Water flows from a large tank through a large pipe that splits into two smaller pipes as shown in figure below. Height, H=15m. The density of water is 1000kg/m3, atmospheric pressure patm = 101.325kPa and gravitational acceleration g = 9.81m/s2.
Regarding all mentioned information and the figure file attached, whilst viscous effects are negligible, determine: - the velocity (in m/s) through pipe exit 2. - The velocity (in m/s) through pipe exit 3. - The pressure (in kPa) at point 1 in the large pipe.
I'm wondering if we can use bournelli's law for this. considering that the total mechanical energy is conserved. delta E = 0. \[KE_{1}+PE_{1} = KE_{f}+PE_{f}\] This translates to the following: \[\frac{ 1 }{ 2 }mv^{2}_{1}+mgh_{1} = \frac{ 1 }{ 2 }mv^{2}_{2}+mgh_{2}\] we need to express this in terms of density: \[\rho = \frac{ m }{ v }\] let's express it this way. \[m = \rho*v \] \[\frac{ 1 }{ 2 }rho*v*v^{2}_{1}+rho*v*gh_{1} = \frac{ 1 }{ 2 } rho*v*v^{2}_{2}+rho*v*gh_{2}\] which gives us \[\rho*\frac{ 1 }{2 }m_{1}v^{2}_{1}+\rho*g*h + p_{i} = \rho*\frac{ 1 }{ 2 }m_{2}v^{2}_{2}+\rho*gh_{2}+p_{2}\]
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