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The second law is offered as a simple observation in the same essay but its status as Clarke's second law was conferred by others. It was initially a derivative of the first law and formally became Clarke's second law where the author proposed the third law in the 1973 revision of Profiles of the Future, which included an acknowledgement. [4]
With the development of statistical mechanics, the third law of thermodynamics (like the other laws) changed from a fundamental law (justified by experiments) to a derived law (derived from even more basic laws). The basic law from which it is primarily derived is the statistical-mechanics definition of entropy for a large system:
The first law of thermodynamics is a version of the law of conservation of energy, adapted for thermodynamic processes. In general, the conservation law states that the total energy of an isolated system is constant; energy can be transformed from one form to another, but can be neither created nor destroyed.
The Sir Arthur C. Clarke Memorial Trophy Inter School Astronomy Quiz Competition, held in Sri Lanka every year and organised by the Astronomical Association of Ananda College, Colombo. The competition started in 2001 as "The Sir Arthur C. Clarke Trophy Inter School Astronomy Quiz Competition" and was renamed after his death. [156] [157]
Clarke's three laws, three adages from British science-fiction writer Arthur C. Clarke's extensive writings about the future; Three Laws of Robotics, a set of rules devised by the science fiction author Isaac Asimov
The third law of thermodynamics states: As the temperature of a system approaches absolute zero, all processes cease and the entropy of the system approaches a minimum value. This law of thermodynamics is a statistical law of nature regarding entropy and the impossibility of reaching absolute zero of temperature. This law provides an absolute ...
Researchers have made a breakthrough in applying the first law of thermodynamics to complex systems, rewriting the way we understand complex energetic systems.
However, it is known from thermodynamics that the slope of the ΔG curve is −ΔS. Since the slope shown here reaches the horizontal limit of 0 as T → 0 then the implication is that Δ S → 0, which is the Nernst heat theorem.