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 ...
Chapter 3 Experimental Work Page 3.11 (c) Pressure Transducers A Gould PD3000 pressure transducer was used for differential pressure measurement. The transducer employs a strain gauge bridge to convert differential pressure to an electrical output which can
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Chapter 3 Experimental Work Page 3.11<br />
(c) Pressure Transducers<br />
A Gould PD3000 pressure transducer was used for differential pressure measurement.<br />
The transducer employs a strain gauge bridge to c<strong>on</strong>vert differential pressure to an<br />
electrical output which can <str<strong>on</strong>g>the</str<strong>on</strong>g>n be read. The diaphragm is made <str<strong>on</strong>g>of</str<strong>on</strong>g>Hastelloy C with<br />
a 316 stainless steel body.<br />
3.3.2 Flow Measurement<br />
(a) Magnetic Flow Meters<br />
The magnetic flow meters that were used for <str<strong>on</strong>g>the</str<strong>on</strong>g> East Rig were manufactured by Kent<br />
Instruments (80mm pipeline) and Kr<strong>on</strong>e Instruments (150mm & 200mm pipelines).<br />
The principle <str<strong>on</strong>g>of</str<strong>on</strong>g> operati<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> both magnetic flow meters used is similar. Firstly, a<br />
magnetic field is set up across <str<strong>on</strong>g>the</str<strong>on</strong>g> bore <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>the</str<strong>on</strong>g> magnetic flow meter. Liquid flowing<br />
through <str<strong>on</strong>g>the</str<strong>on</strong>g> metering tube will cut <str<strong>on</strong>g>the</str<strong>on</strong>g> magnetic field and thus develop an induced emf<br />
in <str<strong>on</strong>g>the</str<strong>on</strong>g> liquid. This emfis detected by two electrodes in <str<strong>on</strong>g>the</str<strong>on</strong>g> wall <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>the</str<strong>on</strong>g> metering tube.<br />
The emfis proporti<strong>on</strong>al to <str<strong>on</strong>g>the</str<strong>on</strong>g> flow velocity multiplied by <str<strong>on</strong>g>the</str<strong>on</strong>g> magnetic field strength.<br />
The transducer signal is digitised by a data logger.<br />
3.4 CALIBRATION<br />
The transducers and magnetic flux flow meters are re-ealibrated at regular intervals to ensure<br />
accuracy for collecting research data. The transducers are calibrated at <str<strong>on</strong>g>the</str<strong>on</strong>g> start <str<strong>on</strong>g>of</str<strong>on</strong>g>each day<br />
and <str<strong>on</strong>g>the</str<strong>on</strong>g> flow meters at <str<strong>on</strong>g>the</str<strong>on</strong>g> start <str<strong>on</strong>g>of</str<strong>on</strong>g> each week as well as during a test run.<br />
3.4.1 Pipeline<br />
(a) Pipeline Diameter<br />
The internal pipeline diameter (D) is measured by filling a known length (L) <str<strong>on</strong>g>of</str<strong>on</strong>g> pipe<br />
with water. The amount <str<strong>on</strong>g>of</str<strong>on</strong>g> water required to fill <str<strong>on</strong>g>the</str<strong>on</strong>g> pipe is weighed (Mw) and <str<strong>on</strong>g>the</str<strong>on</strong>g>