The viscous drag acting on a metal sphere of diameter \(1\) mm, falling through a fluid of viscosity \(0.8\) Pa-s with a velocity of \(2\) m s–1 is nearly equal to:
1.
\(15\times 10^{-3}~\text{N}\)
2.
\(30\times 10^{-3}~\text{N}\)
3.
\(1.5\times 10^{-3}~\text{N}\)
4.
\(20\times 10^{-3}~\text{N}\)
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Subtopic: Stokes' Law |
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NEET - 2023
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The terminal velocity of a copper ball of radius \(5~\text{mm}\) falling through a tank of oil at room temperature is \(10~\text{cm}~\text{s}^{-1}\) . If the viscosity of oil at room temperature is \(0.9~\text{kg}~\text{m}^{-1}~\text{s}^{-1}\), the viscous drag force is:
1.
\(8.48 \times10^{-3}\) N
2.
\(8.48 \times10^{-5}\) N
3.
\(4.23 \times10^{-3}\)N
4.
\(4.23 \times10^{-6}\) N
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Subtopic: Stokes' Law |
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NEET - 2022
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