Edexcel M4 2017 June — Question 5 9 marks

Exam BoardEdexcel
ModuleM4 (Mechanics 4)
Year2017
SessionJune
Marks9
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicVectors Introduction & 2D
TypeApparent wind problems
DifficultyChallenging +1.2 This is a standard M4 apparent wind problem requiring vector subtraction to find true wind from two apparent wind observations. While it involves multiple steps (setting up two vector equations, solving simultaneously using components), the method is well-practiced in M4 and follows a predictable template. The geometry is straightforward with standard compass bearings, making it moderately above average difficulty but not requiring novel insight.
Spec1.10a Vectors in 2D: i,j notation and column vectors1.10b Vectors in 3D: i,j,k notation1.10c Magnitude and direction: of vectors1.10d Vector operations: addition and scalar multiplication1.10g Problem solving with vectors: in geometry

5. A cyclist riding due north at a steady speed of \(12 \mathrm {~km} \mathrm {~h} ^ { - 1 }\) notices that the wind appears to come from the north-west. At the same time, another cyclist, moving on a bearing of \(120 ^ { \circ }\) and also riding at a steady speed of \(12 \mathrm {~km} \mathrm {~h} ^ { - 1 }\), notices that the wind appears to come from due south. The velocity of the wind is assumed to be constant. Find
  1. the wind speed,
  2. the direction from which the wind is blowing, giving your answer as a bearing.

AnswerMarks Guidance
One correct triangleB1
Two triangles combined using their common w. (seen or implied)B1
\(12\cos 30° = x\cos 45°\)M1 Horizontal components equal
\(x = 12\sqrt{\frac{3}{2}} (= 6\sqrt{6} = 14.6......)\)A1
\(w^2 = 12^2 + x^2 - 2 \times 12 \times \cos 45°\)M1 Cosine rule
\(w = 10.5 \text{ (km h}^{-1})\)A1
EITHER: Sine Rule: \(\frac{\sin\theta}{x} = \frac{\sin 45°}{w}\) or \(\frac{\sin\theta}{\sin 60°} = \frac{12}{w}\)M1
\(\theta = 81.2°\)A1
Direction 261°A1
OR: \(\uparrow w\cos\theta = 12 - 12\cos 30°\) \(\leftrightarrow w\sin\theta = 12\cos 30°\)
\(\Rightarrow \tan\theta = \frac{\cos 30°}{1 - \cos 30°}\)(M1)
\(\theta = 81.2°\)(A1)
Direction 261°(A1)
(9)
Question 5alt
AnswerMarks Guidance
\(\mathbf{w} = \begin{pmatrix} x\cos 45° \\ 12 - x\cos 45° \end{pmatrix}\)B1 w expressed as a vector
\(\mathbf{w} = \begin{pmatrix} 12\cos 30° \\ -12\sin 30° + y \end{pmatrix}\)B1 Second expression of w as a vector
\(12\cos 30° = x\cos 45°\)M1 Horizontal components equal
\(x\cos 45° = 6\sqrt{3}\)A1 Or \(x = 6\sqrt{6}\)
\(\\mathbf{w}\ ^2 = 3 \times 36 + (12 - 6\sqrt{3})^2\)
\(\\mathbf{w}\ = 10.5 \text{ (km h}^{-1})\)
\(\tan\theta = \frac{6\sqrt{3}}{12 - 6\sqrt{3}}\)M1 Correct method for direction of w
\(\theta = 81.2°\)A1
Direction 261°A1
(9) [9]
Question 6a
AnswerMarks Guidance
\(\frac{7e}{0.8} = 0.2g\)B1 \(T = mg\) at equilibrium (\(e = 0.224\))
\(0.2\ddot{x} = 0.2g - \frac{7(x+e)}{0.8} - 2v\)M1 Equation of motion. No missing/additional terms. Condone sign error(s). Allow with m and l
A1At most one error. m and l substituted
\(\left(0.2\ddot{x} = -\frac{7x}{0.8} - 2\dot{x}\right)\)A1 Correct unsimplified equation. m and l substituted
\(\ddot{x} + 10\dot{x} + 43.75x = 0\)A1 *given answer*
(5)
Question 6b
AnswerMarks Guidance
AE: \(m^2 + 10m + 43.75 = 0\), \(m = -5 \pm \frac{5\sqrt{3}}{2}\)M1 Form and solve AE
\(x = e^{-5t}\left(A\cos\frac{5\sqrt{3}}{2}t + B\sin\frac{5\sqrt{3}}{2}t\right)\)A1
\(t = 0, x = 0.2 \Rightarrow A = 0.2\)B1
\(\dot{x} = -5e^{-5t}(A\cos\omega t + B\sin\omega t) + e^{-5t}(-A\omega\sin\omega t + B\omega\cos\omega t)\)M1
\(0 = -5A + B\omega = -1 + B\omega\), \(B = \frac{2}{5\sqrt{3}}\)M1 Use of \(t = 0, \dot{x} = 0\) to find B
\(x = \frac{e^{-5t}}{5}\left(\cos\frac{5\sqrt{3}}{2}t + \frac{2}{\sqrt{3}}\sin\frac{5\sqrt{3}}{2}t\right)\)A1
(6)
Question 6c
AnswerMarks Guidance
instantaneous rest when \(t = \frac{\pi}{\omega}\) (s)M1 Use of periodic time \(= \frac{2\pi}{\omega}\)
\(= \frac{2\pi}{5\sqrt{3}} = 0.73\)A1
(2)
Question 6c alt
AnswerMarks Guidance
\(\dot{x} = -5e^{-5t}\left(\frac{1}{5}\cos\omega t + \frac{2}{5\sqrt{3}}\sin\omega t\right) + e^{-5t}\left(-\frac{1}{5}\omega\sin\omega t + \frac{2\omega}{5\sqrt{3}}\cos\omega t\right)\)
\(= 3e^{-5t}\sin\frac{5\sqrt{3}}{2}t = 0\)M1 Solve \(\dot{x} = 0\)
\(\Rightarrow \frac{5\sqrt{3}}{2}t = \pi\), \(t = \frac{2\pi}{5\sqrt{3}} = 0.73\text{s}\)A1
(2) [13]
Question 7a
AnswerMarks Guidance
PE of mass at C \(= -3mg \times 4a\cos\theta\)B1
PE of rods \(= -2mg \times a\cos\theta - 2mg \times 3a\cos\theta\)B1
Extension in the spring \(= 4a\cos\theta - 2a\)B1
\(\frac{7mg(4a\cos\theta - 2a)^2}{4a} - 20mga\cos\theta\)M1 Total PE
\(= 7mga(4\cos^2\theta - 4\cos\theta + 1) - 20mga\cos\theta\)
\(= 28mga\cos^2\theta - 48mga\cos\theta + \text{constant}\)A1 *given answer*
(5)
Question 7b
AnswerMarks Guidance
\(\frac{dV}{d\theta} = -56mga\cos\theta\sin\theta + 48mga\sin\theta\)M1 Differentiate
\(8\sin\theta(-7\cos\theta + 6) = 0\)M1 \(\frac{dV}{d\theta} = 0\) and solve for θ
\(\Rightarrow \theta = \cos^{-1}\frac{6}{7}(31°, 0.54r)\)A1
(4)
Question 7c
AnswerMarks Guidance
\(\frac{d^2V}{d\theta^2} = -56mga(\cos^2\theta - \sin^2\theta) + 48mga\cos\theta\)M1 Differentiate to obtain second derivative
\(= -56mga\left(2 \times \frac{36}{49} - 1\right) + 48mga \times \frac{6}{7}\)DM1 Find value of second derivative when \(\theta = \cos^{-1}\frac{6}{7}\). Dependent on preceding M1
\(= \frac{728}{49}mga > 0\), stableA1 (14.8...mga)
(4) [13]
| One correct triangle | B1 | |
| Two triangles combined using their common w. (seen or implied) | B1 | |
| $12\cos 30° = x\cos 45°$ | M1 | Horizontal components equal |
| $x = 12\sqrt{\frac{3}{2}} (= 6\sqrt{6} = 14.6......)$ | A1 | |
| $w^2 = 12^2 + x^2 - 2 \times 12 \times \cos 45°$ | M1 | Cosine rule |
| $w = 10.5 \text{ (km h}^{-1})$ | A1 | |
| EITHER: Sine Rule: $\frac{\sin\theta}{x} = \frac{\sin 45°}{w}$ or $\frac{\sin\theta}{\sin 60°} = \frac{12}{w}$ | M1 | |
| $\theta = 81.2°$ | A1 | |
| Direction 261° | A1 | |
| OR: $\uparrow w\cos\theta = 12 - 12\cos 30°$ $\leftrightarrow w\sin\theta = 12\cos 30°$ | | |
| $\Rightarrow \tan\theta = \frac{\cos 30°}{1 - \cos 30°}$ | (M1) | |
| $\theta = 81.2°$ | (A1) | |
| Direction 261° | (A1) | |
| | | (9) |

## Question 5alt

| $\mathbf{w} = \begin{pmatrix} x\cos 45° \\ 12 - x\cos 45° \end{pmatrix}$ | B1 | w expressed as a vector |
| $\mathbf{w} = \begin{pmatrix} 12\cos 30° \\ -12\sin 30° + y \end{pmatrix}$ | B1 | Second expression of w as a vector |
| $12\cos 30° = x\cos 45°$ | M1 | Horizontal components equal |
| $x\cos 45° = 6\sqrt{3}$ | A1 | Or $x = 6\sqrt{6}$ |
| $\|\mathbf{w}\|^2 = 3 \times 36 + (12 - 6\sqrt{3})^2$ | M1 | Use of Pythagoras |
| $\|\mathbf{w}\| = 10.5 \text{ (km h}^{-1})$ | A1 | |
| $\tan\theta = \frac{6\sqrt{3}}{12 - 6\sqrt{3}}$ | M1 | Correct method for direction of w |
| $\theta = 81.2°$ | A1 | |
| Direction 261° | A1 | |
| | | (9) [9] |

## Question 6a

| $\frac{7e}{0.8} = 0.2g$ | B1 | $T = mg$ at equilibrium ($e = 0.224$) |
| $0.2\ddot{x} = 0.2g - \frac{7(x+e)}{0.8} - 2v$ | M1 | Equation of motion. No missing/additional terms. Condone sign error(s). Allow with m and l |
| | A1 | At most one error. m and l substituted |
| $\left(0.2\ddot{x} = -\frac{7x}{0.8} - 2\dot{x}\right)$ | A1 | Correct unsimplified equation. m and l substituted |
| $\ddot{x} + 10\dot{x} + 43.75x = 0$ | A1 | *given answer* |
| | | (5) |

## Question 6b

| AE: $m^2 + 10m + 43.75 = 0$, $m = -5 \pm \frac{5\sqrt{3}}{2}$ | M1 | Form and solve AE |
| $x = e^{-5t}\left(A\cos\frac{5\sqrt{3}}{2}t + B\sin\frac{5\sqrt{3}}{2}t\right)$ | A1 | |
| $t = 0, x = 0.2 \Rightarrow A = 0.2$ | B1 | |
| $\dot{x} = -5e^{-5t}(A\cos\omega t + B\sin\omega t) + e^{-5t}(-A\omega\sin\omega t + B\omega\cos\omega t)$ | M1 | |
| $0 = -5A + B\omega = -1 + B\omega$, $B = \frac{2}{5\sqrt{3}}$ | M1 | Use of $t = 0, \dot{x} = 0$ to find B |
| $x = \frac{e^{-5t}}{5}\left(\cos\frac{5\sqrt{3}}{2}t + \frac{2}{\sqrt{3}}\sin\frac{5\sqrt{3}}{2}t\right)$ | A1 | |
| | | (6) |

## Question 6c

| instantaneous rest when $t = \frac{\pi}{\omega}$ (s) | M1 | Use of periodic time $= \frac{2\pi}{\omega}$ |
| $= \frac{2\pi}{5\sqrt{3}} = 0.73$ | A1 | |
| | | (2) |

## Question 6c alt

| $\dot{x} = -5e^{-5t}\left(\frac{1}{5}\cos\omega t + \frac{2}{5\sqrt{3}}\sin\omega t\right) + e^{-5t}\left(-\frac{1}{5}\omega\sin\omega t + \frac{2\omega}{5\sqrt{3}}\cos\omega t\right)$ | | |
| $= 3e^{-5t}\sin\frac{5\sqrt{3}}{2}t = 0$ | M1 | Solve $\dot{x} = 0$ |
| $\Rightarrow \frac{5\sqrt{3}}{2}t = \pi$, $t = \frac{2\pi}{5\sqrt{3}} = 0.73\text{s}$ | A1 | |
| | | (2) [13] |

## Question 7a

| PE of mass at C $= -3mg \times 4a\cos\theta$ | B1 | |
| PE of rods $= -2mg \times a\cos\theta - 2mg \times 3a\cos\theta$ | B1 | |
| Extension in the spring $= 4a\cos\theta - 2a$ | B1 | |
| $\frac{7mg(4a\cos\theta - 2a)^2}{4a} - 20mga\cos\theta$ | M1 | Total PE |
| $= 7mga(4\cos^2\theta - 4\cos\theta + 1) - 20mga\cos\theta$ | | |
| $= 28mga\cos^2\theta - 48mga\cos\theta + \text{constant}$ | A1 | *given answer* |
| | | (5) |

## Question 7b

| $\frac{dV}{d\theta} = -56mga\cos\theta\sin\theta + 48mga\sin\theta$ | M1 | Differentiate |
| $8\sin\theta(-7\cos\theta + 6) = 0$ | M1 | $\frac{dV}{d\theta} = 0$ and solve for θ |
| $\Rightarrow \theta = \cos^{-1}\frac{6}{7}(31°, 0.54r)$ | A1 | |
| | | (4) |

## Question 7c

| $\frac{d^2V}{d\theta^2} = -56mga(\cos^2\theta - \sin^2\theta) + 48mga\cos\theta$ | M1 | Differentiate to obtain second derivative |
| $= -56mga\left(2 \times \frac{36}{49} - 1\right) + 48mga \times \frac{6}{7}$ | DM1 | Find value of second derivative when $\theta = \cos^{-1}\frac{6}{7}$. Dependent on preceding M1 |
| $= \frac{728}{49}mga > 0$, stable | A1 | (14.8...mga) |
| | | (4) [13] |
5. A cyclist riding due north at a steady speed of $12 \mathrm {~km} \mathrm {~h} ^ { - 1 }$ notices that the wind appears to come from the north-west. At the same time, another cyclist, moving on a bearing of $120 ^ { \circ }$ and also riding at a steady speed of $12 \mathrm {~km} \mathrm {~h} ^ { - 1 }$, notices that the wind appears to come from due south. The velocity of the wind is assumed to be constant.

Find\\
(i) the wind speed,\\
(ii) the direction from which the wind is blowing, giving your answer as a bearing.

\hfill \mbox{\textit{Edexcel M4 2017 Q5 [9]}}