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Transmutation of metal at low energy in a confined ... - LENR-CANR

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4. Experimental evidence<br />

Fig. 11. View <strong>of</strong> the plasma he<strong>at</strong> transfer mechanism<br />

Once a stable plasma has been achieved for more than 500 sec., we can compare the <strong>in</strong>put <strong>energy</strong>,<br />

electrical power, with the quantity <strong>of</strong> <strong>energy</strong> necessary to warm up and evapor<strong>at</strong>e the solution<br />

w<strong>at</strong>er. Omitted from this calcul<strong>at</strong>ion is <strong>energy</strong> associ<strong>at</strong>ed with chemical reactions; <strong>energy</strong> rel<strong>at</strong>ed to<br />

the he<strong>at</strong><strong>in</strong>g-up and fusion <strong>of</strong> the tungsten; <strong>energy</strong> used <strong>in</strong> expand<strong>in</strong>g gas and steam leav<strong>in</strong>g the cell;<br />

<strong>energy</strong> lost by thermal and electromagnetic radi<strong>at</strong>ion; and loss <strong>of</strong> he<strong>at</strong> through the <strong>in</strong>sul<strong>at</strong>ion. Even<br />

though this extra <strong>energy</strong> is omitted from the calcul<strong>at</strong>ion, the cell is found to produce more <strong>energy</strong><br />

than is be<strong>in</strong>g applied. If the <strong>energy</strong> needed to warm-up the electrolyte to 100°C and then produce<br />

evapor<strong>at</strong>ion is taken <strong>in</strong>to account, values <strong>of</strong> output/<strong>in</strong>put = 1.2 to 1.4 are obta<strong>in</strong>ed.<br />

Us<strong>in</strong>g an SEM (scann<strong>in</strong>g electron microscope), the presence <strong>of</strong> rhenium, osmium, gold, hafnium,<br />

thulium, erbium, and ytterbium are found on the surface <strong>of</strong> the c<strong>at</strong>hode. These elements were not<br />

previously <strong>in</strong> the appar<strong>at</strong>us (see Fig. 12, 13, 14).

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