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Heat Q vs Work W and efficiency
Carnot cycle reversible Maximal efficiency depends on (TH -TC) Transformation of heat into work always involves losses (QC) 1824 Sadi Carnot ( )
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Fundaments of thermodynamics
First law: conservation of energy U Rudolf Clausius Second law: transformations (processes) 1854 Äquivalenzwert der Verwandlung R. Clausius Philosophical Magazine, 12 (1856) p.81
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Statistical thermodynamics: History
Daniel Bernouilli Hydrodynamica (1738): Heat = kinetic (movement) energy
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Statistical thermodynamics: History
James Maxwell 1859: Maxwell distribution of velocities in gases
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Statistical thermodynamics: History
Maxwell-Boltzmann distribution Boltzmann Transport Equation (BTE) Number of molecules with velocity v Ludwig Boltzmann 1896: Lectures on gas theory
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Statistical thermodynamic Entropy
1877: Boltzmann entropy S measure for “statistical mixedupness” Ω number of micro states of a system in equilibrium as a macro state Ludwig Boltzmann
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Statistical thermodynamic Entropy
Ω number of micro states of a system in equilibrium as a macro state Ludwig Boltzmann
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Statistical thermodynamic Entropy
Ω number of micro states of a system in equilibrium as a macro state Max Planck Boltzmann constant
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Statistical thermodynamic Entropy
S increases with temperature Ludwig Boltzmann
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Statistical thermodynamic Entropy
Ludwig Boltzmann
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Modern classical thermodynamics
Third law (Nernst) Hermann Walther Nernst
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Statistical thermodynamics: History
Boltzmann distribution Average number of molecules with energy εi Erwin Schrödinger Quantum mechanics: discrete energy states εi
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Statistical thermodynamics: History
Boltzmann distribution Chance of molecule to have energy εi Entropy of the system Erwin Schrödinger
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Statistical thermodynamics: History
Boltzmann Transport Equation (BTE) Ludwig Boltzmann 1896: Lectures on gas theory
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Statistical thermodynamic Entropy
Zentralfriedhof Vienna Ludwig Boltzmann
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Statistical Thermodynamics : Boltzmann distribution
Two level system
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Statistical Thermodynamics: Boltzmann distribution
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