Consider an isentropic flow of air (ratio of specific heats = 1.4) through a duct as shown in the figure.
The variations in the flow across the cross-section are negligible. The flow conditions at Location 1 are given as follows:
π1 = 100 kPa, π1 = 1.2 kg/m3 , π’1= 400 m/s
The duct cross-sectional area at Location 2 is given by A2 = 2A1, where A1 denotes the duct cross-sectional area at Location 1. Which one of the given statements about the velocity π’2 and pressure π2 at Location 2 is TRUE?
Correct Answer :
π’2 > π’1 , π2 < π1
Solution :
The correct option is:
π’2 > π’1 , π2 < π1
Step-by-Step Explanation:
Step 1: Identify the flow conditions at Location 1
We are given the following conditions at Location 1 (as seen in the diagram):
Pressure, π1 = 100 kPa = 100,000 Pa
Density, π1 = 1.2 kg/m3
Velocity, π’1 = 400 m/s
Ratio of specific heats, πΎ = 1.4
Specific gas constant for air, π
= 287 J/(kgΒ·K)
Step 2: Determine the temperature at Location 1
Using the ideal gas equation of state:
Solving for π1:
Step 3: Calculate the local speed of sound at Location 1
Step 4: Find the Mach number at Location 1
Since ππ1 > 1, the flow at Location 1 is supersonic.
Step 5: Analyze the effect of the diverging duct
The relation between cross-sectional area π΄ and flow velocity π’ in a 1D isentropic flow is given by the area-velocity relation:
From the diagram and problem description, the area increases downstream from Location 1 to Location 2 (π΄2 = 2π΄1), meaning:
ππ΄ > 0
Since the flow is supersonic (ππ > 1), we have:
(ππ2 - 1) > 0
To satisfy the relation, the velocity gradient must be positive:
ππ’ > 0 β π’2 > π’1
For a supersonic flow, a diverging duct acts as a nozzle, causing the fluid velocity to increase.
Step 6: Determine the pressure change
According to the 1D momentum equation (Euler's equation) for inviscid flow:
Since ππ’ > 0, the change in pressure must be negative:
ππ < 0 β π2 < π1
Therefore, as the supersonic flow expands through the diverging duct, its velocity increases and its pressure decreases, verifying that:
π’2 > π’1 , π2 < π1
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