Heat engine is defined as a device that converts heat energy into mechanical energy or more exactly
a system which operates continuously and only heat and
work may pass across its boundaries.
The operation of a heat engine can best be represented by a thermodynamic cycle. Some examples are:
Otto, Diesel, Brayton,
Stirling and Rankine cycles.
A forward heat engine has a positive work output such as Rankine or Brayton cycle. Applying
the first law of thermodynamics to the cycle gives:
Q1 - Q2 - W = 0
states that the
thermal efficiency of the cycle, , has an upper limit
(the thermal efficiency of the Carnot cycle), i.e.
It can be shown that:
Q1 > W
which means that it is impossible to convert the whole heat input to work and
Q2 > 0
which means that a minimum of heat supply to the cold reservoir is necessary.
A reverse heat engine has a positive work input such as heat pump and refrigerator. Applying
the first law of thermodynamics to the cycle gives:
- Q1 + Q2 + W = 0
In case of a reverse heat engine the second law of thermodynamics is as follows:
It is impossible to transfer heat from a cooler body to a hotter body without any work input i.e.
W > 0
which means that the coefficient of performance for a heat pump is greater than unity.