The elasticity of low density polyethylene
Elasticity of low density polyethylene - evaluation of crystal and noncrystal orientation from X-ray diffraction and birefringence
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Elasticity of low density polyethylene - evaluation of crystal and noncrystal orientation from X-ray diffraction and birefringence
Morphology of strain-induced crystallization of polyethylene terephthalate
Mechanical properties of polyethylene terephthalate at cryogenic temperatures
Rough surface recrystallization of heated polyethylene extended-chain crystals
A matched set of five tissue-equivalent proportional counters (TEPCs), embedded at the centers of 0 (bare), 3, 5, 8 and 12-inch-diameter polyethylene spheres, were flown on the Shuttle flight STS-81 (inclination 51.65 degrees, altitude approximately 400 km). The data obtained were separated into contributions from trapped protons and galactic cosmic radiation (GCR). From the measured linear energy transfer (LET) spectra, the absorbed dose and dose-equivalent rates were calculated. The results were compared to calculations made with the radiation transport model HZETRN/NUCFRG2, using the GCR free-space spectra, orbit-averaged geomagnetic transmission function and Shuttle shielding distributions. The comparison shows that the model fits the dose rates to a root mean square (rms) error of 5%, and dose-equivalent rates to an rms error of 10%. Fairly good agreement between the LET spectra was found; however, differences are seen at both low and high LET. These differences can be understood as due to the combined effects of chord-length variation and detector response function. These results rule out a number of radiation transport/nuclear fragmentation models. Similar comparisons of trapped-proton dose rates were made between calculations made with the proton transport model BRYNTRN using the AP-8 MIN trapped-proton model and Shuttle shielding distributions. The predictions of absorbed dose and dose-equivalent rates are fairly good. However, the prediction of the LET spectra below approximately 30 keV/microm shows the need to improve the AP-8 model. These results have strong implications for shielding requirements for an interplanetary manned mission.
The results of a Monte Carlo model for calculating fragment fluences and LET spectra are compared to data taken with 600 MeV/nucleon iron ions incident on an accelerator beamline configured for irradiation of biological samples, with no target and with 2, 5 and 8 cm of polyethylene. The model uses a multi-generation nuclear fragmentation code, coupled with a formulation of ionization energy loss based on the Bethe-Bloch equation. In the region where the data are reliable and the experimental acceptance is well understood, many of the features of the experimental spectra are well replicated by the model. To obtain good agreement with the experimental data, the model must allow for at least two generations of fragment production in the target.
The fragmentation of 510 MeV/nucleon iron ions in several thicknesses of polyethylene has been measured. Non-interacting primary beam particles and fragments have been identified and their LETs calculated by measuring ionization energy loss in a stack of silicon detectors. Fluences, normalized to the incident beam intensity and corrected for detector effects, are presented for each fragment charge and target. Histograms of fluence as a function of LET are also presented. Some implications of these data for measurements of the biological effects of heavy ions are discussed.
Primary and secondary particle radiation doses shielded from solar flare and Van Allen belt protons by aluminum and polyethylene slabs
Mechanical properties of polyethylene terephthalate under selected conditions and methods of preparation
Superheated annealing of stirrer crystallized polyethylene, discussing crystal structure
Morphology of polyethylene terephthalate crystallized from glassy amorphous state by annealing, noting spherulite growth
Strain induced crystallization of polyethylene terephthalate by reorganization of paracrystalline ball-like structures present in amorphous material
Biaxially drawn polyethylene terephthalate films structural changes, noting alignment and crystallinity using polarized IR spectroscopy
Crystalline polyethylene heat of fusion using scanning calorimeter
Ethane-butane desorption from polyethylene, determining diffusion coefficients and solubility constants temperature dependences
Density determination by flotation method for solution grown crystals of polyethylene, noting specific volume-heat of fusion relationships
Melt crystallized polyethylene terephthalate examined by polarized light microscopy, electron microscopy and X ray scattering
Regular crystallographic chain folding in polyethylene crystals