When a block of mass \(m\) is placed on an inclined plane with angle of inclination \(\theta\), the gravitational force (\(mg\)) acting vertically downwards can be resolved into two components:
(1) Perpendicular to the plane: \(mg \cos\theta\) (balanced by the normal force).
(2) Parallel to the plane, downwards: \(mg \sin\theta\).
To keep the block in equilibrium (i.
e.
, prevent it from sliding down) on a frictionless incline, an external force must be applied upwards along the plane that exactly balances the downward component of gravity.
Force required (\(F_{req}\)) = Component of gravity parallel to the plane
$$ F_{req} = mg \sin\theta $$
Given:
Mass \(m = 5\) kg
Angle \(\theta = 30^\circ\)
Acceleration due to gravity \(g \approx 9.
8\) m/s\(^2\) (standard value if not given)
\(\sin 30^\circ = 0.
5\)
Substitute the values:
$$ F_{req} = (5 \, \text{kg}) \times (9.
8 \, \text{m/s}^2) \times \sin(30^\circ) $$
$$ F_{req} = 5 \times 9.
8 \times 0.
5 \, \text{N} $$
$$ F_{req} = 5 \times (4)9 \, \text{N} = 2(4)5 \, \text{N} $$
The force required to keep the block in equilibrium is 2(4)5 N.