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    Volta potential 1

    Volta potential

    Volta potential (also called Volta potential difference, or contact potential difference, or outer potential

    difference, , delta psi) in electrochemistry, is the electrostatic potential difference between two points ("1" and

    "2") in the vacuum:

    point "1" close to the surface of metal M1;

    point "2" close to the surface of metal M2

    (or electrolyte);

    where M1

    and M2

    are two metals that are in contact and in thermodynamic equilibrium.[1]

    The Volta potential is named after Alessandro Volta.

    Volta potential between two metals

    When the two metals depicted here are in thermodynamic equilibrium with eachother as shown (equal Fermi levels), the vacuum electrostatic potential is not flat

    due to a difference in work function.

    When two metals are electrically isolated

    from each other, an arbitrary potential

    difference may exist between them.

    However, when two different neutrally

    charged metals are brought into electrical

    contact (even indirectly, say, through a long

    wire), electrons will flow from the metal

    with a higher Fermi level to the metal with

    the lower Fermi level until the Fermi levels

    in the both phases are equal. Once this has

    occurred, the metals are in thermodynamic

    equilibrium with each other (the actual

    number of electrons that passes between thetwo phases is usually small). Just because

    the Fermi levels are equal, however, does

    not mean that the electric potentials are

    equal. The electric potential outside each material is controlled by its work function, and so dissimilar metals can

    show an electric potential difference even at equilibrium.

    The Volta potential is notan intrinsic property of the two bulk metals under consideration, but rather is determined

    by work function differences between the metals' surfaces. Just like the work function, the Volta potential depends

    sensitively on surface state, contamination, and so on.

    http://en.wikipedia.org/w/index.php?title=Work_functionhttp://en.wikipedia.org/w/index.php?title=Work_functionhttp://en.wikipedia.org/w/index.php?title=Fermi_levelhttp://en.wikipedia.org/w/index.php?title=File%3AWork_function_mismatch_gold_aluminum.svghttp://en.wikipedia.org/w/index.php?title=Work_functionhttp://en.wikipedia.org/w/index.php?title=Electrostatic_potentialhttp://en.wikipedia.org/w/index.php?title=Fermi_levelhttp://en.wikipedia.org/w/index.php?title=Alessandro_Voltahttp://en.wikipedia.org/w/index.php?title=Electrolytehttp://en.wikipedia.org/w/index.php?title=Electrostatic_potentialhttp://en.wikipedia.org/w/index.php?title=Electrochemistry
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    Volta potential 2

    Measurement of Volta potential (Kelvin probe)

    Kelvin probe energy diagram at flat vacuum configuration, used for measuring

    Volta potential between sample and probe.

    The Volta potential can be significant (of

    order 1 volt) but it cannot be measured

    directly by an ordinary voltmeter. A

    voltmeter does not measure vacuum

    electrostatic potentials, but instead the

    difference in Fermi level between the two

    materials, a difference that is exactly zero at

    equilibrium.

    The Volta potential however corresponds to

    a real electric field in the spaces between

    and around the two metal objects, a field

    generated by the accumulation of charges at

    their surfaces. The total charge over

    each objects' surface depends on the capacitance between the two objects, by the relation whereis the Volta potential. It follows therefore that the value of the potential can be measured by varying the

    capacitance between the materials by a known amount (e.g., by moving the objects further from each other), and

    measuring the displaced charge that flows through the wire that connects them.

    The Volta potential difference between a metal and an electrolyte can be measured in a similar fashion.[2]

    The Volta

    potential of a metal surface can be mapped on very small scales by use of a Kelvin probe force microscope. In this

    case the capacitance change is not knowninstead, a compensating DC voltage is added to cancel the Volta

    potential so that no current is induced by the change in capacitance. This compensating voltage is the negative of the

    Volta potential.

    References

    [1] IUPAC Gold Book, definition of contact (Volta) potential difference. (http://goldbook. iupac.org/C01293. html)

    [2][2] V.S. Bagotsky, "Fundamentals of Electrochemistry", Willey Interscience, 2006.

    http://goldbook.iupac.org/C01293.htmlhttp://en.wikipedia.org/w/index.php?title=Kelvin_probe_force_microscopehttp://en.wikipedia.org/w/index.php?title=Capacitancehttp://en.wikipedia.org/w/index.php?title=Fermi_levelhttp://en.wikipedia.org/w/index.php?title=Voltmeterhttp://en.wikipedia.org/w/index.php?title=File%3AKelvin_probe_setup_at_flat_vacuum.svg
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    Article Sources and Contributors 3

    Article Sources and ContributorsVolta potential Source: http://en.wikipedia.org/w/index.php?oldid=560343032 Contributors: ChrisCork, Daniele Pugliesi, GregorB, Mcapdevila, Nanite, Randomtime, Sanya3, Stan J Klimas,

    12 anonymous edits

    Image Sources, Licenses and ContributorsFile:Work function mismatch gold aluminum.svg Source: http://en.wikipedia.org/w/index.php?title=File:Work_function_mismatch_gold_aluminum.svg License: Creative Commons Zero

    Contributors: User:Nanite

    File:Kelvin probe setup at flat vacuum.svg Source: http://en.wikipedia.org/w/index.php?title=File:Kelvin_probe_setup_at_flat_vacuum.svg License: Creative Commons Zero Contributors:

    User:Nanite

    License

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