OCR MEI M3 2010 June — Question 4 18 marks

Exam BoardOCR MEI
ModuleM3 (Mechanics 3)
Year2010
SessionJune
Marks18
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicSimple Harmonic Motion
TypeProve motion is SHM from equation
DifficultyStandard +0.3 Part (i) is a straightforward differentiation exercise to verify SHM (2 differentiations). Part (ii) involves routine substitution of initial conditions into three equations. Parts (iii)-(v) require standard SHM formulas and understanding of amplitude/period, but are mostly procedural applications. This is a typical M3/mechanics module question testing standard SHM techniques with no novel insight required, making it slightly easier than average overall.
Spec4.10f Simple harmonic motion: x'' = -omega^2 x

4 A particle P is performing simple harmonic motion in a vertical line. At time \(t \mathrm {~s}\), its displacement \(x \mathrm {~m}\) above a fixed point O is given by $$x = A \sin \omega t + B \cos \omega t$$ where \(A , B\) and \(\omega\) are constants.
  1. Show that the acceleration of P , in \(\mathrm { ms } ^ { - 2 }\), is \(- \omega ^ { 2 } x\). When \(t = 0 , \mathrm { P }\) is 16 m below O , moving with velocity \(7.5 \mathrm {~m} \mathrm {~s} ^ { - 1 }\) upwards, and has acceleration \(1 \mathrm {~m} \mathrm {~s} ^ { - 2 }\) upwards.
  2. Find the values of \(A , B\) and \(\omega\).
  3. Find the maximum displacement, the maximum speed, and the maximum acceleration of P .
  4. Find the speed and the direction of motion of P when \(t = 15\).
  5. Find the distance travelled by P between \(t = 0\) and \(t = 15\).

Question 4:
Part (i)
AnswerMarks Guidance
Answer/WorkingMark Guidance
\(v = \frac{dx}{dt} = A\omega\cos\omega t - B\omega\sin\omega t\)B1
\(a = \frac{d^2x}{dt^2} = -A\omega^2\sin\omega t - B\omega^2\cos\omega t\)M1 Finding the second derivative
\(= -\omega^2(A\sin\omega t + B\cos\omega t) = -\omega^2 x\)E1 Correctly shown
Part (ii)
AnswerMarks Guidance
Answer/WorkingMark Guidance
\(B = -16\)B1
\(\omega = 0.25\)B1
\(A = 30\)B2 When \(A\) is wrong, give B1 for a correct equation involving \(A\) [e.g. \(A\omega = 7.5\) or \(7.5^2 = \omega^2(A^2 + B^2 - 16^2)\)] or for \(A = -30\)
Part (iii)
AnswerMarks Guidance
Answer/WorkingMark Guidance
Maximum displacement is \((\pm)\sqrt{A^2 + B^2}\)M1 Or \(7.5^2 = \omega^2(\text{amp}^2 - 16^2)\); or finding \(t\) when \(v=0\) and substituting to find \(x\)
Maximum displacement is \(34\) mA1
Maximum speed is \((\pm)34\omega\)M1 For either (any valid method)
Maximum acceleration is \((\pm)34\omega^2\)
Maximum speed is \(8.5\ \text{ms}^{-1}\)F1 Only ft from \(\omega \times \text{amp}\)
Maximum acceleration is \(2.125\ \text{ms}^{-2}\)F1 Only ft from \(\omega^2 \times \text{amp}\)
Part (iv)
AnswerMarks Guidance
Answer/WorkingMark Guidance
\(v = 7.5\cos 0.25t + 4\sin 0.25t\)
When \(t=15\): \(v = 7.5\cos 3.75 + 4\sin 3.75 = -8.44\)M1
Speed is \(8.44\ \text{ms}^{-1}\) (3 sf); downwardsA1
Part (v)
AnswerMarks Guidance
Answer/WorkingMark Guidance
Period \(\frac{2\pi}{\omega} \approx 25\) s, so \(t=0\) to \(t=15\) is less than one period
When \(t=15\): \(x = 30\sin 3.75 - 16\cos 3.75 = -4.02\)M1
Distance travelled is \(16 + 34 + 34 + 4.02\)M1 Take account of change of direction
M1Fully correct strategy for distance
Distance travelled is \(88.0\) m (3 sf)A1 cao
# Question 4:

## Part (i)
| Answer/Working | Mark | Guidance |
|---|---|---|
| $v = \frac{dx}{dt} = A\omega\cos\omega t - B\omega\sin\omega t$ | B1 | |
| $a = \frac{d^2x}{dt^2} = -A\omega^2\sin\omega t - B\omega^2\cos\omega t$ | M1 | Finding the second derivative |
| $= -\omega^2(A\sin\omega t + B\cos\omega t) = -\omega^2 x$ | E1 | Correctly shown |

## Part (ii)
| Answer/Working | Mark | Guidance |
|---|---|---|
| $B = -16$ | B1 | |
| $\omega = 0.25$ | B1 | |
| $A = 30$ | B2 | When $A$ is wrong, give B1 for a correct equation involving $A$ [e.g. $A\omega = 7.5$ or $7.5^2 = \omega^2(A^2 + B^2 - 16^2)$] or for $A = -30$ |

## Part (iii)
| Answer/Working | Mark | Guidance |
|---|---|---|
| Maximum displacement is $(\pm)\sqrt{A^2 + B^2}$ | M1 | Or $7.5^2 = \omega^2(\text{amp}^2 - 16^2)$; or finding $t$ when $v=0$ and substituting to find $x$ |
| Maximum displacement is $34$ m | A1 | |
| Maximum speed is $(\pm)34\omega$ | M1 | For either (any valid method) |
| Maximum acceleration is $(\pm)34\omega^2$ | | |
| Maximum speed is $8.5\ \text{ms}^{-1}$ | F1 | Only ft from $\omega \times \text{amp}$ |
| Maximum acceleration is $2.125\ \text{ms}^{-2}$ | F1 | Only ft from $\omega^2 \times \text{amp}$ |

## Part (iv)
| Answer/Working | Mark | Guidance |
|---|---|---|
| $v = 7.5\cos 0.25t + 4\sin 0.25t$ | | |
| When $t=15$: $v = 7.5\cos 3.75 + 4\sin 3.75 = -8.44$ | M1 | |
| Speed is $8.44\ \text{ms}^{-1}$ (3 sf); downwards | A1 | |

## Part (v)
| Answer/Working | Mark | Guidance |
|---|---|---|
| Period $\frac{2\pi}{\omega} \approx 25$ s, so $t=0$ to $t=15$ is less than one period | | |
| When $t=15$: $x = 30\sin 3.75 - 16\cos 3.75 = -4.02$ | M1 | |
| Distance travelled is $16 + 34 + 34 + 4.02$ | M1 | Take account of change of direction |
| | M1 | Fully correct strategy for distance |
| Distance travelled is $88.0$ m (3 sf) | A1 cao | |
4 A particle P is performing simple harmonic motion in a vertical line. At time $t \mathrm {~s}$, its displacement $x \mathrm {~m}$ above a fixed point O is given by

$$x = A \sin \omega t + B \cos \omega t$$

where $A , B$ and $\omega$ are constants.\\
(i) Show that the acceleration of P , in $\mathrm { ms } ^ { - 2 }$, is $- \omega ^ { 2 } x$.

When $t = 0 , \mathrm { P }$ is 16 m below O , moving with velocity $7.5 \mathrm {~m} \mathrm {~s} ^ { - 1 }$ upwards, and has acceleration $1 \mathrm {~m} \mathrm {~s} ^ { - 2 }$ upwards.\\
(ii) Find the values of $A , B$ and $\omega$.\\
(iii) Find the maximum displacement, the maximum speed, and the maximum acceleration of P .\\
(iv) Find the speed and the direction of motion of P when $t = 15$.\\
(v) Find the distance travelled by P between $t = 0$ and $t = 15$.

\hfill \mbox{\textit{OCR MEI M3 2010 Q4 [18]}}