Supersonic Nozzle Flow

Supersonic Nozzle Flow

Nithya Subramani (Vel Tech Rangarajan Dr. Sagunthala R&D Institute of Science and Technology, India), Manigandan Sekar (Sathyabama Institute of Science and Technology, Symbiosis International University, India), Yasin Sohret (Anadolu University, Turkey), and Gowtham Gajapathy (Vel Tech Rangarajan Dr. Sagunthala R&D Institute of Science and Technology, India)
DOI: 10.4018/978-1-6684-4230-2.ch009
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Abstract

The nozzle flow is considered to be much more important in aerospace applications. Based on the pressure, velocity and temperature, flow velocity, Mach number and area, the nozzle shape will vary to meet the required condition. Nozzle is a part where the potential energy is converted into kinetic energy. The high pressure and temperature combustion product of gas is converted into high velocity and low-pressure gas as exhaust. In aviation, the main force of thrust is generated due to high velocity exhaust. This chapter gives an explanation and mathematical expression of various nozzles in both subsonic and supersonic flow along with the flow associated issues. The 3D model of convergent chevron nozzle was analyzed for the characteristics of jet mixing and acoustic effect at the exit. These results were compared with the same dimension chevron nozzle with wedges. The added wedges enhanced the jet mixing.
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Introduction

Characteristics of Flow

Based on Mach number, the fluid flow is characterized in different regions and also the speed of the object is identified. It is an important quantity which has no dimension because of the ratio of two velocities with same dimension and it plays an important role in getting the proper idea of the motion of vehicles especially airplanes and rockets moving in an air medium. Mach number is the ratio between the speed of the object in air medium and the speed of sound. The speed of sound is 343 m/s (meter/second) at the temperature of 20 degrees Celsius in the considered medium.

M = 978-1-6684-4230-2.ch009.m01
  • V = Speed of object

  • C = Speed of sound

Mach number is generally represented with M. When an object is flying in the sky, the air particles around them are disturbed by the speed of the object. If the Mach number is greater than the speed of sound, then the air particles are compressed thus the compressibility effects are taken into account. As a result of identifying the Mach number, it is possible to find whether the flow is compressible or not.

Classification of Flow Regions

According to the Mach number (M) variations, the flow is classified in different regimes. If the Mach number remains less than 0.3 then the flow is said to be Incompressible. If it varies from 0.3 to 0.8, then the flow is called Subsonic. The flow is sonic when the Mach number is equal to one. The flow is said to be transonic when the Mach number is greater than 0.8 and till 1.2. If the Mach number is greater than 1.2 then it is called as supersonic. Hypersonic flows are greater than Mach number 5. The different flow regime according to the Mach number is listen in the table 1

Table 1.
Different flow regime according to Mach number
Flow typeMach number Limits
Incompressible0 to 0.3
Subsonic0.3 to 0.8
Transonic0.8 to 1.2
Sonic1
Supersonic1 to 5
Hypersonic5 to 8

If the Mach number is high, then the fluid is considered as compressible and compressibility effects are significant. Incompressible fluid is the constant density flow. Even if the pressure is changed there is not much difference in volume with the constant temperature too. The change in pressure is related to change in volume with very small amount when the temperature is constant and lies within the regime of incompressible flow. From Bernoulli’s principle, the pressure variation is related to velocity change. The flow is said to be compressible when there is a volume change with the respective pressure variation. For aircrafts, the height is also considered for performance and it changes the Mach number. When the aircraft flies at different altitude, the pressure varies and speeds of sound changes. In that particular, the change of height resulting in change of Mach number creates necessity of the aircraft to adjust itself.

The flow variation is closely considered and monitored since the flow dominates and decides the performance of the engine. The converging nozzle is used when the flow is subsonic. Converging nozzle is the duct in which the area is decreased at certain inclination constantly. When the incoming flow is supersonic, pressure and temperature of the incoming flow are high while the velocity and Mach number of the inlet flow are lower. When the subsonic flow is passed through the convergent nozzle, the pressure and temperature gt reduced while the velocity and Mach number get increased. With the same purpose of increasing the exit velocity of the supersonic incoming flow, the divergent nozzle can be used. For the divergent nozzle with the supersonic flow, the pressure and temperature of the fluid get reduced and conversely the velocity and Mach number are increased. For subsonic flow, the divergent nozzle is acted as diffuser to reduce the speed of the flow. In the same way, the convergent nozzle is acted as diffuser for supersonic flow. When the compressibility effects are considered in the nature of the flow, the shock wave problems are also considered.

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