To solve this problem, we need to use the conservation of mechanical energy principle as the force involved is conservative and there is no energy loss due to friction.
The mechanical energy in a spring-mass system is the sum of kinetic energy (due to motion) and potential energy (stored in the spring).
The initial configuration of the system is when the spring is compressed to 1 m, and the block is released from rest.
Substituting the known values:
\(100 + 0 = \frac{1}{2} \times 200 \times (2 - x)^2 + \frac{1}{2} \times 2 \times v^2\)
Simplifying for \(v^2\):
\(100 = 100 (2 - x)^2 + v^2\) \(v^2 = 100 - 100 (2 - x)^2\) \(v^2 = 100 [1 - (2 - x)^2]\)
Thus, the speed \(v\) is:
\(v = 10 \sqrt{1 - (2 - x)^2}\)
Therefore, the speed of the block at a distance \(x\) from the wall is \(10 \left[ 1 - (2 - x)^2 \right]^{1/2} \, \text{m/s}\), which matches the correct option.
The total mechanical energy is the sum of the potential energy stored in the spring and the kinetic energy of the block. The potential energy \( U \) stored in a spring is given by: \( U = \frac{1}{2} k (x_{\text{spring}})^2 \),
where \( k = 200 \, \text{N/m} \) is the spring constant, and \( x_{\text{spring}} \) is the displacement from the natural length of the spring. The initial displacement of the spring is 1 m (the block is compressed), so the initial potential energy is:
\( U_{\text{initial}} = \frac{1}{2} \times 200 \times (2 - 1)^2 = 100 \, \text{J} \).
The total mechanical energy of the system is constant and is the sum of the kinetic energy \( K = \frac{1}{2} m v^2 \) and the potential energy stored in the spring at any point during the motion.<br>
The total energy \( E \) is given by:
\( E = K + U \).
At any position \( x \), the total energy is:
\( E = \frac{1}{2} m v^2 + \frac{1}{2} k (2 - x)^2 \).
Since the total mechanical energy is conserved and the initial energy is all potential energy, we have:
\( 100 = \frac{1}{2} \times 2 \times v^2 + \frac{1}{2} \times 200 \times (2 - x)^2 \).
Simplifying:
\( 100 = v^2 + 200 (2 - x)^2 \).
Solving for \( v \):
\( v^2 = 100 - 200 (2 - x)^2 \),
\( v = 10 \left[ 1 - (2 - x)^2 \right]^{1/2} \, \text{m/s} \).
Thus, the speed of the block at distance \( x \) from the wall is:
\( \boxed{10 \left[ 1 - (2 - x)^2 \right]^{1/2}} \, \text{m/s} \).
Therefore, the correct answer is Option (3).
