1 australia and nuclear energy power professor peter johnston, rmit

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1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

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Page 1: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

1

Australia and Nuclear Energy Power

Professor Peter Johnston, RMIT

Page 2: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

2

Nuclear Fuel Cycle

Page 3: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

3

Mining and Milling

• Uranium is extracted from the ground, removed from the host rock and daughter products

• Uranium is made into Uranium Ore Concentrate “Yellowcake” which is a hydrated Uranium Oxide of 80-95% purity depending on the temperature of calcining the product.

• Yellowcake is often green.

Page 4: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

4

Australia has the world’s largest U resources (38%) but only 2nd largest producer (23%)

0

200

400

600

800

1000

1200

1400

'000 t

on

nes U

3O

8

0%

5%

10%

15%

20%

25%

30%

% w

orl

d p

rod

ucti

on

low cost resources production 2005

Page 5: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

5

Uranium deposits are widespread

Page 6: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

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World uranium market outlook• Increasing world demand for uranium

Increased NPP duty cyclesPower upgrades of some plantsIncreased plant lifetimes

• Uranium price increasingUS$10/lb to $86 in 4 years (Jan 21 2008)

• U resources are plentifulnot expected to constrain development of new nuclear power capacity

• Timely opportunity for Australia to increase uranium exports significantly

Page 7: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

7

Downstream value-add: opportunities and challenges

• Uranium exports (presently $0.5 bn) could be transformed into a further $1.8bn in value– Conversion, enrichment and fuel fabrication activities

• However, the challenges are significant

Page 8: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

8

Conversion to UF6 and Enrichment

• Purification of Uranium Ore Concentrate

• Production of UF6 which is a chemical process

involving fluorine. UF6 becomes a gas at 50˚C• Enrichment takes natural U of 0.7% U-235

abundance and increases U-235 abundance to approx. 3.5% typically using centrifuges

• USA and France have gaseous diffusion enrichment plants still operating. Centrifuge technology is 50 times more efficient.

Page 9: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

9

Enrichment is the largest value-add step after uranium mining

Component cost shares of a kg of uranium as enriched reactor fuel

0

500

1000

1500

2000

2500

WNA estimate avg 2005 uranium prices mid-2006 spot prices

U3O8 Conversion Enrichment Fabrication

27%

6.8%

47%

19%

56%

4%

29%

11%

44%

5%

36%

15%

$US

$US1633

US$1255

US$2149

U3O8

Page 10: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

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Enrichment challenges

• Enrichment market is highly concentrated – small number of suppliers worldwide

• High barriers to entry – capital intensive, technology tightly held, trade restrictions, limited access to skill base

• Enrichment technology is proliferation sensitive. It is used for civil and weapons purposes

Page 11: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

11

The fuel fabrication market

• Highly customised products

• Specifications depend on reactor design and a utility’s fuel management strategy

• Forecasts indicate capacity significantly exceeds demand

Boiling water reactor fuel assembly

Page 12: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

12

Nuclear Power for Australia?

• How quickly?

• How expensive?

• How safe – operations, accidents, proliferation, waste?

• Environmental benefits?

• Water requirements?

Page 13: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

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Page 14: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

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Life cycle greenhouse gas emissionsfrom electricity generation

wind21

nuclear60

solar PV106

gas combined

cycle577

black coal supercritical

863

brown coalsubcritical

1175

hydro 15

0

200

400

600

800

1000

1200

1400

1600

kg

CO 2-

e p

er

MW

h

u shows most likely value;bar shows range

Page 15: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

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Ingredients to emissions model

• The large range of values for nuclear contributions to greenhouse gas emissions come from:-- Concentration of U in ore- Enrichment technology used- Electricity source for enrichment

Page 16: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

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Retail Electricity prices 2006

0

50

100

150

200

250

300

Australia France Germany Italy Japan Korea New Zealand United Kingdom United States

$A/M

Wh

(20

06)

Source: IEA Key World Energy Statistics 2006

Page 17: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

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Nuclear power cost ranges

$0

$20

$40

$60

$80

$100

$120

Lev

elis

ed C

ost

s ( A

$ 20

06 /

MW

h )

Tarjanne

Gittus

Chicago

MIT

RAE

Chicago

MIT

Discount Rates (capital spend of A$2 - 3 billion)

Indicative Ranges of Nuclear Power Cost

Low Medium High

Low = 5%Medium = 7-10%High = 11-13%

Page 18: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

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Generation cost comparisons

$20

$30

$40

$50

$60

$70

$80

$90

$100

$110

$120

Le

ve

lise

d C

os

t E

sti

ma

tes

( A

$ 2

00

6 /

MW

h )

Nuclear costs are for an established industry

Nuclear

Coal

Coal - Supercritical Pulverised Coal

Combustion + CCS

Gas - Combined Cycle Gas Turbine

+ CCS

Coal - Integrated Gasification Combined

Cycle + CCS

Renewables

High Capacity Factor Wind / Small Hydro

Solar PV

Solar Thermal / Biomass

Gas - Combined Cycle Gas Turbine

CCS estimates are indicative onlyRenewables have large ranges and substantial overlaps

Page 19: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

19

Generation cost comparisons• Nuclear is least-cost low emission technology

(LET)– Renewables, CCS more expensive on average but

will have substantial role to play

• Nuclear power is internationally proven, least cost option in many countries– Includes waste disposal and decommissioning

• Without carbon constraint all LETs to remain uncompetitive

• Nuclear power can be competitive with low to moderate emissions price– $15 to $40 /tonne CO2-E (ETS €20 12 Feb 2008)– Competitiveness of other LETs would also improve

Page 20: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

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Investment in nuclear power

• Potential investors in nuclear power in Australia require:– A stable policy environment– A predictable licensing and regulatory regime

• Time frame is determined by the timing and nature of this regime.

• Best practice is to establish funds to meet waste and decommissioning costs

Page 21: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

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Nuclear Waste

• Key issue is the quantity of waste.

• One pellet of NPP fuel (~5 g) yields as much energy as 1 tonne of coal.

• The disposal of this fuel pellet generates high level waste, but there are significant quantities of less radioactive waste at the mine site and in the use of uranium,

Page 22: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

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Low and intermediate waste

• Safe disposal demonstrated at many sites across the world, including in Australia

• High standard of management of waste at Australia’s current uranium mines

Page 23: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

23• Relatively small waste volume

Radioactive waste and spent fuel management

Page 24: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

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Reprocessing and high-level waste(HLW) disposal• Reprocessing is technically complex and is

unlikely to be attractive for Australia• Technology exists for safe disposal of HLW and

spent fuel and is being applied in several countries. No HLW yet to operation.

• Areas in Australia are suitable for HLW and spent fuel disposal– not required before 2050 if we adopt nuclear power

Page 25: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

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Implementing deep disposal

Page 26: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

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Why do we think HLW disposal is OK? Natural Analogues

• Ore deposits that have been isolated for millions of years

• Natural Reactors at Oklo and Bangombé in Gabon. The remnants of nuclear reactors nearly two billion years old were found in the 1970s.

• Oklo by-products are being used today to probe the stability of the fundamental constants over cosmological time-scales and to develop more effective means for disposing of human-manufactured nuclear waste.

Page 27: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

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Health and Safety

• Operational – construction, operation of the plant and its decommissioning as well as in the mining of uranium, manufacture of fuel and waste processing.

• Accidents – rare events of high impact

Page 28: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

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Operational Health and safety

• Nuclear power has fewer health and safety impacts than fossil fuel generation and hydro

• Ionising radiation and its health impacts are well understood

• Well established international safety standards which are reflected in Australian practice

Page 29: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

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Health and safety: Accidents Fatal accidents in the worldwide energy sector, 1969–2000*

No. accidents Immediate fatalities

Immediate fatalities per GWe year

Coal 1221 25 107 0.876 Oil 397 20 283 0.436 Coal (China excluded) 177 7090 0.690 Natural gas 125 1978 0.093 LPG 105 3921 3.536 Hydro 11 29 938 4.265 Hydro (Banqiao/Shimantan dam accident excluded)a

10 3938 0.561

Nuclear reactorb 1 31 0.006 a The Banqiao/Shimantan dam accident occurred in 1975 and resulted in 26 000 fatalities b See Box 6.2 for information on long-term impacts of nuclear reactor accidents Source: derived from Burgherr et al[120] and Burgherr and Hirschberg[121] *These figures do not Include latent or delayed deaths such as those caused by air pollution from fires, chemical exposure or radiation exposure that might occur following an industrial accident

Page 30: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

30

Chernobyl

• An uncontained steam/chemical explosion and subsequent fire at Chernobyl in 1986 released radioactive gas and dust

• Wind dispersed material across Finland, Sweden, and central and southern Europe

• People living within a 30 km radius of the plant were relocated— approx 116 000.

Page 31: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

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Chernobyl – Immediate Casualties

• 28 highly exposed reactor staff and emergency workers died from radiation and thermal burns within four months of the accident (160 had radiation sickness. 19 more died by the end of 2004 not necessarily as a result of the accident).

• Two other workers were killed in the explosion from injuries unrelated to radiation

• One person suffered a fatal heart attack.

Page 32: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

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Chernobyl Longer-term• > 4000 mostly children or adolescents at the time of the accident,

have developed thyroid cancer as a result of the contamination, and fifteen of these had died from the disease by the end of 2002.

• Possibly 4000 people in the areas with highest radiation levels may eventually die from cancer caused by radiation exposure. Of the 6.8 million individuals living further from the explosion, who received a much lower dose, possibly another 5000 may die prematurely as a result of that dose.

• The small increase in radiation exposure caused by the accident for the population of Europe and beyond should not be used to estimate future likely possible cancer fatalities. The ICRP states that this approach is not reasonable.

• The Chernobyl Forum report in 2006 clearly identifies the extensive societal disruption in the region as the most significant impact resulting from the accident, compounded by the collapse of the Soviet Union in 1989.

Page 33: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

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Nuclear’s contribution to radiation exposure

Source: United Nations Scientific Committee on the Effects of Atomic Radiation (UNSCEAR)

Page 34: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

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Non-proliferation• Export of Australian uranium takes place within

the international non-proliferation regime • Australia has the most stringent requirements for

the supply of uranium • Actual cases of proliferation have involved illegal

supply networks, secret nuclear facilities and undeclared materials

• An increase in Australian uranium exports would not increase the risk of proliferation

Page 35: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

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Uranium exports and non-proliferation

• The amount of uranium required for a nuclear weapon is relatively small

• Uranium is commonplace in the earth’s crust

• Any country that wished to develop a weapon need not rely on the import of uranium

• The greatest proliferation risk arises from undeclared centrifuge enrichment plants

Page 36: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

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Nuclear security

• Strict physical protection standards apply to nuclear power plants

• Studies have found that containment structures at modern power reactors would not be breached by the impact of a large commercial airliner

Page 37: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

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Water requirements?

• NPPs usually use water for cooling as do coal-fired power plants.

• Current PWRs and BWRs operate at lower temperatures and are therefore less efficient (use slightly more water)

• Coal PPs must be located very near the coal deposit. Transport of ore is a major issue.

• NPPs can be located remote from ore and often on the coast using seawater.

Page 38: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

38

Other Nuclear Power Systems

• Thorium Fuel Cycle

• Gen IV Reactor Systems

• Accelerator Driven Systems

• Fusion (ITER)

Page 39: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

39

Dan’s Questions

• Reactor grade Pu for bombs

• Swedish ‘incident’ of 2007

• Earthquake in Japan

Page 40: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

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Reactor grade Pu for bombs

• Reactor grade Pu contains Pu-239 and Pu-240 is similar quantities.

• Pu-240 is undesirable in weapons manufacture because of short SF half-life

• Certainly a critical assembly could be produced by reactor grade Pu.

• US planned a trial in 1962 – I understand it did not proceed.

• No state player is likely to use such material because the device could not be reliably stored.

Page 41: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

41

2007 Earthquake at Kashiwazaki Kariwa NPP

• 7965 MWe nuclear power plant• Earthquake produces ground accelerations to

0.68g at plant – locally 11 killed, 2000 injured• Design criteria was to withstand 0.27g• Off-site power fail expected at 0.25g• Plants shut down automatically without problem• Radioactivity release – sloshing of water in spent

fuel pond and leak through cable penetrations (IAEA judged leak trivial)

Page 42: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

42

scram of the Forsmark unit 1 reactor on 25 July 2006

• Electricity failure caused by the short circuit in the switchyard

• Forsmark 1 reactor was scrammed and a number of safety systems were activated

• Two of four emergency generators failed to start. This common cause fault resulted in INES level 2 report.

• Position of the control rods was unclear due to lack of power supply.

Page 43: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

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Conclusions

• Australia has the opportunity to expand uranium mining.

• Enrichment may represent an opportunity for Australia – the business case is not clear.

• Regulation needs review and a new regulatory system created if nuclear power is pursued.

• Australia must deal with existing and future nuclear waste, but reprocessing and taking other countries waste are unlikely to be attractive

• Nuclear Power is the lowest cost low emission technology for baseload power generation.

Page 44: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

44

Potential emission cuts from nuclear build

Page 45: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

45

Questions?The UMPNER report

is available from the National Library Pandora archive website:

http://pandora.nla.gov.au/tep/66043

Page 46: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

46

Thorium Fuel Cycle

• Thorium is a naturally occurring element• Th is three times more abundant than U• Th like U-238 is fertile, not fissile• U-233 can be bred from Th and used like U-235• Requires reprocessing cycle to extract U-233,

Th much less soluble than U.• Side product U-232 gives radiation protection

problem.• Proliferation issues raised by U-233.

Page 47: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

47

Gen IV Reactor Systems

• Six reactor concepts judged to be most promising by collaborating nations.

• Technical goalsProvide sustainable energy generation that meets clean air objectives and promotes long term availability of systems and effective fuel utilisation for worldwide energy productionMinimise and manage nuclear waste, notably reducing the long term stewardship burden in the future and thereby improving protection for the public health and the environmentIncrease assurances against diversion of theft of weapons-usable materialEnsure high safety and reliabilityDesign systems with very low likelihood and degree of reactor core damageCreate reactor designs that eliminate the need for offsite emergency responseEnsure that systems have a clear life cycle cost advantage over other energy sourcesCreate systems that have a level of financial risk that is comparable to other energy projects.

Page 48: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

48

Gen IV Reactor SystemsReactor type Coola

ntTem

p (oC)

Pressure

Waste recycling Output Research needs Earliest delivery

Gas-cooled fast reactor (GFR)

Helium 850 High YesElectricity

and hydrogen

Irradiation-resistant materials, helium turbine, new fuels, core design, waste recycling

2025

Lead-cooled fast reactor (LFR)

Lead-bismut

h

550–800

Low YesElectricity

and hydrogen

Heat-resistant materials, fuels, lead handling, waste recycling 2025

Molten salt reactor (MSR)

Fluoride salts

700–800

Low YesElectricity

and hydrogen

Molten salt chemistry and handling, heat- and corrosion-resistant materials, reprocessing cycle

2025

Sodium-cooled fast reactor (SFR)

Sodium

550 Low Yes Electricity Safety, cost reduction, hot-fuel fabrication, reprocessing cycle 2015

Supercritical-water-cooled reactor (SCWR)

Water510–550

Very high

Optional ElectricityCorrosion and stress corrosion cracking, water chemistry,

ultra strong non-brittle materials, safety2025

Very-high-temperature reactor (VHTR)

Helium 1000 HighNo – waste goes

directly to repository

Electricity and

hydrogen

Heat-resistant fuels and materials, temperature control in the event of an accident, high fuel burn-ups

2020

Page 49: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

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Accelerator Driven Systems

• The need for fissile material is partly replaced by using a spallation source of neutrons

• Accelerator-driven systems consist of three main units — the accelerator, target/blanket and separation units.

• The accelerator generates high energy (around 1 GeV) charged particles (usually protons) which strike a heavy material target producing spallation surrounded by a blanket of fertile material.

• The system works like a reactor without a critical assembly and can burn or breed fissile material.

Page 50: 1 Australia and Nuclear Energy Power Professor Peter Johnston, RMIT

50

Fusion (ITER)

• The experimental fusion reactor ITER is a major international research collaboration.

• To be built at Cadarache in France

• Cost €10 billion, half to construct the reactor over the next seven years and the remainder to operate it for 20 years and then decommission the facility.

• Power 300 MW for up to 30 minutes.