inluence o the chamber. Next, need to place a small mass o tissue at the center o the beam, who's radius is equal to depth dmax. The dose at the center o the mass o tissue is reerred to as the dose in "ree space" X exposure which is equal to: X exposure Meter reading C T,P,S N x D s X exposure tissue A eq where: END Dose in Free Space tissue is the Roentgen to rad conversion actor or tissue next BackScatter Factor DFS 2

7 BackScatter Factor BackScatter Factor BSF 0

8 BackScatter Factor ixed distance (usually machine operating distance) generally 100 cm Linac 80 cm Co60 central axis beam Find dose in "ree space on the central axis. D.s. D.s. Find maximum dose in a phantom on the central axis at a ixed distance. D dmax D dmax BSF 1

9 BackScatter Factor NOTE: Deinition: D dmax BSF D.s. Since the dose at Dmax (D dmax ) will always be equal to OR greater then the dose in ree space (D.s. ), BackScatter Factors (BSF) will always be equal to OR greater then 1. As the photon energy increases the BSF will become closer to 1. BSF is dependent on: D.s. D dmax 1) Energy increase in energy decrease in BSF (max BSF.6 to.8 mm Cu HVL) depending on ield size can be as large as 1.5 2) Field Size increase in F.S. increases BSF 3) SSD independent o SSD BSF 2

10 Percentage Depth Dose Percentage Depth Dose PDD 0

11 Percentage Depth Dose Beam Fixed SSD central axis generally 100 cm Linac 80 cm Co60 Find maximum dose on central axis. D dmax D dmax D d phantom Find dose at some other depth on central axis. D d PDD 1

12 Percentage Depth Dose Percentage Depth depth has been deined as: depth PDD d 100% Dmax D PDD d d 100% D dmax D dmax D d PDD 2

13 Percentage Depth Dose PDD is dependent on: Percentage Depth depth has been deined as: depth PDD d 100% Dmax D PDD d d 100% D dmax D dmax D d SSD 1) Energy an increase in energy increases PDD 2) Field Size an increase in F.S. increases PDD (because o an increase in scatter) 3) Depth o Tissue an increase in depth decreases PDD 4) SSD an increase in SSD increases PDD ( due to the inverse square law and the act that PDD is deined at two dierent points ) two dierent distances rom the source SSD + dmax SSD + depth PDD 3

14 Tissue Air Ratio Tissue Air Ratio TAR 0

15 Tissue Air Ratio Distance rom source Beam generally 100 cm Linac 80 cm Co60 central axis Find dose in "ree space on the central axis. D.s. D.s. TAR 1

16 Tissue Air Ratio Distance rom source Beam generally 100 cm Linac 80 cm Co60 central axis d Find dose in "ree space on the central axis. D.s. D.s. Find dose in phantom at depth on the central axis at the same distance rom source. D d D d TAR 2

17 Tissue Air Ratio Distance rom source Beam generally 100 cm Linac 80 cm Co60 central axis d Deinition: D TAR d d D.s. D.s. TAR is dependent on: 1) Energy an increase in energy increases TAR 2) Field Size an increase in F.S. increases TAR (because o an increase in scatter) 3) Depth o Tissue an increase in depth decreases TAR D d 4) SAD (distance) independent o distance both reading at same distance rom the source D.s. D d TAR 3

18 Tissue Air Ratio Distance rom source Beam Note: I depth is changed to dmax then: D TAR dmax dmax D BSF dmax D.s. D.s. generally 100 cm Linac 80 cm Co60 central axis d Deinition: D TAR d d D.s. D.s. TAR is dependent on: 1) Energy an increase in energy increases TAR 2) Field Size an increase in F.S. increases TAR (because o an increase in scatter) 3) Depth o Tissue an increase in depth decreases TAR D dmax 4) SAD (distance) independent o distance both reading at same distance rom the source D.s. D d TAR 3

19 Tissue Maximum Ratio Tissue Maximum Ratio TMR 0

20 Tissue Maximum Ratio Distance rom source generally 100 cm Linac 80 cm Co60 Beam central axis Place phantom such that the ionization chamber is at depth o maximum dose. depth dmax Ionization Chamber D dmax dmax Turn beam on and record dose reading. D dmax TMR 1

21 Tissue Maximum Ratio 100 cm Linac 80 cm Co60 central axis Find dose at depth in the phantom at the same distance rom the source. D d central axis d dmax D dmax D d TMR 2

22 Tissue Maximum Ratio Deinition: 100 cm Linac 80 cm Co60 central axis D TMR d d D dmax central axis d dmax D dmax D d TMR is dependent on: 1) Energy an increase in energy increases TMR 2) Field Size an increase in F.S. increases TMR (because o an increase in scatter) 3) Depth o Tissue an increase in depth decreases TMR 4) SAD (distance) independent o distance both reading at same distance rom the source D dmax. D d TMR 3

23 Relationship between BSF, PDD, TAR, TMR Relationship between BSF, PDD, TAR, TMR REL 0

24 Relationship between BSF, PDD, TAR, TMR SOURCE (SAD) IONIZATION CHAMBER BUILDUP CAP BSF REL 1

25 Relationship between BSF, PDD, TAR, TMR SOURCE (SAD) d 1 BSF TAR d1 REL 2

26 Relationship between BSF, PDD, TAR, TMR SOURCE (SAD) d 1 BSF TAR d1 TMR.s.1 REL 3

27 Relationship between BSF, PDD, TAR, TMR SOURCE (SAD) (ODI,SSD) d 1 dmax2 Note: d 1 BSF TAR d1 TMR.s.1 PD REL 4

28 Relationship between BSF, PDD, TAR, TMR (SAD) d 1 (ODI,SSD) dmax2 Note: d 1 BSF TAR TMR d1 PD.s.1 REL 6

29 Relationship between BSF, PDD, TAR, TMR (SAD) d 1 (ODI,SSD) dmax2 Note: d 1 BSF TAR TMR d1 PD.s.1 solve BSF equation or solve TAR d1 equation or BSF TAR d1 Both equations are equal to "Dose in ree space", thereore they are equal to each other. REL 7

30 Relationship between BSF, PDD, TAR, TMR (SAD) d 1 (ODI,SSD) dmax2 Note: d 1 BSF TAR TMR d1 PD.s.1 BSF rearranging terms: TAR d1 REL 8

31 Relationship between BSF, PDD, TAR, TMR (SAD) d 1 (ODI,SSD) dmax2 Note: d 1 BSF TAR TMR d1 PD.s.1 BSF rearranging terms: TAR d1 TAR d1 BSF TMR BUT: dmax1 thereore: TMR d1 TAR d1 BSF rearranging terms: TAR d1 TMR d1 BSF REL 9

32 Relationship between BSF, PDD, TAR, TMR (SAD) d 1 (ODI,SSD) dmax2 Note: d 1 BSF TAR TMR d1 PD.s.1 TAR d1 TMR d1 BSF One other important relationship is between TAR's and BSF. TAR d1 I depth d1 is equal to dmax1 then: TAR d1 BUT: Thereore: At depth Dmax TARs are equal to BSFs REL 10

33 Conversion between PDD & TAR (& TMR) Conversion between PDD & TAR (also TMR) TMR 0

34 Conversion between PDD & TAR (& TMR) SOURCE (SAD) (ODI,SSD) d 1 dmax2 Note: d 1 D.s.2 TMR 1

35 Conversion between PDD & TAR (& TMR) (SAD) d 1 (ODI,SSD) dmax2 Note: d 1 D.s.2 TMR 2

36 Conversion between PDD & TAR (& TMR) (SAD) d 1 (ODI,SSD) dmax2 Note: d 1 D.s.2 BSF 1 note: This is or ield size at distance TMR 3

37 Conversion between PDD & TAR (& TMR) (SAD) d 1 (ODI,SSD) dmax2 Note: d 1 D.s.2 BSF 1 TAR D 2.s.1 D.s.2 note: This is or depth d2. This is or the ield size at a distance equal to + d2. Which can be said to be an SAD equal to + d2. TMR 4

38 Conversion between PDD & TAR (& TMR) (SAD) d 1 (ODI,SSD) dmax2 Note: d 1 D.s.2 BSF 1 TAR D 2.s.1 PDD D 2.s.2 TMR 5

39 Conversion between PDD & TAR (& TMR) (SAD) d 1 (ODI,SSD) dmax2 Note: d 1 D.s.2 Solving this equation or BSF 1 TAR D 2.s.1 PDD D 2.s.2 I 1 I 2 2 d1 2 TAR 2 Substitute this into PDD 2 equation or. D.s.2 PDD 2 TAR 2 D.s.2 At this point need to realize that D max1 and D max2 are related by the "Inverse Square Law" Thus: TMR 6

40 Conversion between PDD & TAR (& TMR) (SAD) d 1 (ODI,SSD) dmax2 Note: d 1 D.s.2 BSF 1 TAR D 2.s.1 PDD D 2.s.2 I 1 I 2 2 d1 2 PDD 2 TAR 2 D.s.2 2 TMR 7

41 Conversion between PDD & TAR (& TMR) (SAD) d 1 (ODI,SSD) dmax2 Note: d 1 D.s.2 BSF 1 TAR D 2.s.1 PDD D 2.s.2 I 1 I 2 2 d1 2 ( + dm) 2 2 PDD 2 TAR 2 D.s.2 TMR 8

42 Conversion between PDD & TAR (& TMR) (SAD) d 1 (ODI,SSD) dmax2 Note: d 1 D.s.2 BSF 1 TAR D 2.s.1 PDD D 2.s.2 I 1 I 2 2 d1 2 PDD 2 TAR 2 D.s.2 ( + dm) 2 solving this equation or: 2 2 ( + dm) 2 Substitute this into PDD 2 equation. PDD 2 TAR 2 D.s.2 TMR 9

43 Conversion between PDD & TAR (& TMR) (SAD) d 1 (ODI,SSD) dmax2 Note: d 1 D.s.2 BSF 1 TAR D 2.s.1 PDD D 2.s.2 I 1 I 2 2 d1 2 PDD 2 TAR 2 D.s.2 ( + dm) ( + dm) 2 TAR 2 D.s.2 ( + dm) 2 PDD 2 2 TMR 10

44 Conversion between PDD & TAR (& TMR) (SAD) d 1 (ODI,SSD) dmax2 Note: d 1 D.s.2 BSF 1 TAR D 2.s.1 PDD D 2.s.2 TAR 2 D.s.2 ( + dm) 2 PDD 2 2 BUT: BSF 1 Solving or: D max1 BSF 1 TMR 11

45 Conversion between PDD & TAR (& TMR) (SAD) d 1 (ODI,SSD) dmax2 Note: d 1 D.s.2 BSF 1 TAR D 2.s.1 PDD D 2.s.2 TAR 2 D.s.2 ( + dm) 2 PDD 2 2 BUT: BSF 1 Solving or: D max1 TAR 2 D.s.2 ( + dm) 2 PDD 2 BSF 2 1 BSF 1 Substituting or: D max1 TMR 12

46 Conversion between PDD & TAR (& TMR) (SAD) d 1 (ODI,SSD) dmax2 Note: d 1 D.s.2 BSF 1 TAR D 2.s.1 PDD D 2.s.2 TAR 2 D.s.2 ( + dm) 2 PDD 2 2 TAR 2 D ( + dm) 2.s.2 PDD 2 BSF 2 1 BUT the relationship between and D.s.2 is by the "Inverse Square Law". THUS: substituting into the equation invert I 1 D.s.2 I 2 I 2 2 d1 2 I 1 d 1 2 d2 2 2 ( + ) 2 substituting into the equation TMR 13

47 Conversion between PDD & TAR (& TMR) (SAD) d 1 (ODI,SSD) dmax2 Note: d 1 D.s.2 BSF 1 TAR D 2.s.1 PDD D 2.s.2 TAR 2 D.s.2 ( + dm) 2 PDD 2 2 TAR 2 PDD 2 BSF 1 2 ( + dm) 2 ( + ) 2 2 D.s.2 2 ( + ) 2 TMR 14

48 Conversion between PDD & TAR (& TMR) (SAD) d 1 (ODI,SSD) dmax2 Note: d 1 D.s.2 BSF 1 TAR D 2.s.1 PDD D 2.s.2 TAR 2 D.s.2 ( + dm) 2 PDD 2 2 TAR ( + dm) 2 PDD 2 BSF 2 1 ( + ) 2 TAR 2 + dm PDD 2 BSF 1 ( + ) 2 ( ) 2 END TMR 15

Clinical Physics. Dr/Aida Radwan Assistant Professor of Medical Physics Umm El-Qura University

Clinical Physics. Dr/Aida Radwan Assistant Professor of Medical Physics Umm El-Qura University Clinical Physics Dr/Aida Radwan Assistant Professor of Medical Physics Umm El-Qura University Physics of Radiotherapy using External Beam Dose distribution PHANTOMS Basic dose distribution data are usually

More information

The Geometry of Perspective Projection

The Geometry of Perspective Projection The Geometry o Perspective Projection Pinhole camera and perspective projection - This is the simplest imaging device which, however, captures accurately the geometry o perspective projection. -Rays o

More information

Challenges in small field MV photon dosimetry

Challenges in small field MV photon dosimetry Challenges in small field MV photon dosimetry Maria Mania Aspradakis Cantonal Hospital of Lucerne, Lucerne, Switzerland Cantonal Hospital of Lucerne, Lucerne, Switzerland maria.aspradakis@ksl.ch Why are

More information

Chapter 8 ELECTRON BEAMS: PHYSICAL AND CLINICAL ASPECTS

Chapter 8 ELECTRON BEAMS: PHYSICAL AND CLINICAL ASPECTS Chapter 8 ELECTRON BEAMS: PHYSICAL AND CLINICAL ASPECTS W. STRYDOM Department of Medical Physics, Medical University of Southern Africa, Pretoria, South Africa W. PARKER, M. OLIVARES Department of Medical

More information

The effects of radiation on the body can be divided into Stochastic (random) effects and deterministic or Non-stochastic effects.

The effects of radiation on the body can be divided into Stochastic (random) effects and deterministic or Non-stochastic effects. RADIATION SAFETY: HOW TO EDUCATE AND PROTECT YOURSELF AND YOUR STAFF John Farrelly, DVM, MS, ACVIM (Oncology), ACVR (Radiation Oncology) Cornell University Veterinary Specialists The Veterinary Cancer

More information

Irradiation Field Size: 5cmX5cm 10cmX10cm 15cmX15cm 20cmX20cm. Focus-Surface Distance: 100cm. 20cm Volume of Ion Chamber : 1cmX1cmX1cm

Irradiation Field Size: 5cmX5cm 10cmX10cm 15cmX15cm 20cmX20cm. Focus-Surface Distance: 100cm. 20cm Volume of Ion Chamber : 1cmX1cmX1cm Proceedings of the Ninth EGS4 Users' Meeting in Japan, KEK Proceedings 200-22, p.5-8 MONTE CARLO SIMULATION ANALYSIS OF BACKSCATTER FACTOR FOR LOW-ENERGY X-RAY K. Shimizu, K. Koshida and T. Miyati Department

More information

Clinical Photon Beams

Clinical Photon Beams Dosimetric Characteristics of Clinical Photon Beams Jatinder R Palta PhD University of Florida Department of Radiation Oncology Gainesville, Florida Disclosures Research development grants from Philips

More information

Reduction of Electron Contamination Using a Filter for 6MV Photon Beam

Reduction of Electron Contamination Using a Filter for 6MV Photon Beam J. Korean Soc Ther Radiol Oncol : Vol. 15, No. 2, June, 1997 Reduction of Electron Contamination Using a Filter for 6MV Photon Beam Choul Soo Lee, MPH., Myung Jin Yoo, Ph.D. and Ha Yong Yum, M.D. Department

More information

AAPM s TG-51 protocol for clinical reference dosimetry of high-energy photon and electron beams

AAPM s TG-51 protocol for clinical reference dosimetry of high-energy photon and electron beams AAPM s TG-51 protocol for clinical reference dosimetry of high-energy photon and electron beams Peter R. Almond Brown Cancer Center, Louisville, Kentucky 40202 Peter J. Biggs Department of Radiation Oncology,

More information

Study the Quality Assurance of Conventional X-ray Machines Using Non Invasive KV meter

Study the Quality Assurance of Conventional X-ray Machines Using Non Invasive KV meter Study the Quality Assurance of Conventional X-ray Machines Using Non Invasive KV meter T.M.Taha Radiation Protection Department, Nuclear Research Center, Atomic Energy Authority, Cairo.P.O.13759 Egypt.

More information

5.2 ASSESSMENT OF X-RAY TUBE LEAKAGE RADIATION AND X-RAY TUBE OUTPUT TOTAL FILTRATION

5.2 ASSESSMENT OF X-RAY TUBE LEAKAGE RADIATION AND X-RAY TUBE OUTPUT TOTAL FILTRATION 5.2 ASSESSMENT OF X-RAY TUBE LEAKAGE RADIATION AND X-RAY TUBE OUTPUT TOTAL FILTRATION 5.2.1 Task The bremsstrahlung produced by the X-ray tube has a continuous spectrum, limited by the set and spreads

More information

ACCELERATORS AND MEDICAL PHYSICS 2

ACCELERATORS AND MEDICAL PHYSICS 2 ACCELERATORS AND MEDICAL PHYSICS 2 Ugo Amaldi University of Milano Bicocca and TERA Foundation EPFL 2-28.10.10 - U. Amaldi 1 The icone of radiation therapy Radiation beam in matter EPFL 2-28.10.10 - U.

More information

3D SCANNER. 3D Scanning Comes Full Circle. Your Most Valuable QA and Dosimetry Tools

3D SCANNER. 3D Scanning Comes Full Circle. Your Most Valuable QA and Dosimetry Tools 3D SCANNER 3D Scanning Comes Full Circle Your Most Valuable QA and Dosimetry Tools BETTER OUTCOMES THROUGH TECHNOLOGY The 3D SCANNER is different by design. 3D SCANNER has been developed from the ground

More information

Dose Measurement in Mammography; What are we measuring? David E. Hintenlang, Ph.D. DABR University of Florida

Dose Measurement in Mammography; What are we measuring? David E. Hintenlang, Ph.D. DABR University of Florida Dose Measurement in Mammography; What are we measuring? David E. Hintenlang, Ph.D. DABR University of Florida Average Glandular Dose Required measurement performed by medical physicist as part of Mammography

More information

In room Magnetic Resonance Imaging guided Radiotherapy (MRIgRT( MRIgRT) Jan Lagendijk and Bas Raaymakers

In room Magnetic Resonance Imaging guided Radiotherapy (MRIgRT( MRIgRT) Jan Lagendijk and Bas Raaymakers In room Magnetic Resonance Imaging guided Radiotherapy (MRIgRT( MRIgRT) Jan Lagendijk and Bas Raaymakers : Chris Bakker Boxue Liu Alexander Raaijmakers Rajko Topolnjak Richard van de Put Uulke van der

More information

Worldwide Quality Assurance networks for radiotherapy dosimetry

Worldwide Quality Assurance networks for radiotherapy dosimetry Worldwide Quality Assurance networks for radiotherapy dosimetry Joanna Izewska Dosimetry and Medical Radiation Physics Section dosimetry@iaea.org Audit in radiotherapy dosimetry Objectives to enhance confidence

More information

RADIATION THERAPY. Dosimetry Pioneers since 1922 NEW

RADIATION THERAPY. Dosimetry Pioneers since 1922 NEW RADIATION THERAPY Dosimetry Pioneers since 1922 NEW New Product Releases 2015 One phantom multiple options 4D Patient and Machine QA Modular Phantom for Stay flexible. Go modular. } Revolutionary new modular

More information

Use of the VALIDATOR Dosimetry System for Quality Assurance and Quality Control of Blood Irradiators

Use of the VALIDATOR Dosimetry System for Quality Assurance and Quality Control of Blood Irradiators Technical Note: 9 Use of the VALIDATOR Dosimetry System for Quality Assurance and Quality Control of Blood Irradiators 1- Introduction The VALIDATOR, model TN-ID-60, is a compact, and stand-alone dosimetry

More information

AAPM protocol for 40 300 kv x-ray beam dosimetry in radiotherapy and radiobiology

AAPM protocol for 40 300 kv x-ray beam dosimetry in radiotherapy and radiobiology AAPM protocol for 40 300 kv x-ray beam dosimetry in radiotherapy and radiobiology C.-M. Ma, Chair a) Radiation Oncology Dept., Stanford University School of Medicine, Stanford, California 94305-5304 and

More information

The electrical field produces a force that acts

The electrical field produces a force that acts Physics Equipotential Lines and Electric Fields Plotting the Electric Field MATERIALS AND RESOURCES ABOUT THIS LESSON EACH GROUP 5 alligator clip leads 2 batteries, 9 V 2 binder clips, large computer LabQuest

More information

Portuguese Health Physics Society: Calibrating Pen Dosimeters with and without a Phantom

Portuguese Health Physics Society: Calibrating Pen Dosimeters with and without a Phantom Portuguese Health Physics Society: Calibrating Pen Dosimeters with and without a Phantom Fernanda B. C. Nonato, Claudinei T. Cescon and Linda V. E. Caldas, Instituto de Pesquisas Energéticas e Nucleares,

More information

ABSORBED DOSE DETERMINATION IN EXTERNAL BEAM RADIOTHERAPY

ABSORBED DOSE DETERMINATION IN EXTERNAL BEAM RADIOTHERAPY TECHNICAL REPORTS SERIES No. 398 Absorbed Dose Determination in External Beam Radiotherapy An International Code of Practice for Dosimetry Based on Standards of Absorbed Dose to Water Sponsored by the

More information

Historical Reconstruction of Co-60 Radiotherapy Doses to Patients with Hodgkin s Lymphoma

Historical Reconstruction of Co-60 Radiotherapy Doses to Patients with Hodgkin s Lymphoma Historical Reconstruction of Co-60 Radiotherapy Doses to Patients with Hodgkin s Lymphoma Heather M. Petroccia, MS Advanced Laboratory for Radiation Dosimetry Studies (ALRADS) Medical Physics Program J.

More information

3D SCANNERTM. 3D Scanning Comes Full Circle. s u n. Your Most Valuable QA and Dosimetry Tools A / B / C. The 3D SCANNER Advantage

3D SCANNERTM. 3D Scanning Comes Full Circle. s u n. Your Most Valuable QA and Dosimetry Tools A / B / C. The 3D SCANNER Advantage 3D SCANNERTM 3D Scanning Comes Full Circle Relative 3D Dosimetry offering the easiest setup, most objectivity, and best consistency available The 3D SCANNER Advantage Advanced Design Ring and diameter

More information

N K. dn dt. Theory of the dynamics of fisheries exploitation, and the concept of Maximum Sustainable Yield (MSY)

N K. dn dt. Theory of the dynamics of fisheries exploitation, and the concept of Maximum Sustainable Yield (MSY) Theory o the dynamics o isheries exploitation, and the concept o Maximum Sustainable ield (MS One o the most logically compelling ideas in population biology, but perhaps one o the most diicult to demonstrate

More information

Performance evaluation and quality assurance of Varian enhanced dynamic wedges

Performance evaluation and quality assurance of Varian enhanced dynamic wedges JOURNAL OF APPLIED CLINICAL MEDICAL PHYSICS, VOLUME 7, NUMBER 1, WINTER 2006 Performance evaluation and quality assurance of Varian enhanced dynamic wedges Parham Alaei and Patrick D. Higgins Department

More information

Facility Start Up, Training, and Operational Issues AT PTC H or Protons A Positive Marathon Inelastic Collision Experience

Facility Start Up, Training, and Operational Issues AT PTC H or Protons A Positive Marathon Inelastic Collision Experience Facility Start Up, Training, and Operational Issues AT PTC H or Protons A Positive Marathon Inelastic Collision Experience Presented from a Physics Bias Michael Gillin, Ronald Zhu, Narayan Sahoo And Many

More information

DETERMINATION OF THE EFFECTIVE VOLUME OF AN EXTRAPOLATION CHAMBER FOR X-RAY DOSIMETRY

DETERMINATION OF THE EFFECTIVE VOLUME OF AN EXTRAPOLATION CHAMBER FOR X-RAY DOSIMETRY X Congreso Regional Latinoamericano IRPA de Protección y Seguridad Radiológica Radioprotección: Nuevos Desafíos para un Mundo en Evolución Buenos Aires, 12 al 17 de abril, 2015 SOCIEDAD ARGENTINA DE RADIOPROTECCIÓN

More information

Technical limits of Human Exposure to RF from Cellular Base Stations and Handsets

Technical limits of Human Exposure to RF from Cellular Base Stations and Handsets Ministry of Environmental Protection Ministry of Communications Technical limits of Human Exposure to RF from Cellular Base Stations and Handsets Based on author s PhD thesis/book- An analysis of regulatory

More information

Advanced variance reduction techniques applied to Monte Carlo simulation of linacs

Advanced variance reduction techniques applied to Monte Carlo simulation of linacs MAESTRO Advanced variance reduction techniques applied to Monte Carlo simulation of linacs Llorenç Brualla, Francesc Salvat, Eric Franchisseur, Salvador García-Pareja, Antonio Lallena Institut Gustave

More information

Recognition. Radiation Survey Objectives. Objectives. Part 1 Documentation Radiation Source Survey Objectives Radiation Detectors Techniques

Recognition. Radiation Survey Objectives. Objectives. Part 1 Documentation Radiation Source Survey Objectives Radiation Detectors Techniques Recognition I will take this opportunity to recognize and thank the following people s contributions to this presentation. Considerations for: Diagnostic Radiology, Nuclear Medicine and, Oncology M. S.

More information

TEACHING RADIOTHERAPY PHYSICS CONCEPTS USING SIMULATION: EXPERIENCE WITH STUDENT RADIOGRAPHERS IN LIVERPOOL, UK

TEACHING RADIOTHERAPY PHYSICS CONCEPTS USING SIMULATION: EXPERIENCE WITH STUDENT RADIOGRAPHERS IN LIVERPOOL, UK TEACHING RADIOTHERAPY PHYSICS CONCEPTS USING SIMULATION: EXPERIENCE WITH STUDENT RADIOGRAPHERS IN LIVERPOOL, UK M C Kirby, PhD Directorate of Medical Imaging and Radiotherapy, School of Health Sciences,

More information

Image Quality and Radiation Dose for Intraoral Radiography: Hand-Held Held (Nomad), Battery Powered

Image Quality and Radiation Dose for Intraoral Radiography: Hand-Held Held (Nomad), Battery Powered Image Quality and Radiation Dose for Intraoral Radiography: Hand-Held Held (Nomad), Battery Powered vs. Wall-Mount X-Ray X Systems Edgar Bailey*, MSEHE, CHP Consultant Joel Gray*, PhD, FAAPM DIQUAD, LLC

More information

CHAPTER 10. ACCEPTANCE TESTS AND COMMISSIONING MEASUREMENTS

CHAPTER 10. ACCEPTANCE TESTS AND COMMISSIONING MEASUREMENTS Review of Radiation Oncology Physics: A Handbook for Teachers and Students CHAPTER 10. ACCEPTANCE TESTS AND COMMISSIONING MEASUREMENTS JOHN L. HORTON Department of Radiation Physics University of Texas

More information

Chapter 7 CLINICAL TREATMENT PLANNING IN EXTERNAL PHOTON BEAM RADIOTHERAPY

Chapter 7 CLINICAL TREATMENT PLANNING IN EXTERNAL PHOTON BEAM RADIOTHERAPY Chapter 7 CLINICAL TREATMENT PLANNING IN EXTERNAL PHOTON BEAM RADIOTHERAPY W. PARKER, H. PATROCINIO Department of Medical Physics, McGill University Health Centre, Montreal, Quebec, Canada 7.1. INTRODUCTION

More information

Chapter 12 QUALITY ASSURANCE OF EXTERNAL BEAM RADIOTHERAPY

Chapter 12 QUALITY ASSURANCE OF EXTERNAL BEAM RADIOTHERAPY Chapter 12 QUALITY ASSURANCE OF EXTERNAL BEAM RADIOTHERAPY D.I. THWAITES Department of Oncology Physics, Edinburgh Cancer Centre, University of Edinburgh, Western General Hospital, Edinburgh, United Kingdom

More information

Lecture 2 Macroscopic Interactions. 22.106 Neutron Interactions and Applications Spring 2010

Lecture 2 Macroscopic Interactions. 22.106 Neutron Interactions and Applications Spring 2010 Lecture 2 Macroscopic Interactions 22.106 Neutron Interactions and Applications Spring 2010 Objectives Macroscopic Interactions Atom Density Mean Free Path Moderation in Bulk Matter Neutron Shielding Effective

More information

Physics testing of image detectors

Physics testing of image detectors Physics testing of image detectors Parameters to test Spatial resolution Contrast resolution Uniformity/geometric distortion Features and Weaknesses of Phantoms for CR/DR System Testing Dose response/signal

More information

External dosimetry Dosimetry in new radiotherapeutic techniques

External dosimetry Dosimetry in new radiotherapeutic techniques External dosimetry Dosimetry in new radiotherapeutic techniques Albert Lisbona Medical Physics Department CLCC René Gauducheau 44805 Saint-Herblain France a-lisbona@nantes.fnclcc.fr Objective : To describe

More information

Chapter 9 CALIBRATION OF PHOTON AND ELECTRON BEAMS

Chapter 9 CALIBRATION OF PHOTON AND ELECTRON BEAMS Chapter 9 CALIBRATION OF PHOTON AND ELECTRON BEAMS P. ANDREO Department of Medical Radiation Physics, University of Stockholm, Karolinska Institute, Stockholm, Sweden J.P. SEUNTJENS, E.B. PODGORSAK Department

More information

Development of on line monitor detectors used for clinical routine in proton and ion therapy

Development of on line monitor detectors used for clinical routine in proton and ion therapy Development of on line monitor detectors used for clinical routine in proton and ion therapy A. Ansarinejad Torino, february 8 th, 2010 Overview Hadrontherapy CNAO Project Monitor system: Part1:preliminary

More information

Energy. Mechanical Energy

Energy. Mechanical Energy Principles of Imaging Science I (RAD119) Electromagnetic Radiation Energy Definition of energy Ability to do work Physicist s definition of work Work = force x distance Force acting upon object over distance

More information

Monte Carlo Simulations: Efficiency Improvement Techniques and Statistical Considerations

Monte Carlo Simulations: Efficiency Improvement Techniques and Statistical Considerations Monte Carlo Simulations: Efficiency Improvement Techniques and Statistical Considerations Daryoush Sheikh-Bagheri, Ph.D. 1, Iwan Kawrakow, Ph.D. 2, Blake Walters, M.Sc. 2, and David W.O. Rogers, Ph.D.

More information

Department of Radiation Oncology H. Lee Moffitt Cancer Center Khosrow Javedan M.S, Craig Stevens MD, Ph.D., Ken Forster Ph.D.

Department of Radiation Oncology H. Lee Moffitt Cancer Center Khosrow Javedan M.S, Craig Stevens MD, Ph.D., Ken Forster Ph.D. Efficacy of IMRT with dot decimal compensators for radiotherapy of malignant pleural mesothelioma post extrapleural pneumonectomy Department of Radiation Oncology H. Lee Moffitt Cancer Center Khosrow Javedan

More information

X-ray Production. Target Interactions. Principles of Imaging Science I (RAD119) X-ray Production & Emission

X-ray Production. Target Interactions. Principles of Imaging Science I (RAD119) X-ray Production & Emission Principles of Imaging Science I (RAD119) X-ray Production & Emission X-ray Production X-rays are produced inside the x-ray tube when high energy projectile electrons from the filament interact with the

More information

Production of X-rays and Interactions of X-rays with Matter

Production of X-rays and Interactions of X-rays with Matter Production of X-rays and Interactions of X-rays with Matter Goaz and Pharoah. Pages 11-20. Neill Serman Electrons traveling from the filament ( cathode) to the target (anode) convert a small percentage

More information

World-first Proton Pencil Beam Scanning System with FDA Clearance

World-first Proton Pencil Beam Scanning System with FDA Clearance Hitachi Review Vol. 58 (29), No.5 225 World-first Proton Pencil Beam Scanning System with FDA Clearance Completion of Proton Therapy System for MDACC Koji Matsuda Hiroyuki Itami Daishun Chiba Kazuyoshi

More information

Principles of dosimetry The ionization chamber

Principles of dosimetry The ionization chamber Principles of dosimetry The ionization chamber FYS-KJM 4710 Audun Sanderud Department of Physics Ionometry 1) Ionometry: the measurement of the number of ionizations in substance The number of ionizations

More information

Design Project 2. Sizing of a Bicycle Chain Ring Bolt Set. Statics and Mechanics of Materials I. ENGR 0135 Section 1040.

Design Project 2. Sizing of a Bicycle Chain Ring Bolt Set. Statics and Mechanics of Materials I. ENGR 0135 Section 1040. Design Project 2 Sizing of a Bicycle Chain Ring Bolt Set Statics and Mechanics of Materials I ENGR 0135 Section 1040 November 9, 2014 Derek Nichols Michael Scandrol Mark Vavithes Nichols, Scandrol, Vavithes

More information

High-Energy Electron Beam Therapy Dosimetry with Ionisation Chambers

High-Energy Electron Beam Therapy Dosimetry with Ionisation Chambers Schweizerische Gesellschaft für Strahlenbiologie und Medizinische Physik Société Suisse de Radiobiologie et de Physique Médicale Società Svizzera di Radiobiologia e di Fisica Medica Swiss Society of Radiobiology

More information

Monte Carlo simulation of a scanning whole body counter and the effect of BOMAB phantom size on the calibration.

Monte Carlo simulation of a scanning whole body counter and the effect of BOMAB phantom size on the calibration. Monte Carlo simulation of a scanning whole body counter and the effect of BOMAB phantom size on the calibration. Gary H. Kramer, Linda C. Burns and Steven Guerriere Human Monitoring Laboratory, Radiation

More information

Production of X-rays. Radiation Safety Training for Analytical X-Ray Devices Module 9

Production of X-rays. Radiation Safety Training for Analytical X-Ray Devices Module 9 Module 9 This module presents information on what X-rays are and how they are produced. Introduction Module 9, Page 2 X-rays are a type of electromagnetic radiation. Other types of electromagnetic radiation

More information

Tom Wilson Product Marketing Manager Delivery Systems Varian Medical Systems International AG. CERN Accelerator School, May 2015

Tom Wilson Product Marketing Manager Delivery Systems Varian Medical Systems International AG. CERN Accelerator School, May 2015 INDUSTRIAL DESIGN Tom Wilson Product Marketing Manager Delivery Systems Varian Medical Systems International AG VARIAN ONCOLOGY SYSTEMS 1 VARIAN ONCOLOGY SYSTEMS CERN Accelerator, May 2015 Industrial Design

More information

Appendix I: Cryogenic Reference Tables

Appendix I: Cryogenic Reference Tables Appendix I: Cryogenic Reerence Tables Appendices 217 Appendix I: Cryogenic Reerence Tables Cryogenic heat low calculations The heat low Q conducted across small temperature dierences can be calculated

More information

INFO-0545 RADIOISOTOPE SAFETY MONITORING FOR RADIOACTIVE CONTAMINATION

INFO-0545 RADIOISOTOPE SAFETY MONITORING FOR RADIOACTIVE CONTAMINATION INFO-0545 RADIOISOTOPE SAFETY MONITORING FOR RADIOACTIVE CONTAMINATION 1. INTRODUCTION This document provides general guidance for monitoring and controlling radioactive contamination, and relating the

More information

Scan Time Reduction and X-ray Scatter Rejection in Dual Modality Breast Tomosynthesis. Tushita Patel 4/2/13

Scan Time Reduction and X-ray Scatter Rejection in Dual Modality Breast Tomosynthesis. Tushita Patel 4/2/13 Scan Time Reduction and X-ray Scatter Rejection in Dual Modality Breast Tomosynthesis Tushita Patel 4/2/13 Breast Cancer Statistics Second most common cancer after skin cancer Second leading cause of cancer

More information

THE IMPOSSIBLE DOSE HOW CAN SOMETHING SIMPLE BE SO COMPLEX? Lars Hode

THE IMPOSSIBLE DOSE HOW CAN SOMETHING SIMPLE BE SO COMPLEX? Lars Hode THE IMPOSSIBLE DOSE HOW CAN SOMETHING SIMPLE BE SO COMPLEX? Lars Hode Swedish Laser-Medical Society The dose is the most important parameter in laser phototherapy. At a first glance, the dose seem very

More information

Radiation Safety Characteristics of the NOMAD Portable X-ray System

Radiation Safety Characteristics of the NOMAD Portable X-ray System Radiation Safety Characteristics of the NOMAD Portable X-ray System D. Clark Turner 1, Donald K. Kloos 1, Robert Morton 2 1 Aribex, Inc., 754 South 400 East, Orem, UT 84097 USA, www.aribex.com 2 Quality

More information

Proton Radiotherapy. Cynthia Keppel Scientific and Technical Director Hampton University Proton Therapy Institute. Lead Virginia.

Proton Radiotherapy. Cynthia Keppel Scientific and Technical Director Hampton University Proton Therapy Institute. Lead Virginia. Proton Radiotherapy Cynthia Keppel Scientific and Technical Director Hampton University Proton Therapy Institute Lead Virginia g October 16, 2009 About Proton Therapy Cancer is the (2nd) largest cause

More information

NATIONAL SENIOR CERTIFICATE GRADE 12

NATIONAL SENIOR CERTIFICATE GRADE 12 NATIONAL SENI CERTIFICATE GRADE 1 PHYSICAL SCIENCES: PHYSICS (P1) NOVEMBER 010 MEMANDUM MARKS: 150 This memorandum consists o 3 pages. NOTE: Marking rule 1.5 was changed according to decisions taken at

More information

Rainfall generator for the Meuse basin

Rainfall generator for the Meuse basin KNMI publication; 196 - IV Rainall generator or the Meuse basin Description o 20 000-year simulations R. Leander and T.A. Buishand De Bilt, 2008 KNMI publication = KNMI publicatie; 196 - IV De Bilt, 2008

More information

Feasibility Study of Neutron Dose for Real Time Image Guided. Proton Therapy: A Monte Carlo Study

Feasibility Study of Neutron Dose for Real Time Image Guided. Proton Therapy: A Monte Carlo Study Feasibility Study of Neutron Dose for Real Time Image Guided Proton Therapy: A Monte Carlo Study Jin Sung Kim, Jung Suk Shin, Daehyun Kim, EunHyuk Shin, Kwangzoo Chung, Sungkoo Cho, Sung Hwan Ahn, Sanggyu

More information

Our Department: structure and organization

Our Department: structure and organization EORTC meeting for Radiation Therapy Technologists: RTT s role in the modernization of radiotherapy 10th October 2014, Villejuif (Grand Paris), France Elekta Stereotactic Body Frame: transmission modelled

More information

Characterisation of two new ionisation chamber types for use in reference electron dosimetry in the UK

Characterisation of two new ionisation chamber types for use in reference electron dosimetry in the UK NPL REPORT DQL-RD001 Characterisation of two new ionisation chamber types for use in reference electron dosimetry in the UK Julia A D Pearce September 2004 September 2004 CHARACTERISATION OF TWO NEW IONISATION

More information

THE DIFFERENCE BETWEEN COEFFICIENT-OF-FRICTION AND DRAG FACTOR

THE DIFFERENCE BETWEEN COEFFICIENT-OF-FRICTION AND DRAG FACTOR THE DIERECE BETWEE COEICIET-O-RICTIO AD DRAG ACTOR Mark George, Am SAE-A Director, Accident Investigation Services Pty Ltd, Sydney, Australia. May 2005 The terms coeicient-o-riction (µ) and drag actor

More information

Pipe flow with friction losses solutions using HP and TI calculators By Gilberto E. Urroz, October 2005

Pipe flow with friction losses solutions using HP and TI calculators By Gilberto E. Urroz, October 2005 Pipe low with riction losses solutions using HP and TI calculators By Gilberto E. Urroz, October 005 1. arcy-weisbach Equation and riction actor The basic equation governing riction losses in a pipeline

More information

Solar Energy. Outline. Solar radiation. What is light?-- Electromagnetic Radiation. Light - Electromagnetic wave spectrum. Electromagnetic Radiation

Solar Energy. Outline. Solar radiation. What is light?-- Electromagnetic Radiation. Light - Electromagnetic wave spectrum. Electromagnetic Radiation Outline MAE 493R/593V- Renewable Energy Devices Solar Energy Electromagnetic wave Solar spectrum Solar global radiation Solar thermal energy Solar thermal collectors Solar thermal power plants Photovoltaics

More information

THE EFFECT OF THE SPINDLE SYSTEM ON THE POSITION OF CIRCULAR SAW TEETH A STATIC APPROACH

THE EFFECT OF THE SPINDLE SYSTEM ON THE POSITION OF CIRCULAR SAW TEETH A STATIC APPROACH TRIESKOVÉ A BEZTRIESKOVÉ OBRÁBANIE DREVA 2006 12. - 14. 10. 2006 305 THE EFFECT OF THE SPINDLE SYSTEM ON THE POSITION OF CIRCULAR SAW TEETH A STATIC APPROACH Roman Wasielewski - Kazimierz A. Orłowski Abstract

More information

Atomic and Nuclear Physics Laboratory (Physics 4780)

Atomic and Nuclear Physics Laboratory (Physics 4780) Gamma Ray Spectroscopy Week of September 27, 2010 Atomic and Nuclear Physics Laboratory (Physics 4780) The University of Toledo Instructor: Randy Ellingson Gamma Ray Production: Co 60 60 60 27Co28Ni *

More information

Calibration and Uncertainties of Pipe Roughness Height

Calibration and Uncertainties of Pipe Roughness Height 9 th IWA/IAHR Conerence on Urban Drainage Modelling Calibration and Uncertainties o Pipe Roughness Height Kailin Yang, Yongxin Guo, Xinlei Guo,Hui Fu and Tao Wang China Institute o Water Resources and

More information

BB-18 Black Body High Vacuum System Technical Description

BB-18 Black Body High Vacuum System Technical Description BB-18 Black Body High Vacuum System Technical Description The BB-18 Black Body is versatile and is programmed for use as a fixed cold target at 80 K or variable target, at 80 K- 350 K no extra cost. The

More information

Financial Services [Applications]

Financial Services [Applications] Financial Services [Applications] Tomáš Sedliačik Institute o Finance University o Vienna tomas.sedliacik@univie.ac.at 1 Organization Overall there will be 14 units (12 regular units + 2 exams) Course

More information

The Tangled Web of Agricultural Insurance: Evaluating the Impacts of Government Policy

The Tangled Web of Agricultural Insurance: Evaluating the Impacts of Government Policy The Tangled Web o Agricultural Insurance: Evaluating the Impacts o Government Policy Jason Pearcy Vincent Smith July 7, 2015 Abstract This paper examines the eects o changes in major elements o the U.S.

More information

The University of Southern Maine. XRF X-Ray Radiation Protection Program

The University of Southern Maine. XRF X-Ray Radiation Protection Program The University of Southern Maine XRF X-Ray Radiation Protection Program 1 University of Southern Maine Department of Environmental Sciences 105 Bailey Gorham Hand Held XRF Analyzer X-Ray Radiation Protection

More information

How To Know If You Are Safe To Use An Antenna (Wired) Or Wireless (Wireless)

How To Know If You Are Safe To Use An Antenna (Wired) Or Wireless (Wireless) 1 2 The range of RF spans 3 KHz (3000 Hz) to 300 GHz (300 million Hz) Frequencies of RF devices range from the low frequency AM broadcasts (80 MHz) to higher frequency mobile phones (1900 MHz) smart meters

More information

Responses to SSM on Hydrogeology

Responses to SSM on Hydrogeology Responses to SSM on Hydrogeology Lee Hartley and Steve Joyce, AMEC, 23 rd May 2013 Question 1 A response will be prepared to this question by December 2013. Question 2 The properties o each inite-element

More information

CHAPTER 5 QC Test For Radiographic Equipment. Prepared by:- Kamarul Amin bin Abdullah @ Abu Bakar School of Medical Imaging KLMUC

CHAPTER 5 QC Test For Radiographic Equipment. Prepared by:- Kamarul Amin bin Abdullah @ Abu Bakar School of Medical Imaging KLMUC CHAPTER 5 QC Test For Radiographic Equipment Prepared by:- Kamarul Amin bin Abdullah @ Abu Bakar School of Medical Imaging KLMUC Lesson Outcomes Describe the objectives of each QC test done.(importance)

More information

JP Tribander Owner Manual

JP Tribander Owner Manual JP Tribander Owner Manual JP-Tribander Technical overview JP-Tribander is effective tribander beam for 20m, 15m and 10meters with full size elements without traps. Antenna is designed using latest computer

More information

New Trend In Classification Of Hazard Of Explosive Atmosphere In Laboratory Workplaces

New Trend In Classification Of Hazard Of Explosive Atmosphere In Laboratory Workplaces New Trend In Classiication O Hazard O Explosive Atmosphere In Laboratory Workplaces Di Benedetto A. 1, Dolcetti G. 2, Grimaz S. 3., Russo P. 4, Salzano E. 1 1 Istituto di Ricerche sulla Combustione, Consiglio

More information

Orbital Mechanics. Angular Momentum

Orbital Mechanics. Angular Momentum Orbital Mechanics The objects that orbit earth have only a few forces acting on them, the largest being the gravitational pull from the earth. The trajectories that satellites or rockets follow are largely

More information

Radiographic Grid. Principles of Imaging Science II (RAD 120) Image-Forming X-Rays. Radiographic Grids

Radiographic Grid. Principles of Imaging Science II (RAD 120) Image-Forming X-Rays. Radiographic Grids Principles of Imaging Science II (RAD 120) Radiographic Grids 1 Image-Forming X-Rays Four X-ray paths a. X-rays interact with patient and scatter away from the receptor b. X-rays interact and are absorbed

More information

Lesson 3: Isothermal Hydrostatic Spheres. B68: a self-gravitating stable cloud. Hydrostatic self-gravitating spheres. P = "kt 2.

Lesson 3: Isothermal Hydrostatic Spheres. B68: a self-gravitating stable cloud. Hydrostatic self-gravitating spheres. P = kt 2. Lesson 3: Isothermal Hydrostatic Spheres B68: a self-gravitating stable cloud Bok Globule Relatively isolated, hence not many external disturbances Though not main mode of star formation, their isolation

More information

The Tangled Web of Agricultural Insurance: Evaluating the Impacts of Government Policy

The Tangled Web of Agricultural Insurance: Evaluating the Impacts of Government Policy Journal o Agricultural and Resource Economics 40(1):80 111 ISSN 1068-5502 Copyright 2015 Western Agricultural Economics Association The Tangled Web o Agricultural Insurance: Evaluating the Impacts o Government

More information

kv-& MV-CBCT Imaging for Daily Localization: Commissioning, QA, Clinical Use, & Limitations

kv-& MV-CBCT Imaging for Daily Localization: Commissioning, QA, Clinical Use, & Limitations kv-& MV-CBCT Imaging for Daily Localization: Commissioning, QA, Clinical Use, & Limitations Moyed Miften, PhD Dept of Radiation Oncology University of Colorado Denver Questions Disease Stage (local, regional,

More information

2. To set the number of data points that will be collected, type n.

2. To set the number of data points that will be collected, type n. Force and Motion In this experiment, you will explore the relationship between force and motion. You are given a car with tabs, a string, a pully, a weight hanger, some weights, and the laser gate you

More information

International Journal of Pure and Applied Sciences and Technology

International Journal of Pure and Applied Sciences and Technology Int. J. Pure Appl. Sci. Technol., 18(1) (213), pp. 43-53 International Journal o Pure and Applied Sciences and Technology ISS 2229-617 Available online at www.iopaasat.in Research Paper Eect o Volatility

More information

Variance reduction techniques used in BEAMnrc

Variance reduction techniques used in BEAMnrc Variance reduction techniques used in BEAMnrc D.W.O. Rogers Carleton Laboratory for Radiotherapy Physics. Physics Dept, Carleton University Ottawa, Canada http://www.physics.carleton.ca/~drogers ICTP,Trieste,

More information

1. Provide clinical training in radiation oncology physics within a structured clinical environment.

1. Provide clinical training in radiation oncology physics within a structured clinical environment. Medical Physics Residency Program Overview Our Physics Residency Training is a 2 year program typically beginning July 1 each year. The first year resident will work closely with medical physicists responsible

More information

Exponential Functions

Exponential Functions Eponential Functions Deinition: An Eponential Function is an unction that has the orm ( a, where a > 0. The number a is called the base. Eample:Let For eample (0, (, ( It is clear what the unction means

More information

Chapter 7: Acceleration and Gravity

Chapter 7: Acceleration and Gravity Chapter 7: Acceleration and Gravity 7.1 The Principle o Equivalence We saw in the special theory o relativity that the laws o physics must be the same in all inertial reerence systems. But what is so special

More information

Non-Ionizing Electromagnetic Radiation

Non-Ionizing Electromagnetic Radiation This work is licensed under a Creative Commons Attribution-NonCommercial-ShareAlike License. Your use of this material constitutes acceptance of that license and the conditions of use of materials on this

More information

IAC Ch 41, p.1. Procedure means a stereotactically guided breast biopsy performed on a patient for diagnostic purposes.

IAC Ch 41, p.1. Procedure means a stereotactically guided breast biopsy performed on a patient for diagnostic purposes. IAC Ch 41, p.1 641 41.7 (136C) X-ray machines used for stereotactically guided breast biopsy. 41.7(1) Definitions. In addition to the definitions provided in rules 641 38.2(136C), 641 40.2(136C), and 641

More information

Specific Absorption Rate (SAR) Induced in Human Heads of Various Sizes When Using a Mobile Phone

Specific Absorption Rate (SAR) Induced in Human Heads of Various Sizes When Using a Mobile Phone , June 30 - July 2, 2010, London, U.K. Specific Absorption Rate (SAR) Induced in Human Heads of Various Sizes When Using a Mobile Phone Adel Z. El Dein Alaeddin Amr Abstract - This paper analyzes the specific

More information

The benefit of LED lighting in multilayer cultivation

The benefit of LED lighting in multilayer cultivation Horticulture LED Solutions GreenPower LED string The benefit of LED lighting in multilayer cultivation Helping your business to blossom Philips GreenPower LED string 2 Philips GreenPower LED string The

More information

NIA RADIATION ONCOLOGY CODING STANDARD. Dosimetry Planning

NIA RADIATION ONCOLOGY CODING STANDARD. Dosimetry Planning NIA RADIATION ONCOLOGY CODING STANDARD Dosimetry Planning CPT Codes: 77295, 77300, 77301, 77306, 77307, 77321, 77316, 77317, 77318, 77331, 77399 Original Date: April, 2011 Last Reviewed Date: November,

More information

INTRODUCTION. A. Purpose

INTRODUCTION. A. Purpose New York State Department of Health Bureau of Environmental Radiation Protection Guide for Radiation Safety/Quality Assurance Programs Computed Radiography INTRODUCTION A. Purpose This guide describes

More information

VISCOSITY OF A LIQUID. To determine the viscosity of a lubricating oil. Time permitting, the temperature variation of viscosity can also be studied.

VISCOSITY OF A LIQUID. To determine the viscosity of a lubricating oil. Time permitting, the temperature variation of viscosity can also be studied. VISCOSITY OF A LIQUID August 19, 004 OBJECTIVE: EQUIPMENT: To determine the viscosity of a lubricating oil. Time permitting, the temperature variation of viscosity can also be studied. Viscosity apparatus

More information

Prelab Exercises: Hooke's Law and the Behavior of Springs

Prelab Exercises: Hooke's Law and the Behavior of Springs 59 Prelab Exercises: Hooke's Law and the Behavior of Springs Study the description of the experiment that follows and answer the following questions.. (3 marks) Explain why a mass suspended vertically

More information

PUMPED Nd:YAG LASER. Last Revision: August 21, 2007

PUMPED Nd:YAG LASER. Last Revision: August 21, 2007 PUMPED Nd:YAG LASER Last Revision: August 21, 2007 QUESTION TO BE INVESTIGATED: How can an efficient atomic transition laser be constructed and characterized? INTRODUCTION: This lab exercise will allow

More information

Standard Test Method for Classification of Film Systems for Industrial Radiography 1

Standard Test Method for Classification of Film Systems for Industrial Radiography 1 Designation: E 1815 96 (Reapproved 2001) Standard Test Method for Classification of Film Systems for Industrial Radiography 1 This standard is issued under the fixed designation E 1815; the number immediately

More information