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  1. 3 days ago · 2. Around 1850, Rudolf Clausius and William Thomson introduced thermodynamics and established the first two laws: the first law states that total energy is conserved, and the second law states that heat does not spontaneously flow from cold to hot bodies. 3.

  2. 6 days ago · Rudolf Clausius, the originator of the entropy concept in 1865, defined entropy change mathematically as the amount of energy transferred to a substance by heating (or cooling, in which case the transfer is negative) divided by the temperature.

  3. 5 days ago · Thermodynamics is the study of how energy behaves as it moves from one place to another and as it transforms from one form to another. The second law of thermodynamics states that in an isolated system, entropy (disorder) will always increase with the passage of time. This law was formulated by German physicist Rudolf Clausius in 1850.

  4. 4 days ago · The second law of thermodynamics—formulated in the 19th century by Lord Kelvin and Rudolf Clausius— was discovered as a side effect of research on improving the efficiency of steam engines. As each machine transforms only a portion of energy into work—the rest is released as heat ‘waste’—a good engine design aims to waste as little energy as possible.

  5. 4 days ago · Instead, it is determined by the temperature of the lower atmosphere and surface through a physical relationship known as the Clausius-Clapeyron equation, named for 19th-century German physicist Rudolf Clausius and 19th-century French engineer Émile Clapeyron.

  6. 4 days ago · Hint:Clausius equality and inequality are two terms which come into picture while finding the closed integral of the ratio of change of heat to the temperature of a thermodynamic system. Complete step by step answer: Assume: \[d{Q_1}\] is the amount of heat supplied to both the heat engines.

  7. 3 days ago · Clausius–Clapeyron relation - The Clausius–Clapeyron relation, named after Rudolf Clausius and Benoît Paul Émile Clapeyron, is a way of characterizing a discontinuous phase transition between two phases of matter of a sin

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