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Material Science for Understanding the Fleischmann and Pons Effect

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New advancements on the Fleischmann-Pons Effect European Parliament Bruxelles 03/06/2013 V. Violante Ph D ENEA LENR Research Coordinator Material Science for Understanding the Fleischmann and Pons Effect Cooperation frame: ENEA-NRL-SRI-University of Missouri Re-Research, Consorzio Veneto Ricerca
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New advancements on the Fleischmann-Pons Effect European Parliament Bruxelles 03/06/2013

V. Violante Ph D ENEA LENR Research Coordinator

Material Science for Understanding the Fleischmann and Pons Effect

Cooperation frame: ENEA-NRL-SRI-University of Missouri

Re-Research, Consorzio Veneto Ricerca

Revision of the Effect: Government supported Research Projects have been conceived and developed in Italy and US, during the last decade, to verify the existence of the Effect .

Results with signals well above the measurement uncertainties are confirming the anomalous production of excess of power during electrochemical loading of Palladium with Deuterium.

Excess of power has the following features: 1) Threshold effect (loading D/Pd > 0.9) 2) Unobserved with hydrogen 3) Unexplainable as chemical effect 4) Occurs only if materials are showing specific characteristics

New advancements on the Fleischmann-Pons Effect – Bruxelles 03/06/2013

The Fleischmann and Pons Effect is the appearance of excess energy when a Pd cathode is electrolyzed in heavy water (D2O).

Calorimetry (Mass Flow): Closed Cells

PdPt

PdPt

PdPt

PdPt

Catalyst

Cathode -

Anode +

Closed Electrochemical Cell

New advancements on the Fleischmann-Pons Effect – Bruxelles 03/06/2013

LiOD

D2+O2

D2O

H2O + LiOH

Input and Output Energy and Power (Efficiency 97%)

Electrode operated with H2O

Roma 04-06 -2013

L17 experiment. Excess of power: the output power becomes 5 times larger than the input.

25

25.5

26

26.5

27

27.5

28

28.5

29

29.5

30

200000 220000 240000 260000 280000 300000

T_cell (ーC)

T_box (ーC)

Electrolyte temperature

An excess of power

(observed during revision studies)

Electrolyte temperature increasing during the excess.

New advancements on the Fleischmann-Pons Effect – Bruxelles 03/06/2013

0

0.1

0.2

0.3

0.4

0.5

0.6

0.7

200000 220000 240000 260000 280000 300000

W_in (W)

W_out (W)

Pout (W)

Pin (W)

500% Excess

Pow

er (

W)

Reproducibility 60% in ENEA and 70% at SRI

80

500

100

37

24

80

12 13

43

15

12

200

50

10

100

1000

14 15 16 17 18 19 20 21 22 23 24 25

Per

cen

tag

e E

xce

ss P

ow

er [

PX

S/P

In]

ENEA Cathode Material Designation L#

ENEA

SRI

New advancements on the Fleischmann-Pons Effect – Bruxelles 03/06/2013

Important evidence: Only active cathodes in ENEA were active also at SRI

Experienced At ENEA only

The occurrence of the effect is depending on the material status

Material giving excess

A different behavior related to the material status was observed above the loading threshold D/Pd (atomic fraction) =0.9:

1) High power gain during the excess. 2) Low power gain during excess. 3) No excess.

Material Behavior and Role

Material not giving excess

Different contaminants give different charcteristics by using the same treatment

New advancements on the Fleischmann-Pons Effect – Bruxelles 03/06/2013

Contaminants may act on:

- Grain size

- Crystal orientation

Contaminants Effects on Material Behavior

- Grain boundary

- Etching Surface Morphology Acts on Electrochemistry

Acts on Electrochemistry

Controls Loading

Controls Loading

Contaminants at ppm level have been identified to be responsible for material

characteristics and behavior

New advancements on the Fleischmann-Pons Effect – Bruxelles 03/06/2013

The experimental evidences have led to a production of a material having characteristics close to the ones belonging to the active samples

Designing Materials (Doping and Alloys)

e.g. Palladium was doped with Platinum to have a spectrum of contaminants closer to the ones of the rough palladium giving active samples

NRL: Palladium Rhodium Alloy

New advancements on the Fleischmann-Pons Effect – Bruxelles 03/06/2013

L66 (120-160) Adding Platinum

L66 (160-200) Adding Platinum

ENEA Palladium doped by Platinum , up to 25-30% excess ENEA

Material not giving excess (low Pt content)

Applying NRL- Electrolysis Protocol

Electrode surface after electrolysis

L99(175-215) HM Pt doped

ENEA Palladium doped by Platinum

New advancements on the Fleischmann-Pons Effect – Bruxelles 03/06/2013

NRL Differential calorimetry

500 mW Heat Burst

Addition of Fe,Cu,Al

The large amount of produced energy (> 10 eV per atom) is impossible to be interpreted as a chemical process.

Progress in the field requires well conceived coordinated research projects involving modern instrumentation.

Material status is the key to observe the effect. Material science is the key to understand it, since some material characteristics support some processes rather than others.

By applying the scientific method future work should be oriented towards the definition of the effect rather than its demonstration.

Concluding Remarks

New advancements on the Fleischmann-Pons Effect – Bruxelles 03/06/2013

Reprducibility of the Effect requires the reproducibility of the material status.


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