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Ben-Gurion University of the Negev Jacob Blaustein Institutes for ...

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28<br />

3.5.1 Positive Cij<br />

Given a pipeline network <strong>of</strong> a specific diameter and with a specific friction index, <strong>the</strong><br />

cost <strong>of</strong> transportation depends on pumping costs which are strictly related to electricity<br />

costs. The amount <strong>of</strong> energy required to move every unit <strong>of</strong> water depends on <strong>the</strong><br />

specific arc <strong>of</strong> transportation in which <strong>the</strong> water is moving. The energy applied depends<br />

on: 1) <strong>the</strong> distance between source i and destination j; 2) <strong>the</strong> difference in elevation<br />

between source i and destination; 3) <strong>the</strong> diameter and <strong>the</strong> type <strong>of</strong> <strong>the</strong> pipe utilized, o<strong>the</strong>r<br />

factors were neglected. Maintenances costs were not included in <strong>the</strong> computation.<br />

Let us consider total required head (minor losses due to bends, valves, etc, are<br />

neglected), ∆ H,<br />

to be given by:<br />

where<br />

∆H<br />

= ∆Z<br />

+ ∆h<br />

f<br />

∆ Z = difference in elevation between a source and a destination (m);<br />

∆hf= pressure friction losses (m)<br />

The energy requirements at <strong>the</strong> pump used to convey <strong>the</strong> water to demand site are<br />

given (Jensen, 1983) by:<br />

HP=<br />

Where:<br />

Q∆H<br />

2. 7η<br />

H = pressure head, (m)<br />

HP = <strong>the</strong> power <strong>of</strong> <strong>the</strong> pump in horsepower (1HP=0.746 kW)<br />

Q = flow rate (m 3 /h)<br />

η = pump efficiency ( %)<br />

The energy loss ∆hf (m) in pipes depends on several factors, water flow, pipe’s length,<br />

pipe's materials and shape.<br />

The gradient <strong>of</strong> <strong>the</strong> energy loss in a pipe is usually expressed in ‰ (part per thousand)<br />

J(‰), as:<br />

J f<br />

= 1000*<br />

∆ h / L<br />

The gradient <strong>of</strong> <strong>the</strong> head loss J(‰), due to friction is assessed by Hazen-Williams<br />

equation (Jensen, 1983) :<br />

1.<br />

852<br />

J = 1.<br />

131*<br />

10 ( Q/<br />

C)<br />

D<br />

12 −4.<br />

87<br />

J = gradient <strong>of</strong> <strong>the</strong> head loss (‰);<br />

Q = flow rate (m 3 /h);<br />

D = internal diameter <strong>of</strong> a pipe (mm);<br />

(11)<br />

(12)<br />

(13)<br />

(14)

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