Design an experiment to determine h_{p} for a pump.
Design an experiment to determine h_{p} for a pump.
Experimentalists seek to design tests that are theoretically motivated while easily performed and interpreted. To determine h_{p} for a pump, for example, one would seek to eliminate all minor losses as well as the gravita-tional effects if possible. Consider, for example, Figure 10.16 for which the pipe flow equation is
\left(\frac{p_{1}}{\rho _{1}}+\frac{1}{2}\alpha _{1}\overline{\nu }^{2}_{1} \right)-\left(\frac{p_{2}}{\rho _{2}}+\frac{1}{2}\alpha _{2}\overline{\nu }^{2}_{2} \right)=f\left(Re,\frac{e}{D} \right)\left(\frac{L_{1}}{D} \right)\frac{\overline{\nu }^{2}_{1} }{2}+f\left(Re,\frac{e}{D} \right)\left(\frac{L_{2}}{D} \right)\frac{\overline{\nu }^{2}_{2} }{2}-h_{p}
and from which h_{p} can be solved in terms of measurable quantities. Of course, balance of mass requires that Q_{1} = Q_{2} and thus \overline{\nu }_{1} = \overline{\nu }_{2} in a constant
Control Volume and Semi-empirical Methods FIGURE 10.16 Simple experimental setup to determine the geometric loss (actually gain) due to a particular pump. cross-section pipe. If the flow is the same at 1 and 2, either turbulent or laminar, then our data reduction simplifies. Indeed, if we are able to measure the inlet p_{3} and outlet p_{4} pressures very near the pump, then
\frac{p_{3}-p_{4}}{\rho }=-h_{p}\rightarrow h_{p}=\frac{p_{4}-p_{3}}{\rho },where p_{4}\gt p_{3} due to the pump. Hence, the gain (or, a negative loss) due to a pump is determined primarily by the pressure jump across the pump.