OCR MEI M1 2008 January — Question 6 17 marks

Exam BoardOCR MEI
ModuleM1 (Mechanics 1)
Year2008
SessionJanuary
Marks17
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicProjectiles
TypeBasic trajectory calculations
DifficultyModerate -0.3 This is a standard M1 mechanics question testing Newton's second law and kinematics with constant acceleration. Part (i) uses basic SUVAT equations, parts (ii) and (iii) apply F=ma in straightforward contexts, and part (iv) requires considering two connected bodies but with clear force diagrams. All techniques are routine for M1 with no novel problem-solving required, making it slightly easier than average.
Spec3.02d Constant acceleration: SUVAT formulae3.03c Newton's second law: F=ma one dimension3.03k Connected particles: pulleys and equilibrium

A helicopter rescue activity at sea is modelled as follows. The helicopter is stationary and a man is suspended from it by means of a vertical, light, inextensible wire that may be raised or lowered, as shown in Fig. 6.1. \includegraphics{figure_6_1}
  1. When the man is descending with an acceleration 1.5 m s\(^{-2}\) downwards, how much time does it take for his speed to increase from 0.5 m s\(^{-1}\) downwards to 3.5 m s\(^{-1}\) downwards? How far does he descend in this time? [4]
The man has a mass of 80 kg. All resistances to motion may be neglected.
  1. Calculate the tension in the wire when the man is being lowered
    1. with an acceleration of 1.5 m s\(^{-2}\) downwards,
    2. with an acceleration of 1.5 m s\(^{-2}\) upwards. [5]
Subsequently, the man is raised and this situation is modelled with a constant resistance of 116 N to his upward motion.
  1. For safety reasons, the tension in the wire should not exceed 2500 N. What is the maximum acceleration allowed when the man is being raised? [4]
At another stage of the rescue, the man has equipment of mass 10 kg at the bottom of a vertical rope which is hanging from his waist, as shown in Fig. 6.2. The man and his equipment are being raised; the rope is light and inextensible and the tension in it is 80 N. \includegraphics{figure_6_2}
  1. Assuming that the resistance to the upward motion of the man is still 116 N and that there is negligible resistance to the motion of the equipment, calculate the tension in the wire. [4]

(i)
AnswerMarks Guidance
\(3.5 = 0.5 + 1.5T^2\) so \(T = 2\) so \(2\) sM1, A1 Suitable uvast, condone sign errors. cao
\(s = \frac{3.5 + 0.5}{\sqrt{2}} \times 2\) so \(s = 4\) so \(4\) mM1, F1 Suitable uvast, condone sign errors. FT their \(T\). [If \(s\) found first then it is cao. In this case when finding \(T\), FT their \(s\), if used.]
Sub: 4
(ii)(A)
AnswerMarks Guidance
N2L \(\downarrow: 80 \times 9.8 - T = 80 \times 1.5\)M1 Use of N2L. Allow weight omitted and use of \(F = ma\). Condone errors in sign but do not allow extra forces.
\(T = 664\) so \(664\) NB1, A1 weight correct (seen in (A) or (B)). cao
Sub: 5
(ii)(B)
AnswerMarks Guidance
N2L \(\downarrow: 80 \times 9.8 - T = 80 \times (-1.5)\)M1 N2L with all forces and using \(F = ma\). Condone errors in sign but do not allow extra forces.
\(T = 904\) so \(904\) NA1 cao [Accept 904 N seen for M1 A1]
Sub: 5
(iii)
AnswerMarks Guidance
N2L \(\uparrow: 2500 - 80 - 9.8 - 116 = 80a\)M1 Use of N2L with \(F = ma\). Allow 1 force missing. No extra forces. Condone errors in sign.
\(a = 20\) so \(20\) m s\(^{-2}\) upwards.A1, A1, A1 \(\pm20\), accept direction wrong or omitted. upwards made clear (accept diagram)
Sub: 4
(iv)
AnswerMarks Guidance
N2L \(\uparrow\) on equipment: \(80 - 10 \times 9.8 = 10a\)M1 Use of N2L on equipment. All forces. \(F = ma\). No extra forces. Allow sign errors. Allow \(\pm1.8\)
\(a = -1.8\)A1
N2L \(\uparrow\)M1 N2L for system or for man alone. Forces correct (with no extras); accept sign errors; their \(\pm1.8\) used
either all: \(T - (80 + 10) \times 9.8 - 116 = 90 \times (-1.8)\)
or on man: \(T - (80 \times 9.8) - 116 - 80 = 80 \times (-1.8)\) \(T = 836\) so \(836\) NA1 cao [NB: The answer 836 N is independent of the value taken for \(g\) and hence may be obtained if all weights are omitted.]
Sub: 4
### (i)
$3.5 = 0.5 + 1.5T^2$ so $T = 2$ so $2$ s | M1, A1 | Suitable uvast, condone sign errors. cao

$s = \frac{3.5 + 0.5}{\sqrt{2}} \times 2$ so $s = 4$ so $4$ m | M1, F1 | Suitable uvast, condone sign errors. FT their $T$. [If $s$ found first then it is cao. In this case when finding $T$, FT their $s$, if used.]
| Sub: 4

### (ii)(A)
N2L $\downarrow: 80 \times 9.8 - T = 80 \times 1.5$ | M1 | Use of N2L. Allow weight omitted and use of $F = ma$. Condone errors in sign but do not allow extra forces.

$T = 664$ so $664$ N | B1, A1 | weight correct (seen in (A) or (B)). cao
| Sub: 5

### (ii)(B)
N2L $\downarrow: 80 \times 9.8 - T = 80 \times (-1.5)$ | M1 | N2L with all forces and using $F = ma$. Condone errors in sign but do not allow extra forces.

$T = 904$ so $904$ N | A1 | cao [Accept 904 N seen for M1 A1]
| Sub: 5

### (iii)
N2L $\uparrow: 2500 - 80 - 9.8 - 116 = 80a$ | M1 | Use of N2L with $F = ma$. Allow 1 force missing. No extra forces. Condone errors in sign.

$a = 20$ so $20$ m s$^{-2}$ upwards. | A1, A1, A1 | $\pm20$, accept direction wrong or omitted. upwards made clear (accept diagram)
| Sub: 4

### (iv)
N2L $\uparrow$ on equipment: $80 - 10 \times 9.8 = 10a$ | M1 | Use of N2L on equipment. All forces. $F = ma$. No extra forces. Allow sign errors. Allow $\pm1.8$

$a = -1.8$ | A1 | 

N2L $\uparrow$ | M1 | N2L for system or for man alone. Forces correct (with no extras); accept sign errors; their $\pm1.8$ used

either all: $T - (80 + 10) \times 9.8 - 116 = 90 \times (-1.8)$ | | 

or on man: $T - (80 \times 9.8) - 116 - 80 = 80 \times (-1.8)$ $T = 836$ so $836$ N | A1 | cao [NB: The answer 836 N is independent of the value taken for $g$ and hence may be obtained if all weights are omitted.]
| Sub: 4

---
A helicopter rescue activity at sea is modelled as follows. The helicopter is stationary and a man is suspended from it by means of a vertical, light, inextensible wire that may be raised or lowered, as shown in Fig. 6.1.

\includegraphics{figure_6_1}

\begin{enumerate}[label=(\roman*)]
\item When the man is descending with an acceleration 1.5 m s$^{-2}$ downwards, how much time does it take for his speed to increase from 0.5 m s$^{-1}$ downwards to 3.5 m s$^{-1}$ downwards?

How far does he descend in this time? [4]
\end{enumerate}

The man has a mass of 80 kg. All resistances to motion may be neglected.

\begin{enumerate}[label=(\roman*)]
\setcounter{enumi}{1}
\item Calculate the tension in the wire when the man is being lowered
\begin{enumerate}[label=(\Alph*)]
\item with an acceleration of 1.5 m s$^{-2}$ downwards,
\item with an acceleration of 1.5 m s$^{-2}$ upwards. [5]
\end{enumerate}
\end{enumerate}

Subsequently, the man is raised and this situation is modelled with a constant resistance of 116 N to his upward motion.

\begin{enumerate}[label=(\roman*)]
\setcounter{enumi}{2}
\item For safety reasons, the tension in the wire should not exceed 2500 N. What is the maximum acceleration allowed when the man is being raised? [4]
\end{enumerate}

At another stage of the rescue, the man has equipment of mass 10 kg at the bottom of a vertical rope which is hanging from his waist, as shown in Fig. 6.2. The man and his equipment are being raised; the rope is light and inextensible and the tension in it is 80 N.

\includegraphics{figure_6_2}

\begin{enumerate}[label=(\roman*)]
\setcounter{enumi}{3}
\item Assuming that the resistance to the upward motion of the man is still 116 N and that there is negligible resistance to the motion of the equipment, calculate the tension in the wire. [4]
\end{enumerate}

\hfill \mbox{\textit{OCR MEI M1 2008 Q6 [17]}}