In thermodynamics and fluid mechanics, the stagnation enthalpy of a fluid is the static enthalpy of the fluid at a stagnation point. The stagnation enthalpy is also called total enthalpy. At a point where the flow does not stagnate, it corresponds to the static enthalpy of the fluid at that point assuming it was brought to rest from velocity
V
Stagnation enthalpy, or total enthalpy, is the sum of the static enthalpy (associated with the temperature and static pressure at that point) plus the enthalpy associated with the dynamic pressure, or velocity. This can be expressed in a formula in various ways. Often it is expressed in specific quantities, where specific means mass-specific, to get an intensive quantity:
h0=h+
V2 | |
2 |
where:
h0=
h=
V=
V2 | |
2 |
=
The volume-specific version of this equation (in units of energy per volume, [J/m^3] is obtained by multiplying the equation with the fluid density
\rho
* | |
h | |
0 |
=h*+\rho
V2 | |
2 |
where:
* | |
h | |
0 |
=
h*=
V=
\rho=
\rho | V2 |
2 |
=
The non-specific version of this equation, that means extensive quantities are used, is:
H0=H+m
V2 | |
2 |
where:
H0=
H=
m=
V=
m | V2 |
2 |
=
The suffix ‘0’ usually denotes the stagnation condition and is used as such here.[3]
Enthalpy is the energy associated with the temperature plus the energy associated with the pressure. The stagnation enthalpy adds a term associated with the kinetic energy of the fluid mass.
The total enthalpy for a real or ideal gas does not change across a shock. The total enthalpy can not be measured directly. Instead, the static enthalpy and the fluid velocity can be measured. Static enthalpy is often used in the energy equation for a fluid.
http://ocw.mit.edu/ans7870/16/16.unified/thermoF03/chapter_6.htm