Published 1988 | Version v1
Book

Implementation of a body-contour orbit on a microprocessor-controlled gantry

Description

For single-photon-emission CT, body-counter orbits minimize the gap between patient and detector. The optimal orbit is peanut shaped: R = (b2sin2θ + a2cos2θ)12/, where R is the orbit radius. An approximation to this orbit has been implemented on a microprocessors system dedicated to gantry motion control (Picker SX300): R = b + (a - b)[sinθ] + z, where z is a safety correction factor for the tomographic table. For a typical patient, this orbit transcribes an area 34% less than that of a circular orbit. With a centered line source (26-cm-diameter water-filled cylinder), the contour orbit (34 X 56 cm) full width at half maximum resolution was 16.6 mm compared with 20.6 mm from a circular orbit (56-cm diameter)

Additional details

Publishing Information

Publisher
Radiological Society of North America Inc.
Imprint Place
Oak Brook, IL (USA)
Imprint Title
Radiological Society of North America 74th scientific assembly and annual meeting (Abstracts)
Imprint Pagination
395 p.
Journal Page Range
p. 214.

Conference

Title
74. scientific assembly and annual meeting of the Radiological Society of North America (RSNA).
Dates
27 Nov - 2 Dec 1988.
Place
Chicago, IL (USA).

INIS

Country of Publication
United States
Country of Input or Organization
United States
INIS RN
21007372
Subject category
S62: RADIOLOGY AND NUCLEAR MEDICINE; S61: RADIATION PROTECTION AND DOSIMETRY;
Resource subtype / Literary indicator
Conference
Descriptors DEI
BODY; DIAGNOSIS; PATIENTS; RADIATION DETECTORS; RESOLUTION; SAFETY; SHAPE; SINGLE PHOTON ECT
Descriptors DEC
COMPUTERIZED TOMOGRAPHY; EMISSION COMPUTED TOMOGRAPHY; MEASURING INSTRUMENTS; TOMOGRAPHY

Optional Information

Secondary number(s)
CONF-8811134--.