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:
\[ 5 \sqrt{3} \, \text{N}. \]List-I | List-II | ||
P | The capacitance between S1 and S4, with S2 and S3 not connected, is | I | \(3C_0\) |
Q | The capacitance between S1 and S4, with S2 shorted to S3, is | II | \(\frac{C_0}{2}\) |
R | The capacitance between S1 and S3, with S2 shorted to S4, is | III | \(\frac{C_0}{3}\) |
S | The capacitance between S1 and S2, with S3 shorted to S1, and S2 shorted to S4, is | IV | \(2\frac{C_0}{3}\) |
\[2C_0\] |
A body of mass 1000 kg is moving horizontally with a velocity of 6 m/s. If 200 kg extra mass is added, the final velocity (in m/s) is: