Neutron Imaging for the Hydrogen Economy Neutrons see material differently than x-rays The fine details of the water in this Asiatic Lily are clear to.

Slides:



Advertisements
Similar presentations
By Zach Lytle, Jared Freeman, Kyle Lewiecki. Overview of Solar Power The solar power is energy produced by the sun It is produced through nuclear fusion.
Advertisements

Neutron Imaging Facility: Neutron Radiography and Tomography Facilities at NIST to Analyze In-Situ PEM.
X-Ray Astronomy Lab X-rays Why look for X-rays? –High temperatures –Atomic lines –Non-thermal processes X-ray detectors X-ray telescopes The Lab.
Ion Beam Analysis techniques:
Computed Tomography II
Detection of Gamma-Rays and Energetic Particles
LHCf: a LHC Detector for Astroparticle Physics LHCf: a LHC Detector for Astroparticle Physics Lorenzo Bonechi on behalf of the LHCf Collaboration * University.
Neutral Particles. Neutrons Neutrons are like neutral protons. –Mass is 1% larger –Interacts strongly Neutral charge complicates detection Neutron lifetime.
RESMDD'02 pCT: Hartmut F.-W. Sadrozinski, SCIPP INITIAL STUDIES on PROTON COMPUTED TOMOGRAPHY USING SILICON STRIP DETECTORS L. Johnson, B. Keeney, G. Ross,
Design on Target and Moderator of X- band Compact Electron Linac Neutron Source for Short Pulsed Neutrons Kazuhiro Tagi.
ADC PRE-PATIENT COLLIMATION POST-PATIENT COLLIMATION.
Neutron Generation and Detection Lee Robertson Instrument & Source Division Oak Ridge National Laboratory 17 th National School on Neutron and X-ray Scattering.
Dott. Dario Tresoldi CNR IPCF ME
NIST Non-Destructive Evaluation David Jacobson Muhammad Arif Ionizing Radiation Division.
A-LEVEL PHYSICS 15/09/ :49 Medical Physics.
1 ETRR-2 Neutron Radiography Facility ETRR-2 Neutron Radiography Facility T. Mongy Atomic Energy Authority (AEA) of Egypt, ETRR-2.
Chp 4.2- Structure of the Atom
Space Instrumentation. Definition How do we measure these particles? h p+p+ e-e- Device Signal Source.
Interactions of Neutrons
Nuclear Symbols Element symbol Mass number (p + + n o ) Atomic number (number of p + )
For each atom, in its natural state, the number of electrons and the number of protons is equal. This number may or may not be the same as the number.
Neutron Metrology for Fuel Cells David Jacobson, National Institute of Standards & Technology (NIST) Phenomena Probed in Hydrogenous Materials Very large.
LOGO ภาควิชาอิเล็กทรอนิกส์ คณะวิศวกรรมศาสตร์ สถาบันเทคโนโลยีพระจอมเกล้าเจ้าคุณทหารลาดกระบัง.
Neutron Imaging of Fuel Cells at NIST: Present and Future Plans.
Elements of DR Imaging Systems
Modern Physics Model of the atom Radioactivity. Introduction - Today we expand our discussion of explaining what happens at the nuclear level atoms. Radioactivity.
Advanced semiconductor detectors of neutrons
High resolution X-ray analysis of a proximal human femur with synchrotron radiation and an innovative linear detector M.Bettuzzi, R. Brancaccio, F.Casali,
A Silicon vertex tracker prototype for CBM Material for the FP6 Design application.
Multi-colour sctintillator-based ion beam profiler James Green, Oliver Ettlinger, David Neely (CLF / STFC) 2 nd Ion diagnostic workshop June 7-8 th.
1 Interaction Between Ionizing Radiation And Matter, Part 3 Neutrons Audun Sanderud Department of Physics University of Oslo.
The Sun and Us The Sun’s Energy. Energy leaves the sun in the form of heat and electromagnetic radiation Result from the fusion reactions in the sun.
Chapter 5 Interactions of Ionizing Radiation. Ionization The process by which a neutral atom acquires a positive or a negative charge Directly ionizing.
2 pt 3 pt 4 pt 5pt 1 pt 2 pt 3 pt 4 pt 5 pt 1 pt 2pt 3 pt 4pt 5 pt 1pt 2pt 3 pt 4 pt 5 pt 1 pt 2 pt 3 pt 4pt 5 pt 1pt Chapter 25 Chapter 15,16, 19 Chapter.
Institute of Experimental and Applied Physics Czech Technical University in Prague IEAP – CTU Prague 1 Current status and future development of neutron.
Neutron Imaging at NIST: An in situ method for visualizing and quantifying water dynamics in low temperature PEM fuel cells. National Institute of Standards.
Neutron Probes for the Hydrogen Economy David Jacobson, Terry Udovic, and Jack Rush, Muhammad Arif, National Institute of Standards & Technology (NIST)
Understanding mass transport in fuel cells using neutron imaging
The Structure and Dynamics of Solids
Analog Imaging III By Professor Stelmark.
Medical applications of particle physics General characteristics of detectors (5 th Chapter) ASLI YILDIRIM.
Add to table of Contents: Fusion/Fission LabPg. 74 Fission and FusionPg. 75.
Goddard February 2003 R.Bellazzini - INFN Pisa A new X-Ray Polarimeter based on the photoelectric effect for Black Holes and Neutron Stars Astrophysics.
Fluoroscopy. Real-time imaging Most general-purpose fluoroscopy systems use TV technology, operating at 30 frames/sec May be recorded (barium swallow.
Review of Fundamentals
GD AND GD2O3 COATINGS AS NEUTRON CONVERTERS Dorothea Pfeiffer
23.1 Atomic structure The Rutherford scattering experiment  In 1911, Ernest Rutherford carried out the famous Rutherford scattering experiment to explore.
1. What is ionising radiation? 1.Radiation which detaches electrons 2.Radiation which fuses iron nuclei 3.Radiation emitted by the moon Io 4.Radiation.
DIGITAL RADIOGRAPHY.
Copyright © 2012, 2006, 2000, 1996 by Saunders, an imprint of Elsevier Inc. 1 Digital Imaging Instead of Radiography.
Radiography. What are some ways we can see inside of something?
1) How is the mass number calculated (2).
Unit 4 Lesson 3 Nuclear Reactions
Unit 4 Lesson 3 Nuclear Reactions
Efficient transfer reaction method with RI BEams
Chapter 5 Interactions of Ionizing Radiation
Monte Carlo simulation of the GEM-based neutron detector
PHYS 3446 – Lecture #14 Energy Deposition in Media Particle Detection
Neutron detectors for the NMX instrument
Chapter 4 The Nuclear Atom.
כיצד נרכשת התמונה בסרט הרנטגני?
Outside the nucleus, the beta decay {image} will not occur because the neutron and electron have more total mass than the proton. This process can occur.
Neutron Detectors for Materials Research
Unit 4 Lesson 3 Nuclear Reactions
Structure of the Atom (Section 4.2)
RADIATION.
Unit 4 Nuclear Chemistry.
Fission & Fusion.
Computed Tomography (C.T)
PHYS 3446 – Lecture #14 Energy Deposition in Media Particle Detection
Presentation transcript:

Neutron Imaging for the Hydrogen Economy Neutrons see material differently than x-rays The fine details of the water in this Asiatic Lily are clear to neutrons even in a lead cask Subtle changes in the water distribution inside a running fuel cell impact performance and durability Neutron Imaging measures these small changes at video frame rate

Radiography X-ray radiograph Photo Neutron Radiographs

Neutrons are an excellent probe for hydrogen in metal since metals can have a much smaller cross section to thermal neutrons than hydrogen does. Comparison of the relative size of the x-ray and thermal neutron scattering cross section for various elements. x-ray cross section HDCOAlSiFe neutron cross section Sample t  N – numerical density of sample atoms per cm 3  I 0 - incident neutrons per second per cm 2   - neutron cross section in ~ cm 2  t - sample thickness Why Neutrons

How an image is acquired Point Source Sample (a small motor in this case Neutron sensitive screen

Neutron scintillator Converts neutrons to light 6 LiF/ZnS:Cu,Al,Au Charged particles from nuclear reaction come to rest in ZnS and cause scintillation of green light Resolution limited to about 0.2 mm New technology has reduced this to mm 6 Li absorbs neutrons, then promptly splits apart into energetic charged particles Neutron absorption cross section for 6 Li is huge (940 barns) Nuclear reaction produces energetic charged particles Charged particles come to rest in 10 – 15 microns in the ZnS ZnS:Cu,Al,Au produces green light Unfortunately light easily propagates through the screen expanding to a 200 micron blob that degrades the spatial resolution 6 Li + n 0  4 He + 3 H MeV Scintillator Neutrons in Green light out 0.3 mm thick 20 % efficient

Real-Time Detector Technology Amorphous silicon Radiation hard High frame rate (30 fps) 127 micron spatial resolution Picture is of water with He bubbling through it No optics – scintillator directly couples to the sensor to optimize light input efficiency Data rate is 42 Megabytes per second (160 gigabytes per hour) Most users opt for lower data rates due to the enormous pressure to download the data during and after the experiment Neutron beam scintillator aSi sensor Side view Readout electronics Scintillator aSi sensor Front view Helium through water at 30 fps

How an image is acquired Point Source Sample (a small motor in this case Neutron sensitive screen

All Slice Reconstructions 3D Reconstruction Tomography Radiographs Slice Reconstruction