Conservation of Mass - Clarkson University
Conservation of Mass - Clarkson University
Conservation of Mass - Clarkson University
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Applying the definition given in Equation (12) yieldsRQ 1 2V = av2πrV ( r) dr rV ( r)drπR = πR = R2 2 20 0R∫ ∫ (13)Two example problems are considered next. The first example involves using the steady version<strong>of</strong> the equation <strong>of</strong> conservation <strong>of</strong> mass to make calculations involving a natural gas pipeline(source: Fluid Mechanics for Chemical Engineers by Noel de Nevers). The second exampleshows how to use the unsteady version <strong>of</strong> the equation <strong>of</strong> conservation <strong>of</strong> mass to calculate therate <strong>of</strong> change <strong>of</strong> the height <strong>of</strong> liquid in a tank.Example 1 -- Natural Gas PipelineD1 = 2.00 ftD2 = 2.50V1 = 33.7 ft / sV2= ?ft1 2p1 = 820 psiap2 = 450 psiaT1 = 70 FT2 = 58 FGas Constant R = 10.73g( f/ )2 3lb in • ftMolecular Weight = 16• R( lb mole)lblb moleFind m, V2 2This is a long pipeline, which is shown schematically. The natural gas flows through a section <strong>of</strong>circular pipe <strong>of</strong> diameter 2.00 feet for some distance, and then through a larger section <strong>of</strong> circularpipe <strong>of</strong> diameter 2.50 feet. The pressure and temperature at locations 1 and 2 are specified. Weneed to find the velocity at location 2, and the mass flow rate at location 2.6