carnot's heat heat engine is also known as ideal heat engine.because in carnot's the precess is
reversible .Total heat converted into work .
The efficiency is maximum for carnot's heat engine.
difference schematic diagram between carnot heat engine and heat engine
Carnot heat engine was develop in 1824 by Nicolas Leonard.
The Carnot cycle is a mathematical description of an engine that derives its power from heat.
Three scientists who have studied heat are James Prescott Joule, Sadi Carnot, and Joseph Black. Joule is known for his work on the conservation of energy, Carnot for his development of the concept of heat engines, and Black for his work on latent heat.
The Carnot engine problem refers to the theoretical limit on the efficiency of heat engines, as described by the Carnot cycle. This problem highlights that no real heat engine can be 100 efficient, as some energy is always lost as heat. The efficiency of a heat engine is limited by the Carnot efficiency, which depends on the temperatures of the heat source and sink. This concept helps engineers understand and improve the efficiency of real-world heat engines.
The Carnot Heat Engine Cycle and the Carnot Heat Pump Cycle are reversible cycles and do not exist in any actual operation. However, they are very useful for predicting maximum possible thermal efficiencies and coefficients of performance using the absolute temperature of the heat source and the absolute temperature of the heat sink. The Carnot Cycle consists of two reversible and adiabatic ( isentropic ) steps and two reversible and isothermal steps.
Sadi Carnot discovered that the transformation of heat into mechanical energy could only occur when thermal energy flows from a hot object to a cool object. he also discovered that in this process some heat was always lost.
No. Carnot's theorem applies to heat engines - machines that convert heat to other types of energy.
The efficiency of a quasi-static or reversible Carnot cycle depends only on the temperatures of the two heat reservoirs, and is the same, whatever the working substance. A Carnot engine operated in this way is the most efficient possible heat engine using those two temperatures
The Carnot efficiency of a heat engine can be calculated by dividing the temperature difference between the hot and cold reservoirs by the temperature of the hot reservoir. The formula is: Carnot efficiency 1 - (Tc/Th), where Tc is the temperature of the cold reservoir and Th is the temperature of the hot reservoir.
The Carnot cycle gives the theoretical maximum efficiency of an engine operating between two heat reservoirs. The Carnot cycle is an idealized engine cycle that is thermodynamically reversible. Real systems such as power plants are not reversible, and the entropy of a real material changes with temperature (which is not accounted for by the Carnot cycle). A steam power plant operates closer to a cycle known as the Rankine cycle.
The Carnot COP is significant in the efficiency of heat engines because it represents the maximum possible efficiency that a heat engine can achieve. It serves as a benchmark for comparing the performance of real-world heat engines, helping engineers to design more efficient systems.