IOP PUBLISHING MEASUREMENT SCIENCE AND TECHNOLOGY
Meas. Sci. Technol. 19 (2008) 094004 (10pp) doi:10.1088/0957-0233/19/9/094004
Positron imaging techniques for process
engineering: recent developments at
Birmingham
D J Parker, T W Leadbeater, X Fan, M N Hausard, A Ingram and Z Yang
University of Birmingham Positron Imaging Centre, School of Physics and Astronomy,
University of Birmingham, Birmingham B15 2TT, UK
Received 13 January 2008, in final form 5 June 2008
Published 24 July 2008
Online at stacks.iop.org/MST/19/094004
Abstract
For over 20 years the University of Birmingham has been using positron-emitting radioactive
tracers to study engineering processes. The imaging technique of positron emission
tomography (PET), widely used for medical applications, has been adapted for these studies,
and the complementary technique of positron emission particle tracking (PEPT) has been
developed. The radioisotopes are produced using the Birmingham MC40 cyclotron, and a
variety of techniques are employed to produce suitable tracers in a wide range of forms.
Detectors originally designed for medical use have been modified for engineering applications,
allowing measurements to be made on real process equipment, at laboratory or pilot plant
scale. This paper briefly reviews the capability of the techniques and introduces a few of the
many processes to which they have been applied.
Keywords: PET, PEPT, radioactive tracers
(Some figures in this article are in colour only in the electronic version)
1. Introduction
Over the last 25 years, positron emission tomography (PET)
has been widely developed as a functional imaging technique
in medicine. Detailed information on metabolism is obtained
by mapping the concentration of a radioactively-labelled
species as a function of time following introduction. The
radioisotope used undergoes β
+
decay, emitting a positron
which then annihilates with an electron to produce two
511 keV γ -rays which are emitted almost exactly back-to-
back, 180
◦
apart to within about 0.5
◦
. A PET scanner,
comprising rings of hundreds of small γ -ray detectors
operating in coincidence, is used to detect these back-to-back
γ -ray pairs. The detected events are binned into histograms
(‘sinograms’) representing the total tracer activity along each
measured line of response (LOR), from which (after correcting
for effects such as attenuation and deadtime) a quantitative map
of tracer concentration is obtained by filtered backprojection
or iterative reconstruction. The spatial resolution is primarily
defined by the size of the individual detector elements and
is around 5 mm in the latest generation of clinical PET
scanners, while some systems designed for small animal
imaging achieve resolution of around 1 mm.
Meanwhile the University of Birmingham Positron
Imaging Centre has pioneered the use of positron-emitting
tracers for studying flow in physics and engineering. The
first application was to investigate lubrication of aero-engines
in collaboration with Rolls Royce, for which a purpose-built
‘positron camera’ was developed by the Rutherford Appleton
Laboratory and commenced operation in 1984 [1]. Shortly
afterwards the Birmingham group developed the technique
of positron emission particle tracking (PEPT) [2] by which
a single tracer particle can be accurately tracked as it moves
within the field of view of the positron camera. Whereas
measurement of a PET image is relatively slow, requiring
acquisition of millions of events, if only a single positron-
emitting source is present its location can be determined very
quickly by triangulation of only a small number of events
(typically around 100 are used), permitting tracking of a fast
moving tracer.
The original Birmingham positron camera comprised a
pair of large area multi-wire proportional chambers operating
in coincidence. Its use for PET and PEPT studies of
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