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In [[thermodynamics]] and [[fluid mechanics]], '''stagnation temperature''' is the [[temperature]] at a [[stagnation point]] in a fluid flow. At a stagnation point the speed of the fluid is zero and all of the [[kinetic energy]] has been converted to [[internal energy]] (adiabatically) and is added to the local [[Enthalpy|static enthalpy]]. In [[incompressible flow|incompressible fluid flow]], and in [[isentropic]] [[compressible flow]], the stagnation temperature is equal to the ''total temperature'' at all points on the streamline leading to the stagnation point.
<ref>Van Wylen and Sonntag, ''Fundamentals of Classical Thermodynamics'', section 14.1</ref> See [[gas dynamics]].
 
==Derivation==
 
===Adiabatic===
Stagnation temperature can be derived from the [[First Law of Thermodynamics]].  Applying the Steady Flow Energy Equation
<ref>Van Wylen and Sonntag, ''Fundamentals of Classical Thermodynamics'', equation 5.50</ref> and ignoring the work, heat and gravitational potential energy terms, we have:
 
:<math>h_0 = h + \frac{V^2}{2}\,</math>
 
where:
 
:<math>h_0 =\,</math> stagnation (or total) enthalpy at a stagnation point
 
:<math>h =\,</math> static enthalpy at the point of interest along the stagnation streamline
 
:<math>V =\,</math> velocity at the point of interest along the stagnation streamline
 
Substituting for enthalpy by assuming a constant specific heat capacity at constant pressure (<math>h = C_p T</math>) we have:
 
:<math>T_0 = T + \frac{V^2}{2C_p}\,</math>
 
or
 
:<math>\frac{T_0}{T} =  1+\frac{\gamma-1}{2}M^2\,</math>
 
where:
 
:<math>C_p =\,</math> [[specific heat capacity]] at constant pressure
 
:<math>T_0 =\,</math> stagnation (or total) temperature at a stagnation point
 
:<math>T =\,</math> temperature (or static temperature) at the point of interest along the stagnation streamline
 
:<math>V = \,</math> velocity at the point of interest along the stagnation streamline
 
:<math>M =\,</math> Mach number at the point of interest along the stagnation streamline
 
:<math>\gamma =\,</math> [[Heat capacity ratio|Ratio of Specific Heats]] (<math>C_p/C_v</math>), ~1.4 for air at ~300 K
 
===Flow with Heat Addition===
:<math>h_{02} = h_{01} + q </math>
:<math>T_{02} = T_{01} + \frac{q}{C_p} </math>
:q = Heat per unit mass added into the system
 
Strictly speaking, enthalpy is a function of both temperature and density. However, invoking the common assumption of a calorically perfect gas, enthalpy can
be converted directly into temperature as given above, which enables one to define a stagnation temperature in terms of the more fundamental property,
stagnation enthalpy.
 
Stagnation properties (e.g. stagnation temperature, stagnation pressure) are useful in [[jet engine]] performance calculations. In engine operations, stagnation temperature is often called [[total air temperature]].  A bimetallic thermocouple is often used to measure stagnation temperature, but allowances for thermal radiation must be made.
 
==Solar Thermal Collectors==
Solar Thermal Collector performance testing utilizes the term stagnation temperature to indicate the maximum achievable collector temperature with a stagnant fluid (no motion), an ambient temperature of 30C, and incident solar radiation of 1000W/m^2. The aforementioned figures are just arbitrary values and do possess any true meaning without a proper context.
 
==See also==
*[[Stagnation point]]
*[[Stagnation pressure]]
*[[Total air temperature]]
 
==References==
*Van Wylen, G.J., and Sonntag, R.E. (1965), ''Fundamentals of Classical Thermodynamics'', John Wiley & Sons, Inc., New York
 
{{Reflist}}
 
[[Category:Fluid dynamics]]

Revision as of 17:40, 24 July 2013

In thermodynamics and fluid mechanics, stagnation temperature is the temperature at a stagnation point in a fluid flow. At a stagnation point the speed of the fluid is zero and all of the kinetic energy has been converted to internal energy (adiabatically) and is added to the local static enthalpy. In incompressible fluid flow, and in isentropic compressible flow, the stagnation temperature is equal to the total temperature at all points on the streamline leading to the stagnation point. [1] See gas dynamics.

Derivation

Adiabatic

Stagnation temperature can be derived from the First Law of Thermodynamics. Applying the Steady Flow Energy Equation [2] and ignoring the work, heat and gravitational potential energy terms, we have:

h0=h+V22

where:

h0= stagnation (or total) enthalpy at a stagnation point
h= static enthalpy at the point of interest along the stagnation streamline
V= velocity at the point of interest along the stagnation streamline

Substituting for enthalpy by assuming a constant specific heat capacity at constant pressure (h=CpT) we have:

T0=T+V22Cp

or

T0T=1+γ12M2

where:

Cp= specific heat capacity at constant pressure
T0= stagnation (or total) temperature at a stagnation point
T= temperature (or static temperature) at the point of interest along the stagnation streamline
V= velocity at the point of interest along the stagnation streamline
M= Mach number at the point of interest along the stagnation streamline
γ= Ratio of Specific Heats (Cp/Cv), ~1.4 for air at ~300 K

Flow with Heat Addition

h02=h01+q
T02=T01+qCp
q = Heat per unit mass added into the system

Strictly speaking, enthalpy is a function of both temperature and density. However, invoking the common assumption of a calorically perfect gas, enthalpy can be converted directly into temperature as given above, which enables one to define a stagnation temperature in terms of the more fundamental property, stagnation enthalpy.

Stagnation properties (e.g. stagnation temperature, stagnation pressure) are useful in jet engine performance calculations. In engine operations, stagnation temperature is often called total air temperature. A bimetallic thermocouple is often used to measure stagnation temperature, but allowances for thermal radiation must be made.

Solar Thermal Collectors

Solar Thermal Collector performance testing utilizes the term stagnation temperature to indicate the maximum achievable collector temperature with a stagnant fluid (no motion), an ambient temperature of 30C, and incident solar radiation of 1000W/m^2. The aforementioned figures are just arbitrary values and do possess any true meaning without a proper context.

See also

References

  • Van Wylen, G.J., and Sonntag, R.E. (1965), Fundamentals of Classical Thermodynamics, John Wiley & Sons, Inc., New York

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  1. Van Wylen and Sonntag, Fundamentals of Classical Thermodynamics, section 14.1
  2. Van Wylen and Sonntag, Fundamentals of Classical Thermodynamics, equation 5.50