Air enters an adiabatic nozzle at 400kPa and 900K with negligible velo...
Problem Statement:
Air enters an adiabatic nozzle at 400 kPa and 900 K with negligible velocity. If the flow is ideal and exit pressure is 100 kPa, the exit temperature in K and the exit velocity in m/s are respectively?
Solution:
Given,
Inlet pressure (P1) = 400 kPa
Inlet temperature (T1) = 900 K
Exit Pressure (P2) = 100 kPa
Velocity at the inlet (V1) = 0 m/s
Assumption:
The flow is ideal and adiabatic.
Formula:
The temperature at the exit of the nozzle (T2) can be calculated using the isentropic relation,
T2 = T1*(P2/P1)^((γ-1)/γ)
where γ = Cp/Cv is the ratio of specific heats.
The velocity at the exit of the nozzle (V2) can be calculated using the Bernoulli's equation,
P1 + ½ρV1^2 = P2 + ½ρV2^2
where ρ is the density of air.
Calculation:
Given, Cp/Cv = γ = 1.4 for air.
Using the isentropic relation,
T2 = T1*(P2/P1)^((γ-1)/γ)
T2 = 900*(100/400)^((1.4-1)/1.4)
T2 = 536.24 K
Using the Bernoulli's equation,
P1 + ½ρV1^2 = P2 + ½ρV2^2
Since the velocity at the inlet (V1) is negligible, V1^2 can be neglected.
Hence, P1 = P2 + ½ρV2^2
The density of air (ρ) can be calculated using the ideal gas law,
P1V1/T1 = P2V2/T2
ρ = P1/(RT1)
where R = 287 J/kg.K is the gas constant for air.
Substituting the values, we get,
ρ = 400000/(287*900)
ρ = 1.627 kg/m^3
Substituting the values in the equation P1 = P2 + ½ρV2^2
400000 = 100000 + ½*1.627*V2^2
V2 = 365.26 m/s
Answer:
The exit temperature of air (T2) is 536.24 K and the exit velocity of air (V2) is 365.26 m/s.
Conclusion:
The exit temperature and velocity of air in an adiabatic nozzle can be calculated using the isentropic relation and Bernoulli's equation respectively.
Air enters an adiabatic nozzle at 400kPa and 900K with negligible velo...
To make sure you are not studying endlessly, EduRev has designed Mechanical Engineering study material, with Structured Courses, Videos, & Test Series. Plus get personalized analysis, doubt solving and improvement plans to achieve a great score in Mechanical Engineering.