| Mass of the body, \(m\) | \(= 5\ \text{kg}\) |
| Force \(F_1\) | \(= 8\ \text{N}\) |
| Force \(F_2\) | \(= 6\ \text{N}\) |
| Angle between forces | \(= 90^\circ\) (perpendicular) |
Since the two forces are perpendicular, the magnitude of the resultant force \(F_R\) is:
\[ F_R = \sqrt{F_1^2 + F_2^2} \] \[ F_R = \sqrt{8^2 + 6^2} = \sqrt{64 + 36} = \sqrt{100} = 10\ \text{N} \]
Using Newton’s second law:
\[ a = \frac{F_R}{m} = \frac{10}{5} = 2\ \text{m s}^{-2} \]
Let \(\theta\) be the angle that the resultant (and hence acceleration) makes with the direction of the 8 N force.
\[ \tan\theta = \frac{F_2}{F_1} = \frac{6}{8} = \frac{3}{4} \] \[ \theta = \tan^{-1}\left(\frac{3}{4}\right) \approx 36.9^\circ \]
So the acceleration is at an angle of about \(37^\circ\) to the 8 N force, towards the 6 N force.
Magnitude of acceleration: \[ a = 2\ \text{m s}^{-2} \] Direction of acceleration: at \[ \theta \approx 37^\circ \] with the 8 N force, towards the 6 N force.
Find external force F so that block can move on inclined plane with constant velocity. 