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**Authors :**V. I. Pinchukov -
**Paper ID :**IJERTV8IS070094 -
**Volume & Issue :**Volume 08, Issue 07 (July 2019) -
**Published (First Online):**18-07-2019 -
**ISSN (Online) :**2278-0181 -
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**License:**This work is licensed under a Creative Commons Attribution 4.0 International License

#### Supersonic Flows near Blunted Cylinders, Giving off Opposite Jets: CFD Search for Self-Oscillatory Regimes

V. I. Pinchukov

In-te of Computational Technologies, Siberian division of Russian Academy of Sc., Novosibirsk, Russia

Abstract – Parametric numerical studies of supersonic flows near spherically blunted cylinders, giving off opposite supersonic jets from forehead surfaces, are carried out. Two-dimensional Euler equations of a polytropic gas with the specific heats ratio 1.4 are applied. An explicit Godunov second order scheme is used. Self-oscillatory flows are found for free stream Mach numbers 1.1 M 2.3. It is

shown, that flows are steady for sufficiently large jet half-angles, jets are destroying and a process of this destroying produces self-oscillations for middle jet half-angles, jets propagate at a greater distance from spherical blunts of cylinders for sufficiently small jet half-angles. This paper is devoted to investigations of unsteady flows mainly for middle jet half-angles.

Keywords – Euler equations, CFD studies, self-oscillations, compressible flows

INTRODUCTION

This paper is devoted to continuation of a search for unsteady compressible flows, started in [1]. Flow self-oscillations are supposed to be resulted from resonance interactions of flow active elements, namely, elements, which amplify disturbances. The hypothesis [1] is used that contact discontinuities and intersection points (lines in 3d case) of shocks with shocks or shocks with contact discontinuities compose the flow set of active elements. A search for new unsteady flows is conducted by inves- tigations of flows, containing the most number of active elements.

Opposite jets, out-flowing from forehead surfaces of blunted bodies, may be used for protecting bodies from heating by a mainstream (see, for example, [2]-[4]). Self-oscillatory regimes are not observed in previous investigations. At the same time calculated here flow fields contain three shock waves, two contact discontinuities and some intersection points [1]. So these flows may be supposed to produce self-oscillations, according to the formulated above hypothesis. It seems that there is contradiction between present results and other investigations. To settle this contradiction it should be noted that, first, flows near blunted bodies with opposite jets are defined by large number of control parameters and depend on body and nozzle forms, consequently, require more thorough investigations, second, subsonic or transonic jets are usually used for cooling of the bodies while present

considerations deal with jet Mach numbers M jet 2.5.

Numerical studies of supersonic flows near blunted cylinders, giving of opposite jets, started in [1], where existence of un- steady regimes was noted. Self-oscillatory regime of flows near blunted cylinders with opposite jets were studied in [5],[6] at free stream Mach numbers, closed to 1. Here these investigations are continued.

A class of jet flows with self-sustained oscillations contains three families. Besides present new family, there are two known families, containing: 1. Flows near supersonic jets, inflowing to forward facing cavities (see, for example, [7]-[10]); 2. Flows near supersonic jets, impinging on plates [11]-[19].

CFD DESIGN APPROACH

A computational domain and a mesh may be seen in figure 1. The blunted cylinder wall is shown by a bold line. Opposite supersonic jets outflow from nozzles in forehead parts of blunted cylinders. These jets are supposed to be spherically symmetrical. Jet velocities at exits of nozzles are normal to spherical surfaces.

Fig. 1. Mesh and computational domain schematic representation.

Boundary conditions for computations are zero value of the normal velocity and extrapolation relations for all other variables along the body surface (boundary DC), extrapolations on the outflow boundary BC at right side of numerical domain (see fig 1), prescribed variables on the inflow forehead boundary AB and on the spherical boundary DE, corresponding to the opposite jet, zero value of the radial velocity and extrapolations at symmetry axis AE.

The second order two step version of Godunov conservative method [20] with approximate linear solution of Riman problem is employed here. Algorithms of slopes limitation of left and right extrapolation curves are used to damp false oscillations near discontinuities. Review of such algorithms of damping false oscillations are presented in [21]. Navier-Stokes viscous terms are included to Euler equations and the Smagorinsky artificial viscosity [22] is used for additional damping of false oscillations. This viscosity is calculated by equations

2 1 / 2

Âµ= |S|(C s ) , |S| = (2S ik S ik ) , (1)

S = ( u / x + u / x

)/2, = (x

y – y x )/(Min( 2 ( x 2 +y 2

2 1 / 2

), ( x 2 +y 2 ))) ,

ik i k k i

where functions x=x( ,), y=y( ,) perform mapping of the unit square {0 1, 0 1} to a curvilinear quadrangle on the plane of physical variables, =1/N , =1/N , N , N – numbers of intervals of the quadrangular mesh in a unit square,

C s – constant, which is chosen in trial computations, C s =0.85. The 490 544 mesh is used.

Numerical calculations deal with dimensionless variables. These variables are defined as relations of initial variables and next

parameters of the free stream flow or radiuses of cylinders r: p – for pressure, – for density,

p

for velocity, r

for space variables, r/

p

for time.

The intensity of flow oscillations may be measured by sound pressure level at some point:

ref

ref

SPL=10 Log 10 ( p '2 /p 2 ),

p '2 = (p – p ) 2 /N, p ref =20mkPa/p ,

n

n

n

where p =101325Pa (the air pressure under normal conditions) is used since dimensionless variables are dealt here. Sound pressure levels at the intersection point of spherical and cylindrical parts are represented in three tables below.

FREE STREAM MACH NUMBERS 1.1 M 1.3.

Main purpose of this paper is to find unsteady compressible flows near blunted cylinders, giving off supersonic opposite jets, at free stream Mach numbers, exceeding Mach numbers, considered in (Pinchukov, 2014, 2016, 2018). Studied here flows

are defined by five control parameters: M , M jet , jet , p jet , jet – free stream and jet Mach numbers, jet density, jet pressure,

a jet half-angle. Large number of control parameters makes systematic parametric study of these flows too expensive. A search for new self-oscillatory flows is performed by moving step by step in the greater Mach number direction from any initial flows, for example, published in [5], [6]. Results of a search are represented in table 1-3. The first column of these tables contains numbers of variants, columns 2-6 show control parameters of calculated flows, the last column shows results of computations, namely, SPL data at the intersection point of spherical and cylindrical parts of considered bodies.

Table 1

Sound pressure levels at 1.1 M 1.3.

3.0

N

M

M jet

P jet

jet

Sin( jet )

SPL,db

1

1.1

0.5

0.583

12/30

174.8

2

1.1

3.5

0.4

0.625

1/3

l72.3

3

1.1

3.5

0.4

0.223

11/30

165.1

4

1.2

3.0

0.5

0.340

1/3

165.4

5

1.2

3.0

0.3

0.567

11/30

163.0

6

1.2

4.0

0.292

0.469

1/3

169.6

7

1.3

3.0

0.502

0.484

1/3

164.4

8

1.3

4.5

0.233

0.465

13/30

150.7

9

1.3

4.5

0.233

0.465

12/30

162.2

10

1.3

4.5

0.233

0.465

11/30

170.0

11

1.3

4.5

0.233

0.465

1/3

169.8

12

1.3

4.5

0.233

0.465

9/30

167.5

13

1.3

4.5

0.233

0.465

8/30

–

It is interesting to consider variants 8-13 in this table. Control parameters M , M jet , jet , p jet , are identical for these var- iants, the parameter jet is varied from arcsin(13/30) to arcsin(8/30). It may be seen (column 7 of table 1), that oscillations of the variant 8 with the largest parameter jet are weak. If to increase the parameter jet , then the steady state regime is observed. Figure 2a shows the density distribution in the flow number 8.

ab

Figs. 2. Density distributions, a – jet =arcsin(13/30), b – jet =arcsin(1/3).

Decreasing of the parameter jet results appearing of more intensive oscillations. Figure 2b shows the density distribution in

the flow number 11. Intensive oscillations near the bold part of the cylinder produce shock waves, moving towards the main shock wave, and vortexes, drifting above cylinder surface.

Next decreasing of the parameter jet changes the flow regime. If variants 8-12 correspond to destroying of out-flowing jet,

and a process of jet destroying provides generation of fluctuations, the variant 13 corresponds to propagation of the jet towards the inflow boundary. Figure 3 shows the density distribution in the flow number 13. The flow regime is not defined at this time instant. If to continue modeling of this flow, the main shock wave gets the inflow boundary AB. Next calculations of this flow become unable. Present CFD approach is not applicable to calculations of such flows.

Fig. 3. The density distribution, jet =arcsin(8/30).

Similar dependence of flow regimes on a jet half-angle jet is observed for all considered here free stream Mach numbers. But

flows with new regime (like the flow 13) and flows with weak oscillations (like the flow 8) are omitted for other free stream Mach numbers.

FREE STREAM MACH NUMBERS 1.4 M 1.8.

Results of a CFD search for middle Mach numbers are represented in table 2.

Table 2

Sound pressure levels at 1.4 M 1.8.

N

M

M jet

P jet

jet

Sin( jet )

SPL,db

1

1.4

4.5

0.233

0.465

12/30

161.7

2

1.4

5.5

0.157

0.459

1/3

168.3

3

1.4

5.5

0.394

0.289

1/3

170.0

4

1.4

5.5

0.25

0.347

1/3

179.5

5

1.5

5.5

0.25

0.289

1/3

177.6

6

1.5

5.5

0.25

0.347

1/3

174.3

7

1.6

5.5

0.25

0.289

1/3

176.3

8

1.6

5.5

0.2

0.289

12/30

164.0

9

1.7

5.5

0.25

p>0.289 1/3

179.2

10

1.7

5.5

0.25

0.347

1/3

173.53

11

1.7

5.5

0.25

0.347

12/30

151.9

12

1.8

5.5

0.25

0.289

1/3

169.5

13

1.8

5.5

0.25

0.347

1/3

174.2

Figure 4a shows the density distribution for the unsteady flow 6 in table 2. Intensive self-oscillations produce shock waves, moving towards the main bold shock wave, and vortexes, drifting above the cylinder surface.

a b

Figs. 4. M =1.5, a – the density distribution, b – the pressure history.

The pressure history is shown in figure 4a for this flow. Seven points of minimal values of pressure may be seen in this figure.

So main tone period of this flow may be evaluated approximately by the formulae = (t 7 -t 1 )/6 = 1.68.

Free Stream Mach Numbers 1.9 M 2.3.

Examples of numerically found self-oscillatory flows are shown in table 3.

Table 3

Sound pressure levels at 1.9 M 2.5.

N

M

M jet

p jet

jet

Sin( jet )

SPL,db

1

1.9

5.5

0.25

0.289

1/3

170.0

2

1.9

5.5

0.25

0.405

1/3

169.0

3

2.0

4.5

0.50

0.432

1/3

169.1

4

2.0

5.5

0.25

0.405

1/3

163.3

5

2.0

5.5

0.35

0.289

1/3

171.7

6

2.15

4.5

0.5

0.432

1/3

166.9

7

2.15

4.5

0.5

0.432

9/30

171.2

8

2.15

4.5

0.5

0.432

8/30

166.3

9

2.3

4.5

0.5

0.289

9/30

169.5

10

2.3

5.5

0.5

0.289

9/30

175.6

11

2.3

5.5

0.5

0.434

12/30

172.8

12

2.3

4.5

0.5

0.648

1/3

168.9

13

2.3

5.5

0.5

0.434

9/30

177.2

14

2.3

5.5

0.5

0.434

8/30

172.4

Figure 5a shows the density distribution for the flow 11 in table 3. This figure shows shock waves moving from the body bold region to the main forehead shock wave, and vortexes, appearing near the body bold and moving downstream along the cylinder.

a b

Figs. 5. M =2.3, a -the density distribution, b – the pressure history.

Figure 5b shows the pressure history for this flow at the interface point of spherical and cylindrical parts of the body. Five points of pressure minimal values in this figure divide this graph on periods. So present flow may be considered very approxi-

mately as periodical with the period = (t 5 -t 1 )/4=0.90.

CONCLUTIONS

Interactions of supersonic streams with blunted bodies, giving off supersonic jets, are studied. Previous investigations [5]-[6] allowed to find unsteady regimes of these interactions at free stream Mach numbers, closed to 1. The Mach numbers interval

M 2.3 of unsteady regimes is established here.

Comparison of variants 8-13 in table 1 shows, that flows are steady for sufficiently large jet half-angles, jets are destroying and a process of this destroying produces self-oscillations for middle jet half-angles, jets get greater distance from spherical blunts of cylinders for sufficiently small jet half-angles.

As a jet velocity or jet pressure or jet density decreases, a jet gets less distance from spherical blunt as a result of jet braking by a contrary free stream. A steady state regime takes place, if this distance is sufficiently small.

To define more exactly regions with any flow regimes in 5D space of control parameters, both CFD modeling and ex- perimental studies are necessary.

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