The thermal efficiency of a heat engine is the amount of useful work an engine can do based on the amount of heat input. The thermal efficiency is represented by the symbol , and given by the equation
is the useful work and
is the total heat energy input from the hot source.
Heat engines often operate at around 30% to 50% efficiency, due to practical limitations. It is impossible for heat engines to achieve 100% thermal efficiency () according to the Second law of thermodynamics. This is impossible because some waste heat is always produced produced in a heat engine, shown in Figure 1 by the term. Although complete efficiency in a heat engine is impossible, there are many ways to increase a system's overall efficiency.
This same result can be gained by measuring the waste heat of the engine. For example, if 200 J is put into the engine, and observe 120 J of waste heat, then 80 J of work must have been done, giving 40% efficiency.
There is a maximum attainable efficiency of a heat engine which was derived by physicist Sadi Carnot. Following laws of thermodynamics the equation for this turns out to be
is the temperature of the cold 'sink' and
is the temperature of the heat reservoir.
This describes the efficiency of an idealized engine, which in reality is impossible to achieve. From this equation, the lower the sink temperature or the higher the source temperature , the more work is available from the heat engine. The energy for work comes from a decrease in the total energy of the fluid used in the system. Therefore the greater the temperature change, the greater this decrease in the fluid and thus the greater energy available to do work is.
Click here to learn about how a heat engine works.
For thermal efficiency of car engines, click here.