Explanations & Calculations
- Those given conditions are valid only at the pump outlet where the water is ejected at the speed of "\\small 30\\,ms^{-1}" and beyond that these calculations may not seem to be effective.
- The power, as it is defined is = "\\Large \\frac{\\Delta\\text{work}}{\\Delta\\text{time}}"
- And the work done at the outlet is "\\small W= \\small \\frac{1}{2}mv^2" and lets assume that this work is done at a small duration of "\\small t(s)". Then the power needed is
"\\qquad\\qquad\n\\begin{aligned}\n\\small P&=\\small \\frac{W}{t}=\\frac{1}{2}\\Big(\\frac{m}{t}\\Big)v^2\n\\end{aligned}"
- That term within the parentheses is the rate of mass flow which can be deduced to be "\\small Av\\rho" where A is the are of the pump.
- Then,
"\\qquad\\qquad\n\\begin{aligned}\n\\small P&=\\small \\frac{1}{2}(Av\\rho)v^2\\\\\n&=\\small \\frac{1}{2}Av^3\\rho\\\\\n&=\\small \\frac{1}{2}(\\pi(0.01m)^2\\times(30ms^{-1})^3\\times1000kgm^{-3})\\\\\n&=\\small \\bold{4241.15\\,W\\approx4.2kW}\n\\end{aligned}"
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