text: The efficiency of a heat engine relates how much useful work is output for a given amount of heat energy input.
  From the laws of thermodynamics, after a completed cycle:
  :and therefore
  :where
  : is the net work extracted from the engine in one cycle. (It is negative, in the IUPAC convention, since work is done by the engine.)
  : is the heat energy taken from the high temperature heat source in the surroundings in one cycle. (It is positive since heat energy is added to the engine.)
  : is the waste heat given off by the engine to the cold temperature heat sink. (It is negative since heat is lost by the engine to the sink.)
  In other words, a heat engine absorbs heat energy from the high temperature heat source, converting part of it to useful work and giving off the rest as waste heat to the cold temperature heat sink.
  In general, the efficiency of a given heat transfer process is defined by the ratio of "what is taken out" to "what is put in". (For a refrigerator or heat pump, which can be considered as a heat engine run in reverse, this is the coefficient of performance and it is ≥ 1.) In the case of an engine, one desires to extract work and has to put in heat , for instance from combustion of a fuel, so the engine efficiency is reasonably defined as
  The efficiency is less than 100% because of the waste heat  unavoidably lost to the cold sink (and corresponding compression work put in) during the required recompression at the cold temperature before the power stroke of the engine can occur again.
  The theoretical maximum efficiency of any heat engine depends only on the temperatures it operates between. This efficiency is usually derived using an ideal imaginary heat engine such as the Carnot heat engine, although other engines using different cycles can also attain maximum efficiency. Mathematically, after a full cycle, the overall change of entropy is zero:
  Note that  is positive because isothermal expansion in the power stroke increases the multiplicity of the working fluid while  is negative since recompression decreases the multiplicity. If the engine is ideal and runs reversibly,  and , and thus
  which gives  and thus the Carnot limit for heat-engine efficiency,
  where  is the absolute temperature of the hot source and  that of the cold sink, usually measured in kelvins.
  The reasoning behind this being the maximal efficiency goes as follows. It is first assumed that if a more efficient heat engine than a Carnot engine is possible, then it could be driven in reverse as a heat pump. Mathematical analysis can be used to show that this assumed combination would result in a net decrease in entropy. Since, by the second law of thermodynamics, this is statistically improbable to the point of exclusion, the Carnot efficiency is a theoretical upper bound on the reliable efficiency of any thermodynamic cycle.
  Empirically, no heat engine has ever been shown to run at a greater efficiency than a Carnot cycle heat engine.
  Figure 2 and Figure 3 show variations on Carnot cycle efficiency with temperature. Figure 2 indicates how efficiency changes with an increase in the heat addition temperature for a constant compressor inlet temperature. Figure 3 indicates how the efficiency changes with an increase in the heat rejection temperature for a constant turbine inlet temperature.