Development of an Electron Microbeam for Cell Culture Studies T. W. Botting, L. A. Braby, and J. R. Ford Texas A&M University.

Slides:



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

Radiation biology and protection in dental radiology
ANALYTICAL X-RAY SAFETY User Training Centre for Environmental Health, Safety and Security Management.
Production of X-rays (1)
Chapter’s 2, 3. & 4 By Garland Fisher
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.
Radiation Physics II.
Medical Imaging X-Rays I.
PSSC Space Instrument Laboratory Plasma instrument calibration system provides an ion beam of energy range up to 130keV/charge in a clean room To develop.
MARY NORRIS, STEPHENVILLE HIGH SCHOOL LIN SHAO, ASSISTANT PROFESSOR NUCLEAR ENGINEERING TEXAS A&M UNIVERSITY The research question: How Does Radiation.
Technical studies for the HIE- ISOLDE Frontend upgrade Jacobo Montaño Marie Curie Fellow; CATHI Project * The research project has been supported by a.
BME 560 Medical Imaging: X-ray, CT, and Nuclear Methods X-ray Instrumentation Part 1.
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
Richard M. Bionta XTOD October 12, 2004 UCRL-PRES-XXXXX X Ray Transport, Optics, and Diagnostics, Overview Facility Advisory Committee.
Richard M. Bionta XTOD Layout and Diagnostic October 12-13, 2004 UCRL-PRES-XXXXX XTOD Layout and Diagnostic Systems Facility Advisory.
Seeram Chapter 5: Data Acquisition in CT
Engineering in our World Colleen Knight Bay City ISD MENTOR: Dr. John R. Ford, Jr. Associate Professor Texas A&M University Department of Nuclear Engineering.
Bystander Effects.
8.1 PRODUCTION AND CHARACTERISTICS OF X-RAYS
X-Ray Production & Emission
Elsevier items and derived items © 2009 by Mosby, Inc., an affiliate of Elsevier Inc. X-Ray Production Chapter 8.
Conventional and Computed Tomography
Bubble Chamber Planning Meeting 04 September
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.
Electron Microscopy.
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.
SMURF Research at Texas A&M
Radiation and Fluoroscopic Equipment Tour of Ionizing Lab 1.
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.
Radiation Protection in Radiotherapy
CHAPTER 3 EQUIPMENT OPERATION AND QUALITY CONTROL
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.
Last time we defined a crystal as a solid containing translational symmetry. The directions of translation can be used to from a unit cell. A primitive.
Chapter 3 in Massa X-rays What are they? How are they produced? How do x-rays interact with matter? How does the nature of the crystal effect that interaction?
What is the Research Question? Teacher - Cindy Johnson School - Palacios High School Mentor – Dr. John Ford Department of Nuclear Engineering (Radiation.
V.Grishin, A.Koshelev, A.Larionov A.Pushkarev, V.Seleznev, M.Sleptsov A.Sytin.
Basic radiation protection & radiobiology
PRINCIPLES OF TECHNIQUE AND EXPOSURE
Ferris State University & Michigan Department of Career Development 1 Radiation Safety Study Guide.
SEM- Schematic Overview. Electron Detection Tungsten Filament Electron Source.
COMPUTED TOMOGRAPHY - I RAD 365 CT - Scan
3rd NoRDHia 1 TITLE INVESTIGATION OF DIAMOND SAMPLES UNDER HIGH DOSES OF ELECTROMAGNETIC IRRADIATION (at S-DALINAC) Wolfgang Lange, DESY Zeuthen.
UK Neutrino Factory Meeting Front End Test Stand (F.E.T.S.) Engineering Status by P. Savage 22nd April 2009.
Developments of the FETS Ion Source Scott Lawrie.
Polarized source upgrade RSC, January 11, OPPIS LINAC Booster AGS RHIC ( ) ∙10 11 p/bunch 0.6mA x 300us→11∙10 11 polarized H - /pulse. ( )
Bubble Chamber Planning Meeting 07 August
Resident Physics Lectures Christensen, Chapter 2C Production of X-Rays George David Associate Professor Department of Radiology Medical College of Georgia.
Introduction By Dr. Nimer Khraim DVMS,BVMS,MVSc.
X-ray tube.
An early x-ray by Wilhem Rontgen
Treatment Machines for External Beam Radiotherapy
FETS Ion Source Diagnostics: The Pepperpot
Chapter 4: Diagnostic X-Ray Production
Computed Tomography Data Acquisition
X-RAY PRODUCTION AND EXPOSURE FACTORS
CELLION Technical Report
Single Ion Bombardment of Living Cells at LIPSION - Status Report -
The status of the GCI microprobe
X-Radiation.
RADIATION PROTECTION.
Bystander Effects.
Topic 1: Introduction to Histology
Characteristic Radiation in Tungsten Targets Shell # of electrons Binding energy L Char M N O P Eff X-ray Energy K
Beam Tests of Ionization Chambers for the NuMI Neutrino Beam Monitoring System MINOS.
Resident Physics Lectures (Year 1)
RADIATION TERMS AND UNITS
Resident Physics Lectures (Year 1)
Machine Sources of Radiation
Presentation transcript:

Development of an Electron Microbeam for Cell Culture Studies T. W. Botting, L. A. Braby, and J. R. Ford Texas A&M University

Overview Background Construction Operation Current Experiments Future

Objective Our main objective is to achieve a better understanding of the risk to human health due to everyday exposure to low doses of ionizing radiation.

Most occupational and public radiation exposures are due to x and  rays so concern is about the effects of small numbers of moderate energy electrons (10 to 1000 keV)

How do we study this directly? –Need source for low-to-moderate energy electrons –Need method to deliver them exactly where desired We have used an electron microbeam to try to quantify bystander effects produced by moderate energy electrons

 beam delivery of electron dose Targeting irradiation paths discrete locations Dose duration intensity Energy

Electron Beam Production Electron source low-power tungsten filament low voltage power supply isolation transformer Accelerator Tube custom-made 3-section ceramic equipotential rings high voltage power supply

Beam Delivery Collimator Assembly capillary tube swivel mounts for alignment Cell dish stage x-y motion control Microscope and camera targeting

Electron Microbeam Apparatus Less than 4 feet high Capillary-style collimator Accelerator tube up to 100,000 Volts to produce up to 100keV electrons

Source and Accelerator - Source - Accelerator tube Voltage dividers - \ Faraday Cup control Turbo pump - Equipotential rings Equipotential rings/

3D Schematic

Collimator Stand and Microscope X-Y motion control | CCD camera - - Stage \ Capillary Collimator Capillary Collimator Light Source /

Cell culture dishes

Final Construction Details Voltage dividers 30 M  per tube section for smooth gradient Exit collimation 5  m and 300  m exit aperatures Exit window 2  m thick mylar (same as cell dishes)

Operation Electron source provides electron beam up to 1 nanoamp on the Faraday cup Stable at up to 85 kV so far beams at up to 90kV Software control of targeting line traces discrete spots

Desired Improvements Beam stability Beam current Beam transmission

Bystander Effect Experiments Irradiate nearly confluent cells CDKN1A and PCNA versus distance AG 1522 human fibroblasts Clone 9 rat liver line RIE mouse intestine line HBEC human primary bronchial cells Micronuclei assay AG 1522 human fibroblasts

Some Future Directions… Further micronuclei assays Clone 9 rat liver line RIE mouse intestine line HBEC human primary bronchial cells NTEC Rat primary tracheal cells All three methods (CDKN1A, PCNA, micronuclei) Complete comparison matrix with our positive ion  beam results as a control