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This project will be aimed at modelling the supersonic flow inside Scramjet engine using the Computational Fluid Dynamics CFD ANSYS Fluent. Scramjet Engine starts at a hypersonic free stream Mach no. 5.00. When pressures and temperatures become so high in supersonic flight that it is no longer efficient to slow the oncoming flow to subsonic speeds for combustion, a scramjet (supersonic combustion ramjet) is used in place of a ramjet. Supersonic flow from a nozzle that represents the exhaust nozzle of a supersonic combustion ramjet SCRAMJET is modelled. Jet from the nozzle is issued into a domain which is bounded on one side by an after body wall which is parallel to the center line of the nozzle. Shocks propagating from the nozzle exit reflect from the after body. Outflow from scramjet engines can have a significant impact on both the heat transfer and the pressure distribution on the section of the aircraft that lies downstream. Most importantly, reflecting shock waves lead to large peaks in the distributions. Two geometrical configurations for the after body are tested. Experimental values are used because this span wise region is closest to the centre of the experimental model where the threedimensional effects are minimal. Measured values of the distribution of wall pressure and heat transfer rate along the after body are used to validate the CFD simulation.
Keywords 
Scramjet; Nozzle; Shock waves; Ansys; Computational fluid dynamics 
Introduction 
A ramjet is a form of air breathing jet engine that uses the engine's forward motion to compress incoming air without an axial compressor. A ramjet has no moving parts. Air entering the intake is compressed using the forward speed of the aircraft. The intake air is then slowed from a high subsonic or supersonic speed to a low subsonic speed by aerodynamic diffusion created by the inlet and diffuser, as seen in Figure 1. Fuel is then injected into the combustion chamber where burning takes place. The expansion of hot gases then accelerates the subsonic exhaust air to a supersonic speed. This results in a forward velocity. Ramjets work most efficiently at supersonic speeds around Mach 3 (2,284 mph; 3,675 km/h) [15]. 
A scramjet (supersonic combusting ramjet) is a variant of a ramjet air breathing jet engine in which combustion takes place in supersonic airflow. As in ramjets, a scramjet relies on high vehicle speed to forcefully compress the incoming air before combustion, but a ramjet decelerates the air to subsonic velocities before combustion, while airflow in a scramjet is supersonic throughout the entire engine. Scramjets on the other hand do not slow the free stream air down through the combustion chamber rather keeping it at some supersonic speed. This allows the scramjet to operate efficiently at extremely high speeds: theoretical projections place the top speed of a scramjet between Mach 12 (8,400 mph; 14,000 km/h) and Mach 24 (16,000 mph; 25,000 km/h). 
Keeping the free stream flow supersonic enables the scramjet to fly at much higher speeds. Supersonic flow is needed at higher speeds to maximize efficiency through the combustion process (Figure 2). 
Theory of a scramjet 
All scramjet engines have fuel injectors, a combustion chamber, a thrust nozzle and an inlet, which compresses the incoming air. Sometimes engines also include a region which acts as a flame holder (a component of a jet engine designed to help maintain continual combustion), although the high stagnation temperatures mean that an area of focused waves may be used, rather than a discrete engine part as seen in turbine engines. Other engines use pyrophoric (a substance that ignites spontaneously) fuel additives, such as saline, to avoid such concerns. 
An isolator between the inlet and combustion chamber is often included to improve the homogeneity of the flow in the combustor and to extend the operating range of the engine. A scramjet is reminiscent of a ramjet. In a typical ramjet, the supersonic inflow of the engine is decelerated at the inlet to subsonic speeds and then reaccelerated through a nozzle to supersonic speeds to produce thrust. This deceleration which is produced by a normal shock (a type of propagating disturbance), creates a total pressure loss which limits the upper operating point of a ramjet engine. 
For a scramjet, the kinetic energy of the free stream air entering the scramjet engine is large compared to the energy released by the reaction of the oxygen content of the air with fuel hydrogen. Thus the heat released from combustion at Mach 25 is around 10% of the total enthalpy of the working fluid. Thus the design of a scramjet engine is as much about minimizing drag as maximizing thrust. Therefore, throttling of the entrance to the thrust nozzle is not a usable control technique. In effect, a block of gas entering the combustion chamber must mix with fuel and have sufficient time for initiation and reaction, all the while travelling supersonically through the combustion chamber, before the burned gas is expanded through the thrust nozzle. This places stringent requirements on the pressure and temperature of the flow, and requires that the fuel injection and mixing to be extremely efficient. Usable dynamic pressures lie in the range 20 to 200 kPa (0.22 bar), 
q=1/2 ρv^2 
Where q is the dynamic pressure of the gas, ρ (rho) is the density of the gas, v is the velocity of the gas. 
Features that scramjets inlets will likely contain 
• All of the design surfaces are used to compress the flow, resulting in a complicated 3D shock system. 
• Adjustable surfaces and variable geometry are used to support flights from supersonic to hypersonic speeds. 
• The inlet through the use of an isolator will have to be compatible with the combustion pressure rise. 
• The inlet must be integrated with the fuselage design to accommodate the long compression ramps. 
• Finally, the inlet will be arranged in a single segment or in several. 
Methodology 
Flow simulation solves the governing equations with the finite volume method on a spatially quadrilateral computational mesh designed in the Cartesian coordinate system with the planes orthogonal to its axes and refined locally at the solid/fluid interface and in the fluid region during calculation. The governing equations are discretized in a conservative form due to the finite volume method. The governing equations are integrated over a control volume which is a grid cell, and then approximated with the cellcentred values of the physical variables. The spatial derivatives are approximated with implicit difference operators of secondorder accuracy. The time derivatives are approximated with an implicit firstorder Euler scheme. The numerical solution technique uses stages to create a locally refined quadrilateral computational mesh and used then for solving the governing equations on it. The meshing procedures are performed before the calculation. The first procedure uses partial cells for near wall conditions to monitor heat and mass fluxes; and uses a basic rectangular mesh, which is determined by the computational domain and not dependent on the solid/fluid interface. The next stage allows cells to either merge or split further to refine the mesh at the solid/fluid interface curvatures. The final stage allows the mesh to be refined by using a narrow channel criterion. This results in cells being merged in low gradient regions and splitting of cells in highgradient regions. The algorithmic parameters are stated to be velocity, temperature, density, turbulent energy, turbulent dissipation rate, and component concentrations in fluid mixtures. The numerical algorithm in Flow Simulation solves for fully implicit discrete convection/diffusion equations. These equations obtain the intermediate values of momentum and the final values of turbulent parameters, temperature, and species concentrations. The pressure correction and a final momentum field are combined to satisfy the discrete fully implicit continuity equation. In order to decrease the solution time, Flow Simulation uses a technique called the multigrid method. Given the mesh, a sequence of grids (grid levels) is constructed, with decreasing nodes. On every such grid, the residual of the associated system of algebraic equations is restricted to a coarser grid level, forming the right hand side of the system on that grid. When the solution on the coarse grid is computed, it is interpolated to the finer grid and used there as a correction to the result of the previous iteration. 
CFD models 
0° After body, with wedge shock generator configuration shown below implies that one parallel to the nozzle centreline called the 0° after body. Provision was made for mounting shock wave generators on the cowl lip. With the 0° afterbody a shock generator inclined 3° to the nozzle axis was used (Figure 3a and 3b) (Tables 1 and 2). 
CFD meshing 
Twodimensional grids were made for the test of the 0° geometry. The CFD mesh was a39230cell mesh made entirely out of quadrilateral cells. For the 20° geometry, a single quadrilateral 36270cell mesh was made (Figures 4a and 4b). 
Results and Discussions 
The 2D contour plots for flow variables as obtained from FLUENT for the supersonic Flow case have been presented for Mach number, static pressure and static temperature. The pressure contours for the 0° after body using an adapted quadrilateral mesh. Normalized pressure is maximum at the nozzle end of about 130.1kpa, exhaust gas as it moves away from the nozzle end normalized pressure around 70 kpa (Figures 5a5l). Pressure variation along the centreline 0° after body with wedge as a function of horizontal distance. The reflecting shock on the after body leads to a large jump in both pressure and Temperature. Pressure concentration near wedge is maximum as observed in the Figure 6 because of 0° after body inclination with respect to the nozzle axis. The thrust generation is minimum due to reflecting shock on the afterbody narrow to the shock generator. All are in excellent agreement with experimental data. 
Across the wedge pressure again reduces because of 20° after body inclination with respect to nozzle axis. Shock waves generate from the wedge impinging on after body and these shock waves is much more diffuse by the time it reflects off the after body (Figure 7). 
Compares pressure ratio as a function of horizontal distance for the experimental results and simulated results of 0° after body with wedge. All are in excellent agreement. Pressure is normalized by the entrance value, Pe (Figure 8a8c). 
Conclusion 
By this Analysis we can conclude the “K epsilon turbulence model exactly simulates the flow field characteristics in supersonic and hypersonic conditions” in capturing shocks at leading edges and shock trains in the isolator. Supersonic flow from a nozzle that represents the exhaust nozzle of a supersonic combustion ramjet (SCRAMJET) is modelled using ANSYS Fluent. Jet from the nozzle is issued into a domain which is bounded on one side by an after body wall which is parallel to the centreline of the nozzle. Shocks propagating from the nozzle exit reflect from the after body. Measured values of (i) the distribution of wall pressure and (ii) heat transfer rate along the after body are used to validate the CFD simulation. 
It is interesting to note that obtaining experimental pressure measurements was a quicker process than CFD modelling in terms of both overall time taken and the time to investigate each configuration. However, CFD generates a much larger number of flow parameters than can be experimentally determined and is significantly less expensive, in terms of both personnel and equipment, than performing experiments in the shock tunnel. Simulation has been validated for a twodimensional scramjet outlet flow. In particular, we compared pressures and heat transfer on the after body for 0° and 20° configurations. 
Future Work 
The first of these is that analysing three dimensional scramjet and the next is application of a fully designed expansion system employing the use of method of characteristics or CFD codes. This will enable more precise calculations of performance, as well as provide more realistic overall engine lengths to be obtained, as the nozzle does not have to be fully expanded to free stream conditions to gain a satisfactory amount of thrust. As for the practical design of this scramjet, the use of cavitybased fuel injectors should be explored. 
This project looked at a two dimensional model of the Scramjet exhaust. The logical extension to this would be to use a three dimensional model, Also the shock waves produce on the side walls could be captured. Three dimensional models would be impractical unless a CFD package with shockcapturing features could be used. 
References 

Table 1  Table 2 
Figure 1  Figure 2  Figure 3a  Figure 3b  Figure 4a 
Figure 4b  Figure 5a  Figure 5b  Figure 5c  Figure 5d 
Figure 5e  Figure 5f  Figure 5g  Figure 5h  Figure 5i 
Figure 5j  Figure 5k  Figure 5l  Figure 6  Figure 7 
Figure 8a  Figure 8b  Figure 8c 