OCR MEI M1 2005 January — Question 6 19 marks

Exam BoardOCR MEI
ModuleM1 (Mechanics 1)
Year2005
SessionJanuary
Marks19
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicConstant acceleration (SUVAT)
TypeParticle moving through liquid or resistance
DifficultyModerate -0.8 This is a straightforward M1 mechanics question requiring basic SUVAT application, reading values from a speed-time graph, calculating areas under graphs, and simple integration. All parts are routine textbook exercises with no problem-solving insight required—easier than average A-level maths.
Spec3.02c Interpret kinematic graphs: gradient and area3.02d Constant acceleration: SUVAT formulae3.02f Non-uniform acceleration: using differentiation and integration3.02h Motion under gravity: vector form

6 In this question take \(g\) as \(10 \mathrm {~m \mathrm {~s} ^ { - 2 }\).} A small ball is released from rest. It falls for 2 seconds and is then brought to rest over the next 5 seconds. This motion is modelled in the speed-time graph Fig. 6. \begin{figure}[h]
\includegraphics[alt={},max width=\textwidth]{c84a748a-a6f4-48c5-b864-fe543569bdf5-5_659_1105_578_493} \captionsetup{labelformat=empty} \caption{Fig. 6}
\end{figure} For this model,
  1. calculate the distance fallen from \(t = 0\) to \(t = 7\),
  2. find the acceleration of the ball from \(t = 2\) to \(t = 6\), specifying the direction,
  3. obtain an expression in terms of \(t\) for the downward speed of the ball from \(t = 2\) to \(t = 6\),
  4. state the assumption that has been made about the resistance to motion from \(t = 0\) to \(t = 2\). The part of the motion from \(t = 2\) to \(t = 7\) is now modelled by \(v = - \frac { 3 } { 2 } t ^ { 2 } + \frac { 19 } { 2 } t + 7\).
  5. Verify that \(v\) agrees with the values given in Fig. 6 at \(t = 2 , t = 6\) and \(t = 7\).
  6. Calculate the distance fallen from \(t = 2\) to \(t = 7\) according to this model.

Part (i)
AnswerMarks Guidance
Area under curve \(0.5 \times 2 \times 20 + 0.5 \times (20 + 10) \times 4 + 0.5 \times 10 \times 1 = 85\) mM1 Attempt to find any area under curve or use const accn results
B1Any area correct (Accept 20 or 60 or 5 without explanation)
A1cao
Total: 3
Part (ii)
AnswerMarks Guidance
\(\frac{20 - 10}{4} = 2.5\) upwardsM1 \(\Delta v / \Delta t\)
A1accept \(\pm 2.5\)
B1Accept – 2.5 downwards (allow direction specified by diagram etc). Accept 'opposite direction to motion'.
Total: 3
Part (iii)
AnswerMarks Guidance
\(v = -2.5t + c\)M1 Allow their \(a\) in the form \(v = \pm at + c\) or \(v = \pm a(t - 2) + c\)
\(v = 20\) when \(t = 2\)M1
\(v = -2.5t + 25\)A1 cao [Allow \(v = 20 - 2.5(t - 2)\)] [Allow 2/3 for different variable to \(t\) used, e.g. \(x\). Allow any variable name for speed]
Total: 3
Part (iv)
AnswerMarks Guidance
Falling with negligible resistanceE1 Accept 'zero resistance', or 'no resistance' seen.
Total: 1
Part (v)
AnswerMarks Guidance
\(-1.5 \times 4 + 9.5 \times 2 + 7 = 20\)E1 One of the results shown
\(-1.5 \times 36 + 9.5 \times 6 + 7 = 10\)E1
\(-1.5 \times 49 + 9.5 \times 7 + 7 = 0\)E1 All three shown. Be generous about the 'show'.
Total: 2
Part (vi)
AnswerMarks Guidance
\(\int_2^7 (-1.5t^2 + 9.5t + 7) dt\)M1 Limits not required
\(= [-0.5t^3 + 4.75t^2 + 7t]_2^7\)A1 A1 for each term. Limits not required. Condone \(+ c\)
A1
\(= \left( -\frac{343}{2} - \frac{19 \times 49}{4} + 49 \right) - (-4 + 19 + 14)\)M1 Attempt to use both limits on an integrated expression
A1Correct substitution in their expression including subtraction (may be left as an expression).
\(= 81.25\) mA1 cao.
Total: 7
**Part (i)**

| Area under curve $0.5 \times 2 \times 20 + 0.5 \times (20 + 10) \times 4 + 0.5 \times 10 \times 1 = 85$ m | M1 | Attempt to find any area under curve or use const accn results |
| | B1 | Any area correct (Accept 20 or 60 or 5 without explanation) |
| | A1 | cao |
| | | **Total: 3** |

**Part (ii)**

| $\frac{20 - 10}{4} = 2.5$ upwards | M1 | $\Delta v / \Delta t$ |
| | A1 | accept $\pm 2.5$ |
| | B1 | Accept – 2.5 downwards (allow direction specified by diagram etc). Accept 'opposite direction to motion'. |
| | | **Total: 3** |

**Part (iii)**

| $v = -2.5t + c$ | M1 | Allow their $a$ in the form $v = \pm at + c$ or $v = \pm a(t - 2) + c$ |
| $v = 20$ when $t = 2$ | M1 | |
| $v = -2.5t + 25$ | A1 | cao [Allow $v = 20 - 2.5(t - 2)$] [Allow 2/3 for different variable to $t$ used, e.g. $x$. Allow any variable name for speed] |
| | | **Total: 3** |

**Part (iv)**

| Falling with negligible resistance | E1 | Accept 'zero resistance', or 'no resistance' seen. |
| | | **Total: 1** |

**Part (v)**

| $-1.5 \times 4 + 9.5 \times 2 + 7 = 20$ | E1 | One of the results shown |
| $-1.5 \times 36 + 9.5 \times 6 + 7 = 10$ | E1 | |
| $-1.5 \times 49 + 9.5 \times 7 + 7 = 0$ | E1 | All three shown. Be generous about the 'show'. |
| | | **Total: 2** |

**Part (vi)**

| $\int_2^7 (-1.5t^2 + 9.5t + 7) dt$ | M1 | Limits not required |
| $= [-0.5t^3 + 4.75t^2 + 7t]_2^7$ | A1 | A1 for each term. Limits not required. Condone $+ c$ |
| | A1 | |
| $= \left( -\frac{343}{2} - \frac{19 \times 49}{4} + 49 \right) - (-4 + 19 + 14)$ | M1 | Attempt to use both limits on an integrated expression |
| | A1 | Correct substitution in their expression including subtraction (may be left as an expression). |
| $= 81.25$ m | A1 | cao. |
| | | **Total: 7** |

---
6 In this question take $g$ as $10 \mathrm {~m \mathrm {~s} ^ { - 2 }$.}
A small ball is released from rest. It falls for 2 seconds and is then brought to rest over the next 5 seconds. This motion is modelled in the speed-time graph Fig. 6.

\begin{figure}[h]
\begin{center}
  \includegraphics[alt={},max width=\textwidth]{c84a748a-a6f4-48c5-b864-fe543569bdf5-5_659_1105_578_493}
\captionsetup{labelformat=empty}
\caption{Fig. 6}
\end{center}
\end{figure}

For this model,\\
(i) calculate the distance fallen from $t = 0$ to $t = 7$,\\
(ii) find the acceleration of the ball from $t = 2$ to $t = 6$, specifying the direction,\\
(iii) obtain an expression in terms of $t$ for the downward speed of the ball from $t = 2$ to $t = 6$,\\
(iv) state the assumption that has been made about the resistance to motion from $t = 0$ to $t = 2$.

The part of the motion from $t = 2$ to $t = 7$ is now modelled by $v = - \frac { 3 } { 2 } t ^ { 2 } + \frac { 19 } { 2 } t + 7$.\\
(v) Verify that $v$ agrees with the values given in Fig. 6 at $t = 2 , t = 6$ and $t = 7$.\\
(vi) Calculate the distance fallen from $t = 2$ to $t = 7$ according to this model.

\hfill \mbox{\textit{OCR MEI M1 2005 Q6 [19]}}