
To resolve this issue, we must examine the forces acting on the system. A horizontal force \( F \) is applied at the rope's midpoint, causing it to form a \( 45^\circ \) angle with the vertical, as illustrated in the accompanying image.
\(T_1 \cos(45^\circ) = mg\)
Given \( m = 1 \, \text{kg} \) and \( g = 10 \, \text{m/s}^2 \), we have:
\(T_1 \times \frac{1}{\sqrt{2}} = 1 \times 10\)
\(T_1 = 10 \sqrt{2} \, \text{N}\)
\(T_1 \sin(45^\circ) = F\)
Substituting the value of \( T_1 \):
\(10 \sqrt{2} \times \frac{1}{\sqrt{2}} = F\)
\(F = 10 \, \text{N}\)
Consequently, the correct answer is \( 10 \, \text{N} \).

