design and analysis of fuel flow in bend pipes · design and analysis of fuel flow in bend pipes...

8
DESIGN AND ANALYSIS OF FUEL FLOW IN BEND PIPES 1 R.Sharavanan, 2 R.J.Golden Renjith 1,2 Assistant Professor Department of Mechanical Engineering, BIST, BIHER, Bharath University, Chennai. 1 [email protected] Abstract: Pipe flow, a branch of Hydraulics and Fluid Mechanics, was a type of liquid flow within a closed conduit (conduit in the sense of a means of containment). The other type of flow within a conduit is open channel flow. These two types of flow were similar in many ways, but differ in one important respect. Pipe flow does not have a free surface which is found in open-channel flow. Pipe flow, being confined within closed conduit, does not exert direct atmospheric pressure, but does exert hydraulic pressure on the conduit. 1. Introduction Generally any application involving pipe flow will not only consist of flow through straight pipes. It will also comprise of fluid flow through pipes of varying cross sections, predominantly classified as expansion and contraction. These in turn can be subdivided into sudden and gradual change. The pipeline may also consist of pipe bends of various angles and types like mitred bends, sharp bends, filleted bends etc.[1-5] 2. Literature Review The phenomenon of flow through pipes has been studied and subjected to research throughout the years. Amongst the various literatures on flow through pipes, the recent work focuses on pressure and velocity variations in pipe bends and variable flow areas[6-9] A. S. Nejad and S. A. Ahmed (1992) [8] studied the Flow field characteristics of an axisymmetric sudden-expansion pipe flow with different initial swirl distribution. The results of an experimental investigation depicting the effects of swirl profile on confined flows in a sudden-expansion coaxial dump combustor are presented. Three swirlers (freevortex, forced vortex, and constant angle) with the same nominal swirl number were designed and fabricated to study the effects of swirl type on the isothermal dump combustor flow field. They found, upon imparting swirl to the inlet flow resulted in a considerable reduction of the corner recirculation length, a marked increase in turbulent mixing activity, and in one case creation of a central recirculation zone. Their work highlights the importance of the combustor inlet swirl profile and shows that swirl type as well as swirl strength can affect the flow field significantly. The present database is well suited for numerical codes development and validation[10-16] Conditions For Analysis: Diesel has been chosen as the fluid for analysis. Properties of diesel: Density = 730 kg/m 3 Viscosity = 0.0024 kg/m-s Reynolds Number has been chosen for laminar is2000. For this Reynolds’s number the velocity of Diesel was found to be 0.13 m/s. Reynolds Number has chosen for Turbulent is 5000. For this Reynolds number the velocity of diesel was found to be 0.3287 m/s. 2.1straightpipe: Figure 2.1 Figure 5.1 shows the pressure contour of fluid for the pipe. This figure clearly shows the decrease in pressure with respect to length. International Journal of Pure and Applied Mathematics Volume 116 No. 15 2017, 59-65 ISSN: 1311-8080 (printed version); ISSN: 1314-3395 (on-line version) url: http://www.ijpam.eu Special Issue ijpam.eu 59

Upload: others

Post on 30-Apr-2020

9 views

Category:

Documents


0 download

TRANSCRIPT

DESIGN AND ANALYSIS OF FUEL FLOW IN BEND PIPES

1R.Sharavanan,

2 R.J.Golden Renjith

1,2Assistant Professor Department of Mechanical Engineering,

BIST, BIHER, Bharath University, Chennai. [email protected]

Abstract: Pipe flow, a branch of Hydraulics and Fluid

Mechanics, was a type of liquid flow within a

closed conduit (conduit in the sense of a means of

containment). The other type of flow within a conduit

is open channel flow. These two types of flow were

similar in many ways, but differ in one important

respect. Pipe flow does not have a free surface which is

found in open-channel flow. Pipe flow, being confined

within closed conduit, does not exert direct atmospheric

pressure, but does exert hydraulic pressure on the

conduit.

1. Introduction

Generally any application involving pipe flow will not

only consist of flow through straight pipes. It will also

comprise of fluid flow through pipes of varying cross

sections, predominantly classified as expansion and

contraction. These in turn can be subdivided into

sudden and gradual change. The pipeline may also

consist of pipe bends of various angles and types like

mitred bends, sharp bends, filleted bends etc.[1-5]

2. Literature Review

The phenomenon of flow through pipes has been

studied and subjected to research throughout the years.

Amongst the various literatures on flow through pipes,

the recent work focuses on pressure and velocity

variations in pipe bends and variable flow areas[6-9]

A. S. Nejad and S. A. Ahmed (1992) [8] studied

the Flow field characteristics of an axisymmetric

sudden-expansion pipe flow with different initial swirl

distribution. The results of an experimental

investigation depicting the effects of swirl profile on

confined flows in a sudden-expansion coaxial dump

combustor are presented. Three swirlers (freevortex,

forced vortex, and constant angle) with the same

nominal swirl number were designed and fabricated to

study the effects of swirl type on the isothermal dump

combustor flow field. They found, upon imparting swirl

to the inlet flow resulted in a considerable reduction of

the corner recirculation length, a marked increase in

turbulent mixing activity, and in one case creation of a

central recirculation zone. Their work highlights the

importance of the combustor inlet swirl profile and shows

that swirl type as well as swirl strength can affect the flow

field significantly. The present database is well suited for

numerical codes development and validation[10-16]

Conditions For Analysis:

● Diesel has been chosen as the fluid for analysis.

Properties of diesel:

Density = 730 kg/m3

Viscosity = 0.0024 kg/m-s

● Reynolds Number has been chosen for laminar

is2000. For this Reynolds’s number the velocity of

Diesel was found to be 0.13 m/s.

● Reynolds Number has chosen for Turbulent is

5000. For this Reynolds number the velocity of

diesel was found to be 0.3287 m/s.

2.1straightpipe:

Figure 2.1

Figure 5.1 shows the pressure contour of fluid for the pipe.

This figure clearly shows the decrease in pressure with

respect to length.

International Journal of Pure and Applied MathematicsVolume 116 No. 15 2017, 59-65ISSN: 1311-8080 (printed version); ISSN: 1314-3395 (on-line version)url: http://www.ijpam.euSpecial Issue ijpam.eu

59

Figure 2.2. depicts the velocity contour of straight pipe

Figure 2.3. shows the velocity vectors of straight pipe.

graph shows the velocity profile of straight pipe

5.2 Pipe With 30 Degree Fillet Bend

Figure 2.4

Figure 5.4 shows the velocity contour of fluid for the

pipe with 30 Degree Fillet Bend. This figure clearly

shows the advantages of fillet bends and the turbulence

created is a lot less when compared to prev

cases.[17-23]

depicts the velocity contour of straight pipe

shows the velocity vectors of straight pipe.

graph shows the velocity profile of straight pipe

Figure 5.4 shows the velocity contour of fluid for the

pipe with 30 Degree Fillet Bend. This figure clearly

shows the advantages of fillet bends and the turbulence

created is a lot less when compared to previous

Figure 2.5. depicts the velocity contour of straight pipe

Figure 2.6

Figure 5.6 displays the velocity vector of fluid for the pipe

with 30 Degree Fillet Bend. It can be clearly observed that

there is very less or no recirculation

bend[24-28].

Figure 2.7. shows the velocity vectors of fluid at various

sections of the pipe with 30 Degree Fillet Bend.

Figure 2.8

Figure 5.8 displays the velocity plots of fluid at various

sections of the pipe with 30 Degree

only a sight disturbance at the region of the bend which

fades out over the course of the flow.

depicts the velocity contour of straight pipe

.6

Figure 5.6 displays the velocity vector of fluid for the pipe

with 30 Degree Fillet Bend. It can be clearly observed that

there is very less or no recirculation regions in case of fillet

shows the velocity vectors of fluid at various

sections of the pipe with 30 Degree Fillet Bend.

.8

Figure 5.8 displays the velocity plots of fluid at various

sections of the pipe with 30 Degree Fillet Bend. There is

only a sight disturbance at the region of the bend which

fades out over the course of the flow.

International Journal of Pure and Applied Mathematics Special Issue

60

2.2 Pipe With 30 Degree Fillet Bend With Turbulent

Flow As Inlet

Figure 2.9

Figure 5.9 shows the velocity contour of fluid for the

pipe with 30 Degree Fillet Bend with Turbulent Flow as

inlet. The figure clearly shows the advantages of having

a Turbulent flow for fillet pipes with less angle of bend

as the flow is almost not affected at all[29-30].

Figure 2.10. depicts the pressure contour of fluid for

the pipe with 30 Degree Fillet Bend with Turbulent

Flow as inlet.

Figure 2.11

Figure 5.11 shows the velocity vectors of fluid at

various sections of the pipe with 30 Degree Fillet Bend

with Turbulent Flow as inlet.

Figure 2.12

Figure 5.12 shows the velocity vectors of fluid in a pipe

after the30 Degree Fillet Bend with Turbulent Flow as

inlet.

Figure 2.13

Figure 5.13 displays the velocity plots of fluid at various

sections of the pipe with 30 Degree Fillet Bend with

Turbulent Flow as inlet. The boundary layer is almost

unaffected.

2.3 Pipe With 60 Degree Fillet Bend :

Figure 2.14

International Journal of Pure and Applied Mathematics Special Issue

61

Figure 5.14 shows the velocity contour of fluid for the

pipe with 60 Degree Fillet Bend. The fillet bend

prevents the formation of turbulence in fluid flow when

compared to sharp bends.

Figure 2.15. depicts the pressure contour of fluid for

the pipe with 60 Degree Fillet Bend.

Figure 2.16. displays the velocity vector of fluid for the

pipe with 60 Degree Fillet Bend

Figure 2.16. shows the velocity vectors of fluid at

various sections of the pipe with 60 Degree Fillet Bend

Figure 2.17. displays the velocity plots of fluid at various

sections of the pipe with 60 Degree Fillet Bend.

2.4 Pipe With 60 Degree Fillet Bend With Turbulent

Flow As Inlet

Figure 2.18

Figure 5.18 shows the velocity contour of fluid for the pipe

with 60 Degree Fillet Bend with Turbulent Flow as inlet.

From this figure it can be clearly concluded that fillet

bends are better than sharp bends and that Turbulent flow

must always be attained before the bend if the fluid flow

needs to be unaffected by the bend .

Figure 2.19

Figure 5.19 depicts the pressure contour of fluid for the

pipe with 60 Degree Fillet Bend with Turbulent Flow as

inlet.

International Journal of Pure and Applied Mathematics Special Issue

62

Figure 2.20

Figure 5.20 displays the velocity vector of fluid for the

pipe with 60 Degree Fillet Bend with Turbulent Flow as

inlet.

Figure 2.21

Figure 5.21 shows the velocity vectors of fluid at

various sections of the pipe with 60 Degree Fillet Bend

with Turbulent Flow as inlet.

Figure 2.22

Figure 5.22 displays the velocity plots of fluid at

various sections of the pipe with 60 Degree Fillet Bend

with Turbulent Flow as inlet. There is just a slight

disturbance at the bend which is insignificant since the

flow attains stability further downstream.

3. Conclusion

The analysis of a pipe flow with various pipe

configurations was done using ANSYS Fluent 15.0 and the

results were obtained. The results clearly show the

following,

● In case of sudden contraction in pipes, there is

abrupt rise in fluid velocity at the region of

contraction which is termed Vena Contracta. It is

formed due to the convergence of flow as shown

by the vector plot.

● In case of sudden expansion in pipes, there is a

drop in velocity after a certain distance from the

region of expansion which is basically determined

by the velocity of fluid flow which in our case is

0.73 m/s. The fluid slowly starts to stabilize, but it

can be properly visualized only if the length of the

pipe is longer than the configuration that has been

used. Negative pressure is formed at the region of

recirculation, and the phenomena can more clearly

be explained by using a finer mesh.

● In case of 30 degree bends, the pressure losses

were more at the region of sharp bends than the

filleted bends. The Turbulent flow was found to be

more stable than the flow with constant velocity at

inlet.

● The results found in 60 degree and 90 degree

bends with configurations

(Fillet and constant velocity at inlet & Turbulent

flow at inlet), were found to be similar as in the

case of 30 degree configuration. The only

significant difference found was that the rise in

velocity was proportional to the angle of bend (i.e.

the larger the angle of bend, the greater the rise in

velocity at the point of bend)

References

[1] Arun Kumar N., Srinivasan V., Krishna Kumar P.,

Analysing the strength of unidirectional fibre orientations

under transverse static load, International Journal of

Applied Engineering Research, v-9, i-22, pp-7749-7754,

2014.

[2] Srinivasan V., Analysis of static and dynamic load

on hydrostatic bearing with variable viscosity and pressure,

Indian Journal of Science and Technology, v-6, i-

SUPPL.6, pp-4777-4782, 2013.

[3] Srinivasan V., Optimizing air traffic conflict and

congestion using genetic algorithm, Middle - East Journal

of Scientific Research, v-20, i-4, pp-456-461, 2014.

[4] Praveen R., Achudhan M., Optimization of jute

composite as a noise retardant material, International

Journal of Applied Engineering Research, v-9, i-22, pp-

7627-7632, 2014.

International Journal of Pure and Applied Mathematics Special Issue

63

[5] Raja Kumar G., Achudhan M., Srinivasa Rao G.,

Studies on corrosion behaviour of borated stainless

steel (304B) welds, International Journal of Applied

Engineering Research, v-9, i-22, pp-7767-7772, 2014.

[6] Ganeshram V., Achudhan M., Design and

moldflow analysis of piston cooling nozzle in

automobiles, Indian Journal of Science and

Technology, v-6, i-SUPPL.6, pp-4808-4813, 2013.

[7] Ganeshram V., Achudhan M., Synthesis and

characterization of phenol formaldehyde resin as a

binder used for coated abrasives, Indian Journal of

Science and Technology, v-6, i-SUPPL.6, pp-4814-

4823, 2013.

[8] Achudhan M., Prem Jayakumar M.,

Mathematical modeling and control of an electrically-

heated catalyst, International Journal of Applied

Engineering Research, v-9, i-23, pp-23013-, 2014.

[9] Anbazhagan R., Satheesh B., Gopalakrishnan K.,

Mathematical modeling and simulation of modern cars

in the role of stability analysis, Indian Journal of

Science and Technology, v-6, i-SUPPL5, pp-4633-

4641, 2013.

[10] Udayakumar R., Kaliyamurthie K.P., Khanaa,

Thooyamani K.P., Data mining a boon: Predictive

system for university topper women in academia,

World Applied Sciences Journal, v-29, i-14, pp-86-90,

2014.

[11] Kaliyamurthie K.P., Parameswari D.,

Udayakumar R., QOS aware privacy preserving

location monitoring in wireless sensor network, Indian

Journal of Science and Technology, v-6, i-SUPPL5, pp-

4648-4652, 2013.

[12] Kumar J., Sathish Kumar K., Dayakar P., Effect

of microsilica on high strength concrete, International

Journal of Applied Engineering Research, v-9, i-22, pp-

5427-5432, 2014.

[13] Dayakar P., Vijay Ruthrapathi G., Prakesh J.,

Management of bio-medical waste, International

Journal of Applied Engineering Research, v-9, i-22, pp-

5518-5526, 2014.

[14] Iyappan L., Dayakar P., Identification of

landslide prone zone for coonoortalukusing

spatialtechnology, International Journal of Applied

Engineering Research, v-9, i-22, pp-5724-5732, 2014.

[15] Swaminathan N., Dayakar P., Resource

optimization in construction project, International

Journal of Applied Engineering Research, v-9, i-22, pp-

5546-5551, 2014.

[16] Swaminathan N., Sachithanandam P., Risk

assessment in construction project, International Journal

of Applied Engineering Research, v-9, i-22, pp-5552-

5557, 2014.

[17] Srividya T., Kaviya B., Effect on mesh

reinforcement on the permeablity and strength of

pervious concrete, International Journal of Applied

Engineering Research, v-9, i-22, pp-5530-5532, 2014.

[18] Sandhiya K., Kaviya B., Safe bus stop location in

Trichy city by using gis, International Journal of Applied

Engineering Research, v-9, i-22, pp-5686-5691, 2014.

[19] Ajona M., Kaviya B., An environmental friendly

self-healing microbial concrete, International Journal of

Applied Engineering Research, v-9, i-22, pp-5457-5462,

2014.

[20] Kumar J., Sachithanandam P., Experimental

investigation on concrete with partial replacement of scrap

rubber to granite stones as coarse aggregate, International

Journal of Applied Engineering Research, v-9, i-22, pp-

5733-5740, 2014.

[21] Sachithanandam P., Meikandaan T.P., Srividya T.,

Steel framed multi storey residential building analysis and

design, International Journal of Applied Engineering

Research, v-9, i-22, pp-5527-5529, 2014.

[22] Srividya T., Saritha B., Strengthening on RC beam

elements with GFRP under flexure, International Journal

of Applied Engineering Research, v-9, i-22, pp-5443-5446,

2014.

[23] Saraswathy R., Saritha B., Planning of integrated

satellite township at Thirumazhisai, International Journal

of Applied Engineering Research, v-9, i-22, pp-5558-5560,

2014.

[24] Saritha B., Rajasekhar K., Removal of malachite

green and methylene blue using low cost adsorbents from

aqueous medium-a review, Middle - East Journal of

Scientific Research, v-17, i-12, pp-1779-1784, 2013.

[25]

International Journal of Pure and Applied Mathematics Special Issue

64

65

66