The force acting on the block is given by:
\[ F = -20x + 10. \]
Using Newton’s second law, \( F = ma \), where \( m = 5 \) kg:
\[ a = \frac{F}{m} = \frac{-20x + 10}{5} = -4x + 2. \]
At equilibrium, \( a = 0 \):
\[ -4x + 2 = 0 \Rightarrow x = 0.5 \text{ m}. \]
This is the **mean position (M.P.)** of the block.
For small oscillations about the equilibrium position:
\[ a = -4(x - 0.5). \]
Comparing with the standard SHM equation \( a = -\omega^2 x \), we get:
\[ \omega^2 = 4 \Rightarrow \omega = 2 \text{ rad/s}. \]
The general equation of motion is:
\[ x = 0.5 + A \cos(\omega t). \]
At \( t = 0 \), \( x = 1 \) m:
\[ 1 = 0.5 + A \Rightarrow A = 0.5. \]
Thus, the position function becomes:
\[ x = 0.5 + 0.5 \cos(2t). \]
\[ x = 0.5 + 0.5 \cos\left(2 \times \frac{\pi}{4}\right) = 0.5 + 0.5 \cdot 0 = 0.5 \text{ m}. \]
The velocity is given by:
\[ v = \frac{dx}{dt} = -0.5 \cdot 2 \sin(2t) = -\sin(2t). \]
At \( t = \frac{\pi}{4} \):
\[ v = -\sin\left(2 \times \frac{\pi}{4}\right) = -\sin\left(\frac{\pi}{2}\right) = -1 \text{ m/s}. \]
Momentum is given by:
\[ p = m \cdot v = 5 \times (-1) = -5 \text{ kg m/s}. \]