Chapter2 : Fluid Statics
Lecture 3 :


Isothermal and Non-Isothermal Fluids

Isothermal Fluid (Constant Temperature Solution)

Recap equation (1.7)

 

The equation of state for a compressible system generally relates its density to its pressure and temperature. If the fluid is a perfect gas at rest at constant temperature, it can be written from eq (1.7) that

Since ,                                                                  

 = constant

 
(3.17)

Where po and ro are the pressure and density at some reference horizontal plane. With the help of Eq. (3.17), Eq. (3.14) becomes,

(3.18)
(3.19)

where z and z0 are the vertical coordinates of the plane concerned for pressure p and the reference plane respectively from any fixed datum.

Non-isothermal Fluid

The temperature of the atmosphere up to a certain altitude is frequently assumed to decrease linearly with the altitude z as given by

(3.20)

where T0 is the absolute temperature at sea level and the constant a is known as lapse rate.

For the standard atmosphere, a = 6.5 K/km and T0= 298 K.

With the help of =rRT and (3.20), the Eq. (3.14) can be written as,

(3.21)

 


Integration of Eq. (3.21) yields

 

 

Hence,

(3.22)

 

The altitude z in Eq. (3.22) is measured from the sea level where the pressure is po.

 

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