In the history of science, the caloric theory is a theory that heat consists of a fluid called "caloric" that flows from hotter to colder bodies. Caloric was also thought of as a weightless gas that could pass in and out of pores in solids and liquids. The "caloric theory" was abandoned by the mid-19th century in favor of the theory of heat.
The caloric theory was introduced by Antoine Lavoisier. Lavoisier had discovered the explanation of combustion in terms of oxygen in the 1770s. In his book Réflexions sur le phlogistique (1783), Lavoisier argued that phlogiston theory was inconsistent with his experimental results, and proposed a 'subtle fluid' called caloric as the substance of heat. According to this theory, the quantity of this substance is constant throughout the universe, and it flows from warmer to colder bodies.
Since heat was a material substance in caloric theory, and therefore could neither be created nor destroyed, conservation of heat was a central assumption.See, for example, Carnot, Sadi (1824). Reflexions on the motive power of fire.
The introdution of the Caloric theory was also influenced by the experiments of Joseph Black related to the thermal properties of materials. Besides the caloric theory, another theory existed in the late eighteenth century that could explain the phenomena of heat: the kinetic theory. The two theories were considered to be equivalent at the time, but caloric theory was the more modern one, as it used a few ideas from atomic theory and could explain both combustion and calorimetry.
We can explain the expansion of air under heat: caloric is absorbed into the molecules of air, which increases its volume. If we say a little more about what happens to caloric during this absorption phenomenon, we can explain the radiation of heat, the state changes of matter under various temperatures, and deduce nearly all of the gas laws.
Sadi Carnot developed his principle of the Carnot cycle, which as of 2005 still forms the basis of heat engine theory, solely from the caloric viewpoint.
However, one of the greatest confirmations of the caloric theory was Pierre-Simon Laplace's theoretical correction of Sir Isaac Newton’s pulse equation. Laplace, a calorist, added a constant to Newton’s equation, which we refer to today as the adiabatic index of a gasLaplace, P.-S. (1816). Sur la vitesse dus son dans l'air et dans l'eau. In Annales de Chimie et de Physique.. This addition not only substantially corrected the theoretical prediction of the speed of sound, but also continued to make even more accurate predictions for almost a century afterward, even as measurements of the index became more precise.
His results were not seen as a "threat" to caloric theory at the time, as this theory was considered to be equivalent to the alternative kinetic theory.See for example Lavoisier, A.-L. de (1783). Mémoire sur la chaleur, lu à l'Académie royale des sciences, le 28 juin 1783, par MM. Lavoisier et de La Place. In fact, to some of his contemporaries, the results added to the understanding of caloric theory.
Rumford's experiment inspired the work of James Prescott Joule and others towards the middle of the 19th century. In 1850, Rudolf Clausius published a paper showing that the two theories were indeed compatible, as long as the calorists' principle of the conservation of heat was replaced by a principle of conservation of energy. In this way, the caloric theory was absorbed into the annals of physics, and evolved into modern thermodynamics, in which heat is the kinetic energy of molecules.
Obsolete scientific theories | Thermodynamics | History of physics | History of chemistry | History of ideas
Kalorische Theorie | カロリック説 | Теплород | Kalorikki | Caloric
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