June 2025 Paper 2 Q15
15 A particle moves under the actions of two forces, \(\mathbf{F}_1\) and \(\mathbf{F}_2\)
\(\mathbf{F}_1\) has magnitude 17 newtons and acts due East.
\(\mathbf{F}_2\) has magnitude 26 newtons and acts at a bearing of 310°
The resultant of \(\mathbf{F}_1\) and \(\mathbf{F}_2\) is \(\mathbf{R}\)
(a) Show that the magnitude of \(\mathbf{R}\) is 17.0 newtons, correct to three significant figures. [4 marks]
(b) Find the angle that \(\mathbf{R}\) makes with \(\mathbf{F}_1\)
Give your answer to the nearest degree.
[2 marks](c) A third force, \(\mathbf{F}_3\), acts upon the particle so that the particle is in equilibrium.
(i) State the magnitude of \(\mathbf{F}_3\) [1 mark]
(ii) State the bearing on which \(\mathbf{F}_3\) acts. [1 mark]
| Scheme | Marks | AO |
|---|---|---|
| Resolves horizontally or vertically to find a correct expression for one of the i or j components of the resultant force. Or Uses the cosine rule with b = 17 and c = 26 | M1 | 3.3 |
| Resolves horizontally and vertically to find a correct expression for both i and j components of the resultant force PI by H: AWRT \(\pm\) 2.9 V: AWRT \(\pm\)16.7 Or Uses the cosine rule to obtain a2 = AWRT 287.8 | A1 | 1.1b |
| Finds the magnitude of the resultant vector of their horizontal and vertical components Or Finds the square root of their expression for b2 + c2 − 2bcCosA PI by AWFW [16.96, 16.97] | M1 | 1.1a |
| Completes reasoned argument showing a full method to obtain AWFW [16.96, 16.97] and concludes that the magnitude of R is 17.0 Condone 17 AG | R1 | 2.1 |
| (4) |
Typical solution
Horizontally: \(17 - 26\cos(40)\)
\[= -2.917\ldots\]Vertically: \(26\sin(40)\)
\[= 16.712\ldots\]\[\sqrt{(-2.917)^2 + 16.712^2} = 16.97\ \text{N}\]\[\approx 17.0\ \text{N}\]| Scheme | Marks | AO |
|---|---|---|
| Uses an appropriate trigonometric equation using their components for R Or Deduces that the two 17N forces make this an isosceles triangle, eg: 180 − (2 x 40) PI AWRT 79 or 80 | M1 | 3.1a |
| Obtains any of the following angles AWRT 100, 101, \(\pm 259\), \(\pm 260\) | A1 | 1.1b |
| (2) |
Typical solution
\[\tan^{-1}\left(\frac{16.712}{2.917}\right) = 80^\circ\]\[180 - 80 = 100^\circ\]| Scheme | Marks | AO |
|---|---|---|
| (i) States 17.0 PI by AWRT 17 | B1 | 2.2a |
| (1) | ||
| (ii) States 170° PI by AWRT 170 | B1 | 2.2a |
| (1) | ||
| (8 marks) |
Typical solution
(c)(i)
17.0 N
(c)(ii)
170°