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SHREE SA’D VIDYA MANDAL INSTITUTE OF TECHNOLOGY DEPARTMENT OF CIVIL ENGINEERING
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Reynold number (Fluid Mechanics)(FM)

Jan 09, 2017

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Page 1: Reynold number (Fluid Mechanics)(FM)

SHREE SA’D VIDYA MANDAL INSTITUTE OF TECHNOLOGY

DEPARTMENT OF CIVIL ENGINEERING

Page 2: Reynold number (Fluid Mechanics)(FM)

Subject:-Fluid Mechanics

Topic:-Reynolds experiment

Page 3: Reynold number (Fluid Mechanics)(FM)

-:PRESENTED BY:-

Name Arvindsai

Dhaval

Fahim Patel

Navazhushen Patel

M.Asfak Patel

Enrollment no.130454106002

130454106001

140453106005

140453106008

140453106007

Page 4: Reynold number (Fluid Mechanics)(FM)

INTRODUCTIONProf. Osborne Reynolds conducted

the experiment in the year 1883.This was conducted to demonstrate

the existence of two types of flow :-1.Laminar Flow2.Turbulent Flow

Page 5: Reynold number (Fluid Mechanics)(FM)

1.Laminar Flow:-

Laminar flow is defined as that type of flow in which the fluid particles move along well-defined paths or stream lines and all the stream lines are straight and parallel.

Factors responsible for laminar flow are:-

- High viscosity of fluid.- Low velocity of flow.- Less flow area.

For example, ‐ Flow through pipe of uniform cross-

section.

Page 6: Reynold number (Fluid Mechanics)(FM)

2.Turbulent Flow:- Turbulent flow is defined as that type of flow in which the fluid particles move is a zigzag way. The Fluid particles crosses the paths of each other.

For example, - Flow in river at the time of flood.- Flow through pipe of different cross-

section.

Page 7: Reynold number (Fluid Mechanics)(FM)

What is Reynolds Number ?

The ratio of inertia force to viscous force is said to be the Reynolds number (RN).

Page 8: Reynold number (Fluid Mechanics)(FM)

APPARATUS

Page 9: Reynold number (Fluid Mechanics)(FM)

Observation by Reynolds1. At low velocity,

the dye will move in a line parallel to the tube and also it does not get dispersed.

2. At velocity little more than before the dye moves in a wave form.

3. At more velocity the dye will no longer move in a straight-line.

Page 10: Reynold number (Fluid Mechanics)(FM)

FORMULAS

Where,ρ =density of liquid (Kg/m3 ) V=mean velocity of liquid m/SD=diameter of pipe(m)µ=dynamic velocity(N.S/m2 ) =kinematic viscosity(m2 /S)

Where

Reynold number is a dimensionless quantity.

νVxDR

μρxVxDR

Force ViscousForce InertiaR

N

N

N

Page 11: Reynold number (Fluid Mechanics)(FM)

Types Of Flows Based On Reynold Number:-

If Reynold number, RN < 2000 the flow is laminar flow.

If Reynold number, RN > 4000 the flow is turbulent flow.

Page 12: Reynold number (Fluid Mechanics)(FM)

If Reynold number i.e. 2000 < RN < 4000,we observe a flow in which we can see both laminar and turbulent flow to gather. This flow is called Transition flow.

RN = 2300 is usually accepted as the value at transition , RN that exists anywhere in the transition region is called the critical Reynolds number.

Page 13: Reynold number (Fluid Mechanics)(FM)
Page 14: Reynold number (Fluid Mechanics)(FM)

EXAMPLE

Page 15: Reynold number (Fluid Mechanics)(FM)

Example 1 :- An oil of viscosity 0.5 stoke is flowing through a pipe of 30 cm in diameter at a rate of 320 liters per second. Find the head loss due to friction for the pipe length of 60 cm.

Solution:-Q=320 liters/second =0.32 m3/s d=30 cm=0.30 m x 0.302

=0.070m2

L=60 m =0.5 stoke

= 0.5 x 10-4 m2/s V= Q/A=0.32/0.0707 =4.52 m/s

Page 16: Reynold number (Fluid Mechanics)(FM)

Reynolds number(RN):-

/sm 10 x 6.156

RN1/40.079

f

Turbulent. is Flow4000) ( 27,120

4)-10 x (0.5

0.30) x (4.52

νVxD

R

μρxVxD

R

24-

N

N

Page 17: Reynold number (Fluid Mechanics)(FM)

• Head loss due to Friction:-

m 5.128

0.30 x 9.81 x 2

(4.52) x 60 x 10 x 6.156 x 4

2.g.d4.f.l.V

hf

23-

2

Page 18: Reynold number (Fluid Mechanics)(FM)

Example 2:- An oil of viscosity 0.9 and viscosity 0.06 poise is flowing through a pipe of diameter 200 mm at the rate of 60 liters per second. Find the head loss due to friction for a 500 m length of pipe. find the power required to maintain this flow

Solution:-Q = 60 liters/second x 0.202 = 0.0314 m2

= 0.06 m3/s d = 200 cm ρ = 0.9 x1000 =

900kg/m3 = 0.20 m L = 500 m µ = 0.6 poise = 0.006 Ns/m3

Page 19: Reynold number (Fluid Mechanics)(FM)

Reynolds number(RN):-

0.0051

1/4(0.079)/RN f

m/s 1.91

Q/AV

Turbulent is Flow4000) ( 57,300

(0.006

0.20 x 1.91 x 900

Page 20: Reynold number (Fluid Mechanics)(FM)

Head loss due to Friction:-

• Power required:-

kW 5.02 P1000

9.48 x 0.06 x 9.81 x 900

μhf x Qx x P

P

waterof m 9.48

02x9.81x0.2(1.91 x 30 x 0.0051 x 4

2.g.d4.f.l.V

hf

g

)2

2

Page 21: Reynold number (Fluid Mechanics)(FM)

Example 3:- oil of Sp. Gr 0.095 is flowing through a pipe of 20 cm in diameter. if a rate of flow 50 liters/second and viscosity of oil is 1 poise , decide the type of flow.

Solution:-Q = 50 liters/second x 0.202

=0.314 m2

= 0.05m3/sD =20 cm = 0.20 m ρ=0.95 x 1000

=950 kg/m3 µ = 1.0poise = 0.1 Ns/m3 V= Q/A=0.05/0.0314

=1.59m/s

Page 22: Reynold number (Fluid Mechanics)(FM)

Reynolds number(RN):-

.Transition is Flow 4000)Rn(2000 3021

0.1

0.20 x 1.59 x 950

μD x V x ρ

R N

..

Page 23: Reynold number (Fluid Mechanics)(FM)

Example 4:- Liquid is flowing through a pipe of 200 mm in diameter. Tube with mean viscosity of oil 2 m/sec. If density of liquid is 912 kg/ m3 and viscosity is 0.38 N.S/m2 the type of flow.

Solution:-V= 2 m/secd= 20 cm=0.20 m x

0.202=0.314m2

µ = 0.38 Ns/m3

ρ =950 kg/m3

Page 24: Reynold number (Fluid Mechanics)(FM)

Reynolds number(RN):-

Laminar. is Flow(2000) 960

0.38

0.20 x 2 x 912

μD x V x ρ

R N

Page 25: Reynold number (Fluid Mechanics)(FM)