result for laminar flow
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Transcript of result for laminar flow
Results
Low Flow RateLaminar Flow (Armfield Experimental Rig), Pipe Length = 500mm, Pipe Diameter 3mm
NoFlow RateWater TemperatureWater ManometerWater Density
Air
DensityDynamic
Viscosity
Volume (ml)Time (s)((C)h1(mm)h2(mm)water (kg/m3)air (kg/m3)water (kg/ms)
15860.1931.0280300995.411.14810.000781
212460.1231.0270310995.411.14810.000781
318060.3433.5260320994.61.13970.000742
428060.4433.5240335994.61.13970.000742
533060.3134.0225350994.431.13810.000734
634060.2534.0205370994.431.13810.000734
732060.1234.5215360994.261.13640.000727
836060.0634.5190380994.261.13640.000727
939060.1835.0180390994.081.13480.00072
1039060.1235.0170400994.081.1348
Table 1. Raw experimental data.NoVolumetric Flowrate, Q ( 10-6 m3/s)Velocity, v (m/s)Reynolds NumberPressure drop, P (Pa)Head loss, hloss (m)Friction factor, fEstimated friction factor, f =16/Re Percentage Error, %
10.960.136521195.070.0200.1270.03175.74
22.060.2921116390.150.0390.0550.01474.04
32.980.4221697584.750.0590.0400.00976.20
44.630.6552636925.860.0950.0260.00676.66
55.470.77431461218.020.1250.0250.00579.27
65.640.79832451607.800.1650.0300.00583.80
75.320.75330891412.670.1450.0300.00582.78
85.990.84834791851.080.1890.0310.00585.20
96.480.91737972045.570.2100.0290.00485.66
106.490.91838012240.380.2300.0320.00486.89
Table 2. Calculated Data
Graph 1. Graph of Friction Factor against Reynolds Number for Low Flow Rate.High Flow RateTurbulent Flow (Lotus Scientific), Pipe Length = 425 mm, Pipe Diameter = 7.74 mmNoFlow RateWater TemperatureMercury ManometerWater Density
Mercury DensityDynamic
Viscosity
Volume (ml)Time (s)((C)h1(mm)h2(mm)water (kg/m3)mercury (kg/m3)water (kg/ms)
11803.5830.53055995.5613553.450.000789
21802.6931.32065995.3113551.500.000776
31802.2232.01075995.0913549.800.000765
41802.0232.0085995.0913549.800.000765
52001.9932.2-1095995.0213549.310.000762
62001.7332.3-20105994.9913549.070.000760
72001.6332.3-30115994.9913549.070.000760
82001.5033.0-40125994.7613547.370.000749
Table 3. Raw Experimental Data.NoVolumetric Flowrate, Q ( 10-5 m3/s)Velocity, v (m/s)Reynolds NumberPressure drop, P (Pa)Head loss, hloss (m)Friction factor, f
15.031.069104363079.820.3150.099
26.691.422141185542.930.5680.100
38.111.723173498005.510.8200.099
48.911.8941906710468.741.0720.107
510.052.1362158812931.551.3250.104
611.562.4572489715394.441.5770.093
712.272.6082642517857.551.8300.096
813.332.8342913020318.282.0820.093
Table 4. Calculated Experimental DataGraph 2. Graph of Friction Factor against Reynolds Number for High Flow Rate.
From Moody Chart,
Therefore = 0.08 0.00774 = 0.0006192mmDynamic viscosity of water, water estimationReynolds NumberPressure change, P (Pa)Volumetric Flow Rate, Q ( 10-6 m3/s)
521195.070.96
1116390.152.06
1697584.752.98
2636925.864.63
Table 5. Data used to plot , P against Q graph.From Graph 1 above, Reynolds Number from 521 to 2636 fall within the laminar region and the rest are within the transition region. Therefore, pressure change, P and volumetric flow rate, Q data from Re 521 to 2636 was taken to plot P against Q graph.
Graph 3. Graph of Pressure Change, P against Volumetric Flow Rate, Q in laminar region
From equation displayed on graph above, the gradient is 200.54, therefore
= 7.97 10-10 kg/ms
= 7.62 10-4 kg/ms The average dynamic viscosity of water, water from property table is 7.62 10-4 kg/msThe percentage error of the value obtained experimentally is:
Appendix
Figure : Experimental Setup for Low Flow Rate.
Sample Calculations for Low Flow Rates ExperimentVolumetric Flow Rate, Q :
Velocity of water at the inlet and out of the pipe :
Reynolds Number :
Pressure drop, P (Pa) :P = (water - air) g (h2 h1)
= (995.41 - 1.1481) 9.81 (0.3 0.28)m
= 195.07 Pa
From First Law of Thermodynamics for a steady state one-dimensional flow with one inlet and outlet, conservation of energy can be applied to a control volume
Eqn (1)
PQ flow energy, where Q is the volumetric flow rate
Dividing Eqn (1) by g, and assume T is very small therefore neglect U, the equation reduces to
Eqn (2)
Eqn (3)
f friction factor
L length of pipe
D diameter of pipe
KL loss coefficient due to pipe fittings or accessories
Since mass flow rate is conserved,
Assuming fluid is incompressible and are at the inlet and outlet are equal
Since no fitting on the pipe,
Friction factor for low flow rate :
= 0.127 EMBED Equation.3
_1443865985.unknown
_1443866002.unknown
_1443634805.unknown