The first principle establishes the equivalence of the different formsof energy (radiant, chemical, physical, electrical, and thermal), the possibilityof transformation from one form to another, and the laws that govern thesetransformations. This is the principleof the degradation of energy. The second law of thermodynamics states that the quality of this energy is degraded irreversibly.
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This is the principle of theconservation of energy.
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The first law of thermodynamics says that the total quantityof energy in the universe remains constant. The universe in its totality might be considered a closedsystem of this type this would allow the two laws to be applied to it. in terms of information theory, which demonstrates the equivalence of neguentropy (the opposite of entropy) and information - as a result of the work of Szilard, Gabor, Rothstein,and Brillouin (1940-1950)The two principal laws of thermodynamics apply only to closed systems,that is, entities with which there can be no exchange of energy, information,or material.in terms of statistical theory, which fosters theequivalence of entropy and disorder - as a result of the work ofMaxwell, Gibbs, and Boltzmann (1875), and.in terms of thermodynamics (the science of heat), where the names of Mayer, Joule, Carnot, and Clausius (1865) are important.There are at least three ways of defining entropy: Unfortunately, physicists,engineers, and sociologists use indiscriminately a number of terms thatthey take to be synonymous with entropy, such as disorder, probability,noise, random mixture, heat or they use terms they consider synonymouswith antientropy, such as information, neguentropy, complexity, organization,order, improbability. Today the word entropy is as much a part of the language of thephysical sciences as it is of the human sciences. The second law, known as Carnot'sprinciple, is controlled by the concept of entropy.
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Entropy and the Laws of Thermodynamics The principal energy laws that govern every organization are derivedfrom two famous laws of thermodynamics.