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9709 · 4.1

Forces and equilibrium — practice questions

Practice and worked examples for 9709 Forces and equilibrium. Short previews only — attempt the full question in MarkScheme against the official scheme.

Worked example 1

A particle is held in equilibrium by three forces, F1\mathbf{F}_1, F2\mathbf{F}_2 and F3\mathbf{F}_3. Given that F1=(6i−2j)\mathbf{F}_1 = (6\mathbf{i} - 2\mathbf{j}) N and F2=(−2i+5j)\mathbf{F}_2 = (-2\mathbf{i} + 5\mathbf{j}) N, find the force F3\mathbf{F}_3 and calculate its magnitude and the angle it makes with the positive x-axis.

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For the particle to be in equilibrium, the vector sum of the forces must be zero.
F1+F2+F3=0\mathbf{F}_1 + \mathbf{F}_2 + \mathbf{F}_3 = \mathbf{0}
(6i−2j)+(−2i+5j)+F3=0(6\mathbf{i} - 2\mathbf{j}) + (-2\mathbf{i} + 5\mathbf{j}) + \mathbf{F}_3 = \mathbf{0}
(4i+3j)+F3=0(4\mathbf{i} + 3\mathbf{j}) + \mathbf{F}_3 = \mathbf{0}
F3=−4i−3j\mathbf{F}_3 = -4\mathbf{i} - 3\mathbf{j} N.\

To find the magnitude of F3\mathbf{F}_3:
∣F3∣=(−4)2+(−3)2=16+9=25=5|\mathbf{F}_3| = \sqrt{(-4)^2 + (-3)^2} = \sqrt{16 + 9} = \sqrt{25} = 5 N.\

To find the angle, let's first find the angle α\alpha the vector makes with the negative x-axis in the third quadrant.
tan⁡α=oppositeadjacent=34\tan \alpha = \frac{\text{opposite}}{\text{adjacent}} = \frac{3}{4}
α=tan⁡−1(0.75)≈36.9∘\alpha = \tan^{-1}(0.75) \approx 36.9^\circ.
This angle is measured from the negative x-axis into the third quadrant. The angle measured anti-clockwise from the positive x-axis is θ=180∘+36.9∘=216.9∘\theta = 180^\circ + 36.9^\circ = 216.9^\circ.
Alternatively, the angle is −(180∘−36.9∘)=−143.1∘- (180^\circ - 36.9^\circ) = -143.1^\circ from the positive x-axis. Both 217∘217^\circ and −143∘-143^\circ (to 3 s.f.) are acceptable answers.

Worked example 2

A block of mass 20 kg rests on a rough plane inclined at 25∘25^\circ to the horizontal. The coefficient of friction between the block and the plane is 0.3. A force of magnitude PP N acts on the block, parallel to a line of greatest slope. Find the range of possible values of PP for the block to remain in equilibrium. (Use g=9.8 m s−2g = 9.8 \text{ m s}^{-2})

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First, draw a free-body diagram and resolve the weight (20g20g N) into components parallel and perpendicular to the plane.
Weight component perpendicular to plane: W⊥=20gcos⁡(25∘)W_\perp = 20g \cos(25^\circ).
Weight component parallel to plane: W∥=20gsin⁡(25∘)W_\parallel = 20g \sin(25^\circ).\

Step 1: Find the normal reaction, R. Resolve forces perpendicular to the plane.
∑F⊥=0  ⟹  R−20gcos⁡(25∘)=0\sum F_\perp = 0 \implies R - 20g \cos(25^\circ) = 0
R=20(9.8)cos⁡(25∘)=196×0.9063...=177.63...R = 20(9.8) \cos(25^\circ) = 196 \times 0.9063... = 177.63... N.\

Step 2: Find the maximum possible frictional force, FmaxF_{max}.
Fmax=μR=0.3×177.63...=53.29...F_{max} = \mu R = 0.3 \times 177.63... = 53.29... N.\

Step 3: Find the maximum value of P (PmaxP_{max}). This occurs when the block is about to slide UP the plane, so friction acts DOWN the plane.
Resolve forces parallel to the plane: ∑F∥=0\sum F_\parallel = 0
Pmax−W∥−Fmax=0P_{max} - W_\parallel - F_{max} = 0
Pmax=20gsin⁡(25∘)+FmaxP_{max} = 20g \sin(25^\circ) + F_{max}
Pmax=20(9.8)sin⁡(25∘)+53.29...P_{max} = 20(9.8) \sin(25^\circ) + 53.29...
Pmax=196×0.4226...+53.29...=82.83...+53.29...=136.12...P_{max} = 196 \times 0.4226... + 53.29... = 82.83... + 53.29... = 136.12... N.\

Step 4: Find the minimum value of P (PminP_{min}). This occurs when the block is about to slide DOWN the plane, so friction acts UP the plane.
Resolve forces parallel to the plane: ∑F∥=0\sum F_\parallel = 0
Pmin+Fmax−W∥=0P_{min} + F_{max} - W_\parallel = 0
Pmin=W∥−FmaxP_{min} = W_\parallel - F_{max}
Pmin=82.83...−53.29...=29.54...P_{min} = 82.83... - 53.29... = 29.54... N.\

Step 5: State the final answer.
The block remains in equilibrium if 29.5≤P≤13629.5 \le P \le 136. (Values given to 3 significant figures).