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ABSTRACT
In this experiment, the characteristics of the flow in a fluid in a pipe were measured by using Reynolds number. The objective for this experiment were to compute Reynolds number (Re) and to observe laminar, transitional, and turbulent flow.
There were several steps taken to conduct the experiment. Inlet valve, V1, was opened to allow water to enter the stilling tank and was allowed to settle for a few minutes before flowing into the visualisation tube. Dye was injected into the stream to identify the current flow in the tube. Water inlet valve, V1, and outlet valve, V2, were regulated until a straight identifiable dye line is achieved. The flow rate at the outlet valve, V2, was measured using volumetric method. Constant the time taken for each collected volume of water and replicate it 3 times. The experiment was repeated in the same manner but regulate V1 and V2 to produce transitional and turbulent flow.
The result of Reynolds number obtained from the experiment were 177 for laminar flow, 2826.36 for transitional flow and 4098 for turbulent flow.
1
TABLE OF CONTENT
INDEX PAGE
INTRODUCTION 3
OBJECTIVES 4
THEORY 5
DIAGRAM AND DESCRIPTON OF APPARATUS 6
PROCEDURES 8
RESULTS AND DISCUSSION 9
SAMPLE CALCULATIONS 12
CONCLUSION 12
RECOMMENDATION 13
REFERENCES 13
APPENDICES 14
2
INTRODUCTION
Reynolds number, denoted as Re, is said to be a dimensionless quantity that
is used to help predict similar flow patterns in different fluid flow situations. For flow
in a pipe or a sphere moving in a fluid the diameter is generally used today. Other
shapes (such as rectangular pipes or non-spherical objects) have an equivalent
diameter defined. For fluids of variable density (e.g. compressible gasses) or
variable viscosity (non-Newtonian fluids) special rules apply. The velocity may also
be a matter of convention in some circumstances, notably stirred vessels.
The Reynolds number is defined as the ratio of inertial forces
to viscous forces and consequently quantifies the relative importance of these two
types of forces for given flow conditions. Reynolds numbers frequently arise when
performing scaling of fluid dynamics problems, and as such can be used to
determine dynamic similitude between two different cases of fluid flow. They are also
used to characterize different flow regimes within a similar fluid, such
as laminar or turbulent flow: laminar flow occurs at low Reynolds numbers, where
viscous forces are dominant, and is characterized by smooth, constant fluid motion;
turbulent flow occurs at high Reynolds numbers and is dominated by inertial forces,
which tend to produce chaotic eddies, vortices and other flow instabilities.
In practice, matching the Reynolds number is not on its own sufficient to
guarantee similitude. Fluid flow is generally chaotic, and very small changes to
shape and surface roughness can result in very different flows. Nevertheless,
Reynolds numbers are a very important guide and are widely used.
3
The Reynolds experiment is conducted to observe and determine the type of
flow of a water stream in a glass tube and to determine its Reynolds number. This
experiment is done by injecting red dye into the stream and the flow of the red dye is
observed. To calculate the Reynolds number of the water stream, the volume of the
outflow water stream is measured using a measuring cylinder at a constant time
taken. With the given and obtained information, all are then used into the formula;
ℜ= ρνdμ
OBJECTIVE
The purpose of the Reynolds experiment is to illustrate laminar, transitional
(intermittently turbulent), and fully turbulent pipe flows along with the conditions
under which these types of flow occur, to compute Reynolds number (Re), and to
prove that the Reynolds number is dimensionless.
4
THEORY
Reynolds number can be defined for a number of different situations where a
fluid is in relative motion to a surface. The definitions generally include the fluid
properties of density, ρ and viscosity, μ, plus a velocity, ν, and a characteristic length
or characteristic dimension, d. This dimension is a matter of convention for example
a radius or diameters are equally valid for spheres or circles, but one is chosen by
convention.
The critical velocity, v averaged over the cross section at which laminar pipe
flow changes to transitional flow, or transitional flow changes to turbulent flow, is
believed to be a function primarily of the pipe diameter, d, the fluid density, ρ, and
the fluid dynamic viscosity, μ. In mathematical terms,
V=V (d , ρ, μ)
Using dimensional reasoning, one can show that the relation among the
parameters must be;
ℜ= ρνdμ = dimensionless parameter
It is a ratio of the inertial (destabilizing) force to the viscous damping
(stabilizing) force. As Re increases, the inertial forces grow relatively larger, and the
flow gets destabilized into full-blown turbulence.
The Reynolds experiment used to demonstrate the critical velocity based on
the nature of the two modes of motion flowing in a tube, i. e. laminar and turbulent.
Reynolds investigated these two fluid motions. Fluid motion was found to be laminar
for Re numbers below 2000 and turbulent flows for Re greater than 4000. Thus, the
critical velocity, v will be directly proportional to the mass flow rate, m.
5
DIAGRAM AND DESCRIPTION OF APPARATUS
Reynolds flow apparatus: dye injector, stilling tank, glass tube
300 ml measuring cylinder
A stopwatch
Color dye
Figure 1: Schematic diagram of an Osbourne Reynolds apparatus
6
Figure 2: Osbourne Reynolds flow apparatus
The apparatus is set up by filling the dye reservoir with color dye liquid. Dye reservoir
is connected to the flow control valve to ensure the flow of dye liquid can be
controlled. From the injection needle, we can observed that the liquid dye is flowing
through the glass tube and is based on the velocity of the fluid. Laminar, transitional
and turbulent flow should be obtained. The water flows out from the outlet valve is
collected and the time is taken to determine the flow rate.
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Dye reservoir
Flow control valve
Injection needle
Glass tube
Water outlet valve
Safety and precautions
This apparatus should be in a separate room or away from other experiments
because any vibration from them or students bumping/leaning on the counter will
cause errors.
EXPERIMENTAL PROCEDURE
EXPERIMENT A
1. The dye injector is lowered until it is seen in the glass tube.
2. The inlet valve, V1 is opened and water is allowed to enter stilling tank.
3. A small overflow spillage through the over flow tube is ensured to maintain a
constant level.
4. Water is allowed to settle for a few minutes.
5. The flow control valve is opened fractionally to let water flow through the
visualizing tube.
6. The dye control needle valve is slowly adjusted until a slow flow with dye
injection is achieved.
7. The water inlet valve, V1 and outlet valve, V2 is regulated until a straight
identifiable dye line is achieved. The flow will be laminar.
8. The flow rate is measured using volumetric method.
9. The experiment is repeated by regulating water inlet valve, V1 and outlet
valve, V2 to produce transitional and turbulent flow.
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RESULTS
VOLUME
(L)
TIME
(s)
FLOWRATE,
Q (L/s)
FLOWRATE, Q
(m3/s)
Re= ρvdμ =
Q XDA X μ
TYPES OF
FLOW
0.058
0.058
0.058
30
30
30
1.933 x 10 -3
1.933 x 10 -3
1.933 x 10 -3
1.933 x 10 -6
1.933 x 10 -6
1.933 x 10 -6
177.00
177.00
177.00
LAMINAR
FLOW
Re < 2100Reavg =
177
0.168
0.146
0.148
5
5
5
0.0336
0.0292
0.0296
3.35 x 10-5
2,92 x 10-5
2.96 x 10-5
3083.00
2679.68
2716.40
TRANSITION
FLOW
2100< Re <
4000
Reavg =
2826.36
0.220
0.226
0.224
5
5
5
0.0440
0.0452
0.0448
4.4 x 10-5
4.52 x 10-5
4.48x 10-5
4037
4148
4111.3
TURBULENT
FLOW
Re > 4000Re avg =
4098
Given: Diameter, D = 0.0156 m
Area, A = 1.91 x 10-4 m2
Viscosity , v = 25 kg/m.s
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Kinematic = 0.89 x 10-6 m2/s
DISCUSSION
The results taken shows the Reynolds number of each set of flow. The
Reynolds number can be defined for a number of different situations where a fluid is
in relative motion to a surface.
This Osbourne Reynolds experiment used to demonstrate the critical velocity
based on the nature of the two modes of motion flowing in a tube. Laminar flow,
transitional flow as well as turbulent flow have different value of Reynolds Number.
The table above shows the results obtained from sets of experiment done with
the flowmeter apparatus. Apparently, we repeat the experiment to get the average
Reynolds Number that we want hence approving the expectation and theory with the
result we get.
For first set of experiment, we recorded the volume of liquid collected within
30 seconds to find the flow rate of the flow. The results shows the Re avg = 177. This
value lies below Re<2000, proving that it is a laminar flow. Laminar is characterized
by streamlines and highly-ordered motion and the flow rate of the fluid is the lowest
among the three test.
Secondly, we change the flow of the fluid. This time with the increment of flow
rate that been determined manually, the Reynolds Number shows the value of Reavg=
2826. This value lies between 2000< Re<4000, hence the flow is transition flow.
The third set was done the same as the two sets before, the Reavg= 4098
which the value lies in Re>4000. The flow was decided to be the turbulent flow.
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Turbulent in the second case where it is characterized by velocity fluctuations and
highly disordered motion.
The observation that we obtained from the results for laminar is the dye that
flow has straight and smooth line, for transition the flow of dye has bursts of
fluctuations and for turbulent the dye has zigzas rapidly and randomly.
The results that we get in this experiment was approximately according to
theory of Osbourne Reyolds. Increse in flowrate effected the flow which the highest
flowrate causing the turbulent flow and vice versa.
The properties for each flow determined by the Osbourne method practically
can be differentiate using data below:
Laminar Turbulent Transition
low flowrate
Lowest Reynolds
Number
Re<2000
The ink injected
forming a visible
straight line
High flowrate
High Reynolds
value Re>4000
The ink injected
observed to be
very inconsistent
and no visible
line form
Flowrate lies between
laminar and turbulent
The Reynolds number lies
between laminar and
turbulrent flow.
2000<Re<4000
The line visible until reach
turbulent flow
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12
SAMPLE CALCULATION
Given Diameter = 0.0156 m
Area = 1.91x10-4 m2
Kinematic viscosity = 0.89x10-6 m2/s
Re = Qx DA x µ
Average volume=0.058+0.058+0.0583
=0.058 L
Flowrate(m3s )=0.058 L30 s
¿(1.933×10−3L /s)( 0.001m31 L ) = 1.933x10-6 m3
ℜ= (1.933 x10−6m3 /s ) (0.0156m )(1.91 x10−4m2 ) (0.89 x10−6m2/s )
=177.39
CONCLUSION
In conclusion, the results that we obtained after calculate the Reynold’s
number were 177 for laminar, 2826.36 for transitional and 4098 for turbulent. The
theories of this Reynold’s number state that if it is below than 2000, it is laminar. The
transition states occur at Reynold’s number range between 2000 and 4000.
Meanwhile, for turbulent flow the Reynold’s number is above 4000. Thus the results
obtained are similar as the theories stated. The flow of each laminar, transition and
turbulent can also be seen clearly based on the behaviour of the liquid inside the
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pipe. For laminar, the dye remained straight and parallel to the streamline as
entering the observation tube. While for transition, the dye start to mix with the
streamline and the behaviour is differ with the laminar flow. Turbulent flow shows
that the dye starts to disperse as they entered the observation tube. The theories
stated and the results and observation that we obtain from this experiment are exact
hence this experiment was considered as successful.
RECOMMENDATION
It is recommended that the water sink plug is changed to a more efficient
design so water leaks can be overcome faster and thus saving precious experiment
time. The dye used during the experiment was not thick due to the face that I could
cause a blockage to the dye injector. It turns out that a few extra drop of dye wouldn’t
turn it into a worst case scenario. So in short, use a thicker dye.
REFERENCES
Osbourne Reynolds’ experiment. (2011). Retrieved September 5, 2014, from
http://prezi.com/yia-jutherne/osborne-reynolds-experiment/
http://research.me.udel.edu/~lywang/meeg331/labs/reynolds.pdf
http://www.scribd.com/doc/39165338/Osbourne-Reynolds-Apparatus-
Experiment
www.wikipedia.org/Reynolds_number
www.engineeringtoolbox.com/reynolds-number-d_237.html
V. L. Streeter, (1962). Fluid Mechanics (3rd Edition) McGraw-Hill.
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15
APPENDICES
App. 1: Laminar flow App. 2: Transitional flow
App. 3: Turbulent flow
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