40
Guenter JaneschitzThe Long Term Future: Nuclear Fusion, 27 June 2016 Page 1 The Long Term Future: Nuclear Fusion Guenter Janeschitz Deputy Head of Central Integration Office ITER Organisation

The Long Term Future: Nuclear Fusion

  • Upload
    dohanh

  • View
    219

  • Download
    1

Embed Size (px)

Citation preview

Page 1: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 1

The Long Term Future: Nuclear Fusion

Guenter Janeschitz

Deputy Head of Central Integration Office

ITER Organisation

Page 2: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 2

Outline

Motivation for fusion development, Fusion Basics and History of ITER (very brief):

ITER and its mission,

Road-map and Technologies needed for DEMO (very brief)

Conclusion

Page 3: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 3

Primary Energy usage in Germany 2013

We have finite oil and gas resources and reserves

Depending on growth oil / gas could be very expensive within 2 decades

To replace only half of it means Terra W of energy from other sources (nuclear,

coal, renewables, fusion)

Climate change prevents the increase of coal usage !!

Page 4: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 4

What is the Economic Environment Fusion

has to compete in ?

• Looking 50 years into the future the time of cheap oil and

gas will be over

– 2.5 billion people (IN, CN) having an increase of use of oil of 5% to 8%/a

– Even with Fracking the present reserves are final => higher prices

– We enter the electric century => traffic, heating, industry => electric !!

– Significant increase of electricity production will be needed > factor 2

– Air transport still needs fuel => Bio mass !!

• => remaining options beside Fusion are:

– Renewables, Fission, Coal

– Coal is problematic => climate change, pollution

– Fission is a good solution but has acceptance issues in some countries

– => Fusion needed in mid- to long term as base energy source !!

Page 5: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 5

Schematic View of a future Fusion Power Reactor

Fusion can

be a long

term solution

not a short term fix

Power

generated

by hot plasma

(20 keV =

200 Mio °C)

4/5 th of

Power

transported

by 14 MeV Neutrons

Page 6: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 6

Energy Gain from Nuclear

Reactions

The Quantum mechanic tunnel

effect makes fusion possible

Page 7: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 7

• Which

• Fusion

• reaction ?

Page 8: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 8

Tritium T3: ~ 150 kg/a

Needed resources for Fusion energy production

breeding with Lithium reaction

Only 300 kg Li6 needed per year

6Li + n 3T + 4He + 4.8 MeV

Deuterium D2: ~ 100 kg/a in 5*1016 kg Oceans

About 1011 kg Lithium in

landmass

Sufficient for 30’000 years

About 1014 kg Lithium in oceans

Sufficient for 30 million years !!

Sufficient for 30 billion years !!

Considering all energy in the world is produced by fusion

1. one year operation of a D-T-Fusion Power Plant, ~1000 MW

electrical

Page 9: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 9

Magnetic Confinement of a plasma with 10 to 20 keV

Coils Plasma Magnetic Fieldline

Stellarator

W7X

Tokamak

Helical field

required

A toroidal magnetic system

needs:

• a helical field configuration

to compensate drifts

• a magnetic well

Two successful systems:

Stellarator / Tokamak - ITER

Page 10: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 10

A modern Tokamak – Vertical-, Radial-, Divertor Fields

Divertor

Transformator

Poloidal field coils Vertical Field

Magnetic well

Radial control

Radial Field

vertical control

Page 11: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 11

Methods for the heating the tokamak plasma

antenna

wave guide

HIGH

FREQUENCY

HEATING

plasma current

OHMIC HEATING

ion

source

neutralis

er

„ion cemetery“

high energetic

atoms

accelerator

transmission line

source: Forschungszentrum Jülich

ICRH

ECRH

HEATING BY

NEUTRAL BEAM

INJECTION

ionized

atoms

Page 12: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 12

Energy and particle Transport is governed by turbulence

Radial size of turbulent

structures can be reduced

by ExB shear, by

magnetic shear and by

zonal flows produced by

the turbulence itself

Ion Turbulent energy

transport sets in at a

critical temperature

gradient which depends

on the local temperature

Page 13: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 13

ITER Cooperation

• 1978 (November): First “Steering

Committee of the INTOR Workshop”

convenes in Vienna. INTOR was the

first attempt at building a truly

international fusion programme.

INTOR was very close to ITER in its

concept.

• 1985 (November): At Geneva

Superpower Summit in 1985

US president Reagan and Secretary

General Gorbatchev propose an

international effort to develop fusion

energy... "as an inexhaustible source

of energy for the benefit of mankind".

This is the first political step to the

ITER programme

Page 14: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 14

21/11/2006: ITER Agreement Signed

Page 15: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 15

The ITER Machine - V: 840m3

R/a: 6.2m /2m

Vertical elongation: 1.85

Triangularity: 0.45

- Density: 1020m- 3

- PeakTemperature:17keV

-Fusion gain Q = 10

-Fusion Power: ~500MW

-Ohmic burn 400 sec

-Goal Q=5 for 3000 sec

- Plasma Current : 15MA

- Toroidal field: 5.4T

Page 16: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 16

Physics Goals:

• ITER is designed to produce a plasma dominated by a-particle heating

• produce a significant fusion power amplification factor (Q ≥ 10) in long-pulse operation

• aim to achieve steady-state operation of a tokamak (Q = 5)

• retain the possibility of exploring ‘controlled ignition’ (Q ≥ 30)

Technology Goals:

• demonstrate integrated operation of technologies for a fusion power plant

• test components required for a fusion power plant

• test concepts for a tritium breeding blanket

Goals of ITER – Design Specification

Page 17: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 17

Tokamak Machine and Complex

Page 18: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 18

PF Coil Facility

ITER IO Headquarters

Contractors area

Tokamak Complex Construction underway

Assembly Hall Construction underway

400 kV switchyard

Cryostat Workshop

Headquarters extension

Storage area 2 Storage area 3

Storage area 1

Batching plant

Cryoplant Construction underway

Preparatory works

Cooling systems

Preparatory works

Control Building

Cleaning facility Construction underway

(Aerial Photo April 2015)

Preparatory works

Magnet Conversion Power

Transformers

Worksite progress

Service Building

Page 19: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 19

Tokamak

building

Hot Cell

building

ITER Assembly / Remote Handling / Hot Cell

PBS 23-3

Transfer cask

PBS 23-6

Hot Cell RH

PBS 23-5

NB RH

Page 20: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 20

Overview of Sector Sub-Assembly

Installation on Transport

Frame

Upending of VV Sector

Installation on Sector Sub-Assembly

Tool

Page 21: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 21

Assembly Hall

Before being integrated in the machine, the components will be prepared and pre-assembled in this 6,000 m2,

60-metre high building. The Assembly Hall will be equipped with a double overhead travelling crane with a lifting

capacity of 1,500 tons, whose installation is scheduled in June.

Page 22: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 22

• The ITER magnet system is made up of

− 18 Toroidal Field (TF) Coils, (EU&JA)

− a 6-module Central Solenoid (CS), (US)

− 6 Poloidal Field (PF) Coils, (EU&RF)

− 9 pairs of Correction Coils (CC). (CN)

− 31 Feeders (CN)

Pair of

TF Coils

PF & CC Coils

ITER Magnets are Produced in a World wide Collaboration

CS Coil

TF Cross

section

Page 23: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 23

1st TF Coil Winding Pack - Europe

European Domestic

Agency contractors have

made significant

progress in

the fabrication of the first

toroidal field winding

pack—the 110-ton inner

core of ITER's D-shaped

superconducting Toroidal

Field Coils.

Following sophisticated,

multi-stage winding

operations, seven layers

of coiled superconducting

cable (double pancakes)

have now been

successfully stacked and

electrically insulated.

Page 24: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 24

Too large to be transported by road, four of ITER’s six ring-shaped magnets (the poloidal field coils)

will be assembled by Europe in this 12,000 m² facility. “White rooms” are currently being equipped

prior to the start of manufacturing operations (mockup) in the summer of 2016.

PF Coil winding facility

Page 25: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 25

Manufacturing Central Solenoid - US

General Atomics (GA) has

launched fabrication of the

1,000-ton superconducting

Central Solenoid. The

component It will be among the

most powerful magnets ever

built with each of the six

modules containing the

equivalent energy of 1,000 cars

racing 150 km/h.

A major milestone was achieved

on 6 April with the winding the

first Central Solenoid module.

Page 26: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 26

Cryostat Workshop - India

The Indian Domestic Agency has erected the Cryostat Workshop for the assembly of the 30 x 30 m.

cryostat, or giant “thermos”, that will completely enclose the ITER Tokamak. The first cryostat

elements, shown here, arrived at ITER in December, achieving the first Milestone ahead of schedule.

Page 27: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 27

Dec 2015

69,47%

8,57%

3,43%

3,89% 4,98%

4,67% 4,98%

The international staff of the ITER Organization (Central Team) comprises ~ 650

persons (35 countries). An equivalent number of contractors and experts are

directly working for ITER in Saint-Paul-lez-Durance. More than 2,000 specialists

work for ITER throughout the world.

IO Staff distribution by ITER Member

Who works for ITER?

Page 28: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 28

Outline Research Plan Structure (staged approach)

Page 29: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 29

The knowledge and the know-how gained during the ITER construction

and the exploration of ITER’s hot plasmas will be used to conceive a

prototype fusion reactor that will test the large-scale production of

electrical power and tritium fuel self-sufficiency: DEMO

ITER is the key facility in this strategy and the DEMO design/R&D will

benefit largely from the experience gained with ITER construction.

The term DEMO describes more of a phase than a single machine.

For the moment, different conceptual DEMO projects are under

consideration by all of the Member nations participating in ITER and it’s

too early to say whether DEMO will be an international collaboration like

ITER, or a series of national projects.

What comes after ITER ? The Road Map to a Reactor

Page 30: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 30

Pebble

Bed

Blanket

400-550°C

Vacuum

Vessel

~100°C

DEMO = Demonstration Fusion Reactor Plant

Main Technology Developments needed for DEMO

Vertical

Manifold

~320°C

Strong

Ring

Shield

~320°C

He cooled

Breeding Blanket

and T-extraction

He cooled Divertor

Low Activation Structural

Material for the “In

Vessel” Components

which can withstand the

large neutron fluence

(150 dpa end of life)

Allows 5 year lifetime for

blanket

Erosion will determine

lifetime for Divertor = 2

years Heating Systems

extended to Steady state

(ITER -> 3000 sec) and

high availability – a

challenge today !!

Improved RH Systems

which can act faster than

presently foreseen in

ITER have to be

developed - availability

Page 31: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 31

Low activation Structuiral Material Development

Low Activation Structural

Materials

Behaviour of the γ-Dosisrate over

time after neutron irradiation of up

to 12.5 MWa/m2

Page 32: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 32

First Electricity ~2050

Page 33: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 33

Conclusions • While there are still issues in Technology and Physics to solve we have come a long way

already towards being ready for building a Reactor / DEMO – ITER is the most important

step towards this goal

• Due to a practically certain increase of electricity production cost (finite Oil and Gas

resources) Fusion can be competitive without assuming very advanced physics and

technology

– Such advanced physics and technology may be achieved eventually or maybe not; --- but

very likely not very near term (in the next 50 years)

• To be economical one needs large plant sizes (2.5 GW electric) and possibly 3 plants at

one location – share infrastructure

– Strong Grid needed => is anyway driven by renewables

• To reduce the size of the tokamak is not economic because the ratio of electricity into

the Grid and capital costs becomes unattractive

Page 34: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 34

“Inner” Fusion DEMO / Reactor DT Fuel Loop In ITER Tritium recycling

is 350 kg/year

In ITER 1 kg/year burned

Page 35: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 35

• Earlier safety studies of fusion power plant concepts are

relevant to DEMO / Reactor safety

– European Safety and Environment Assessments of Fusion Power

(SEAFP), 1992-99

– European Power Plant Conceptual Studies (PPCS), 2001-05

ITER safety and licensing

– Safety case developed, safety analyses performed, safety design

implemented

– Documented in the Preliminary Safety Report (RPrS)

– Extensive examination by French nuclear regulator

– Decret d’Autorisation de Création granted, November 2012

Safety - ITER is a first Example

Page 36: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 36

Management of major reactor consumables • A viable fusion power reactor is to produce 5 GW FP for ~ 300 fpd/yr,

and 60 to 80 year life, i.e.:

– 10 x times ITER Fusion power and 100 times in duration

another 3 orders of magnitude to go !

• Because of overbreeding, and to bridge long(er) plant outages a

surplus of tritium needs to be stored (>100 kg) (4 kg in ITER)

• The results obtained of fusion materials R&D and reactor studies

show that a viable fusion reactor could have:

– Peak neutron fluence: 30 dpa/yr

– End-of-life fluence: 150 dpa

• For 60 year plant life, it implies that about 10 full blanket

exchanges are needed in addition to10-20 divertor exchanges.

Page 37: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 37

The answer is yes by approximately 10 to 15 years => “Ultra Fast Track” –

Apollo Program like Development

if the construction of a DEMO starts ~ 2020 to 2022 and thus the built-up of a

team, the design and the R&D in 2018 to 2020 !!

Development and construction cost ~ 25 to 30 billion € for the complete

program (including e.g. IFMIF) spread over 15 years

DEMO will demonstrate availability and economic feasibility, see below

In later stages advanced blanket designs can be tested in DEMO =>

Testbed !!

The starting point would be the design of the large ITER machine from the 90th

It will be modified to allow stronger plasma shaping, a bigger major

raidius (~10 m) and to incorporate a He cooled solid breeder blanket

and a He cooled divertor => (~ 1.5 to 2 GW electric net output, 5 to 6

GW thermal)

A ~5 billion R&D and qualification program including IFMIF will be part of

such an endeavor

Can we accelerate fusion development further ?

Page 38: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 38

Cost of Fusion Energy

Typical CoE figures; variability due

to differing assumptions

• Carbon (green) costs could be much

larger than shown – infinite?

• Renewables and nuclear present CoEs

that are dominated by fixed costs

• Assume that fusion costs will not be too

different from fission:

• Take for example, 2GWe, 60 years

lifetime, 70% availability and $33B

capital.

• 4% mortgage (cf 2060 UK Treasury

bonds) over 60(30) years gives a CoE

contribution of 117(77) $/MWh

Source: Wood MacKenzie in http://www.bbc.com/news/business-30919045

Page 39: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 39

2GWe => $30bn capital cost

ITE 60 year loan

(4%)

60 year loan

(3%)

capital cost + interest ($B) 86 71

10 divertor changes ($B) 5 5

10 blanket changes ($B) 5 5

operating costs ($B) 12 12

Total Costs ($B) 108 93

Minimum price ($/MWh) 145 124

• Above have assumed 2GWe , 70% availability & 60 years operation

• Capital cost should not be very sensitive to electrical output power.

• Therefore, 1GWe would nearly double price of electricity!

Page 40: The Long Term Future: Nuclear Fusion

Guenter Janeschitz– The Long Term Future: Nuclear Fusion, 27 June 2016 Page 40

0

5 104

1 105

1,5 105

2 105

2,5 105

3 105

Last100% opt mix

1 2 3 4 5 6 7 8 9 10 11 12

Duration Curves for 100% Renewable Sources

• 100%-case:

back-up energy = surplus energy

• Even for the 100 % case a thermal

back-up system is needed as long

as storage is not available

• Peak supply would require totally

uneconomic installed capacity

• 40% share of renewables is a

realistic maximum

• International inter-connects

improves matters by sharing of

peak supply

• Base load supply needed

• Fusion is needed!

surplus

back-up

time (months)

Supply

Demand

Courtesy of F Wagner