The alternative to Uranium
Thorium is an alternative to Uranium for the production of nuclear energy.
Unfortunately,
only a small part of the nuclear industry selected it to develop civil
power
plants. Instead of that, the great majority decided to invest in the
Uranium-based
technology, originally developed for the submarines. The history showed us
this was
maybe not the best choice, as the fission of Uranium generates very unstable products, in the family of Minor Actinides.
With
a
proper use of Thorium, none of the actual problems faced by the nuclear
industry would have been encountered.
Thorium
history
As
stated by the IAEA(*), “during the
pioneering years of nuclear
energy, from the mid-1950s to mid-1970s, there was considerable
interest
worldwide to develop thorium fuels and fuel cycles in order to
supplement
uranium reserves. The feasibility of thorium utilization has been
demonstrated in
high temperature gas cooled reactors (HTGR), light water reactors
(LWR), pressurized
heavy water reactors (PHWRs), liquid metal cooled fast breeder reactors
(LMFBR)
and molten salt breeder reactors (MSBR).
The initial enthusiasm on
thorium fuels and
fuel cycles was not sustained among the developing countries later, due
to new
discovery of uranium deposits and their improved availability”.
A
second
reason for the disinterest in Thorium-based reactors, lies in the fact
that the
Uranium-based industry received an enormous support from the military
lobby,
because their civil reactors could produce a by-product
they dramatically needed… called Plutonium.
After
the Three
Miles Island accident and the Chernobyl catastrophe in 1986, the growth
of
nuclear power dramatically slowed down, particularly in the USA and
Europe.
Even
the safe
Thorium power plants operating in Germany (THTR300) has been stopped !
Thorium
today
Recent
concerns about global warming, and the Kyoto accords limiting CO2
suggest that future energy demands cannot be met solely through the
burning of
fossil fuels. And on the other end, the sustainable energy sources will
never
be able to provide 100% of the energy needed by our modern
civilization. Taking
those constraints into account, a return to some reliance on the
nuclear option
is required.
In
this context,
Thorium-based cycles that offer proliferation-resistance, that have
improved
waste form characteristics, and that permit reduction of plutonium
inventories receive
renewed interest in in several developed countries.
IAEA
argues also that in the mid-term, Thorium will be mandatory to
replace Uranium in the
actual nuclear industry. “the
annual world requirements of uranium is expected to grow from the
present level
of some 66.000 tonnes ‘U’ to nearly 82.000 tonnes
‘U’ by the year 2025. Nowadays,
the world uranium production (36.042 tonnes) provides about 54% of
world
reactor requirements (66 815 tonnes), with the remainder being met by
secondary
sources, including civilian and military stockpiles, uranium
reprocessing and
re-enrichment of depleted uranium. However, by 2025, secondary sources
will
decline in importance and provide only about 4–6% of
requirements, depending
upon the demand projections used. At that juncture, introduction of
thorium
fuel cycle will play a complementary role” (IAEA,
2005)
Thorium benefits and challenges
According
to
IAEA (IAEA, 2005), Thorium fuels and fuel cycles have the following
benefits
and challenges :
Benefits
• Thorium
is 3 to 4 times more abundant than uranium, widely distributed in
nature as an easily
exploitable resource in many countries and has not been exploited
commercially so
far.
• Thorium
fuel cycle is an attractive way to produce long term nuclear energy
with low radiotoxicity
waste.
• Unlike
natural uranium, which contains ~0.7% ‘fissile’ 235U
isotope,
natural thorium does not contain any ‘fissile’
material and is made up of the
‘fertile’ 232Th isotope
only”. To be able to fission, this fertile
element has to be transformed into fissile 233U
by the capture of
one neutron. The fission further happens by absorption of a second
neutron.
• For
the ‘fissile’ 233U nuclei,
the number of neutrons liberated per
neutron absorbed is greater than 2.0 over a wide range of thermal
neutron
spectrum, unlike 235U and 239Pu.
Thus, contrary to 238U–239Pu
cycle in which breeding can be obtained only with fast neutron spectra,
the 232Th–233U
fuel cycle can operate with fast, epithermal or thermal spectra.
• Thorium
dioxide is chemically more stable and has higher radiation resistance
than uranium
dioxide. The fission product release rate for ThO2–based
fuels are
one order of magnitude lower than that of UO2.
ThO2 has favorable
thermo-physical properties because of the higher thermal conductivity
and lower
co-efficient of thermal expansion compared to UO2.
• ThO2
is relatively inert and does not oxidize unlike UO2,
which oxidizes
easily to U3O8 and UO3.
Hence, long term
interim storage and permanent disposal in repository of spent ThO2–based
fuel are simpler without the problem of oxidation.
• Thorium–based
fuels and fuel cycles have intrinsic proliferation-resistance due to
the formation
of 232U during the production of 233U.
And some of the daughter
products of 232U, like 212Bi
and 208Tl, emit
strong gamma radiations.
• In
232Th–233U fuel
cycle, much lesser quantity of plutonium
and long-lived Minor Actinides (MA: Np, Am and Cm) are formed as
compared to
the 238U–239Pu
fuel cycle, thereby minimizing the
radiotoxicity associated in spent fuel.
Challenges
• The
melting point of ThO2 (3350°C) is much
higher compared to that of UO2
(2800°C). Hence, a much higher sintering temperature
(>2000°C) is required
to produce high density ThO2 and ThO2–based
mixed oxide
fuels.
• As
ThO2 and ThO2–based
mixed oxide fuels are relatively
inert, they do not dissolve easily.
• The
significant amount of gamma emitting products necessitates remote and
automated
reprocessing and re-fabrication in heavily shielded hot cells, which
increases
in the cost of fuel cycle activities.
• In
the conversion chain of 232Th to 233U,
233Pa
is formed as an intermediate, which has a relatively longer half-life
(~27
days) as compared to 239Np (2.35 days) in the
uranium fuel cycle. Thereby
this requires a longer cooling time for completing the decay of 233Pa
to 233U.
• The
three stream process of separation of uranium, plutonium and thorium
from spent
(Th, Pu)O2 fuel, though viable, is yet to be
developed.
• The
database and experience of thorium fuels and thorium fuel cycles are
very
limited, as compared to UO2 and (U, Pu)O2
fuels, and need
to be augmented before large investments are made for commercial
utilization of
thorium fuels and fuel cycles. For example, some radionuclides produced
during
the reaction such as 231Pa, 229Th
and 230U
have radiological impact and have to be managed in the fuel cycle.
(*) IAEA-TECDOC-1450 “Thorium fuel cycle — Potential benefits and challenges” May 2005
.