The correct answer is option (C): \((\frac{4}{3})^{n-1}V_0\)
We are analyzing a sequence of elastic collisions where each ball is lighter than the previous one.
Let the initial velocity of the first ball be \(v_1 = v\) and the second ball be at rest: \(v_2 = 0\).
Using the velocity formula after elastic collision:
\(v_2' = \frac{2m_1}{m_1 + m_2}v_1 + \frac{m_2 - m_1}{m_1 + m_2}v_2\)
Given \(m_2 = \frac{m}{2}\) and \(v_2 = 0\),
\(v_2' = \frac{2m}{m + \frac{m}{2}}v = \frac{2m}{\frac{3m}{2}}v = \frac{4}{3}v\)
Now this ball hits a third ball with mass \(m_3 = \frac{m}{4}\), again initially at rest.
By similar logic, velocity after next collision:
\(v_3' = \frac{2m_2}{m_2 + m_3}v_2' = \frac{2 \cdot \frac{m}{2}}{\frac{m}{2} + \frac{m}{4}} \cdot \frac{4}{3}v = \frac{4}{3} \cdot \frac{4}{3}v = \left(\frac{4}{3}\right)^2 v\)
So, by this pattern, after the \(n^\text{th}\) collision:
\(v_n = \left(\frac{4}{3}\right)^{n-1}v = \left(\frac{4}{3}\right)^{n-1}V_0\)
Therefore, the final velocity of the \(n^\text{th}\) ball is:
\(\boxed{\left(\frac{4}{3}\right)^{n-1}V_0}\)
Suppose collision of two balls is as follows :
By conservation of momentum:
\(mv_0 = mv_1 + \frac{m}{2}v_2\)
\(\Rightarrow v_0 = v_1 + \frac{v_2}{2} \quad \text{...(i)}\)
For elastic collision: \(e = 1 = \frac{v_2 - v_1}{v_0 - 0}\)
\(\Rightarrow v_0 = v_2 - v_1 \quad \text{...(ii)}\)
From equations (i) and (ii):
Add both equations:
\(v_0 + v_0 = v_1 + \frac{v_2}{2} + v_2 - v_1 = \frac{3v_2}{2}\)
\(\Rightarrow 2v_0 = \frac{3v_2}{2}\)
\(\Rightarrow v_2 = \frac{4v_0}{3}\)
Similarly, the velocity of the 3rd ball:
\(v_3 = \left(\frac{4}{3}\right)^2 v_0\)
Therefore, velocity of the \(n^\text{th}\) ball:
\(v_n = \left(\frac{4}{3}\right)^{n-1} v_0\)
So, the correct option is (C): \(\left(\frac{4}{3}\right)^{n-1} V_0\)
A block of certain mass is placed on a rough floor. The coefficients of static and kinetic friction between the block and the floor are 0.4 and 0.25 respectively. A constant horizontal force \( F = 20 \, \text{N} \) acts on it so that the velocity of the block varies with time according to the following graph. The mass of the block is nearly (Take \( g = 10 \, \text{m/s}^2 \)):
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