MHT CET · Physics · Mechanical Properties of Fluids
Water flows through a horizontal pipe at a speed 'V'. Internal diameter of the pipe is 'd'. If the water is emerging at a speed ' \(V_{1}\) ' then the diameter of the nozzle is
- A \(\frac{\mathrm{V}}{\mathrm{V}_{1}}\)
- B \(\mathrm{d} \sqrt{\frac{\mathrm{V}_{1}}{\mathrm{~V}}}\)
- C \(\mathrm{d} \sqrt{\frac{\mathrm{V}}{\mathrm{V}_{1}}}\)
- D \(\frac{\mathrm{d} V_{1}}{\mathrm{~V}}\)
Answer & Solution
Correct Answer
(C) \(\mathrm{d} \sqrt{\frac{\mathrm{V}}{\mathrm{V}_{1}}}\)
Step-by-step Solution
Detailed explanation
By equation of continuity \(A_{1} V_{1}=A_{2} V_{2}\)
\(
\begin{array}{l}
\therefore \frac{\mathrm{V}_{2}}{\mathrm{~V}_{1}}=\frac{\mathrm{A}_{1}}{\mathrm{~A}_{2}}=\frac{\mathrm{d}_{1}^{2}}{\mathrm{~d}_{2}^{2}} \\
\therefore \frac{\mathrm{d}_{2}^{2}}{\mathrm{~d}_{1}^{2}}=\frac{\mathrm{v}_{1}}{\mathrm{v}_{2}} \\
\therefore \frac{\mathrm{d}_{2}}{\mathrm{~d}_{1}}=\sqrt{\frac{\mathrm{v}_{1}}{\mathrm{v}_{2}}} \\
\therefore \mathrm{d}_{2}=\mathrm{d}_{1} \sqrt{\frac{\mathrm{v}_{1}}{\mathrm{v}_{2}}}=\mathrm{d} \sqrt{\frac{\mathrm{v}}{\mathrm{v}_{1}}}
\end{array}
\)
\(
\therefore \mathrm{A} \propto \mathrm{d}^{2}
\)
\(
\begin{array}{l}
\therefore \frac{\mathrm{V}_{2}}{\mathrm{~V}_{1}}=\frac{\mathrm{A}_{1}}{\mathrm{~A}_{2}}=\frac{\mathrm{d}_{1}^{2}}{\mathrm{~d}_{2}^{2}} \\
\therefore \frac{\mathrm{d}_{2}^{2}}{\mathrm{~d}_{1}^{2}}=\frac{\mathrm{v}_{1}}{\mathrm{v}_{2}} \\
\therefore \frac{\mathrm{d}_{2}}{\mathrm{~d}_{1}}=\sqrt{\frac{\mathrm{v}_{1}}{\mathrm{v}_{2}}} \\
\therefore \mathrm{d}_{2}=\mathrm{d}_{1} \sqrt{\frac{\mathrm{v}_{1}}{\mathrm{v}_{2}}}=\mathrm{d} \sqrt{\frac{\mathrm{v}}{\mathrm{v}_{1}}}
\end{array}
\)
\(
\therefore \mathrm{A} \propto \mathrm{d}^{2}
\)
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