helium presenting by naveen in university of technology and management

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helium presenting by naveen

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Slide 1: 

Helium

HeliumThe energy source of tomorrow? : 

HeliumThe energy source of tomorrow? BY NAVEEN

The Truth : 

The Truth Helium has the shape of an pineapple and taste like chicken

Introduction : 

Introduction A helium-neon laser, usually called a He-Ne laser, is a type of small gas laser. HeNe lasers have many industrial and scientific uses, and are often used in laboratory demonstrations of optics. He-Ne laser is a four-level laser. Its usual operation wavelength is 632.8 nm, in the red portion of the visible spectrum. It operates in Continuous Working (CW) mode. The Helium-Neon laser was the first continuous laser.

The Different Types of Fusion : 

The Different Types of Fusion

Helium terms : 

PY3P05 Helium terms Orthohelium states are lower in energy than the parahelium states. Explanation for this is: Parallel spins make the spin part of the wavefunction symmetric. Total wavefunction for electrons must be antisymmetric since electrons are fermions. This forces space part of wavefunction to be antisymmetric. Antisymmetric space wavefunction implies a larger average distance between electrons than a symmetric function. Results as square of antisymmetric function must go to zero at the origin => probability for small separations of the two electrons is smaller than for a symmetric space wavefunction. If electrons are on the average further apart, then there will be less shielding of the nucleus by the ground state electron, and the excited state electron will therefore be more exposed to the nucleus. This implies that it will be more tightly bound and of lower energy.

Deuterium-Helium-3 : 

Deuterium-Helium-3

Deuterium-Helium-3 : 

Deuterium-Helium-3 Because D-He-3 Fusion involves 3 protons as opposed to 2 with DT Fusion, the amount of heat required for good fusion parameters is 100 keV. This is about 10 times greater than the amount needed for DT fusion. At the Naka Fusion Center in Japan, scientists set the world record for the hottest plasma in their advanced tokamak JT-60. This plasma reached 520,000,000 Kelvin, which corresponds to ion energies of 50 keV. Thus the energy requirements for helium-3 fusion are not insurmountable.

Deuterium-Helium-3 : 

Another significant benefit of using Deuterium and Helium-3 fuels is that the reaction products, being charged particles, can be manipulated by electric and magnetic fields and can consequently be used for direct energy conversion which is far more efficient than thermal conversion. Deuterium-Helium-3 D-He-3 reactions produce no high energy neutrons, and consequently the activation of metals is drastically reduced. (Stray D-D reactions will generate some neutrons)

IECInertial Electrostatic Confinement : 

IECInertial Electrostatic Confinement Concept: Using electric fields to accelerate nuclei Potential with D-D, D-T, D-3He, 3He-3He Two common approaches Gridded – direct applied voltage Polywell – voltage derived from electron cloud

IEC : 

IEC UW-Madison leads research in grid IEC Inner sphere and outer sphere Potential depth ~100kV Needs only ~60mA of current compared to ~1MA in Tokamaks

IEC : 

IEC The Polywell Excess electron cloud from injection Solenoids create magnetic confinement field Intrinsically steady-state Most current project: WB-6 Has produced a fusion rate of 109/sec (D-D) Only needed 12.5kV driving to produce 10kV well

IEC : 

IEC Energy Conversion: IEC has most potential for direct energy conversion (charged products) Efficiency ~70%-80% Some loss due to escaping voltage well Thermal cycle still optional Efficiency ~30%

IEC : 

IEC Current Issues/Disadvantages: Limits on core densities For gridded IECs, heat flux For Polywell, electron confinement Feasibility of direct energy conversion

IEC : 

IEC Advantages Relatively simple design (UW-Madison’s ~2’ in diam.) Easily accelerates ions to massive energies Energies of 100keV realistic for D-3He Limited loss of plasma/reactants Low ash accumulation Design allows for easy fuel injection

Helium-3 Manufacturing : 

Helium-3 Manufacturing Helium-3 is a byproduct of tritium decay, and tritium can be produced through neutron bombardment of lithium, boron, or nitrogen targets. Current supplies of helium-3 come, in part, from the dismantling of nuclear weapons where it accumulates; approximately 150 kilograms of it have resulted from decay of US tritium production since 1955, most of which was for warheads. Roughly eighteen tons of tritium stock are required for each ton of helium-3 produced annually by decay. The production rate is N γ = N t½ / (ln2). Note that any breeding of tritium on Earth requires the use of a high neutron flux, which proponents of helium-3 nuclear reactors hope to avoid. Furthermore, the production and storage of huge amounts of the gas tritium appears to be uneconomical.

Lunar Supplies : 

Lunar Supplies Samples collected in 1969 by Neil Armstrong during the first lunar landing showed that helium-3 concentrations in lunar soil are at least 13 parts per billion (ppb) by weight. Levels may range from 20 to 30 ppb in undisturbed soils. Quantities as small as 20 ppb may seem too trivial to consider. But at a projected value of $40,000 per ounce, 220 pounds of helium-3 would be worth about $141 million.

Where does Lunar H-3 come from? : 

Where does Lunar H-3 come from?

Lunar Supplies : 

Lunar Supplies The highest concentrations are in the lunar maria; about half the He3 is deposited in the 20% of the lunar surface covered by the maria. There is an estimated total of 1,100,000 metric tonnes of He3 that have been deposited by the solar wind in the lunar regolith. Since the regolith has been stirred up by collisions with meteorites, we'll probably find He3 down to depths of several meters.

Lunar Supplies : 

Lunar Supplies Ouyang Ziyuan who is now in charge of the Chinese Lunar Exploration Program has stated on many occasions that one of the main goals of the Chinese Lunar program would be the mining of helium-3, from where "each year three space shuttle missions could bring enough fuel for all human beings across the world."

How much would it take to Power the United States? : 

How much would it take to Power the United States? Digging a patch of lunar surface roughly three-quarters of a square mile to a depth of about 9 ft. should yield about 220 pounds of helium-3--enough to power a city the size of Dallas or Detroit for a year. About 25 tonnes of He3 would power the United States for 1 year at our current rate of energy consumption. To put it in perspective: that's about the weight of a fully loaded railroad box car, or a maximum Space Shuttle payload.

Extracting Helium-3 : 

Extracting Helium-3 Extracting the isotope would not be particularly difficult. Heating to 600 degrees Celsius releases gases trapped in the soil. As the vapors are cooled, the various gases present sequentially separate out of the mix. In the final step, special membranes would separate helium-3 from ordinary helium.

Extracting Helium-3 : 

Extracting Helium-3 For every ton of Helium-3 extracted from lunar soil nine tons of oxygen, water and other life-sustaining substances, as well as six tons of hydrogen useful for powering fuel cells, would be yielded. These materials are ideal for sustaining manned mining outposts or even settlements as well as producing fuel for rockets.

The Payoff : 

The Payoff Let's suppose that by the time we're slinging tanks of He-3 off the moon, the world-wide demand is 100 tonnes of the stuff a year, and people are happy to pay $3 billion per tonne. That gives us gross revenues of $300 billion a year. To put that number in perspective: that rate of income would provide for the launch of a Saturn V style rocket every day for the next 10,000 years.

Medical Applications : 

Medical Applications P + Nitrogen gases/Water => C-11, N-13, O-15 Carbon-11 => used to diagnose renal and prostate cancers Oxygen-15 & Nitrogen-13 used in respiratory examinations; esp. PET scans All above have t½ <20 min Availability: Cyclotrons – too big, too few

Conclusions : 

Conclusions Using He-3 as fusion fuel: More efficient electrical conversions Low (negligible) levels of radioactivity Only neutrons from chance D-D fusion in D-3He fuel Little to no activation of nearby structures No radioactive fuel needed (No Tritium!) If priced at ~$1 Billion/ton, He-3 has Energy cost ~equal to oil at $7/barrel In terms of stored energy, He-3 on the Moon has ~10x as much as all economically viable supplies of fossil fuels on the Earth

Bibliography : 

Bibliography Kulcinksi, Cameron, Santarius, Sviatoslavsky, and Wittenberg, "Fusion Energy from the Moon for the 21st Century." 1988. Fusion Technology Institute, University of Wisconsin.   Bennett, Gregory. “Lunar Helium-3 as an Energy Source.” Jun 27, 1999. May 17, 2007. <http://www.asi.org/adb/02/09/he3-intro.html>   Whittington, Mark R. “World’s Next Energy Source may be just a moon away.” USA Today. December 9, 2004.   Liu, Melinda and Carmichael, Mary. “To Reach for the Moon.” Newsweek. February, 12 2007.   Zaterman, Danny. “Helium-3 Fusion.” May 18, 2006. May 17, 2007. < http://ocw.mit.edu/NR/rdonlyres/Nuclear-Engineering/22-012Spring-2006/C3E48256-762A-49FF-9B18-1E5A5D39F89B/0/helium3_fusion.pdf>   DiMare, Paul. “Mining The Moon.” Popular Mechanics. October 2004.

Bibliography : 

Bibliography Black, Harvey. Fusion’s Future. Milwaukee Journal Sentinel. Monday, February 12, 2007.   Santarius, John F. Inertial Electrostatic Confinement Overview. 5/12/07 Fusion Technology Institute. <http://fti.neep.wisc.edu/iec/inertial_electrostatic_confineme.htm>   Kulcinski, G. L. The Significance of Helium-3 Fusion. 5/12/07 Fusion Technology Institute. < http://fti.neep.wisc.edu/neep533/FALL2001/lecture25.pdf>   Polywell. 5/14/07. Wikipedia. 5/14/07. <http://en.wikipedia.org/wiki/Polywell>   Helium-3. 5/13/07. Wikipedia. 5/13/07. <http://en.wikipedia.org/wiki/Helium-3>

Slide 29: 

Thanks For Your Attention

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