Methods that Circumventthe Second Law of Thermodynamics

Maxwell’s Demon: the Proell effectAtmospheric gravity separator: Chas. Steinmetz @ GE

Asymmetrical mechanical processes: Herb JohnsonAsymmetrical atomic processes: thermoelectrics, Daniel Sheehan at the

University of San DiegoAsymmetrical atomic processes: superconductivity, Peter Keefe at the University

of Detroit MercyAsymmetrical atomic processes: inverted populations of phase space, Steven

Smith’s magnetothermodynamics @ www.geocities.com/electrograviticsAsymmetrical atomic processes: infrared photovoltaics

Gibbs Free Energy changes: G = H – TS

Methods that Circumventthe Second Law of Thermodynamics

Maxwell’s Demon: the Proell effectAtmospheric gravity separator: Chas. Steinmetz @ GE

Asymmetrical mechanical processes: Herb JohnsonAsymmetrical atomic processes: thermoelectrics, Daniel Sheehan at the

University of San DiegoAsymmetrical atomic processes: superconductivity, Peter Keefe at the University

of Detroit MercyAsymmetrical atomic processes: inverted populations of phase space, Steven

Smith’s magnetothermodynamics @ www.geocities.com/electrograviticsAsymmetrical atomic processes: infrared photovoltaics

Gibbs Free Energy changes: G = H – TS

Methods that Circumventthe Second Law of Thermodynamics

Maxwell’s Demon: the Proell effectAtmospheric gravity separator: Chas. Steinmetz @ GE

Asymmetrical mechanical processes: Herb JohnsonAsymmetrical atomic processes: thermoelectrics, Daniel Sheehan at the

University of San DiegoAsymmetrical atomic processes: superconductivity, Peter Keefe at the University

of Detroit MercyAsymmetrical atomic processes: inverted populations of phase space, Steven

Smith’s magnetothermodynamics @ www.geocities.com/electrograviticsAsymmetrical atomic processes: infrared photovoltaics

Gibbs Free Energy changes: G = H – TS

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