The block experiences frictional force due to the roughness of the inclined surface. The kinetic friction force \( f_k \) is given by:
\[ f_k = \mu mg \cos \theta, \]where \( \mu = 0.1 \) is the coefficient of friction, \( m = 5 \, \text{kg} \), and \( \theta = 30^\circ \).
Calculating \( f_k \):
\[ f_k = 0.1 \times 5 \times 10 \times \cos 30^\circ = 0.1 \times 50 \times \frac{\sqrt{3}}{2} = 2.5 \sqrt{3} \, \text{N}. \]To move the block up the incline, the force \( F_1 \) must overcome both the component of gravitational force along the incline and the frictional force. Therefore:
\[ F_1 = mg \sin \theta + f_k. \]Substitute the values:
\[ F_1 = 5 \times 10 \times \sin 30^\circ + 2.5 \sqrt{3} = 25 + 2.5 \sqrt{3} \, \text{N}. \]To prevent the block from sliding down, the force \( F_2 \) must balance the component of gravitational force along the incline, reduced by the frictional force. Thus:
\[ F_2 = mg \sin \theta - f_k. \]Substitute the values:
\[ F_2 = 25 - 2.5 \sqrt{3} \, \text{N}. \]The difference \( |F_1 - F_2| \) is:
\[ |F_1 - F_2| = |(25 + 2.5 \sqrt{3}) - (25 - 2.5 \sqrt{3})| = 5 \sqrt{3} \, \text{N}. \]Thus, the answer is:
\[ 5 \sqrt{3} \, \text{N}. \]The portion of the line \( 4x + 5y = 20 \) in the first quadrant is trisected by the lines \( L_1 \) and \( L_2 \) passing through the origin. The tangent of an angle between the lines \( L_1 \) and \( L_2 \) is: