Question Details

Air discharges steadily through a horizontal nozzle and impinges on a stationary vertical plate as shown in figure.

The inlet and outlet areas of the nozzle are 0.1 m2 and 0.02 m2, respectively. Take air density as constant and equal to 1.2 kg/m3. If the inlet gauge pressure of air is 0.36 kPa, the gauge pressure at point O on the plate (the point where the axis of nozzle touches the plate) is ________ kPa (round off to two decimal places).

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Correct Answer :

Correct answer is : 0.375

Mass flow rate through nozzle remain constant

( ρ A V ) i n l e t = ( ρ A V ) o u t l e t 0.1 × V i = 0.02 V O

VO = 5 Vi

∴ V2 = 5 Vi

Bernoulli’s equation for nozzle

P 1 ρ g + V 1 2 2 g = P 2 ρ g + V 2 2 2 g [ z 1 = z 2 ]

0.36 × 10 3 1.2 × 9.81 + V 1 2 2 g ( 5 V 1 ) 2 2 g = P 2 ρ g

0.36 × 10 3 1.2 g 24 V 1 2 2 g = P 2 ρ g

P2 = Patm = 0 (Gauge)

∴ V1 = 5 m/s V2 = 25 m/s

∵ P2 = PO = Patm = 0 (Gauge)

But at point O there will be a pressure due to motion of fluid which will exert a pressure on the plate.

Now,

Bernoulli’s equation between exit point & point O

P 2 ρ g + V 2 2 2 g = P 3 ρ g + V 3 2 2 g

P 3 = 1 2 ρ V 2 2

P 3 = 1 2 × 1.2 × ( 25 ) 2 = 375   P a

∴ P3 = 0.375 kPa

Solution :

The correct answer is 0.375

1. Analysis of the Image and Given Data:
Based on the provided schematic diagram, air discharges steadily from a horizontal converging nozzle and impinges on a stationary vertical plate. The diagram highlights three critical parameters:
- The inlet gauge pressure is labeled as Pinlet=0.36 kPa.
- The outlet discharges into the surrounding environment, which is at atmospheric pressure Patm.
- The dashed horizontal centerline represents the nozzle axis, which terminates at point O on the vertical plate. Since the jet impinges normally on the plate, point O acts as a stagnation point where the air velocity is reduced to zero.

We are given the following values:
- Inlet area, A1=0.1 m2
- Outlet area, A2=0.02 m2
- Air density (constant), ρ=1.2 kg/m3
- Inlet gauge pressure, P1=0.36 kPa=360 Pa

2. Applying the Continuity Equation:
Since the flow is steady and the density of air is constant, the mass flow rate through the nozzle remains constant. The volumetric flow rate is also conserved:

A1V1=A2V2
Substituting the given areas:

0.1×V1=0.02×V2
Simplifying this relation gives:

V2=5V1

3. Applying Bernoulli's Equation to the Nozzle:
Applying Bernoulli's equation between the inlet (section 1) and the outlet (section 2) of the horizontal nozzle (neglecting potential energy differences since the nozzle is horizontal):

P1+12ρV12=P2+12ρV22
Since the nozzle discharges to the atmosphere, the gauge pressure at the outlet is:

P2=0 Pa (gauge)
Substituting the values of P1, ρ, and the velocity relation V2=5V1 into Bernoulli's equation:

360+12(1.2)V12=0+12(1.2)(5V1)2

360+0.6V12=0.6×25V12

360+0.6V12=15V12

14.4V12=360

V12=36014.4=25

V1=5 m/s
Thus, the outlet velocity V2 is:

V2=5×5=25 m/s

4. Applying Bernoulli's Equation along the Free Jet Streamline:
Applying Bernoulli's equation along the central streamline from the nozzle exit (section 2) to the stagnation point O on the plate:

P2+12ρV22=PO+12ρVO2
Since the flow stops completely at the stagnation point O, the velocity at point O is:

VO=0
Thus, the gauge pressure PO is given by:

PO=P2+12ρV22
Substituting P2=0, ρ=1.2 kg/m3, and V2=25 m/s:

PO=0+12(1.2)(25)2

PO=0.6×625=375 Pa
Converting the pressure to kilopascals (kPa):

PO=3751000=0.375 kPa
Therefore, the gauge pressure at point O on the plate is 0.375 kPa.

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