OCR C4 — Question 8 16 marks

Exam BoardOCR
ModuleC4 (Core Mathematics 4)
Marks16
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicHarmonic Form
TypeFind value where max/min occurs
DifficultyStandard +0.3 This is a multi-part geometry/trigonometry question that systematically builds up complexity. Parts (i)-(iii) involve standard angle-chasing and differentiation of trigonometric expressions, while part (iv) is a routine harmonic form conversion (R sin(θ-α)) commonly practiced in C3/C4. The question guides students through each step with clear instructions and 'show that' scaffolding, making it slightly easier than average despite the 16 total marks.
Spec1.05b Sine and cosine rules: including ambiguous case1.05n Harmonic form: a sin(x)+b cos(x) = R sin(x+alpha) etc

In Fig. 6, OAB is a thin bent rod, with OA = \(a\) metres, AB = \(b\) metres and angle OAB = 120°. 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. \includegraphics{figure_6}
  1. Find angle BAC in terms of \(\theta\). Hence show that $$h = a\sin\theta + b\sin(\theta - 60°).$$ [3]
  2. Hence show that \(h = (a + \frac{1}{2}b)\sin\theta - \frac{\sqrt{3}}{2}b\cos\theta\). [3]
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.
  1. Show that OB is horizontal when \(\tan\theta = \frac{\sqrt{3}b}{2a + b}\). [3]
In the case when \(a = 1\) and \(b = 2\), \(h = 2\sin\theta - \sqrt{3}\cos\theta\).
  1. 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 \(\theta\). [7]

Question 8:
AnswerMarks Guidance
8(i) BAC = 120 – 90 – (90 – θ)
= θ – 60
 BC = b sin(θ – 60)
CD = AE = a sin θ
AnswerMarks
 h = BC + CD = a sin θ + b sin (θ – 60°) *B1
M1
E1
[3]
AnswerMarks
(ii)h = a sin θ + b sin (θ – 60°)
= a sin θ + b (sinθ cos 60 – cosθ sin 60)
= a sin θ + ½ b sin θ − √3/2 b cos θ
1 3
=(a+ b)sinθ− bcosθ*
AnswerMarks
2 2M1
M1
E1
AnswerMarks
[3]corr compound angle formula
sin 60 = √3/2, cos 60 = ½
used
AnswerMarks
(iii)OB horizontal when h = 0
1 3
 (a+ b)sinθ− bcosθ=0
2 2
1 3
 (a+ b)sinθ= bcosθ
2 2
3
b
sinθ 2
 =
cosθ 1
a+ b
2
3b
 tanθ= *
AnswerMarks
2a+bM1
M1
E1
AnswerMarks
[3]sinθ
=tanθ
cosθ
AnswerMarks
(iv)2sinθ− 3cosθ= Rsin(θ−α)
= R(sinθcosα−cosθsinα)
 R cos α = 2, R sin α = √3
 R2 = 22 + (√3)2 = 7, R = √7 = 2.646 m
tan α = √3/2, α = 40.9°
So h = √7 sin(θ – 40.9°)
 h = √7 = 2.646 m
max
when θ – 40.9° = 90°
AnswerMarks
 θ = 130.9°M1
B1
M1A1
B1ft
M1
A1
[7]
1 3
(a+ b)sinθ= bcosθ
2 2
3
b
sinθ 2
=
cosθ 1
a+ b
2
3b
tanθ=
2a+b
2sinθ− 3cosθ= Rsin(θ−α)
= R(sinθcosα−cosθsinα)
9(i) cosθ 3 sin+θ= r cos(θ −α)
=Rcosθcosα+Rsinθsinα
⇒Rcosα=1, Rsinα= 3
⇒ R2 = 12 + (√3)2 = 4, R = 2
tan α = √3
AnswerMarks
⇒ α = π/3B1
M1
M1
A1
AnswerMarks
[4]R = 2
equating correct pairs
tan α = √3 o.e.
(ii) derivative of tan θ is sec2θ
π 1 π 1 π
∫ 3 dθ=∫ 3 sec2(θ− )dθ
0 (cosθ+ 3sinθ)2 0 4 3
π
⎡1 π ⎤3
= tan(θ− )
⎢ ⎥
⎣4 3 ⎦
0
= ¼ (0 – (–√3))
AnswerMarks
= √3/4 *B1
M1
A1
E1
AnswerMarks
[4]ft their α
1
[tan (θ – π/3] ft their R,α(in radians)
R2
www
Question 8:
8 | (i) | BAC = 120 – 90 – (90 – θ)
= θ – 60
 BC = b sin(θ – 60)
CD = AE = a sin θ
 h = BC + CD = a sin θ + b sin (θ – 60°) * | B1
M1
E1
[3]
(ii) | h = a sin θ + b sin (θ – 60°)
= a sin θ + b (sinθ cos 60 – cosθ sin 60)
= a sin θ + ½ b sin θ − √3/2 b cos θ
1 3
=(a+ b)sinθ− bcosθ*
2 2 | M1
M1
E1
[3] | corr compound angle formula
sin 60 = √3/2, cos 60 = ½
used
(iii) | OB horizontal when h = 0
1 3
 (a+ b)sinθ− bcosθ=0
2 2
1 3
 (a+ b)sinθ= bcosθ
2 2
3
b
sinθ 2
 =
cosθ 1
a+ b
2
3b
 tanθ= *
2a+b | M1
M1
E1
[3] | sinθ
=tanθ
cosθ
(iv) | 2sinθ− 3cosθ= Rsin(θ−α)
= R(sinθcosα−cosθsinα)
 R cos α = 2, R sin α = √3
 R2 = 22 + (√3)2 = 7, R = √7 = 2.646 m
tan α = √3/2, α = 40.9°
So h = √7 sin(θ – 40.9°)
 h = √7 = 2.646 m
max
when θ – 40.9° = 90°
 θ = 130.9° | M1
B1
M1A1
B1ft
M1
A1
[7]
1 3
(a+ b)sinθ= bcosθ
2 2
3
b
sinθ 2
=
cosθ 1
a+ b
2
3b
tanθ=
2a+b
2sinθ− 3cosθ= Rsin(θ−α)
= R(sinθcosα−cosθsinα)
9(i) cosθ 3 sin+θ= r cos(θ −α)
=Rcosθcosα+Rsinθsinα
⇒Rcosα=1, Rsinα= 3
⇒ R2 = 12 + (√3)2 = 4, R = 2
tan α = √3
⇒ α = π/3 | B1
M1
M1
A1
[4] | R = 2
equating correct pairs
tan α = √3 o.e.
(ii) derivative of tan θ is sec2θ
π 1 π 1 π
∫ 3 dθ=∫ 3 sec2(θ− )dθ
0 (cosθ+ 3sinθ)2 0 4 3
π
⎡1 π ⎤3
= tan(θ− )
⎢ ⎥
⎣4 3 ⎦
0
= ¼ (0 – (–√3))
= √3/4 * | B1
M1
A1
E1
[4] | ft their α
1
[tan (θ – π/3] ft their R,α(in radians)
R2
www
In Fig. 6, OAB is a thin bent rod, with OA = $a$ metres, AB = $b$ metres and angle OAB = 120°. 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.

\includegraphics{figure_6}

\begin{enumerate}[label=(\roman*)]
\item Find angle BAC in terms of $\theta$. Hence show that
$$h = a\sin\theta + b\sin(\theta - 60°).$$ [3]
\item Hence show that $h = (a + \frac{1}{2}b)\sin\theta - \frac{\sqrt{3}}{2}b\cos\theta$. [3]
\end{enumerate}

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.

\begin{enumerate}[label=(\roman*)]
\setcounter{enumi}{2}
\item Show that OB is horizontal when $\tan\theta = \frac{\sqrt{3}b}{2a + b}$. [3]
\end{enumerate}

In the case when $a = 1$ and $b = 2$, $h = 2\sin\theta - \sqrt{3}\cos\theta$.

\begin{enumerate}[label=(\roman*)]
\setcounter{enumi}{3}
\item 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 $\theta$. [7]
\end{enumerate}

\hfill \mbox{\textit{OCR C4  Q8 [16]}}