the effect of the particle size distribution on non-newtonian turbulent ...

the effect of the particle size distribution on non-newtonian turbulent ... the effect of the particle size distribution on non-newtonian turbulent ...

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Chapter 3 Experimental Work Table 3.II: Pipeline Roughness Actual Inside Diameter Pipeline Roughness (mm) (]Lm) 21,6 4 79,0 7 140,7 9 207,0 130 . 3.4.2 Calibration ong>ofong> Differential Pressure Transducer The following procedure is used to calibrate ong>theong> DPT on ong>theong> East and Mini Rig. Page 3.13 1. The transducer and manometer that are to be calibrated are flushed with mains water to ensure that air and any solids have been removed from ong>theong> lines. 2. Air over water manometer head ie. a differential head (H) is set up in ong>theong> glass manometer tubes. 3. . This head is measured and ong>theong> DPT output is logged at ong>theong> same time. 4. Steps 2 and 3 are repeated for different manometer heights over ong>theong> full differential head test range until enough data points have been collected for calibration. A least squares linear regression is performed on ong>theong> measured head and transducer readings in order to obtain ong>theong> calibration equation. A set ong>ofong> N observed measurements Y on ong>theong> corresponding set ong>ofong> N transducer readings X will yield ong>theong> least squares regression line ong>ofong> (Spiegel, 1972) Y:mX+c Where (3.4)

Chapter 3 Experimental Work<br />

Table 3.II: Pipeline Roughness<br />

Actual Inside Diameter Pipeline Roughness<br />

(mm) (]Lm)<br />

21,6 4<br />

79,0 7<br />

140,7 9<br />

207,0 130<br />

.<br />

3.4.2 Calibrati<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> Differential Pressure Transducer<br />

The following procedure is used to calibrate <str<strong>on</strong>g>the</str<strong>on</strong>g> DPT <strong>on</strong> <str<strong>on</strong>g>the</str<strong>on</strong>g> East and Mini Rig.<br />

Page 3.13<br />

1. The transducer and manometer that are to be calibrated are flushed with mains<br />

water to ensure that air and any solids have been removed from <str<strong>on</strong>g>the</str<strong>on</strong>g> lines.<br />

2. Air over water manometer head ie. a differential head (H) is set up in <str<strong>on</strong>g>the</str<strong>on</strong>g><br />

glass manometer tubes.<br />

3. . This head is measured and <str<strong>on</strong>g>the</str<strong>on</strong>g> DPT output is logged at <str<strong>on</strong>g>the</str<strong>on</strong>g> same time.<br />

4. Steps 2 and 3 are repeated for different manometer heights over <str<strong>on</strong>g>the</str<strong>on</strong>g> full<br />

differential head test range until enough data points have been collected for<br />

calibrati<strong>on</strong>.<br />

A least squares linear regressi<strong>on</strong> is performed <strong>on</strong> <str<strong>on</strong>g>the</str<strong>on</strong>g> measured head and transducer readings<br />

in order to obtain <str<strong>on</strong>g>the</str<strong>on</strong>g> calibrati<strong>on</strong> equati<strong>on</strong>. A set <str<strong>on</strong>g>of</str<strong>on</strong>g> N observed measurements Y <strong>on</strong> <str<strong>on</strong>g>the</str<strong>on</strong>g><br />

corresp<strong>on</strong>ding set <str<strong>on</strong>g>of</str<strong>on</strong>g> N transducer readings X will yield <str<strong>on</strong>g>the</str<strong>on</strong>g> least squares regressi<strong>on</strong> line <str<strong>on</strong>g>of</str<strong>on</strong>g><br />

(Spiegel, 1972)<br />

Y:mX+c<br />

Where<br />

(3.4)

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