Caption: Figure 8: Plastic hinge formation in the web-side frame of model 5MBC: (a) first yield ([delta] = 0.62%); (b) secondary column yield ([delta] = 1.03%); (c)
primary beam yield ([delta] = 1.5%); (d) at [delta] = 2%.
For the system with the thick secondary beam, the measured acceleration transmissibility is dominated by the first mode (flexural mode of the
primary beam) at 45 Hz, while at a very low amplitude we observed the torsional mode of the
primary beam and the flexural mode of the secondary beam, as shown in Figure 18.
The spectrometer role is to suppress by a factor of 100 the background from bremsstrahlung events by detecting the
primary beam positrons.
There are very few practices that potentially expose R.T.s and others in the room to the
primary beam. This danger could come from holding the patient or improperly collimating and misdirecting a horizontal tube.
The parameter [T.sup.2.sub.c] = [A.sub.c]/[A.sub.p] is the ratio of the cross section area of the coupling beam to that of the
primary beam.
Small-angle X-ray scattering (SAXS) data were obtained with a KRM-type diffractometer (Kratky collimation;
primary beam intensity control with a monitoring channel; evacuation of the sample chamber) in the range of scattering angles 20 from 3[prime] to 3 deg (copper radiation; nickel filtering of the
primary beam; step-by-step scanning regime: recording of scattering radiation with a scintillation counter and digital conversion).
Regardless of whether the
primary beam is activated or not, it should never be pointed at the technologist or other medical personnel.
The laser beam passes through a beamsplitter oriented so that the first reflected beam strikes a monitor detector and the
primary beam is transmitted to the test meter.
Small-angle X-ray scattering (SAXS) data were obtained with a KRM-type diffractometer (Kratky collimation;
primary beam intensity control with a monitoring channel; evacuation of the sample chamber) in the range of scattering angles 20 from 3[feet] to 5 [degrees] (copper radiation; nickel filtering of the
primary beam; step-by-step scanning regime; recording of scattering radiation with a scintillation counter and digital conversion).
It includes contributions from the
primary beam and also the radiation back scattered from the tissue below the surface.
The instrumental effects related to the use of a polycapillary x-ray lens as
primary beam collimator are here studied and the features observed in the measurements modelled via Monte-Carlo ray-tracing.