| Exam Board | OCR MEI |
|---|---|
| Module | C4 (Core Mathematics 4) |
| Marks | 16 |
| Paper | Download PDF ↗ |
| Mark scheme | Download PDF ↗ |
| Topic | Addition & Double Angle Formulae |
| Type | Applied context with trigonometry |
| Difficulty | Standard +0.3 This is a structured multi-part question testing standard C4 content (addition formulae, double angle identities, and R-formula). Each part guides students through the solution with clear scaffolding. The geometry requires careful angle-chasing but is straightforward, and the trigonometric manipulations are routine textbook exercises. Slightly easier than average due to the extensive scaffolding. |
| Spec | 1.05b Sine and cosine rules: including ambiguous case1.05c Area of triangle: using 1/2 ab sin(C)1.05d Radians: arc length s=r*theta and sector area A=1/2 r^2 theta1.05l Double angle formulae: and compound angle formulae1.05n Harmonic form: a sin(x)+b cos(x) = R sin(x+alpha) etc |
| Answer | Marks |
|---|---|
| \(\text{BAC} = 120 - 90 - (90 - \theta) = \theta - 60\) | B1 |
| \(\text{BC} = b \sin(\theta - 60)\) | M1 |
| \(\text{CD} = \text{AE} = a \sin \theta\) | E1 |
| \(h = \text{BC} + \text{CD} = a \sin \theta + b \sin(\theta - 60°)\) | [3] |
| Answer | Marks |
|---|---|
| \(h = a \sin \theta + b \sin(\theta - 60°)\) | M1 |
| Answer | Marks |
|---|---|
| \(= a \sin \theta + b(\sin\theta \cos 60 - \cos\theta \sin 60)\) | M1 |
| Answer | Marks |
|---|---|
| \(= a \sin \theta + \frac{1}{2}b \sin \theta - \frac{\sqrt{3}}{2}b \cos \theta\) | E1 |
| \(= \left(a + \frac{1}{2}b\right) \sin\theta - \frac{\sqrt{3}}{2}b \cos\theta\) | [3] |
| Answer | Marks |
|---|---|
| OB horizontal when \(h = 0\) | M1 |
| \(\left(a + \frac{1}{2}b\right) \sin\theta - \frac{\sqrt{3}}{2}b \cos\theta = 0\) | M1 |
| \(\left(a + \frac{1}{2}b\right) \sin\theta = \frac{\sqrt{3}}{2}b \cos\theta\) | |
| \(\frac{\sin\theta}{\cos\theta} = \tan\theta\) | |
| \(\tan\theta = \frac{\frac{\sqrt{3}}{2}b}{a + \frac{1}{2}b} = \frac{\sqrt{3}b}{2a + b}\) | E1 |
| Answer | Marks |
|---|---|
| \(2\sin\theta - \sqrt{3}\cos\theta = R\sin(\theta - \alpha)\) | M1 |
| \(= R(\sin\theta \cos\alpha - \cos\theta \sin\alpha)\) | |
| \(R \cos \alpha = 2\), \(R \sin \alpha = \sqrt{3}\) | B1 |
| \(R^2 = 2^2 + (\sqrt{3})^2 = 7\), \(R = \sqrt{7} = 2.646\) m | M1A1 |
| \(\tan \alpha = \frac{\sqrt{3}}{2}\), \(\alpha = 40.9°\) | B1ft |
| So \(h = \sqrt{7} \sin(\theta - 40.9°)\) | |
| \(h_{\max} = \sqrt{7} = 2.646\) m when \(\theta - 40.9° = 90°\) | M1 |
| \(\theta = 130.9°\) | A1 |
| Answer | Marks |
|---|---|
| \(2\sin\theta - \sqrt{3}\cos\theta = R\sin(\theta - \alpha)\) | M1 |
| \(= R(\sin\theta \cos\alpha - \cos\theta \sin\alpha)\) | |
| \(3\cos\theta + 4\sin\theta = R\cos(\theta - \alpha)\) | |
| \(= R(\cos\theta \cos\alpha + \sin\theta \sin\alpha)\) | |
| \(\Rightarrow R \cos \alpha = 3\), \(R \sin \alpha = 4\) | B1 |
| \(\Rightarrow R^2 = 3^2 + 4^2 = 25 \Rightarrow R = 5\) | M1A1 |
| \(\tan \alpha = \frac{4}{3} \Rightarrow \alpha = 0.9273\) | |
| \(5\cos(\theta - 0.9273) = 2\) | M1 |
| \(\cos(\theta - 0.9273) = \frac{2}{5}\) | |
| \(\theta - 0.9273 = 1.1593, -1.1593\) | A1 |
| \(\theta = 2.087, -0.232\) | A1 |
| \(R = 5\) cwo and no others in the range | [7] |
# Question 1
## (i)
$\text{BAC} = 120 - 90 - (90 - \theta) = \theta - 60$ | B1
$\text{BC} = b \sin(\theta - 60)$ | M1
$\text{CD} = \text{AE} = a \sin \theta$ | E1
$h = \text{BC} + \text{CD} = a \sin \theta + b \sin(\theta - 60°)$ | [3]
## (ii)
$h = a \sin \theta + b \sin(\theta - 60°)$ | M1
correct compound angle formula
$= a \sin \theta + b(\sin\theta \cos 60 - \cos\theta \sin 60)$ | M1
$\sin 60 = \frac{\sqrt{3}}{2}$, $\cos 60 = \frac{1}{2}$ used
$= a \sin \theta + \frac{1}{2}b \sin \theta - \frac{\sqrt{3}}{2}b \cos \theta$ | E1
$= \left(a + \frac{1}{2}b\right) \sin\theta - \frac{\sqrt{3}}{2}b \cos\theta$ | [3]
## (iii)
OB horizontal when $h = 0$ | M1
$\left(a + \frac{1}{2}b\right) \sin\theta - \frac{\sqrt{3}}{2}b \cos\theta = 0$ | M1
$\left(a + \frac{1}{2}b\right) \sin\theta = \frac{\sqrt{3}}{2}b \cos\theta$ |
$\frac{\sin\theta}{\cos\theta} = \tan\theta$ |
$\tan\theta = \frac{\frac{\sqrt{3}}{2}b}{a + \frac{1}{2}b} = \frac{\sqrt{3}b}{2a + b}$ | E1
[3]
## (iv)
$2\sin\theta - \sqrt{3}\cos\theta = R\sin(\theta - \alpha)$ | M1
$= R(\sin\theta \cos\alpha - \cos\theta \sin\alpha)$ |
$R \cos \alpha = 2$, $R \sin \alpha = \sqrt{3}$ | B1
$R^2 = 2^2 + (\sqrt{3})^2 = 7$, $R = \sqrt{7} = 2.646$ m | M1A1
$\tan \alpha = \frac{\sqrt{3}}{2}$, $\alpha = 40.9°$ | B1ft
So $h = \sqrt{7} \sin(\theta - 40.9°)$ |
$h_{\max} = \sqrt{7} = 2.646$ m when $\theta - 40.9° = 90°$ | M1
$\theta = 130.9°$ | A1
[7]
---
$2\sin\theta - \sqrt{3}\cos\theta = R\sin(\theta - \alpha)$ | M1
$= R(\sin\theta \cos\alpha - \cos\theta \sin\alpha)$ |
$3\cos\theta + 4\sin\theta = R\cos(\theta - \alpha)$ |
$= R(\cos\theta \cos\alpha + \sin\theta \sin\alpha)$ |
$\Rightarrow R \cos \alpha = 3$, $R \sin \alpha = 4$ | B1
$\Rightarrow R^2 = 3^2 + 4^2 = 25 \Rightarrow R = 5$ | M1A1
$\tan \alpha = \frac{4}{3} \Rightarrow \alpha = 0.9273$ |
$5\cos(\theta - 0.9273) = 2$ | M1
$\cos(\theta - 0.9273) = \frac{2}{5}$ |
$\theta - 0.9273 = 1.1593, -1.1593$ | A1
$\theta = 2.087, -0.232$ | A1
$R = 5$ cwo and no others in the range | [7]
1 In Fig. 6, OAB is a thin bent rod, with $\mathrm { OA } = a$ metres, $\mathrm { AB } = b$ metres and angle $\mathrm { OAB } = 120 ^ { \circ }$. The bent rod lies in a vertical plane. OA makes an angle $\theta$ above the horizontal. The vertical height BD of B above O is $h$ metres. The horizontal through A meets BD at C and the vertical through A meets OD at E .
\begin{figure}[h]
\begin{center}
\includegraphics[alt={},max width=\textwidth]{9ac55ae6-7a7f-47d0-a363-92da179be4ca-1_427_898_464_683}
\captionsetup{labelformat=empty}
\caption{Fig. 6}
\end{center}
\end{figure}
(i) Find angle BAC in terms of $\theta$. Hence show that
$$h = a \sin \theta + b \sin \left( \theta - 60 ^ { \circ } \right) .$$
(ii) Hence show that $h = \left( a + \frac { 1 } { 2 } b \right) \sin \theta - \frac { \sqrt { 3 } } { 2 } b \cos \theta$.
The rod now rotates about O , so that $\theta$ varies. You may assume that the formulae for $h$ in parts (i) and (ii) remain valid.\\
(iii) Show that OB is horizontal when $\tan \theta = \frac { \sqrt { 3 } b } { 2 a + b }$.
In the case when $a = 1$ and $b = 2 , h = 2 \sin \theta - \sqrt { 3 } \cos \theta$.\\
(iv) Express $2 \sin \theta - \sqrt { 3 } \cos \theta$ in the form $R \sin ( \theta - \alpha )$. Hence, for this case, write down the maximum value of $h$ and the corresponding value of $\theta$.
\hfill \mbox{\textit{OCR MEI C4 Q1 [16]}}