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Petroleum Engineering Laboratory Report
NAME: Maximiano Kanda Ferraz
GROUP NUMBER: A9
EXPERIMENT NUMBER: 4 - Flow Characteristics of Valves
DATE OF EXPERIMENT: 03/03/2015
DATE OF REPORT SUBMISSION: 06/03/2015
MARK/10 (for demonstrator use):
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SUMMARY
1 INTRODUCTION ........................................................................................ 3
1.1 Learning Outcome ........................................................................... 3
1.2 Theory .............................................................................................. 3
1.3 Relevance ......................................................................................... 5
2 EXPERIMENTAL WORK........................................................................... 6
2.1 System Used ..................................................................................... 6
2.2 Equipment and Procedure .............................................................. 6
2.3 Hazards ............................................................................................ 7
2.4 Results .............................................................................................. 7
3
CALCULATIONS ..................................................................................... 10
4 DISCUSSIONS ........................................................................................... 11
5 CONCLUSIONS ....................................................................................... 11
6 REFERENCES ........................................................................................... 11
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1. INTRODUCTION
In this section, a brief overview of the experiment is given, such as learning outcomes,
objective, and the theory behind it.
1.1 Learning Outcome
The main learning outcomes of the Flow and valve characteristics experiment are the
application of different types of valves in a pipeline and observe how they behave in terms
of fluid flow through restrictions of area and in relation to degree of opening. Sources of
errors and pressure losses can also be identified.
1.2 Theory
The Globe valve is bigger, has a correct direction of flow due to optimal internal
passageway and can better control the flow than the Gate valve, as show in Figure 1.
Figure 1 – Comparison between Globe valve and Gate valve. Source: [2]
The flange present at the pipeline (component of jointing pipes) is of the Weld-Neck type
and can resist high pressure and temperatures. They fit the inside diameter of the pipe, so
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there isn’t any restriction of flow, preventing turbulence and erosion. Figure 2 show the
types of flanges.
Figure 3 – Venturi Effect. Source: [9]
The orifice plate is a plastic plate that restricts the cross sectional area of flow through the
pipeline abruptally, resulting in a more turbulent flow. The Venturi meter is more expensive, because the gradual reduction of area provides a less turbulent flow. The Venturi effect that
occurs in the Venturi meter is shown in Figure 2, where the fluid velocity increases, as the
area decreases and that results in a pressure drop, noted in the manometer.
Figure 3 – Venturi Effect. Source: [5]
The theory of the experiment consists basically of the application of the Bernoulli
Equation to calculate that pressure drop, as shown in the equation below:
2 +gz+
= Constant Source: [6]
Igualating the equation for the 2 points of the Venturi meter:
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2 +gz+
=
2 +gz+
− = 2 − With the units in the international system of the variables being:
Q: Flow rate (m3 . s
-1)
g: Gravity (m . s-2)
v1: Velocity before entering Venturi meter (slower) (m . s-1)
v2: Velocity after entering Venturi meter (faster) (m . s-1)
P1: Inlet Pressure (Pa) P1: Outlet Pressure (Pa)
ρ: Density of air (kg/m³)
z: Elevation (m)
The Darcy-Weisbach equation of head loss is given by:
∆ =
2
∆ = ²2 Source: [4]
∆: Head loss due to friction (m) L: Length of the pipe (m)
D: Diameter of the pipe (m)
U: Average flow velocityor volumetric flow rate per unit cross-sectional area (m/s)
: Darcy friction coefficient
1.3 Relevance
The relevance of the Flow and valve characteristics experiment is big to the
petroleum engineering field of work, as oil and gas reservoirs are elevated and produced
through a system of pipelines and valves. An example is the Christmas tree, a complex
equipment that contains Valves, connections and installed adapters above the well head in
order to control the flow of fluids to the surface, in which friction losses and Venturi effects
occurs.
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2. EXPERIMENTAL WORK
This section describes the materials, apparatus and systems used, as well as the
procedures made for the successful completion of the experiment.
2.1 System Used
The experiment contains several equipments and instruments:
Air Blower
Gaskets
Pipeline
Globe Valve
Gate Valve
Manometer
Ruler
Wrench
Flanges
Protractor
2.2 Equipments and Procedures
Below, is a list of the procedures of the experiment:
I. First, the Gate Valve is put in the correct position.
II. Turn the Air blower on.III. Starting with the valve closed, measure the mark on the manometer for the inlet and
outlet pressure.
IV. Rotate the valve 90º with the help of the protractor and get the data from the manometer.
V. Repeat Step IV until the valve is completely open.
VI. Repeat steps III to V (Trial 2).
VII. Turn the air blower off.
VIII. Replace the Gate valve for the globe valve (using the wrench, and positioning the
gasket to prevent leakage).
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IX. Repeat steps II to VI for the Globe valve.
X. Turn the Air blower off.
2.2 Hazards
The hazards of the experiment are not really hazards, but precautions to be taken, such as:
Correct handling of the materials (valves, screws)
2.3 Results
The results obtained are displayed on the tables 1 to 4 and Figure 4. The first two
columns of each table shown the opening of the valve in degrees and %. The third andfourth are the heights measured in the manometer, in centimeters. For Tables 1 and 2, there
was a trial 2. The subsequent columns are respectively, the mean ΔH (subtraction of the
outlet height from the inlet), the differential pressure and the calculated flowrates, with the
last column being the relation of Q/Qmax in percentage. The calculations of the pressure
obtained by the manometer is present in the next section (3. CALCULATIONS).
Table 1 - Measured Differential Pressure with Gate Valve through Venturi Meter
Trial 2 Trial 3
Valve Open Valve Open Inlet Height Outlet Height Inlet Height Outlet Height
Mean
ΔH ΔP Q Q/Qmax
[Degrees] % [cm] [cm] [cm] [cm] [mm] [Pa]
~root
ΔH %
0 0,0 37,8 37,8 37,8 37,8 0,0 0,000 0,0000 0,0000
90 4,8 37,8 37,8 37,8 38,0 0,1 0,012 0,3162 7,6472
180 9,7 37,6 38,0 37,5 38,2 0,6 0,065 0,7416 17,9343
270 14,5 37,1 38,6 36,8 38,9 1,8 0,213 1,3416 32,4444
360 19,4 35,8 39,9 35,5 40,3 4,5 0,526 2,1095 51,0133
450 24,2 34,3 41,5 34,4 41,8 7,3 0,862 2,7019 65,3379
540 29,0 33,2 42,6 33,5 42,5 9,2 1,087 3,0332 73,3495
630 33,9 32,4 43,5 32,5 43,4 11,0 1,299 3,3166 80,2047
720 38,7 31,7 44,3 31,8 44,2 12,5 1,476 3,5355 85,4985
810 43,5 31,3 44,6 31,4 44,5 13,2 1,559 3,6332 87,8598
900 48,4 31,0 44,9 31,0 44,9 13,9 1,642 3,7283 90,1594
990 53,2 30,7 45,3 30,6 45,2 14,6 1,724 3,8210 92,4017
1080 58,1 30,4 45,5 30,4 45,5 15,1 1,783 3,8859 93,9706
1170 62,9 30,1 45,8 30,1 45,8 15,7 1,854 3,9623 95,8194
1260 67,7 29,9 46,0 29,9 46,0 16,1 1,902 4,0125 97,0323
1350 72,6 29,8 46,1 29,8 46,1 16,3 1,925 4,0373 97,63311440 77,4 29,6 46,3 29,8 46,2 16,6 1,955 4,0682 98,3790
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1530 82,3 29,5 46,4 29,6 46,4 16,9 1,990 4,1049 99,2667
1620 87,1 29,5 46,4 29,5 46,4 16,9 1,996 4,1110 99,4138
1710 91,9 29,4 46,5 29,5 46,5 17,1 2,014 4,1292 100,0000
1800 96,8 29,4 46,5 29,4 46,5 17,1 2,020 4,1352 100,0000
1860 100,0 29,4 46,5 29,4 46,5 17,1 2,020 4,1352 100,0000
Table 2 - Measured Differential Pressure with Globe Valve through Venturi Meter
Trial 2 Trial 3
Valve Open Valve Open Inlet Height Outlet Height Inlet Height Outlet Height
Mean
ΔH ΔP Q Q/Qmax
[Degrees] % [cm] [cm] [cm] [cm] [mm] [Pa]
~root
ΔH %
0 0,0 37,8 37,8 37,8 37,8 0,00 0,000 0,0000 0,0000
90 4,8 37,5 38,3 37,5 38,3 0,80 0,094 0,8944 27,2168
180 9,7 36,0 39,7 35,9 39,8 3,80 0,449 1,9494 59,3177
270 14,5 34,6 41,2 34,5 41,2 6,65 0,785 2,5788 78,4700
360 19,4 34,3 41,5 34,3 41,5 7,20 0,850 2,6833 81,6505
450 24,2 33,9 41,9 33,7 42,0 8,15 0,963 2,8548 86,8704
540 29,0 33,4 42,4 33,4 42,4 9,00 1,063 3,0000 91,2881
630 33,9 33,2 42,7 33,2 42,6 9,45 1,116 3,0741 93,5424
720 38,7 33,1 42,8 33,0 42,8 9,75 1,152 3,1225 95,0156
810 43,5 33,0 42,9 32,9 42,9 9,95 1,175 3,1544 95,9852
900 48,4 32,9 43,0 32,9 43,0 10,10 1,193 3,1780 96,7060
990 53,2 32,8 43,0 32,8 43,0 10,20 1,205 3,1937 97,1836
1080 58,1 32,8 43,0 32,8 43,0 10,20 1,205 3,1937 97,18361170 62,9 32,8 43,0 32,7 43,1 10,30 1,217 3,2094 97,6588
1260 67,7 32,8 43,0 32,7 43,1 10,30 1,217 3,2094 97,6588
1350 72,6 32,7 43,1 32,7 43,1 10,40 1,228 3,2249 98,1317
1440 77,4 32,7 43,1 32,7 43,1 10,40 1,228 3,2249 98,1317
1530 82,3 32,6 43,2 32,6 43,2 10,60 1,252 3,2558 99,0708
1620 87,1 32,6 43,2 32,6 43,2 10,60 1,252 3,2558 99,0708
1710 91,9 32,6 43,2 32,6 43,2 10,60 1,252 3,2558 99,0708
1800 96,8 32,6 43,3 32,6 43,3 10,70 1,264 3,2711 99,5370
1860 100,0 32,5 43,3 32,6 43,3 10,75 1,270 3,2787 100,0000
Table 3 - Measured Differential Pressure with Gate Valve through Orifice Plate
Valve Open Valve Open Inlet Height Outlet Height Mean ΔH ΔP Q Q/Qmax
[Degrees] % [cm] [cm] [mm] [Pa] ~root ΔH %
0 0,0 34,1 34,1 0,0 0,000 0,0000 0,0000
90 6,3 34,1 34,2 0,2 0,018 0,3873 10,3882
180 12,5 33,9 34,5 0,6 0,071 0,7746 20,7763
270 18,8 33,1 35,2 2,1 0,248 1,4491 38,8689360 25,0 32,1 36,3 4,2 0,496 2,0494 54,9689
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450 31,3 31,1 37,4 6,3 0,744 2,5100 67,3229
540 37,5 30,3 38,3 8,0 0,945 2,8284 75,8643
630 43,8 29,5 39,1 9,6 1,134 3,0984 83,1052
720 50,0 29,0 39,7 10,7 1,264 3,2711 87,7374
810 56,3 28,6 40,1 11,5 1,358 3,3912 90,9581900 62,5 28,2 40,5 12,3 1,453 3,5071 94,0687
990 68,8 28,0 40,7 12,7 1,500 3,5637 95,5860
1080 75,0 27,8 40,9 13,1 1,547 3,6194 97,0797
1170 81,3 27,7 41,1 13,4 1,583 3,6606 98,1850
1260 87,5 27,5 41,2 13,7 1,618 3,7014 99,2780
1350 93,8 27,4 41,3 13,9 1,642 3,7283 100,0000
1440 100,0 27,4 41,3 13,9 1,642 3,7283 100,0000
Table 4 - Measured Differential Pressure with Globe Valve through Orifice Plate
Valve Open Valve Open Inlet Height Outlet Height Mean ΔH ΔP Q Q/Qmax
[Degrees] % [cm] [cm] [mm] [Pa] ~root ΔH %
0 0,0 34,2 34,2 0,0 0,000 0,0000 0,0000
90 9,1 33,4 35,0 1,6 0,189 1,2649 42,6401
180 18,2 32,1 36,1 4,0 0,472 2,0000 67,4200
270 27,3 31,8 36,7 4,9 0,579 2,2136 74,6203
360 36,4 31,1 37,4 6,3 0,744 2,5100 84,6114
450 45,5 30,6 37,9 7,3 0,862 2,7019 91,0794
540 54,5 30,3 38,2 7,9 0,933 2,8107 94,7485
630 63,6 30,2 38,4 8,2 0,969 2,8636 96,5307
720 72,7 30,0 38,6 8,6 1,016 2,9326 98,8571
810 81,8 29,9 38,7 8,8 1,039 2,9665 100,0000
900 90,9 29,9 38,7 8,8 1,039 2,9665 100,0000
990 100,0 29,9 38,7 8,8 1,039 2,9665 100,0000
Figure 4 is the graph of the Percentage of maximum flow rate Vs. Percentage of opening
the valve, for each arrangement (gate valve with venturi meter, globe valve with Venturi
meter, Gate valve with Orifice Plate, Globe Valve with Orifice plate). The arrangements
with orifice plate were made by the other team.
Figure 5 is the graph of behavior of ideal valves. It is possible to observe that the valves
behave like the “Square Root” type valve. With maybe the globe valve with Venturi meter
behaving like a Quick opening valve.
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Figure 4 – Graph of Percentage of Maximum Flow Rate Vs. Percentage of Valve opening
Figure 5 – Ideal Graph of Percentage of Maximum Flow Rate Vs. Percentage of Valve opening
3. CALCULATIONS
The conversion of height to pressure:
= ℎ, = 9.81 , = 20º = 1204 /³
0,0000
10,0000
20,0000
30,0000
40,0000
50,0000
60,0000
70,0000
80,0000
90,0000
100,0000
0,0 20,0 40,0 60,0 80,0 100,0
P e r c e n t a g e o f M a x i m u m F
l o w r a t e
Percentage of Opening of the Valve
Gate Valve-Venturi Meter
Globe Valve-Venturi Meter
Gate Valve-Orifice Plate
Globe Valve-Orifice Plate
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Accumulated error: Considering the error of the manometer being ± 0,0005 m and the error
of the Compass = ± 0,5º
2222
2
c
c
b
b
a
a
Q
Q
²=4² =0.001
( )
= ( )
=0.0001181 4. DISCUSSIONS
The reported petrophysical experiment aimed to determine the behavior of the valves
described. Like any experiment, is subject to measurement errors, errors inherent in
equipments and even human error. However, it was obtained satisfactory and consistent
results with the literature and presented theory.
It is important to note that the Bernoulli’s equation was established under the following
conditions: Incompressible fluid, homogeneous. A way to improve would be to add more
valve types and redo the experiment. Also, redo the experiment, but this time, begin with the
valve open, instead of closed, to confirm the results.
5. CONCLUSIONS
The Venturi effect and the Bernoulli equation are of vital importance to fluid flow. The
different types of valves and its characteristics have to be known to avoid any errors or
hazards when doing an experiment.
6. REFERENCES
[1] Aleem, Hosam, 2015. ‘Class Notes’.
[2] Anish. ‘Globe Valve Used in Ships’. Available at
http://www.marineinsight.com/marine/marine-news/headline/globe-valve-used-on-ships-
design-and-maintenance/ (Accessed: 04/03/2015).
[3] Engineering Toolbox. ‘Density of Air’. Available at: www.engineeringtoolbox.com/
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air-density-specific-weight-d_600.html (Accessed: 04/03/2015).
[4] Engineering Toolbox. ‘Darcy-Weisbach Equation for Pressure and Head Loss’.
Available at: http://www.engineeringtoolbox.com/darcy-weisbach-equation-d_646.html
(Accessed: 04/03/2015).
[5] Chegg. ‘Venturi Effect’. Available at: http://www.chegg.com/homework-help/questions-
and-answers/venturi-meter-used-measure-flow-speed-fluid-pipe-meter-connected-two-
sections-pipe-fig-14--q1236560(Acessed 05/03/2015)
[6] Nina Shokri. ‘Solid Fluid Systems’, 2014. Handbook.
[7] The University of Manchester, 2015. ‘Petroleum Engineering Laboratory’.
[8] Thomas, J. E. ‘Fundamentos de Engenharia do Petróleo’. Rio de Janeiro, Interciência.
[9] Wermac. ‘Definition and Details of Flanges’. Available at:http://www.wermac.org/flanges/flanges_welding-neck_socket-weld_lap-
joint_screwed_blind.html (Acessed 05/03/2015)