The pipe connection shown in the figure below is used to split the flow from one...
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The pipe connection shown in the figure below is used to split the flow from one pipe into two pipes. The pipe connection has a mass m of 100 kg, while the fluid in the pipes is gasoline. The flow rate at section 1 is such that Q₁ = 0.05 m³/s, with 60% of the flow rate passing through section 2, and 40% passing through section 3. The pipe diameters at sections 1, 2, and 3 are d₁ = 20 cm, d₂ = 16 cm, and d3 = 12 cm, respectively, while sections 2 and 3 are at elevations such that %₂ = 1.3 m above, and z3 = 1.0 m below the elevation of section 1. The pipe associated with section 2 is at an angle of 40° to the horizontal, while the pipe associated with section 3 is at an angle of 30°. Finally, the pressure at section 1 is such that p₁ = 400 kPa. Take the density p of gasoline to be 890 kg/m³. Z X 1 2 3 40⁰ 30⁰° The pipe connection shown in the figure below is used to split the flow from one pipe into two pipes. The pipe connection has a mass m of 100 kg, while the fluid in the pipes is gasoline. The flow rate at section 1 is such that Q₁ = 0.05 m³/s, with 60% of the flow rate passing through section 2, and 40% passing through section 3. The pipe diameters at sections 1, 2, and 3 are d₁ = 20 cm, d₂ = 16 cm, and d3 = 12 cm, respectively, while sections 2 and 3 are at elevations such that %₂ = 1.3 m above, and z3 = 1.0 m below the elevation of section 1. The pipe associated with section 2 is at an angle of 40° to the horizontal, while the pipe associated with section 3 is at an angle of 30°. Finally, the pressure at section 1 is such that p₁ = 400 kPa. Take the density p of gasoline to be 890 kg/m³. Z X 1 2 3 40⁰ 30⁰°
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Related Book For
Fundamentals Of Momentum Heat And Mass Transfer
ISBN: 9781118947463
6th Edition
Authors: James Welty, Gregory L. Rorrer, David G. Foster
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