dc.contributor.advisor |
Malherbe, Johan B. |
|
dc.contributor.coadvisor |
Njoroge, E.G. (Eric G.) |
|
dc.contributor.coadvisor |
Hlatshwayo, Thulani Thokozani |
|
dc.contributor.postgraduate |
Innocent, Audu Joseph |
|
dc.date.accessioned |
2020-08-21T09:15:13Z |
|
dc.date.available |
2020-08-21T09:15:13Z |
|
dc.date.created |
2020-10-01 |
|
dc.date.issued |
2020-07-01 |
|
dc.description |
Thesis (PhD (Physics))--University of Pretoria, 2020. |
en_ZA |
dc.description.abstract |
The demand for dry casks for extended storage of radioactive nuclear waste
is driven by dearth of permanent repositories. Most of the dry cask storage
system currently in use are made up of stainless steel which could become
vulnerable to corrosion over a period of time. The service lifetime of these
steel-based canisters can be improved by electrolytic treatment of its outer
surface with layers of glassy carbon and tungsten. This will ensure sufficient
protection against extended long term corrosion and chemical attacks. In
this study, the focus has been on the solid state interaction between the W
films and glassy carbon substrates. W films were sputtered on the glassy
carbon substrates to form diffusion couples. The stability of the diffusion
couples under the heat treatment, the interface interaction and carbide phases
formed have been studied. To gain more insight on the interface mixing re-
gions due to annealing, quantitative measurements of the solid state reactions
between the deposited W films and glassy carbon substrates were carried
out. The as-deposited samples were sequentially annealed isothermally un-
der vacuum at temperatures ranging from 400 to 1000 ◦C in steps of 100 ◦C.
The microstructural changes due to thermal annealing were monitored by
Rutherford backscattering spectrometry (RBS) and grazing incidence X-ray
diffraction (GIXRD). RUMP software was used to simulate the RBS spectra.
The thickness of W thin film deposited, atomic composition of deposited layer
and the intermixed layer growth were deduced from the RUMP simulation
results. The RBS and GIXRD analysis showed that carbide formation was first
observed at an annealing temperature of 900 ◦C. The kinetics of the solid-state
interaction was found to be diffusion controlled at the interface between W
and C. The activation energy for the diffusion of C in W was estimated as
2.23 eV. The XRD results showed that the average crystallite size of the glassy
carbon was estimated as 2.57 nm, while that of the as-deposited W film was
9.77 nm. This value for W film increased with annealing temperature up
to 18.05 nm at 1000 ◦C. The first carbide phase observed was W2C in the
sample annealed at 900 ◦C, while WC was the dominant carbide phase at 1000 ◦C. The surface morphology of the deposited W films was characterized
by scanning electron microscopy (SEM). The SEM micro-graphs showed that
the as-deposited films were smooth and homogeneous. SEM images of the
annealed sample showed complete absence of delamination even at 1000
◦C. This showed that the W films were firmly adhered to the glassy carbon
substrate, indicating that appropriate sputtering parameters were used.
Furthermore, the microstructural changes of GC under the influence of
heat treatments and highly charged ion (HCI) irradiation were monitored
by XRD and Raman techniques. Raman results for the heat treated glassy
carbon samples showed that the graphitic domains experienced a growth in
size upon annealing. On the other hand, under the influence of HCI irradia-
tion, Raman results showed that glassy carbon experienced microstructural
disorder. The crystallite size of the glassy carbon irradiated with fluence of
1.0×1011 ions/cm2 at kinetic energy of 60 keV was estimated as 1.61 nm. This
value decreased to 1.54 nm in the sample bombarded with the highest kinetic
energy 460 keV with intermediate fluence of 5.0×1011 ions/cm2. The atomic force microscopy (AFM) analysis of these irradiated samples showed that the
induced surface roughness increased with both fluence and kinetic energy of
the HCI.
In conclusion, the XRD study of the microstructure of glassy carbon by
method of intensity calculation showed that it is composed of both amorphous
and crystalline carbon materials. The evaluated percentage amorphous and
crystalline contents are 25% and 75%, respectively. |
en_ZA |
dc.description.availability |
Unrestricted |
en_ZA |
dc.description.degree |
PhD (Physics) |
en_ZA |
dc.description.department |
Physics |
en_ZA |
dc.identifier.citation |
Innocent, AJ 2020, Interaction of tungsten films with glassy carbon, PhD (Physics) Thesis, University of Pretoria, Pretoria, viewed yymmdd <http://hdl.handle.net/2263/75845> |
en_ZA |
dc.identifier.uri |
http://hdl.handle.net/2263/75845 |
|
dc.language.iso |
en |
en_ZA |
dc.publisher |
University of Pretoria |
|
dc.rights |
© 2019 University of Pretoria. All rights reserved. The copyright in this work vests in the University of Pretoria. No part of this work may be reproduced or transmitted in any form or by any means, without the prior written permission of the University of Pretoria. |
|
dc.subject |
UCTD |
en_ZA |
dc.subject |
Physics |
en_ZA |
dc.title |
Interaction of tungsten films with glassy carbon |
en_ZA |
dc.type |
Thesis |
en_ZA |