To find the viscosity of the oil, we can use Stokes' Law, which relates the drag force experienced by a sphere moving through a viscous fluid to its radius, speed, and the fluid's viscosity. The formula for terminal velocity under the influence of gravity for a sphere in a viscous medium is given by:
\[v_t = \frac{2}{9} \frac{r^2 ( \rho_s - \rho_f ) g}{\eta}\]where:
We are given:
First, calculate the radius of the sphere:
\(r = \frac{3.6 \times 10^{-3}}{2} \, \text{m} = 1.8 \times 10^{-3} \, \text{m}\)
Substitute these values into the terminal velocity equation and solve for the viscosity (\(\eta\)):
\[2.45 \times 10^{-2} = \frac{2}{9} \times \frac{(1.8 \times 10^{-3})^2 \times (7825 - 925) \times 9.8}{\eta}\]Rearrange to solve for \(\eta\):
\[\eta = \frac{2}{9} \times \frac{(1.8 \times 10^{-3})^2 \times (7825 - 925) \times 9.8}{2.45 \times 10^{-2}}\]Calculating the values inside the equation:
Substitute these into the equation:
\[\eta = \frac{2 \times 3.24 \times 10^{-6} \times 6900 \times 9.8}{9 \times 2.45 \times 10^{-2}}\]After solving, the viscosity of the oil (\(\eta\)) is approximately:
\(1.99 \, \text{Pa s}\)
Therefore, the correct answer is 1.99.
The terminal velocity \( v_T \) of a sphere falling through a viscous fluid is given by Stokes' Law: \[ v_T = \frac{2 r^2 (\rho_s - \rho_l) g}{9 \eta} \] where \( r \) is the radius of the sphere, \( \rho_s \) is the density of the sphere (steel), \( \rho_l \) is the density of the liquid (oil), \( g \) is the acceleration due to gravity, and \( \eta \) is the viscosity of the liquid.
Given:
Diameter of the steel ball \( d = 3.6 \, \text{mm} = 3.6 \times 10^{-3} \, \text{m} \)
Radius of the steel ball \( r = \frac{d}{2} = \frac{3.6 \times 10^{-3}}{2} = 1.8 \times 10^{-3} \, \text{m} \)
Terminal velocity \( v_T = 2.45 \times 10^{-2} \, \text{m/s} \) Density of oil \( \rho_l = 925 \, \text{kg m}^{-3} \)
Density of steel \( \rho_s = 7825 \, \text{kg m}^{-3} \)
Acceleration due to gravity \( g = 9.8 \, \text{m/s}^2 \)
We need to find the viscosity \( \eta \) of the oil.
Rearranging the formula for terminal velocity: \[ \eta = \frac{2 r^2 (\rho_s - \rho_l) g}{9 v_T} \]
Substituting the given values: \[ \eta = \frac{2 (1.8 \times 10^{-3})^2 (7825 - 925) (9.8)}{9 (2.45 \times 10^{-2})} \] \[ \eta = \frac{2 (3.24 \times 10^{-6}) (6900) (9.8)}{9 (2.45 \times 10^{-2})} \] \[ \eta = \frac{2 \times 3.24 \times 10^{-6} \times 6900 \times 9.8}{0.2205} \] \[ \eta = \frac{0.436512}{0.2205} \] \[ \eta \approx 1.98 \, \text{Pa s} \] The viscosity of the oil is approximately 1.98 Pa s, which is close to 1.99.
A flexible chain of mass $m$ is hanging as shown. Find tension at the lowest point. 

In the given figure, the blocks $A$, $B$ and $C$ weigh $4\,\text{kg}$, $6\,\text{kg}$ and $8\,\text{kg}$ respectively. The coefficient of sliding friction between any two surfaces is $0.5$. The force $\vec{F}$ required to slide the block $C$ with constant speed is ___ N.
(Given: $g = 10\,\text{m s}^{-2}$) 
Two circular discs of radius \(10\) cm each are joined at their centres by a rod, as shown in the figure. The length of the rod is \(30\) cm and its mass is \(600\) g. The mass of each disc is also \(600\) g. If the applied torque between the two discs is \(43\times10^{-7}\) dyne·cm, then the angular acceleration of the system about the given axis \(AB\) is ________ rad s\(^{-2}\).
