MHT CET · Physics · Mechanical Properties of Fluids
A gardening pipe having an internal radius ' \(R\) ' is connected to a water sprinkler having ' \(n\) ' holes each of radius ' \(r\) '. The water in the pipe has a speed ' \(v\) '. The speed of water leaving the sprinkler is
- A \(\left(\frac{\mathrm{R}^2}{\mathrm{r}^2}\right) \mathrm{nV}\)
- B \(\frac{R^2 v}{n r^2}\)
- C \(\left(\frac{\mathrm{nr}^2}{\mathrm{R}^2}\right) \mathrm{V}\)
- D \(\left(\frac{n R^2}{r^2}\right) V\)
Answer & Solution
Correct Answer
(B) \(\frac{R^2 v}{n r^2}\)
Step-by-step Solution
Detailed explanation
Using the equation of continuity, we have
\(\mathrm{A}_1 \mathrm{v}=\mathrm{A}_2 \mathrm{v}^{\prime}\)
where \(v\) is speed of water in the pipe and \(v^{\prime}\) is the speed of water leaving the pipe.
Area of the pipe \(=\pi \mathrm{R}^2\)
Area of each hole in the sprinkler \(=\pi r^2\)
\(\therefore \quad\) Total area of the holes in the sprinkler \(=n \pi r^2\)
\(\pi R^2 v=n \pi r^2 v^{\prime}\) ...from (i)
\(\therefore \quad \mathrm{v}^{\prime}=\frac{\mathrm{R}^2 \mathrm{v}}{\mathrm{nr}^2}\)
\(\mathrm{A}_1 \mathrm{v}=\mathrm{A}_2 \mathrm{v}^{\prime}\)
where \(v\) is speed of water in the pipe and \(v^{\prime}\) is the speed of water leaving the pipe.
Area of the pipe \(=\pi \mathrm{R}^2\)
Area of each hole in the sprinkler \(=\pi r^2\)
\(\therefore \quad\) Total area of the holes in the sprinkler \(=n \pi r^2\)
\(\pi R^2 v=n \pi r^2 v^{\prime}\) ...from (i)
\(\therefore \quad \mathrm{v}^{\prime}=\frac{\mathrm{R}^2 \mathrm{v}}{\mathrm{nr}^2}\)
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