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DANCING WITH THE STARS DANCING WITH THE STARS QUEST FOR FUSION ENERGY QUEST FOR FUSION ENERGY Abhay Abhay K. Ram K. Ram PSFC, MIT I A P 2 0 1 0 J a n u a r y 2 0

DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

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Page 1: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

DANCING WITH THE STARSDANCING WITH THE STARS

QUEST FOR FUSION ENERGYQUEST FOR FUSION ENERGY

AbhayAbhay K. RamK. Ram

PSFC, MIT

IAP

2010

January

20

Page 2: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

The sun, with all those planetsrevolving around it, and dependent

on it, can still ripen a bunch of grapesas though it had nothing else in the

universe to do.

Galileo

Page 3: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

I deduce that the creation of the world happened in the beginning of the autumn of 710 JP. Using

astronomical tables, I determined the first Sunday after the autumnal equinox for the year 710 JP (4004 BC(4004 BC) which was October 23 of that year.

….. the preceding evening of October 23,marks the first day of creation and the start of time.

Reverend James UssherArchbishop of Armagh, Church of IrelandThe Annals of the WorldThe Annals of the World (London, 1658)

JP – Julian Year starting at January 1, 4713 BC

Newton: born 1643Newton: born 1643KeplerKepler: 1571 : 1571 –– 16301630

Page 4: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

THE SUN AS A COAL POWER PLANTTHE SUN AS A COAL POWER PLANT

What is the mass of the Sun ??

What is the power output of the Sun ??

How much energy is released in burning coal ??

Page 5: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

THE SUN AS A COAL POWER PLANTTHE SUN AS A COAL POWER PLANT

302 10≈ ×M kg

Power output of the 264 10 = Sun Watts×

2 42 0 /C kgO CO MJ+ → +

Sun's lifet

me

i

6 30

2

11

6

(40 10 / ) (2 1

2 10

0 )4 10 /

.

J kg kg

secJ sec

× ××

×=

=

The Sun would last for about 6300 years.The Sun would last for about 6300 years.

Page 6: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

Charles Darwin (1809 Charles Darwin (1809 ---- 1882)1882)ON THE ORIGIN OF SPECIES BY MEANS OF

NATURAL SELECTION (London, 1859)

I am tempted to give one other case, the well-known denudation of the Weald.

Page 7: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

Hence, under ordinary circumstances, I should infer that for a cliff 500 feet in height, a denudation of one inch per

century for the whole length would be a sufficient allowance. At this rate, on the above data, the denudation

of the Weald must have required 306,662,400 years; or say three hundred million years. But perhaps it would be safer to allow two or three inches per century, and this would reduce the number of years to one hundred and

fifty or one hundred million years.

Charles Darwin, On The Origin of Species

by Means of Natural SelectionLondon (1859)

Page 8: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

Hermann von Helmholtz

Conservation of Energy

Conversion of Mechanical Energy to Heat

William Thomson (Lord Kelvin)

Second Law of Thermodynamics

Absolute Temperature Scale

Page 9: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

SUN AS A GRAVITY DRIVEN HEAT ENGINESUN AS A GRAVITY DRIVEN HEAT ENGINE

0 83 7 12 10 , 0≈ ×× ≈M R mkg

Power output of the = Sun 264 10 Watts×

Potential energySolar power out

Supu

n's lifetime t

146 10 .sec= ×=

The Sun would last for about 20 million years.The Sun would last for about 20 million years.

235

Potential Energ y M

GR

=

11 3 1 26.674 10 G m kg s− − −= ×

Page 10: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

What then are we to think of such geological estimates as 300,000,000 years for the “denudation of the Weald”? Whether is it more probable that the physical conditions

of the sun’s matter differ 1000 times more than dynamics compel us to suppose they differ from of matter in our laboratories; or that a stormy sea, with possible Channel tides of extreme violence, should

encroach of a chalk cliff 1,000 times more rapidly than Mr. Darwin’s estimate of one inch per century?

Sir William Thomson (Lord Kelvin)On the Age of the Sun’s Heat

Macmillan’s Magazine (March 5, 1862)

Page 11: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

It takes a long time to prepare a world for man, such thing is not done in a day. Some of the great scientists,

carefully deciphering the evidences furnished by geology, have arrived at the conviction that our world is

prodigiously old, and they may be right, but Lord Kelvin is not of their opinion. He takes a cautious, conservative

view, in order to be on the safe side, and feels sure it is not so old as they think. As Lord Kelvin is the highest authority in science now living, I think we must yield to

him and accept his view.

Mark TwainWas the World Made for Man

(1903).

Page 12: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

“This study of the radiation and internal conditions of a star brings forward very pressingly a problem often debated in this Section: What is the source

of the heat which the Sun and stars are continually squandering?”

Arthur Eddington, The Observatory, 1920.(Volume XLIII, No. 557, pp. 311-358)

Page 13: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

“Lord Kelvin’s date of the creation of the Sun is treated with no more respect than Archbishop Ussher’s.

………………….

Only the inertia of tradition keeps the contraction hypothesis alive – or rather, not alive, but an unburied

corpse.”

Arthur Eddington, The Observatory, 1920.(Volume XLIII, No. 557, pp. 311-358)

Page 14: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

“A star is drawing on some vast reservoir of energy by means unknown to us. This reservoir can scarcely be other than the sub-atomic energy which, it is known,

exists abundantly in all matter……

There is sufficient in the Sun to maintain its output of heat for 15 billion years.”

Arthur Eddington, The Observatory, 1920.(Volume XLIII, No. 557, pp. 311-358)

Page 15: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

1905: Einstein (E=mc2).1913: Bohr (model of the atom).1920: Eddington’s speech.1928: Analysis of Fraunhofer lines (1814) show that hydrogen is

the most abundant element in the Sun’s atmosphere.1929: Tonks and Langmuir (plasma oscillations).1932: Chadwick (discovery of the neutron).1933: Joliot-Curie (conversion of energy into mass).1933: Cockcroft and Walton (conversion of mass into energy).1938: Bethe (energy production in the Sun and stars through

thermonuclear fusion).

TIME LINE OF SOME IMPORTANT EVENTS

Page 16: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

“If, indeed, the sub-atomic energy in the stars is being freely used to maintain their

great furnaces, it seems to bring a little nearer to fulfilment our dream of controlling this latent power for the well-being of the

human race - or for its suicide.”

Arthur Eddington, The Observatory, 1920.(Volume XLIII, No. 557, pp. 311-358)

Page 17: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

1954: USA tests first hydrogen bombin Bikini.

1956: First experiments on a tokamakin Russia.

1958: Declassification of fusion announced in Geneva.

Page 18: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

DANCING WITH THE STARS:

QUEST FORFUSION ENERGY

Page 19: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

Acknowledgements:

Dr. Jerry Hughes

Mr. Paul Rivenberg

Dr. Charles Kessel

Page 20: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

JUST THE FACTS

Page 21: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

SOME BASIC DIMENSIONS

SIZE OF AN ATOM ~ 10-10 m = 1 Å

SIZE OF A NUCLEUS ~ few 10-15 m = few fm

SIZE OF A PROTON OR NEUTRON ~ 1 fm

Page 22: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

BASIC FORCES IN NATURE

RANGERELATIVESTRENGTH

FORCE

infinite

finite / infinite

~ few fm

~ 0.1% fm

6 x 10-39GRAVITATIONAL

1/137ELECTROMAGNETIC

1STRONG

~10-6WEAK

Page 23: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

No exchange of energy.Exchange of energy through

the field.

Important for magneticfusion on Earth.

Important for fusion inthe Sun.

Magnetic fields existessentially everywhere.

Gravitational fields existeverywhere.

Magnetic field of one movingcharge affects the other.

Gravitational field of one mass affects the other.

Between two movingcharged particles.

Between two masses.

MAGNETIC FORCEGRAVITATIONAL FORCE

Page 24: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

“It appears that the radical element responsible for the continuing thread of cosmic unrest is

the magnetic field.”

Eugene N. Parker (1979).

Page 25: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

NUCLEAR FUSION INTERACTIONS

Page 26: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

If (MA + MB) > (MC +MD) then energy is generated

[E = Mc2]

Page 27: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

FUSION REACTIONS ARE QUANTUM PHENOMENA

Need to overcome the mutual repulsion of ions.

Page 28: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

NUCLEI OF INTEREST IN FUSION ENERGY

Page 29: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

1 eV = 1.6022x10-19 Joule1 eV = 1.16x104 ≈ 12,000 K

0 °C = 32 °F = 273.15 Kenergy required to ionize a hydrogenatom = 13.6 eV ≈ 163,200 K100 Watt bulb lit for one second uses 100 Joules of energy(equivalently, 6.24 x 1020 eV)

1 keV = 1000 eV = 103 eV1 MeV = 1,000,000 eV = 106 eV

Page 30: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

FUSION REACTIONS IN THE SUNFUSION REACTIONS IN THE SUN

Page 31: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

FUSION REACTIONS IN THE SUNFUSION REACTIONS IN THE SUN

Page 32: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

FUSION REACTIONS IN THE SUNEach proton in the solar core leads to 6.55 MeVof electromagnetic energy from the Sun.

The observed solar luminosity requires that3.7x1038 H are converted into 4He per second.

The Sun’s composition and mass shows that itstarted with about 9x1056 hydrogen atoms.

About 10% of the hydrogen in the Sun has beenconsumed in the past 4.5 billion years.

Page 33: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

FUSION REACTIONS IN THE SUNFUSION REACTIONS IN THE SUN

Page 34: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

NUCLEAR REACTION FOR FUSION POWER ON EARTH

Page 35: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

TEMPERATURE DEPENDENCE OF “RATES”FOR FUSION REACTIONS

Page 36: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

MEAN REACTION TIME FOR D-T FUSION

Assume: temperature T = 20 keVdensity n = 1020 nuclei per cubic meter

Then: <σv> ≈ 4x10-22 m3 / sec

So the mean lifetime before fusion reactions is= ≈ 25 seconds

The speed of a deuteron is about 1,000 km / sec.

>< vσ1

n

Page 37: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

NUCLEAR REACTION FOR FUSION POWER ON EARTH

Page 38: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

MAGNETIC CONFINEMENT

Page 39: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

MOTION IN A MAGNETIC FIELD

Motion along the magnetic field line is unconfined.Alcator routinely operates at 5 Tesla magnetic fields

(100,000 times the Earth’s magnetic field)

Page 40: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

MOTION IN A TOROIDAL MAGNETIC FIELD

Electrons and ions drift in opposite directions(ions drift upwards, electrons downwards).

First pointed out by Enrico Fermi.

Page 41: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

MOTION IN A TOROIDAL MAGNETIC FIELD

Page 42: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

TWISTED MAGNETIC FIELD LINES

Create helical magnetic field lines by introducing a toroidal current.

In Alcator currents of the order of 1 MA are generated.

Page 43: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

STARTING THE FUSION ENGINE

Page 44: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

STARTUP PHASE LEADING TO THE SUN

Compression of hydrogen molecular cloud(pressure 10-15 torr ≈ 1.4 x 10-18 atmosphere)Collapsing cloud cores (globules) begin to light up as gravitational potential energy is converted to heat.

Page 45: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

STARTUP PHASE LEADING TO THE SUN

A globule collapses and continues to heat up.

The temperature in the core rises to about150,000 K ( ≈ 13 eV).

Around 107 K (≈ 1 keV)the p-p reaction starts.

Page 46: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

STARTUP PHASE LEADING TO THE SUN

Page 47: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

GIANT MOLECULAR CLOUD

Density ≈ 108 particles per cubic meter; temperature ≈ 100 K

Pressure ≈ 10-15 torr ≈ 1.4 x 10-18 atmosphere

Page 48: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

BIRTH REGION OF STARSBIRTH REGION OF STARS

HH46-47As observed by SPITZERSPITZER

Page 49: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

PROTOSTARSPROTOSTARS

Page 50: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

MAIN SEQUENCE STAR

Page 51: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

EVOLUTION OF THE SOLAR LUMINOSITY

Luminosity is the total electromagnetic power emitted.

Presently, L⊙ = 3.84 x 1026 Watts (solar constant ≈ 1.4 kW / m2) .

Page 52: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

STARTUP OF A LABORATORY FUSION DEVICE

Prior to a discharge create high vacuum (10-6 torr).Hydrogen gas injected into the vacuum vessel (few 10-6 torr).Turn on the toroidal magnetic field coils.Transformer is discharged (the current in the primary is slowly changed).

Page 53: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

STARTUP OF A LABORATORY FUSION DEVICE

The induced voltage in the chamber ionizes the gas creating a plasma.The plasma current, density, and temperature increase.

Page 54: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

EVOLUTION OF A LABORATORY FUSION PLASMA(Alcator C-Mod)

Page 55: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

MAIN SEQUENCE

Page 56: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

COMPARING THE SUN WITH A FUSION COMPARING THE SUN WITH A FUSION REACTORREACTOR

SUNSUN ARIES IVARIES IV

J. N. Bachall & R. K. Ulrich, Reviews of Modern Physics (1988).C. Kessel et al., Fusion Engineering and Design (2006);

and private communications,

Page 57: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

Solar power output = 3.84 x 1028 Watts

Global power consumption = 1.6 x 1013 Watts

Typical power output of a reactor = 1 - 2 x 109 Watts

Page 58: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

ELECTRON DENSITY PROFILESELECTRON DENSITY PROFILESx 1011

n e(1

0 20

) m -3

n e(1

020

) m -3

20 3

19 3

peak density 3.6 10edge density 7.2 0 1

mm

= ×

= ×

31 3

27 3

peak density 6 10edge density 9 10

mm

≈ ×

≈ ×

Sun ARIES

R / R⊙ r / a

a = 1.38 mR⊙ = 108 m

Page 59: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

TEMPERATURE PROFILESTEMPERATURE PROFILES

Sun ARIES

R / R⊙ r / a

T (k

eV)

T (k

eV)

peak temperature 1.35edge tempera

tur e 0.04

keVkeV

==

peak temperature 25edge temperature

0. 1

keVkeV

==

Page 60: DANCING WITH THE STARS QUEST FOR FUSION ENERGYlibrary.psfc.mit.edu/catalog/online_pubs/iap/iap2010/ram.pdfDANCING WITH THE STARS QUEST FOR FUSION ENERGY Abhay K. Ram PSFC, MIT I A

SOLAR LUMONISITY AND ENERGY OUTPUTSOLAR LUMONISITY AND ENERGY OUTPUTL

/ L⊙

R / R⊙d(

Ener

gy)/(

dR/R

⊙)

Energy Production

Luminosity is the total electromagnetic power emitted.

Luminosity

Presently, L⊙ = 3.84 x1026 Watts (solar constant ≈ 1.4 kW / m2)

R / R⊙

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SOLAR LUMONISITY AND ENERGY OUTPUTSOLAR LUMONISITY AND ENERGY OUTPUTL

/ L⊙

R / R⊙d(

Ener

gy)/(

dR/R

⊙)

Energy Production

Luminosity

R / R⊙

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COMPARISON OF PRESSURE PROFILES

ARIES

Sun

Pres

sure

(N /

m2 )

R / R⊙ r / a

Solar pressure normalized to 2.29 x 1016

ARIES pressure normalized to 2.79 x 106

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ENERGY CONFINEMENT TIME

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ENERGY CONFINEMENT TIME

(Watts) rate heating(Joules)energy stored total

τE (sec) =

The goal in fusion is to reach the required temperaturewith the least amount of heating power.

In the Sun the energy confinement time is a million years.

In magnetic fusion devices it is around a second.

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THE PLASMA EDGE

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THE SOLAR CORONA

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THE SOLAR CORONA

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THE SOLAR CORONA

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S. J. Zweben: http://www.pppl.gov/~szweben

THE EDGE IN A LABORATORY FUSION DEVICETHE EDGE IN A LABORATORY FUSION DEVICE

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THE EDGE IN A LABORATORY FUSION DEVICETHE EDGE IN A LABORATORY FUSION DEVICE

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THE EDGE IN A LABORATORY FUSION DEVICE

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THE EDGE IN A LABORATORY FUSION DEVICE

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THE REACTOR WALLTHE REACTOR WALL

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Constraint on a fusion reactor:

No “squandering” of energy

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FUSION BIFUSION BI--PRODUCTSPRODUCTS

Sun: 4He γ ν

Fusion reactor: 4He n

For every reaction cycle producing 4He, about 26 MeV is contained in the core as heat and

about 0.8 MeV is carried away by ν’s.

For every reaction cycle, the energy in 4Heis about 3.5 MeV and that in n is 14.1 MeV.

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Neutrinos they are very small.They have no charge and have no massAnd do not interact at all.The earth is just a silly ballTo them, through which they simply pass,Like dustmaids down a drafty hallOr photons through a sheet of glass.

John UpdikeCosmic Gall

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The neutron releasedblow open some otherswhich release more neutronsand start this all over

Blow open some othersand choirs will crumbleand start this all overwith eyes burned to ashes.

Peter MeinkeAtomic Pantoum

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STEADY STATE OPERATION

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OPERATION OF A LABORATORY FUSION DEVICE

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SOLAR IRRADIANCE OVER “SHORTER” TIME

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TOWARD FULFILLING THE QUESTTOWARD FULFILLING THE QUEST

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D-T operation

Controlling the edge

Plasma facing materials

Energy extraction

Steady state operation

Breeding of Tritium

SOME TOPICS TO PONDER OVERSOME TOPICS TO PONDER OVER

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No problem is so big or so complicatedthat it can't be run away from!

Linus Van Pelt(Peanuts by Charles M. Schulz)

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PROGRESS TOWARDS THE FUTURE

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INTERNATIONAL THERMONUCLEAR EXPERIMENAL REACTOR

30 m

24 m

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INTERNATIONAL THERMONUCLEAR EXPERIMENAL REACTOR

Q =

Demonstrate the scientific and technological feasibility of fusion energyExtended burn of D-T plasmas with steady state operation as a goal.Q > 5Typical fusion power level ~ 500 MW

Plasma current ~ 15 MAToroidal magnetic field of 5.3 TeslaDensity ~ 1020 m-3

inEnergy outEnergy

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MEASURING PERFORMANCE – LAWSON CRITERION

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MEASURING PERFORMANCE – LAWSON CRITERION

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The best way to predict the future is to invent it.

Alan Kay, Computer Scientist (1982).