To solve this problem, we will apply principles from fluid mechanics and the physics of motion under gravity.
Step 1: Calculate the terminal velocity of the ball in water
For a sphere moving through a fluid, the terminal velocity \( v_t \) can be calculated using the formula for Stokes' Law:
\(v_t = \frac{2r^2 (\rho - \rho_w)g}{9\eta}\)
Substituting these values into the formula gives:
\(v_t = \frac{2 \times (1 \times 10^{-4})^2 \times (10^5 - 1000) \times 9.8}{9 \times 9.8 \times 10^{-6}}\)
Calculating this yields approximations for simplification:
\(v_t = \frac{2 \times 10^{-8} \times 99000 \times 9.8}{88.2 \times 10^{-6}} \approx 22 \, \text{m/s}\)
Step 2: Use energy conservation to find \( h \)
The ball falls freely under gravity and so its potential energy converts to kinetic energy before entering the water:
\(mgh = \frac{1}{2} mv_t^2\)
Where \( m \) is the mass of the ball, and \( v_t \) is the terminal velocity.
Cancelling \( m \) from both sides gives:
\(gh = \frac{1}{2}v_t^2\)
Hence,
\(h = \frac{v_t^2}{2g}\)
Substitute the known values:
\(h = \frac{22^2}{2 \times 9.8} \approx 2518 \, \text{m}\)
Conclusion: The height \( h \) from which the ball must fall is approximately 2518 m. Therefore, the correct answer is 2518 m.
The terminal velocity \( V_T \) of the spherical ball in water is given by Stokes' law:
\[ V_T = \frac{2gR^2}{9\eta} (\rho_B - \rho_L), \]
where:
Substitute the values into the formula:
\[ V_T = \frac{2 \cdot 9.8 \cdot (1 \times 10^{-4})^2}{9 \cdot 9.8 \times 10^{-6}} (10^5 - 10^3). \]
\[ V_T = \frac{2}{9} \cdot \frac{10 \cdot (10^{-4})^2}{9.8 \times 10^{-6}} \cdot (10^5 - 10^3), \]
\[ V_T = \frac{2}{9} \cdot \frac{10 \cdot 10^{-8}}{9.8 \times 10^{-6}} \cdot (10^5 - 10^3), \]
\[ V_T = \frac{2}{9} \cdot \frac{10}{9.8} \cdot 10^2 = 224.5 \, \text{m/s}. \]
\[ V = \sqrt{2gh}. \]
Rearranging for \( h \):
\[ h = \frac{V^2}{2g}. \]
Substitute \( V_T = 224.5 \, \text{m/s} \) and \( g = 9.8 \, \text{m/s}^2 \):
\[ h = \frac{(224.5)^2}{2 \cdot 9.8}. \]
\[ h = \frac{50402.25}{19.6} \approx 2571 \, \text{m}. \]
Thus, the height \( h \) is approximately:
\[ \boxed{2518 \, \text{m}}. \]
Inductance of a coil with \(10^4\) turns is \(10\,\text{mH}\) and it is connected to a DC source of \(10\,\text{V}\) with internal resistance \(10\,\Omega\). The energy density in the inductor when the current reaches \( \left(\frac{1}{e}\right) \) of its maximum value is \[ \alpha \pi \times \frac{1}{e^2}\ \text{J m}^{-3}. \] The value of \( \alpha \) is _________.
\[ (\mu_0 = 4\pi \times 10^{-7}\ \text{TmA}^{-1}) \]
A small block of mass \(m\) slides down from the top of a frictionless inclined surface, while the inclined plane is moving towards left with constant acceleration \(a_0\). The angle between the inclined plane and ground is \(\theta\) and its base length is \(L\). Assuming that initially the small block is at the top of the inclined plane, the time it takes to reach the lowest point of the inclined plane is _______. 