2. Methods that Circumvent the Second Law of Thermodynamics Maxwell’s Demon: the Proell effect Atmospheric gravity separator: Chas. Steinmetz @ GE Asymmetrical mechanical processes: Herb Johnson Asymmetrical atomic processes: thermoelectrics, Daniel Sheehan at the University of San Diego Asymmetrical atomic processes: superconductivity, Peter Keefe at the University of Detroit Mercy Asymmetrical atomic processes: inverted populations of phase space, Steven Smith’s magnetothermodynamics @ www.geocities.com/electrograviticswww.geocities.com/electrogravitics Asymmetrical atomic processes: infrared photovoltaics Gibbs Free Energy changes:  G =  H – T  S

4. Methods that Circumvent the Second Law of Thermodynamics Maxwell’s Demon: the Proell effect Atmospheric gravity separator: Chas. Steinmetz @ GE Asymmetrical mechanical processes: Herb Johnson Asymmetrical atomic processes: thermoelectrics, Daniel Sheehan at the University of San Diego Asymmetrical atomic processes: superconductivity, Peter Keefe at the University of Detroit Mercy Asymmetrical atomic processes: inverted populations of phase space, Steven Smith’s magnetothermodynamics @ www.geocities.com/electrograviticswww.geocities.com/electrogravitics Asymmetrical atomic processes: infrared photovoltaics Gibbs Free Energy changes:  G =  H – T  S

9. Methods that Circumvent the Second Law of Thermodynamics Maxwell’s Demon: the Proell effect Atmospheric gravity separator: Chas. Steinmetz @ GE Asymmetrical mechanical processes: Herb Johnson Asymmetrical atomic processes: thermoelectrics, Daniel Sheehan at the University of San Diego Asymmetrical atomic processes: superconductivity, Peter Keefe at the University of Detroit Mercy Asymmetrical atomic processes: inverted populations of phase space, Steven Smith’s magnetothermodynamics @ www.geocities.com/electrograviticswww.geocities.com/electrogravitics Asymmetrical atomic processes: infrared photovoltaics Gibbs Free Energy changes:  G =  H – T  S

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