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Introduction to Nuclear Fusion Prof. Dr. Yong-Su Na

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Page 1: Introduction to Nuclear Fusion - ocw.snu.ac.krocw.snu.ac.kr/sites/default/files/NOTE/INF-2017-10-Pinch.pdf · jz j0 IP Sa for r a r a I B P 2 0 2S P T. 19 Helical kink instability

Introduction to Nuclear Fusion

Prof. Dr. Yong-Su Na

Page 2: Introduction to Nuclear Fusion - ocw.snu.ac.krocw.snu.ac.kr/sites/default/files/NOTE/INF-2017-10-Pinch.pdf · jz j0 IP Sa for r a r a I B P 2 0 2S P T. 19 Helical kink instability

2

To build a sun on earth

Page 3: Introduction to Nuclear Fusion - ocw.snu.ac.krocw.snu.ac.kr/sites/default/files/NOTE/INF-2017-10-Pinch.pdf · jz j0 IP Sa for r a r a I B P 2 0 2S P T. 19 Helical kink instability

3

To build a sun on earth

Page 4: Introduction to Nuclear Fusion - ocw.snu.ac.krocw.snu.ac.kr/sites/default/files/NOTE/INF-2017-10-Pinch.pdf · jz j0 IP Sa for r a r a I B P 2 0 2S P T. 19 Helical kink instability

4

• Bring the Sun on the Earth

Quantity ITER Sun Ratio

Diameter 16.4 m 140x104 km ~ 1/108

Central temp. 200 Mdeg 15 Mdeg 10

Central density ~1020/m3 ~1032/m3 ~1/1012

Central press. ~5 atm ~1012 atm ~1/1011

Power density ~0.6 MW/m3 ~0.3 W/m3 ~2x106

Reaction DT pp

Plasma mass 0.35 g 2x1030 kg ~1/1034

Burn time const. 200 s 1010 years ~1/1015

M. Kikuch, “steady state tokamak reactor and its physics issues”, Talk at SNU, Korea, September 30, 2011

Magnetic Confinement

Page 5: Introduction to Nuclear Fusion - ocw.snu.ac.krocw.snu.ac.kr/sites/default/files/NOTE/INF-2017-10-Pinch.pdf · jz j0 IP Sa for r a r a I B P 2 0 2S P T. 19 Helical kink instability

5

To build a sun on earth

- Open magnetic confinement - Closed magnetic confinement

Page 6: Introduction to Nuclear Fusion - ocw.snu.ac.krocw.snu.ac.kr/sites/default/files/NOTE/INF-2017-10-Pinch.pdf · jz j0 IP Sa for r a r a I B P 2 0 2S P T. 19 Helical kink instability

6

What is open magnetic confinement?

Page 7: Introduction to Nuclear Fusion - ocw.snu.ac.krocw.snu.ac.kr/sites/default/files/NOTE/INF-2017-10-Pinch.pdf · jz j0 IP Sa for r a r a I B P 2 0 2S P T. 19 Helical kink instability

7

• Equilibrium – Radial Force Balance

X Jz

Jz x Bθ

X Bz

Jθ x Bz

BJp

JB

0

0 B

p BJ

Open Magnetic Confinement

http://lasp.colorado.edu/education/outerplanets/solsys_star.php

Page 8: Introduction to Nuclear Fusion - ocw.snu.ac.krocw.snu.ac.kr/sites/default/files/NOTE/INF-2017-10-Pinch.pdf · jz j0 IP Sa for r a r a I B P 2 0 2S P T. 19 Helical kink instability

8

Z pinch θ pinch screw pinch

Magnetic mirror

Open Magnetic Confinement

http://phys.strath.ac.uk/information/history/photos.php http://www.frascati.enea.it/ProtoSphera/ProtoSphera%202001/6.%20Electrode%20experiment.htm

Page 9: Introduction to Nuclear Fusion - ocw.snu.ac.krocw.snu.ac.kr/sites/default/files/NOTE/INF-2017-10-Pinch.pdf · jz j0 IP Sa for r a r a I B P 2 0 2S P T. 19 Helical kink instability

9

What is Z-pinch?

Page 10: Introduction to Nuclear Fusion - ocw.snu.ac.krocw.snu.ac.kr/sites/default/files/NOTE/INF-2017-10-Pinch.pdf · jz j0 IP Sa for r a r a I B P 2 0 2S P T. 19 Helical kink instability

10

• The Z Pinch

Magnetic Pinch

J

B

X Jz

Jz x Bθ

http://www.plasma-universe.com/Pinch_(plasma_physics)?title=Special:Booksources&isbn=0387975756 http://ask.nate.com/qna/view.html?n=6318216

G. Thomson and P. Thonemann

- The Lorenz force created by a lightning strike crushed this hollow lightning rod and led to the discovery of the pinch.

http://joiimg.tistory.com/416 http://www.thunderbolts.info/forum/phpBB3/viewtopic.php?p=731&sid=824cd77d679b252e92355fcbf212ed7a

Page 11: Introduction to Nuclear Fusion - ocw.snu.ac.krocw.snu.ac.kr/sites/default/files/NOTE/INF-2017-10-Pinch.pdf · jz j0 IP Sa for r a r a I B P 2 0 2S P T. 19 Helical kink instability

11

• The Z Pinch

Magnetic Pinch

http://joiimg.tistory.com/416 http://www.thunderbolts.info/forum/phpBB3/viewtopic.php?p=731&sid=824cd77d679b252e92355fcbf212ed7a

http://www.plasma-universe.com/Pinch_(plasma_physics)?title=Special:Booksources&isbn=0387975756 http://ask.nate.com/qna/view.html?n=6318216

G. Thomson and P. Thonemann

- The Lorenz force created by a lightning strike crushed this hollow lightning rod and led to the discovery of the pinch.

J

B

- The plasma carries an electric current and is confined by

the magnetic field induced by this current.

- As the current is increased, the larger magnetic field compresses

the plasma and also raises its temperature by Joule-heating.

- Confinement and heating is simultaneously provided.

Page 12: Introduction to Nuclear Fusion - ocw.snu.ac.krocw.snu.ac.kr/sites/default/files/NOTE/INF-2017-10-Pinch.pdf · jz j0 IP Sa for r a r a I B P 2 0 2S P T. 19 Helical kink instability

12 ZETA (1954-58, UK) P. C. Thonemann et al, Nature 181 217 (1958)

Magnetic Pinch • The Z Pinch X Jz

Jz x Bθ

- The plasma carries an electric current and is confined by

the magnetic field induced by this current.

- As the current is increased, the larger magnetic field compresses

the plasma and also raises its temperature by Joule-heating.

- Confinement and heating is simultaneously provided. Where did the neutrons come from in ZETA?

Page 13: Introduction to Nuclear Fusion - ocw.snu.ac.krocw.snu.ac.kr/sites/default/files/NOTE/INF-2017-10-Pinch.pdf · jz j0 IP Sa for r a r a I B P 2 0 2S P T. 19 Helical kink instability

13

Large current produced by

capacitor

longitudinal plasma current

self field induced by JZ

Magnetic Pinch • The Z Pinch

J.P. Freidberg, “Ideal Magneto-Hydro-Dynamics”, lecture note

- Equilibrium

Sequence of solution of the MHD equilibrium equations

1. The ▽∙B = 0

2. Ampere’s law: μ0J = ▽xB

3. The momentum equation: JxB = ▽p

BJp

JB

0

0 B

How about the pinch effect in a electric cable/wire?

Page 14: Introduction to Nuclear Fusion - ocw.snu.ac.krocw.snu.ac.kr/sites/default/files/NOTE/INF-2017-10-Pinch.pdf · jz j0 IP Sa for r a r a I B P 2 0 2S P T. 19 Helical kink instability

14

0)(0

rB

dr

d

r

B

dr

dp0

2 0

2

0

2

r

BBp

dr

d

tension force by the curvature of the magnetic field lines

particle pressure + magnetic pressure force

Sequence of solution of the MHD equilibrium equations

1. The ▽∙B = 0

2. Ampere’s law: 0J = ▽xB

3. The momentum equation: JxB = ▽p

01

B

r

)(1

0

rB

dr

d

rJ z

dr

dpBJ z

Magnetic Pinch • The Z Pinch

Page 15: Introduction to Nuclear Fusion - ocw.snu.ac.krocw.snu.ac.kr/sites/default/files/NOTE/INF-2017-10-Pinch.pdf · jz j0 IP Sa for r a r a I B P 2 0 2S P T. 19 Helical kink instability

15

22

0

2

2

0

2

2

00

22

0

2

2

00

2

0

2

00

)(8

)(

2

rr

rIp

rr

rIJ

rr

rIB

z

- The magnetic pressure and plasma pressure each produce

positive (outward forces) near the outside of the plasma.

- The plasma is confined by magnetic tension.

- It is the tension force and not the magnetic pressure

gradient that provides radial confinement of the plasma.

Bennett profiles

(Bennett, 1934)

X Jz

Jz x Bθ

Magnetic Pinch • The Z Pinch

02 0

2

0

2

r

BBp

dr

d

J.P. Freidberg, “Ideal Magneto-Hydro-Dynamics”, lecture note

http://scienceray.com/technology/industry/where-do-rubber-bands-come-from/

Page 16: Introduction to Nuclear Fusion - ocw.snu.ac.krocw.snu.ac.kr/sites/default/files/NOTE/INF-2017-10-Pinch.pdf · jz j0 IP Sa for r a r a I B P 2 0 2S P T. 19 Helical kink instability

16

Magnetic Pinch

- Cylindrical co-ordinates: Specify current profile

drdpBz

j / , ,

)2

/(0 aPIjzj for ar

• The Z Pinch

Page 17: Introduction to Nuclear Fusion - ocw.snu.ac.krocw.snu.ac.kr/sites/default/files/NOTE/INF-2017-10-Pinch.pdf · jz j0 IP Sa for r a r a I B P 2 0 2S P T. 19 Helical kink instability

17

Magnetic Pinch • The Z Pinch

2

0

2

2

00

0

0

0

0

222

)(2

2

1

a

rI

a

rI

r

rI

rrdjr

rrdjr

rB PP

rr

ra

IB P

2

0

2

for ar

r

IB P

2

0 for ar

jrBrr 0

)(1

- Ampere‘ law:

)2

/(0 aPIjzj for ar

a

r

Page 18: Introduction to Nuclear Fusion - ocw.snu.ac.krocw.snu.ac.kr/sites/default/files/NOTE/INF-2017-10-Pinch.pdf · jz j0 IP Sa for r a r a I B P 2 0 2S P T. 19 Helical kink instability

18

Magnetic Pinch • The Z Pinch

→ general result for the z-pinch, not dependent on profiles.

- Calculate , we find 2

0

)(

2

aB

pp

1p

- Compute force balance:

ra

I

a

IBj

dr

dp PPz 2

02

2

Boundary condition p(a)=0:

2

142

2

20)(

a

r

a

PI

rp

)2

/(0 aPIjzj for ar

ra

IB P

2

0

2

Page 19: Introduction to Nuclear Fusion - ocw.snu.ac.krocw.snu.ac.kr/sites/default/files/NOTE/INF-2017-10-Pinch.pdf · jz j0 IP Sa for r a r a I B P 2 0 2S P T. 19 Helical kink instability

19

Helical kink instability

Sausage or pinch instability

Magnetic Pinch • The Z Pinch

A. A. Harms et al, “Principles of Fusion Energy”, World Scientific (2000)

- A number of linear Z-pinch experiments were constructed during

the early years of the fusion program.

- Large currents of ~0.1 MA are needed thus rendering the Z pinch

to operate only in short pulses.

- Exhibiting disastrous instabilities, often leading to a complete

quenching of the plasma after ~1-2 μs.

Page 20: Introduction to Nuclear Fusion - ocw.snu.ac.krocw.snu.ac.kr/sites/default/files/NOTE/INF-2017-10-Pinch.pdf · jz j0 IP Sa for r a r a I B P 2 0 2S P T. 19 Helical kink instability

20

"kink instability" in one of the earliest Z-pinch devices, a pyrex tube used by the AEI team at Aldermaston, or earlier while still at Imperial College

Magnetic Pinch • The Z Pinch

- A number of linear Z-pinch experiments were constructed during

the early years of the fusion program.

- Large currents of ~0.1 MA are needed thus rendering the Z pinch

to operate only in short pulses.

- Exhibiting disastrous instabilities, often leading to a complete

quenching of the plasma after ~1-2 μs.

Page 21: Introduction to Nuclear Fusion - ocw.snu.ac.krocw.snu.ac.kr/sites/default/files/NOTE/INF-2017-10-Pinch.pdf · jz j0 IP Sa for r a r a I B P 2 0 2S P T. 19 Helical kink instability

21 θ-direction tension for equilibrium, z-direction tension for stability

Magnetic Pinch • The Z Pinch

- A number of linear Z-pinch experiments were constructed during

the early years of the fusion program.

- Large currents of ~0.1 MA are needed thus rendering the Z pinch

to operate only in short pulses.

- Exhibiting disastrous instabilities, often leading to a complete

quenching of the plasma after ~1-2 μs.

Page 22: Introduction to Nuclear Fusion - ocw.snu.ac.krocw.snu.ac.kr/sites/default/files/NOTE/INF-2017-10-Pinch.pdf · jz j0 IP Sa for r a r a I B P 2 0 2S P T. 19 Helical kink instability

22

What is θ-pinch?

Page 23: Introduction to Nuclear Fusion - ocw.snu.ac.krocw.snu.ac.kr/sites/default/files/NOTE/INF-2017-10-Pinch.pdf · jz j0 IP Sa for r a r a I B P 2 0 2S P T. 19 Helical kink instability

23

• The θ Pinch

Magnetic Pinch

externally

driven

induced

diamagnetic current

X Bz

Jθ x Bz

Page 24: Introduction to Nuclear Fusion - ocw.snu.ac.krocw.snu.ac.kr/sites/default/files/NOTE/INF-2017-10-Pinch.pdf · jz j0 IP Sa for r a r a I B P 2 0 2S P T. 19 Helical kink instability

24

→ Force balance

→ Ampere‘s law

→ Closed magnetic field lines

BJp

JB

0

0 B

• Plasma Equilibrium

kinetic pressure balanced by JxB (Lorentz) force

2,nqB

Bpv pD

2,,B

pBvqnvqnJ eDeeiDii

Diamagnetic current

0 pJ

0 pB

- If B is applied, plasma equilibrium can be built by itself due to

induction of diamagnetic current.

Magnetic and Kinetic Pressure

induced by the pressure gradient: causing a decrease in B → diamagnetism

B

ion

←∇p

x

BJp

Page 26: Introduction to Nuclear Fusion - ocw.snu.ac.krocw.snu.ac.kr/sites/default/files/NOTE/INF-2017-10-Pinch.pdf · jz j0 IP Sa for r a r a I B P 2 0 2S P T. 19 Helical kink instability

26

• The θ Pinch

Magnetic Pinch

externally

driven

induced

diamagnetic current

J.P. Freidberg, “Ideal Magneto-Hydro-Dynamics”, lecture note

X Bz

Jθ x Bz

- Equilibrium

Sequence of solution of the MHD equilibrium equations

1. The ▽∙B = 0

2. Ampere’s law: μ0J = ▽xB

3. The momentum equation: JxB = ▽p

BJp

JB

0

0 B

Page 27: Introduction to Nuclear Fusion - ocw.snu.ac.krocw.snu.ac.kr/sites/default/files/NOTE/INF-2017-10-Pinch.pdf · jz j0 IP Sa for r a r a I B P 2 0 2S P T. 19 Helical kink instability

27

02 0

2

zB

pdr

d

0

2

0

0

2

22 BB

p z

- At any local value of r, the sum of the particle pressure and the magnetic pressure

is a constant, equal to the externally applied magnetic pressure.

- The plasma is confined radially by the pressure of the externally applied magnetic field.

Sequence of solution of the MHD equilibrium equations

1. The ▽∙B = 0

2. Ampere’s law: 0J = ▽xB

3. The momentum equation: JxB = ▽p

0

z

Bz

r

BJ z

0

1

dr

dpBJ z

Magnetic Pinch • The θ Pinch

Page 28: Introduction to Nuclear Fusion - ocw.snu.ac.krocw.snu.ac.kr/sites/default/files/NOTE/INF-2017-10-Pinch.pdf · jz j0 IP Sa for r a r a I B P 2 0 2S P T. 19 Helical kink instability

28

2

000 /2 Bp

2/122

00

22

0

)]/exp(1[

)/exp(

arBB

arpp

z

- Typical example

Magnetic Pinch • The θ Pinch

J.P. Freidberg, “Ideal Magneto-Hydro-Dynamics”, lecture note

0

2

0

0

2

22 BB

p z

- The plasma is confined radially by the pressure of the externally applied magnetic field.

Plot the forces.

Page 29: Introduction to Nuclear Fusion - ocw.snu.ac.krocw.snu.ac.kr/sites/default/files/NOTE/INF-2017-10-Pinch.pdf · jz j0 IP Sa for r a r a I B P 2 0 2S P T. 19 Helical kink instability

29

- One of the early successes of the fusion program in terms of

the performance.

- Ti ~ 1-4 keV, n ~ 1-2x1022 m-3, β(0) ~ 0.7-0.9

- High temperature using the implosion heating method:

rapidly rising magnetic field acting like a piston

- No indication of macroscopic instability (neutrally stable)

- Severe end loss (τ ~ L/VTi, e.g. 10 μs for a 5 m device)

Magnetic Pinch • The θ Pinch

Page 30: Introduction to Nuclear Fusion - ocw.snu.ac.krocw.snu.ac.kr/sites/default/files/NOTE/INF-2017-10-Pinch.pdf · jz j0 IP Sa for r a r a I B P 2 0 2S P T. 19 Helical kink instability

30

What is screw pinch?

Page 31: Introduction to Nuclear Fusion - ocw.snu.ac.krocw.snu.ac.kr/sites/default/files/NOTE/INF-2017-10-Pinch.pdf · jz j0 IP Sa for r a r a I B P 2 0 2S P T. 19 Helical kink instability

31

• The General Screw Pinch

- A hybrid combination of Z pinch and θ pinch

- This combination of fields allows the flexibility to optimise

configurations w.r.t. force balance and stability.

Magnetic Pinch

X Jz

Jz x Bθ

· Bz

Jθ x Bz

- Equilibrium

Sequence of solution of the MHD equilibrium equations

1. The ▽∙B = 0

2. Ampere’s law: μ0J = ▽xB

3. The momentum equation: JxB = ▽p

BJp

JB

0

0 B

Page 32: Introduction to Nuclear Fusion - ocw.snu.ac.krocw.snu.ac.kr/sites/default/files/NOTE/INF-2017-10-Pinch.pdf · jz j0 IP Sa for r a r a I B P 2 0 2S P T. 19 Helical kink instability

32

- Sequence of solution of the MHD equilibrium equations

1. The ▽∙B = 0

2. Ampere’s law: 0J = ▽xB

3. The momentum equation: JxB = ▽p

01

z

BB

r

z

)(1

0

rB

dr

d

rJ z

dr

dpBJBJ zz

r

BJ z

0

1

02 0

2

0

22

r

BBBp

dr

d z

- Even though the equations are nonlinear, the forces superpose because of symmetry.

Magnetic Pinch • The General Screw Pinch

Page 33: Introduction to Nuclear Fusion - ocw.snu.ac.krocw.snu.ac.kr/sites/default/files/NOTE/INF-2017-10-Pinch.pdf · jz j0 IP Sa for r a r a I B P 2 0 2S P T. 19 Helical kink instability

33

- Because of its flexibility the general screw-pinch relation describes

a wide variety of configurations.

Magnetic Pinch • The General Screw Pinch