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 cube of side 10 cm is suspended from one end of a fine string of length 27 cm, and a mass of 200 grams is connected to the other end of the string. When the cube is half immersed in water, the system remains in balance. Find the density of the cube.
