To determine the terminal velocity attained by the small metallic sphere when dropped in glycerine, we can use Stokes' Law, which relates the drag force experienced by a sphere moving through a viscous fluid to its velocity. According to Stokes' Law, the drag force (\(F_d\)) is given by:
\(F_d = 6 \pi \eta r v\)
where:
At terminal velocity, the drag force is equal to the net gravitational force acting on the sphere. The gravitational force (\(F_g\)) is given by the difference between the weight of the sphere and the buoyant force:
\(F_g = V (\rho_{sphere} - \rho_{fluid}) g\)
where:
For a sphere of diameter 2 mm, the radius \(r\) is 1 mm or 0.1 cm.
The volume \(V\) of the sphere (using the formula for the volume of a sphere \(\frac{4}{3} \pi r^3\)) is:
\(V = \frac{4}{3} \pi (0.1)^3 = \frac{4}{3} \times \frac{22}{7} \times 0.001\) cm3
\(V = \frac{88}{21} \times 0.001 = 0.000419 cm^3\)
Substituting the densities: \(\rho_{sphere} = 10.5\) g/cm3, \(\rho_{fluid} = 1.5\) g/cm3, and \(g = 1000\) cm/s2 (since 1 m/s2 = 100 cm/s2), the net force \(F_g\) becomes:
\(F_g = 0.000419 \times (10.5 - 1.5) \times 1000 = 0.000419 \times 9 \times 1000 = 3.771\)
Using \(\eta = 10\) Poise = 1 Pa·s:
Equating \(F_d\) and \(F_g\) for terminal velocity:
\(6 \pi \times 1 \times 0.1 \times v = 3.771\)
\(6 \times \frac{22}{7} \times 0.1 \times v = 3.771\)cm/s
Therefore, the terminal velocity attained by the sphere is 2.0 cm/s, which matches option two.
A wooden cubical block of relative density 0.4 is floating in water. Side of cubical block is $10 \text{ cm}$. When a coin is placed on the block, it dips by $0.3 \text{ cm}$, weight of coin is: