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Copyright © 2013 SCK•CEN The new radioprotection implications of fusion reactors V. Massaut; L. Di Pace; F. Druyts; P . Van Iseghem; F. Vermeersch SCK•CEN/ ENEA (I) International Symposium on the occasion of the 50th anniversary of the Belgian Association for Radiological Protection BVS-ABR (April 2013)

The new radioprotection implications of fusion reactors · Tritium is a weak (mean 5,7 keV) beta emitter. But it is an HYDROGEN isotope, thus forming easily organic compounds and

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Page 1: The new radioprotection implications of fusion reactors · Tritium is a weak (mean 5,7 keV) beta emitter. But it is an HYDROGEN isotope, thus forming easily organic compounds and

Copyright © 2013

SCK•CEN

The new radioprotection

implications of fusion reactors

V. Massaut; L. Di Pace; F. Druyts; P. Van Iseghem; F. Vermeersch

SCK•CEN/ ENEA (I)

International Symposium

on the occasion of the 50th anniversary

of the Belgian Association

for Radiological Protection BVS-ABR (April 2013)

Page 2: The new radioprotection implications of fusion reactors · Tritium is a weak (mean 5,7 keV) beta emitter. But it is an HYDROGEN isotope, thus forming easily organic compounds and

Copyright © 2013

SCK•CEN

Fusion: a fast reminder of how it works

Fusion brings together light atoms to produce energy

Today system is based on the reaction D + T implying the use

and handling of massive amounts of tritium and the production

of highly energetic (14 MeV) neutrons.

Page 3: The new radioprotection implications of fusion reactors · Tritium is a weak (mean 5,7 keV) beta emitter. But it is an HYDROGEN isotope, thus forming easily organic compounds and

Copyright © 2013

SCK•CEN

Fusion: a fast reminder of how it works

Fusion brings together light atoms to produce energy

Today’s system is based on the reaction D + T implying the use

and handling of massive amounts of tritium and the production

of highly energetic (14 MeV) neutrons.

To overcome the positive ion mutual repulsion, one needs to

have either VERY high temperature or VERY high pressure.

This leads to several types of confinment systems.

Tokamaks, Stellarator Huge Laser pulses Sun, stars

Impossible on

Earth

Less developed

today Let us focus on this one

Page 4: The new radioprotection implications of fusion reactors · Tritium is a weak (mean 5,7 keV) beta emitter. But it is an HYDROGEN isotope, thus forming easily organic compounds and

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SCK•CEN

Fusion: further reminders

Tritium is a weak (mean 5,7 keV) beta emitter.

But it is an HYDROGEN isotope, thus forming easily organic

compounds and difficult to confine.

Fortunately, it has a very LOW radio-toxicity !

For tritium gas (T2): 1.8 10-15 Sv/Bq

For tritiated water (HTO): 1.8 10-11 Sv/Bq

But the amount of circulating tritium is rather huge:

E.g. in ITER, 1 kg cycling in the plant, 3kg total storage on site;

to give an idea, 1g T2 = 10 000 Ci …

To compare : annual amount of tritium generated by cosmic rays 200 g

Page 5: The new radioprotection implications of fusion reactors · Tritium is a weak (mean 5,7 keV) beta emitter. But it is an HYDROGEN isotope, thus forming easily organic compounds and

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SCK•CEN

Different aspects of radioprotection in fusion reactors

During operation (handling of T; production of energetic

neutrons 14 MeV)

During maintenance (activated products, presence of

tritium, contamination of cooling loops, presence of

activated dust)

In case of accident (activated dust, presence of tritium,

presence of hydrogen, presence of toxic materials,…)

Waste management (huge amount of exposed and

activated materials, presence of tritium and detritiation,

recycling,…)

See further

Page 6: The new radioprotection implications of fusion reactors · Tritium is a weak (mean 5,7 keV) beta emitter. But it is an HYDROGEN isotope, thus forming easily organic compounds and

Copyright © 2013

SCK•CEN

Radioprotection aspects During operation

Handling of tritium:

Tritium is needed for the D-T reaction

there is continuous tritium cycling through

the reactor;

TBMs: (Test) Blanket Modules, with breeding

of Tritium from Lithium and treatment of the

gas

Page 7: The new radioprotection implications of fusion reactors · Tritium is a weak (mean 5,7 keV) beta emitter. But it is an HYDROGEN isotope, thus forming easily organic compounds and

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SCK•CEN

The tritium plant in ITER: a real gas plant on 7 floors ! !

Courtesy from M. Gugla’s presentation, SOFT 2006

Page 8: The new radioprotection implications of fusion reactors · Tritium is a weak (mean 5,7 keV) beta emitter. But it is an HYDROGEN isotope, thus forming easily organic compounds and

Copyright © 2013

SCK•CEN

Radioprotection aspects During operation

Handling of tritium:

Tritium is needed for the D-T reaction

there is continuous tritium cycling through

the reactor;

TBMs: Test Blanket Modules, with breeding of

Tritium from Lithium and treatment of the gas

Production of energetic neutrons

14 MeV neutrons specific shielding and

long range activation

Activation with threshold reactions

No access to the "galleries" during operation.

Page 9: The new radioprotection implications of fusion reactors · Tritium is a weak (mean 5,7 keV) beta emitter. But it is an HYDROGEN isotope, thus forming easily organic compounds and

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Just an idea of the ITER reactor scale

Page 10: The new radioprotection implications of fusion reactors · Tritium is a weak (mean 5,7 keV) beta emitter. But it is an HYDROGEN isotope, thus forming easily organic compounds and

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ALARA approach for maintenance and operations

Dose targets for personnel (for the public)

Maximum individual dose in normal

operation < 10 mSv/y (≤ 0.1 mSv/y)

Average individual dose < 2.5 mSv/y

Collective dose < 500 mSv/y

Maximum individual dose per incident

<10 mSv (≤ 0.1 mSv)

ALARA in design and operation

Work descriptions and dose evaluation

Dose Simulation programs

VISPLAN 3D ALARA planning tool selection of the optimal solution

Work task description

(manpower, duration,

frequency, personnal

protective equipment)

Work area description

(doserate, radiation

sources, contamination,

shielding…)

Prediction of doses (individual, collective, internal,

external)

Study of different variants, modification of processes and

protections, identification of solutions leading to dose

reduction

"Galleries"

Page 11: The new radioprotection implications of fusion reactors · Tritium is a weak (mean 5,7 keV) beta emitter. But it is an HYDROGEN isotope, thus forming easily organic compounds and

Copyright © 2013

SCK•CEN

Radioprotection aspects During operation

Handling of tritium:

Tritium is needed for the D-T reaction there is continuous tritium cycling through the reactor;

TBMs: Test Blanket Modules, with breeding of Tritium from Lithium and treatment of the gas

Production of energetic neutrons

14 MeV neutrons specific shielding and long range activation

Activation with even threshold reactions

No access to the "galleries" during operation.

Presence of high magnetic field, of beryllium, hydrogen, etc (i.e. other safety aspects to be taken into account)

Page 12: The new radioprotection implications of fusion reactors · Tritium is a weak (mean 5,7 keV) beta emitter. But it is an HYDROGEN isotope, thus forming easily organic compounds and

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Heavy maintenance is foreseen

The divertor has to be replaced regularly (in ITER

after about 3 years of operation) and this

replacement requires opening the tokamak and

handling huge and heavy activated components

Page 13: The new radioprotection implications of fusion reactors · Tritium is a weak (mean 5,7 keV) beta emitter. But it is an HYDROGEN isotope, thus forming easily organic compounds and

Copyright © 2013

SCK•CEN

Heavy maintenance is foreseen

The divertor has to be replaced regularly (in ITER

after about 3 years of operation) and this

replacement requires opening the tokamak and

handling huge and heavy activated components

The First Wall of the Torus chamber will probably

have also to be replaced (at least partially). This

requires the use of complex remote handling system

and the handling of large activated components

Page 14: The new radioprotection implications of fusion reactors · Tritium is a weak (mean 5,7 keV) beta emitter. But it is an HYDROGEN isotope, thus forming easily organic compounds and

Copyright © 2013

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Heavy maintenance is foreseen

The divertor has to be replaced regularly (in ITER

after about 3 years of operation) and this

replacement requires opening the tokamak and

handling huge and heavy activated components .

The First Wall of the Torus chamber will probably

have also to be replaced (at least partially), This

requires the use of complex remote handling system

and the handling of large activated components.

When opening the vacuum vessel, the risk of

contamination by tritium (detrapping from the walls)

and activated dust has to be considered.

While replacing the divertor and first wall, the

primary cooling loop will be open.

Dust traces

in JET

Page 15: The new radioprotection implications of fusion reactors · Tritium is a weak (mean 5,7 keV) beta emitter. But it is an HYDROGEN isotope, thus forming easily organic compounds and

Copyright © 2013

SCK•CEN 15

Remote Handling

Specificity of fusion regarding radioprotection

Hot Cells

Remote handling will be important, however

hands on work will still be necessary.

Page 17: The new radioprotection implications of fusion reactors · Tritium is a weak (mean 5,7 keV) beta emitter. But it is an HYDROGEN isotope, thus forming easily organic compounds and

Copyright © 2013

SCK•CEN

As for all nuclear installations, the case of accidents have to be considered

One has to take into account the presence

(and potential mobilization) of tritium,

activated dust, activated corrosion products

etc…

Specific isotopes from fusion (due to the

materials used for the PFC and the high

energetic neutrons) have to be taken into

account,

Page 18: The new radioprotection implications of fusion reactors · Tritium is a weak (mean 5,7 keV) beta emitter. But it is an HYDROGEN isotope, thus forming easily organic compounds and

Copyright © 2013

SCK•CEN

As for all nuclear installations, the case of accidents have to be considered

One has to take into account the presence

(and potential mobilization) of tritium,

activated dust, activated corrosion products

etc…

Specific isotopes from fusion (due to the

materials used for the PFC and the high

energetic neutrons) have to be taken into

account,

Nevertheless, the current simulations have

shown that for the worst case accident, no

population evacuation would be needed.

Page 19: The new radioprotection implications of fusion reactors · Tritium is a weak (mean 5,7 keV) beta emitter. But it is an HYDROGEN isotope, thus forming easily organic compounds and

Copyright © 2013

SCK•CEN 19

SOURCE

TERMS

ASSESSMENT

Normal working

conditions Occupational dose

IE

AS Thermodynamic transients

Aerosols and H3 transport

Containments

Release from the plant DCF

Overall Plant Analysis

FFMEA

Radioactive waste Operational&Decomm waste

Identification&classification

Management

• On - site

• Recycling

• Final disosal

Effluents

PST

PST EST

DCF

man*Sv/y

dose/sequence

to MEI

frequency*dose

Quantity and

waste

categories

mSv/y

SOURCE

TERMS

Normal working

conditions Occupational dose

PIE Thermodynamic transients

Aerosols and H3 transport

Confinements

Release from the plant DCF

Overall Plant Safety Analysis

FMEA

Radioactive waste

Operational&Decomm waste

Identification&classification

Management

• On site • Recycling • Final disposal

Effluents

PST

PST EST

DCF

person*Sv/y

dose/sequence

to Public

frequency*dose

Quantity and

waste

categories

mSv/y

Probabilistic Safety Analysis

Overall Safety Analysis “Course”

DCF = Dose Conversion Factor; PIE = Postulated Initiating Event

PST = Process Source Term; EST = Environmental Source Term

Page 20: The new radioprotection implications of fusion reactors · Tritium is a weak (mean 5,7 keV) beta emitter. But it is an HYDROGEN isotope, thus forming easily organic compounds and

Copyright © 2013

SCK•CEN 20

SOURCE

TERMS

ASSESSMENT

Normal working

conditions Occupational dose

IE

AS Thermodynamic transients

Aerosols and H3 transport

Containments

Release from the plant DCF

Overall Plant Safety Analysis

Radioactive waste Operational&Decomm waste

Identification&classification

Management

• On - site

• Recycling

• Final disosal

Effluents

PST

PST EST

DCF

man*Sv/y

dose/sequence

to MEI

frequency*dose

Quantity and

waste

categories

mSv/y

SOURCE

TERMS

Normal working

conditions Occupational dose

PIE Thermodynamic transients

Aerosols and H3 transport

Confinements

Release from the plant DCF

FMEA

Radioactive waste

Operational&Decomm waste

Identification&classification

Management

• On site • Recycling • Final disposal

Effluents

PST

PST EST

DCF

person*Sv/y

dose/sequence

to Public

frequency*dose

Quantity and

waste

categories

mSv/y

Deterministic Safety Analysis

Overall Safety Analysis “Course”

DCF = Dose Conversion Factor; PIE = Postulated Initiating Event

PST = Process Source Term; EST = Environmental Source Term

Page 21: The new radioprotection implications of fusion reactors · Tritium is a weak (mean 5,7 keV) beta emitter. But it is an HYDROGEN isotope, thus forming easily organic compounds and

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The Waste management requires specific approach, also from a radioprotection standpoint !

There will be a very huge amount of activated material produced:

During maintenance of the plant (exchange and removal of activated divertor and first wall)

At decommissioning (one of the European designs of DEMO assumes 90,000 tons of activated metals !!! To compare with PWR RPV + internals < 1,000 tons)

Here again, the presence of tritium, exotic materials and dust is an important factor (calculation of the impact of the waste storage or disposal for the biosphere)

The main strategy is to recycle (or release when possible) the materials: needs for specific rules and regulations regarding the specific isotopes.

Page 22: The new radioprotection implications of fusion reactors · Tritium is a weak (mean 5,7 keV) beta emitter. But it is an HYDROGEN isotope, thus forming easily organic compounds and

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Release and Recycling

Release from Regulatory Control

• By exemption or clearance (conditioned or not)

▪ it is necessary to develop internationally agreed limits being

complete and fusion specific

▪ Issues on control and measurement with emphasis on the

correct evaluation of impurities.

Recycling in or out the nuclear industry

• Development of radiation-resistant recycling equipment to

handle high dose rates > 10,000 Sv/h.

• Handling, cutting and dismantling of active material using

remote techniques, particularly the separation of high

activity items.

• Issues of removal and transportation of tritium-containing

materials.

Page 23: The new radioprotection implications of fusion reactors · Tritium is a weak (mean 5,7 keV) beta emitter. But it is an HYDROGEN isotope, thus forming easily organic compounds and

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Radioactive Waste generated in a future Fusion Reactor (Ms thesis M. Desecures)

Case study: activation analysis of two W-based divertor designs

Classification of radwaste as LLW or HLW (according to US regulations) or as MA-VL (according to French regulations) is very dependent on the choice of materials, alloying elements (such as Re, Mo, Ni and Cu), and impurities (especially Nb, Ag)

The main lesson learned is that radioprotection and waste management issues should be taken into account in the first steps of developing new alloys for fusion applications (impurities management down to ppb levels)

Page 24: The new radioprotection implications of fusion reactors · Tritium is a weak (mean 5,7 keV) beta emitter. But it is an HYDROGEN isotope, thus forming easily organic compounds and

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Conclusions

Specificities of fusion for radioprotection purposes

Activation products (exotic PFC materials; high energy neutrons)

specific isotopes for fusion

Contamination products in cooling loops (high energy n + complex

loops)

Tritium aspects (handling, confinment, water/gas)

No fuel (normally no long lived isotopes, but huge amount of

activated materials)

Complex and regular heavy maintenance of the plant

(removal/exchange of PFC and divertor)

Thus: needs for specific approach, at least for operational

planning, for the release and recycling, and probably also for the

accident analysis, for the impact of tritium, etc

This approach should start now !

Page 25: The new radioprotection implications of fusion reactors · Tritium is a weak (mean 5,7 keV) beta emitter. But it is an HYDROGEN isotope, thus forming easily organic compounds and

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Thanks for your attention !

Page 26: The new radioprotection implications of fusion reactors · Tritium is a weak (mean 5,7 keV) beta emitter. But it is an HYDROGEN isotope, thus forming easily organic compounds and

Copyright © 2013

SCK•CEN

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PLEASE NOTE!

This presentation contains data, information and formats for dedicated use ONLY and may not be copied,

distributed or cited without the explicit permission of the SCK•CEN. If this has been obtained, please reference it

as a “personal communication. By courtesy of SCK•CEN”.

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