As a result, the heat never flows spontaneously from cold to hot is comparable to a spontaneous flow of heat needing a positive net entropy change. Hence, the equation of entropy is hereunder: The net entropy change for the two reservoirs is if heat Q travels from R1 to R2. Assume at temperatures T1 and T2 there are two heat reservoirs R1 and R2 (such as the stove and the block of ice). This equation essentially presents an alternate temperature definition that coincides with the standard definition. Formula or Equation of EntropyĪccording to the Clausius definition, if a quantity of heat Q flows into a huge heat reservoir at a temperature T above absolute zero, the entropy increase is S = Q/T. The system is in equilibrium with its surroundings for reversible processes but not for irreversible processes. Because a minor increase in the restraining force can switch the direction of the process from expansion to compression, the latter is reversible. Similarly, compressed gas confined in a cylinder might either expand freely into the atmosphere (an irreversible process) if a valve was opened, or it could accomplish beneficial work by moving a movable piston against the force required to confine the gas. It is reversible because just a minuscule amount of heat is required to reverse the process from progressive freezing to progressive thawing. In contrast, depending on whether a tiny amount of heat is given to or taken from the system, a block of ice placed in an ice-water bath will melt or freeze a bit more.
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