OCR MEI M3 2012 June — Question 3 18 marks

Exam BoardOCR MEI
ModuleM3 (Mechanics 3)
Year2012
SessionJune
Marks18
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicSimple Harmonic Motion
TypeProve motion is SHM from equation
DifficultyModerate -0.3 Part (i) is a straightforward differentiation exercise showing SHM definition (2 marks). Parts (ii)-(v) involve reading values from a graph and applying standard SHM formulas. While multi-part with several marks, all techniques are routine for M3 students with no novel problem-solving required. Slightly easier than average due to the mechanical nature of the tasks.
Spec4.10f Simple harmonic motion: x'' = -omega^2 x

3 A particle Q is performing simple harmonic motion in a vertical line. Its height, \(x\) metres, above a fixed level at time \(t\) seconds is given by $$x = c + A \cos ( \omega t - \phi )$$ where \(c , A , \omega\) and \(\phi\) are constants.
  1. Show that \(\ddot { x } = - \omega ^ { 2 } ( x - c )\). Fig. 3 shows the displacement-time graph of Q for \(0 \leqslant t \leqslant 14\). \begin{figure}[h]
    \includegraphics[alt={},max width=\textwidth]{86dd0c01-970d-4b67-9a6c-5df276a4a2be-4_547_1079_703_495} \captionsetup{labelformat=empty} \caption{Fig. 3}
    \end{figure}
  2. Find exact values for \(c , A , \omega\) and \(\phi\).
  3. Find the maximum speed of Q .
  4. Find the height and the velocity of Q when \(t = 0\).
  5. Find the distance travelled by Q between \(t = 0\) and \(t = 14\).

Question 3(i):
AnswerMarks Guidance
AnswerMarks Guidance
\(\dot{x} = -A\omega\sin(\omega t - \phi)\)B1
\(\ddot{x} = -A\omega^2\cos(\omega t - \phi)\)M1 Obtaining second derivative; allow one error
\(\ddot{x} = -\omega^2(x - c)\)E1 [3] Correctly shown
Question 3(ii):
AnswerMarks Guidance
AnswerMarks Guidance
\(c = 10\)B1
\(A = 6\)B1 Accept \(A = -6\)
\(\frac{2\pi}{\omega} = 10\)M1 Using \(\frac{2\pi}{\omega}\); or other complete method for finding \(\omega\)
\(\omega = \frac{\pi}{5}\)A1 Accept \(\omega = -\frac{\pi}{5}\); allow \(\frac{2\pi}{10}\) etc
\(x = 16\) when \(t = 3 \Rightarrow 3\omega - \phi = 0\)M1 Obtaining simple relationship between \(\phi\) and \(\omega\); NB \(\phi = 3\) is M0; or \(x = 10 + 6\cos\{\frac{\pi}{5}(t-3)\}\)
\(\phi = \frac{3\pi}{5}\)A1 [6] NB other values possible; if exact values not seen give A0A1 for both \(\omega = 0.63\) and \(\phi = 1.9\); e.g. \(\phi = -\frac{7\pi}{5}\), \(\phi = \frac{13\pi}{5}\), \(x = 10 - 6\cos(\frac{\pi}{5}t - \frac{8\pi}{5})\) etc; max 5/6 if values not consistent
Question 3(iii):
AnswerMarks Guidance
AnswerMarks Guidance
Maximum speed is \(A\omega\)M1 Or e.g. evaluating \(\dot{x}\) when \(t = 5.5\)
Maximum speed is \(\frac{6\pi}{5}\) or \(3.77\ \text{ms}^{-1}\) (3 sf)A1 [2] FT is \(
Question 3(iv):
AnswerMarks Guidance
AnswerMarks Guidance
When \(t = 0\), height is \(8.15\) m (3 sf)B1 FT is \(c + A\cos\phi\) (provided \(4 < x < 16\)); must use radians
\(v = -\frac{6\pi}{5}\sin(\frac{\pi t}{5} - \frac{3\pi}{5})\)M1 Or \(v^2 = \left(\frac{\pi}{5}\right)^2(6^2 - 1.854^2)\); allow one error in differentiation
When \(t = 0\), velocity is \(3.59\ \text{ms}^{-1}\) (3 sf)A1 [3] FT is \(A\omega\sin\phi\) (must be positive); \((\phi = 3\) gives \(x = 4.06\), \(v = 0.532)\)
Question 3(v):
AnswerMarks Guidance
AnswerMarks Guidance
When \(t = 0\), \(x = 8.146\) Correct FT value, or evidence of substitution, required \((\phi = 3\) gives \(x = 15.3)\)
When \(t = 14\), \(x = 14.854\)M1 Finding \(x\) when \(t = 14\); requires \(4 < x(14) < 16\)
\((16 - 14.854)\) usedM1 Also requires \(4 < x(0) < 16\)
\((16 - 8.146) + 12 + 12 + (16 - 14.854)\)M1 Fully correct strategy
Distance is \(33\) mA1 [4] CAO
## Question 3(i):

| Answer | Marks | Guidance |
|--------|-------|----------|
| $\dot{x} = -A\omega\sin(\omega t - \phi)$ | B1 | |
| $\ddot{x} = -A\omega^2\cos(\omega t - \phi)$ | M1 | Obtaining second derivative; allow one error |
| $\ddot{x} = -\omega^2(x - c)$ | E1 [3] | Correctly shown |

---

## Question 3(ii):

| Answer | Marks | Guidance |
|--------|-------|----------|
| $c = 10$ | B1 | |
| $A = 6$ | B1 | Accept $A = -6$ |
| $\frac{2\pi}{\omega} = 10$ | M1 | Using $\frac{2\pi}{\omega}$; or other complete method for finding $\omega$ |
| $\omega = \frac{\pi}{5}$ | A1 | Accept $\omega = -\frac{\pi}{5}$; allow $\frac{2\pi}{10}$ etc |
| $x = 16$ when $t = 3 \Rightarrow 3\omega - \phi = 0$ | M1 | Obtaining simple relationship between $\phi$ and $\omega$; NB $\phi = 3$ is M0; or $x = 10 + 6\cos\{\frac{\pi}{5}(t-3)\}$ |
| $\phi = \frac{3\pi}{5}$ | A1 [6] | NB other values possible; if exact values not seen give A0A1 for both $\omega = 0.63$ and $\phi = 1.9$; e.g. $\phi = -\frac{7\pi}{5}$, $\phi = \frac{13\pi}{5}$, $x = 10 - 6\cos(\frac{\pi}{5}t - \frac{8\pi}{5})$ etc; max 5/6 if values not consistent |

---

## Question 3(iii):

| Answer | Marks | Guidance |
|--------|-------|----------|
| Maximum speed is $A\omega$ | M1 | Or e.g. evaluating $\dot{x}$ when $t = 5.5$ |
| Maximum speed is $\frac{6\pi}{5}$ or $3.77\ \text{ms}^{-1}$ (3 sf) | A1 [2] | FT is $|A\omega|$ (must be positive) |

---

## Question 3(iv):

| Answer | Marks | Guidance |
|--------|-------|----------|
| When $t = 0$, height is $8.15$ m (3 sf) | B1 | FT is $c + A\cos\phi$ (provided $4 < x < 16$); must use radians |
| $v = -\frac{6\pi}{5}\sin(\frac{\pi t}{5} - \frac{3\pi}{5})$ | M1 | Or $v^2 = \left(\frac{\pi}{5}\right)^2(6^2 - 1.854^2)$; allow one error in differentiation |
| When $t = 0$, velocity is $3.59\ \text{ms}^{-1}$ (3 sf) | A1 [3] | FT is $A\omega\sin\phi$ (must be positive); $(\phi = 3$ gives $x = 4.06$, $v = 0.532)$ |

---

## Question 3(v):

| Answer | Marks | Guidance |
|--------|-------|----------|
| When $t = 0$, $x = 8.146$ | | Correct FT value, or evidence of substitution, required $(\phi = 3$ gives $x = 15.3)$ |
| When $t = 14$, $x = 14.854$ | M1 | Finding $x$ when $t = 14$; requires $4 < x(14) < 16$ |
| $(16 - 14.854)$ used | M1 | Also requires $4 < x(0) < 16$ |
| $(16 - 8.146) + 12 + 12 + (16 - 14.854)$ | M1 | Fully correct strategy |
| Distance is $33$ m | A1 [4] | CAO |

---
3 A particle Q is performing simple harmonic motion in a vertical line. Its height, $x$ metres, above a fixed level at time $t$ seconds is given by

$$x = c + A \cos ( \omega t - \phi )$$

where $c , A , \omega$ and $\phi$ are constants.\\
(i) Show that $\ddot { x } = - \omega ^ { 2 } ( x - c )$.

Fig. 3 shows the displacement-time graph of Q for $0 \leqslant t \leqslant 14$.

\begin{figure}[h]
\begin{center}
  \includegraphics[alt={},max width=\textwidth]{86dd0c01-970d-4b67-9a6c-5df276a4a2be-4_547_1079_703_495}
\captionsetup{labelformat=empty}
\caption{Fig. 3}
\end{center}
\end{figure}

(ii) Find exact values for $c , A , \omega$ and $\phi$.\\
(iii) Find the maximum speed of Q .\\
(iv) Find the height and the velocity of Q when $t = 0$.\\
(v) Find the distance travelled by Q between $t = 0$ and $t = 14$.

\hfill \mbox{\textit{OCR MEI M3 2012 Q3 [18]}}