He Fusion 2009 A Rat Ay Production

8/3/2019 He Fusion 2009 A Rat Ay Production

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PRODUCTION OF HELIUM AND ENERGY IN THE SOLID FUSION

Y. Arata, Y.C. Zhang, and X.F. Wang

Center for Advanced Science and Innovation, Osaka University

2-1 Yamadaoka, Suita, Osaka, 565-0871, Japan

In this paper, A new type Solid Fusion Reactor has been developed to test the existence of

solid state nuclear fusion ( Solid Fusion): reproducible experiments have been made atroom temperature and without external power input. Both of the energy and Helium

generation affected by the reactor structure, gas flow rate, powder weight, and cooling

condition were studied. Deuterium gas loading processes of two types of nanomaterial

(ZrO2Pd35 and ZrO2Ni30Pd5) were studied respectively in this paper. The results showed

the energy produced in ZrO2Ni30Pd5 is higher than in ZrO2Pd35. Helium as an important

evidence of solid-state fusion was detected by mass analyzer QMS. As result, Solid

Fusion has been confirmed by the helium existence, and then we developed the Helium

production system.

Gas Loading O_1

Session 4


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Production of Helium and Energy

in the Solid Fusion

Y.C. Zhang, and X.F. Wang

Center for Advanced Science and Innovation,Osaka University, Japan

Y. Arata


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Fig.1

Original ZrPd

powder

Counts

ZrPd

(after deoxidization treatment) ZrPd

+D2

(after D2

gas loading)

Fig.1 X-ray diffraction analysis

C

ounts

[C]

PdO(110) P

d(111)

PdO(110) P

d(111)


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Fig.2


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Fig.3[A]

[B]

Fig.3 Distribution of temperature and pressure

Time [min]

Tin

Ts

Tsf

Pin

T=5 CTin,

Ts,

Tsf:Te

mperature[C]

Pin:Pressure[atm]

Room temperature

ZrPd (16[g]) +Pure (Helium free) D2

D2 gas flow rate: 50 [cc]/min09

3/23TinTs

Tsf

Pin

T=5 CTin,

Ts,

Tsf:Temperatu

re[C]

Pin:Pressure[atm]

Room temperature

ZrNiPd (16[g]) + Pure (Helium free) D2D

2gas flow rate: 50[cc]/ [min]

09 3/11-13


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Fig.4

Fig.4 Distribution of temperature and pressure

Tin

Ts

Tsf

Pin

T=5 CTin,T

s,

Tsf:Temperatur

e[C]

Pin:Pressure[atm

]

Room temperature

ZrNiPd (16[g]) + Pure (Helium free) D2

D2 gas flow rate: 50[cc]/ [min]

09 3/11-13

Time [min]

ZrNiPd (16[g]) + Pure (Helium free) D2

D2 gas flow rate: 70[cc]/ [min]09 3/16

Tin

Ts

Tsf

Pin

T=5 CTin,

Ts,

Tsf

:Temperature[C]

Pin:

Pressure[atm]

Room temperature

[A]

[B]


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Fig.5


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Fig.6


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Fig.7


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Fig.8


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Fig.9and10

Fig.9 ZrNiPd powder Fig.10 ZrPd powder

Absorption volume of D2

gas and excess energy of the powder (16[g]) during thepure D2

gas loading under the same conditions except for the cooling condition.

Tp

: powder temperature at the highest point during D2

gas loading

ZrNiPd ZrPd


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Fig11omparison of the absorbed D2

gas volume andexcess energy between ZrNiPd

powder and ZrPd

owder under different gas flow rate.


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Fig.12


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Fig.13

[C]

M4

4He

M4

4He


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Fig.14


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Fig.15 AandB

Fig.15 Spectrum of reaction products

Concentration times : 186 Concentration times: 342

Before concentration Before concentration

(A) ZrNiPd powder (B) ZrPd powder


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Fig.15C

Fig.15C Helium intensity and the intensity ratio of Helium per

Neon22 detected from reacted gas of ZrNiPd powder using QMS

Air gas (Helium/Neon 22=3.2)


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Fig.16Helium intensity relation to concentration Times

with loading using cooling type-3


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Fig.17

Conclusion:


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Conclusion Conclusion: (1)Either excess energy or helium of the ZrNiPd

powder is always about ten times higher thanthat of the ZrPd powder.

(2)By using the weight 16 [g] of the ZrNiPdpowder, the excess power 4 [watt] lasted stably

for one hour, only less than one gram palladium

was consumed. Its cost is lower than the ZrPdpowder. We choose the ZrNiPd powder as a

good material for the solid fusion.

(3)The concentration of helium was verysuccessful. These results indicate that the

reacted gas of solid nuclear fusion" can serve

as a source of helium production.

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He Fusion 2009 A Rat Ay Production