OCR MEI M1 2011 June — Question 8 18 marks

Exam BoardOCR MEI
ModuleM1 (Mechanics 1)
Year2011
SessionJune
Marks18
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicNewton's laws and connected particles
TypeTwo connected particles, horizontal surface
DifficultyStandard +0.3 This is a multi-part connected particles question with straightforward equilibrium and Newton's second law applications. Parts (i)-(iii) involve basic equilibrium with simple trigonometry, (iv) requires F=ma with resolved forces, and (v) involves motion on a slope. All parts use standard M1 techniques with no novel problem-solving required, making it slightly easier than average.
Spec3.03d Newton's second law: 2D vectors3.03e Resolve forces: two dimensions3.03m Equilibrium: sum of resolved forces = 03.03r Friction: concept and vector form

8 A trolley C of mass 8 kg with rusty axle bearings is initially at rest on a horizontal floor.
The trolley stays at rest when it is pulled by a horizontal string with tension 25 N , as shown in Fig. 8.1. \begin{figure}[h]
\includegraphics[alt={},max width=\textwidth]{2efbb554-fe60-42ce-9213-8c66bfdb1d85-5_255_1097_397_523} \captionsetup{labelformat=empty} \caption{Fig. 8.1}
\end{figure}
  1. State the magnitude of the horizontal resistance opposing the pull. A second trolley D of mass 10 kg is connected to trolley C by means of a light, horizontal rod.
    The string now has tension 50 N , and is at an angle of \(25 ^ { \circ }\) to the horizontal, as shown in Fig. 8.2. The two trolleys stay at rest. \begin{figure}[h]
    \includegraphics[alt={},max width=\textwidth]{2efbb554-fe60-42ce-9213-8c66bfdb1d85-5_305_1191_1050_701} \captionsetup{labelformat=empty} \caption{Fig. 8.2}
    \end{figure}
  2. Calculate the magnitude of the total horizontal resistance acting on the two trolleys opposing the pull.
  3. Calculate the normal reaction of the floor on trolley C . The axle bearings of the trolleys are oiled and the total horizontal resistance to the motion of the two trolleys is now 20 N . The two trolleys are still pulled by the string with tension 50 N , as shown in Fig. 8.2.
  4. Calculate the acceleration of the trolleys. In a new situation, the trolleys are on a slope at \(5 ^ { \circ }\) to the horizontal and are initially travelling down the slope at \(3 \mathrm {~m} \mathrm {~s} ^ { - 1 }\). The resistances are 15 N to the motion of D and 5 N to the motion of C . There is no string attached. The rod connecting the trolleys is parallel to the slope. This situation is shown in Fig. 8.3. \begin{figure}[h]
    \includegraphics[alt={},max width=\textwidth]{2efbb554-fe60-42ce-9213-8c66bfdb1d85-5_355_1294_2156_429} \captionsetup{labelformat=empty} \caption{Fig. 8.3}
    \end{figure}
  5. Calculate the speed of the trolleys after 2 seconds and also the force in the rod connecting the trolleys, stating whether this rod is in tension or thrust (compression).

(i)
AnswerMarks Guidance
\(25 \text{ N}\)B1 Condone no units. Do not accept \(-25 \text{ N}\).
1
(ii)
AnswerMarks Guidance
\(50 \cos 25\) \(= 45.31538\ldots\) so \(45.3 \text{ N}\) (3 s.f.)M1 Attempt to resolve 50 N. Accept \(s \leftrightarrow c\). No extra forces.
A1cao but accept \(= -45.3\).
2
(iii)
AnswerMarks Guidance
Resolving verticallyM1 All relevant forces with resolution of 50 N. No extras. Accept \(s \leftrightarrow c\).
\(R + 50 \sin 25 - 8 \times 9.8 = 0\)A1 All correct.
\(R = 57.26908\ldots\) so \(57.3 \text{ N}\) (3 s.f.)A1
3
(iv)
AnswerMarks Guidance
Newton's 2nd Law in direction DCM1 Newton's 2nd Law with \(m = 18\). Accept \(F = ma\). Attempt at resolving 50 N. Allow 20 N omitted and \(s \leftrightarrow c\). No extra forces.
\(50\cos 25 - 20 = 18a\)A1 Allow only sign error and \(s \leftrightarrow c\).
\(a = 1.4064105\ldots\) so \(1.41 \text{ m s}^{-2}\) (3 s.f.)A1 cao
3
Q8 continued
(v)
AnswerMarks Guidance
Resolution of weight down the slopeB1 \(mg\sin 5°\) where \(m = 8\) or 10 or 18, whichever first seen
either
AnswerMarks Guidance
Newton's 2nd Law down slope overallM1 \(F = ma\). Must have 20 N and \(m = 18\). Allow weight not resolved and use of mass. Accept \(s \leftrightarrow c\) and sign errors (including inconsistency between the 15 N and the 5 N).
\(18 \times 9.8 \times \sin 5 - 20 = 18a\)A1 cao
Newton's 2nd Law down slope. Force in rod can be taken as tension or thrust. Taking it as tensionM1 \(F = ma\). Must consider the motion of either C or D and include: component of weight, resistance and \(T\). No extra forces. Condone sign errors and \(s \leftrightarrow c\). Do not condone inconsistent value of mass.
\(T\) gives
For D: \(10 \times 9.8 \times \sin 5 - 15 - T = 10a\)
(For C: \(8 \times 9.8 \times \sin 5 - 5 + T = 8a\))F1 FT only applies to \(a\), and only if direction is consistent. '+T' if \(T\) taken as a thrust. '-T' if \(T\) taken as a thrust
\(T = -3.888\ldots = -3.89 \text{ N}\) (3 s.f.)A1 If \(T\) taken as thrust, then \(T = +3.89\). Dependent on \(T\) correct
The force is a thrustA1
or
AnswerMarks Guidance
Newton's 2nd Law down slope. Force in rod can be taken as tension or thrust. Taking it as tensionM1 \(F = ma\). Must consider the motion of C and include: component of weight, resistance and \(T\). No extra forces. Condone sign errors and \(s \leftrightarrow c\). Do not condone inconsistent value of mass.
\(T\) gives
For C: \(8 \times 9.8 \times \sin 5 - 5 + T = 8a\)
\(a = -0.2569\ldots\), \(T = -3.888\ldots = -3.89 \text{ N}\) (3s.f.)A1 First of \(a\) and \(T\) found is correct. If \(T\) taken as thrust, then \(T = +3.89\).
F1The second of \(a\) and \(T\) found is FT. Award for either the equation for C or the equation for D correct. '-T' if \(T\) taken as a thrust. '+T' if \(T\) taken as a thrust
A1Dependent on \(T\) correct
then
AnswerMarks Guidance
After 2 s: \(v = 3 + 2 \times a\)M1 Allow sign of \(a\) not followed. FT their value of \(a\). Allow change to correct sign of \(a\) at this stage.
\(v = 2.4860303\ldots\) so \(2.49 \text{ m s}^{-1}\) (3 s.f.)F1 FT from magnitude of their \(a\) but must be consistent with its direction.
9
18
**(i)**

$25 \text{ N}$ | B1 | Condone no units. Do not accept $-25 \text{ N}$.

| | 1 |

**(ii)**

$50 \cos 25$ $= 45.31538\ldots$ so $45.3 \text{ N}$ (3 s.f.) | M1 | Attempt to resolve 50 N. Accept $s \leftrightarrow c$. No extra forces.

| A1 | cao but accept $= -45.3$.

| | 2 |

**(iii)**

Resolving vertically | M1 | All relevant forces with resolution of 50 N. No extras. Accept $s \leftrightarrow c$.

$R + 50 \sin 25 - 8 \times 9.8 = 0$ | A1 | All correct.

$R = 57.26908\ldots$ so $57.3 \text{ N}$ (3 s.f.) | A1 |

| | 3 |

**(iv)**

Newton's 2nd Law in direction DC | M1 | Newton's 2nd Law with $m = 18$. Accept $F = ma$. Attempt at resolving 50 N. Allow 20 N omitted and $s \leftrightarrow c$. No extra forces.

$50\cos 25 - 20 = 18a$ | A1 | Allow only sign error and $s \leftrightarrow c$.

$a = 1.4064105\ldots$ so $1.41 \text{ m s}^{-2}$ (3 s.f.) | A1 | cao

| | 3 |

**Q8 continued**

**(v)**

Resolution of weight down the slope | B1 | $mg\sin 5°$ where $m = 8$ or 10 or 18, whichever first seen

**either**

Newton's 2nd Law down slope overall | M1 | $F = ma$. Must have 20 N and $m = 18$. Allow weight not resolved and use of mass. Accept $s \leftrightarrow c$ and sign errors (including inconsistency between the 15 N and the 5 N).

$18 \times 9.8 \times \sin 5 - 20 = 18a$ | A1 | cao

Newton's 2nd Law down slope. Force in rod can be taken as tension or thrust. Taking it as tension | M1 | $F = ma$. Must consider the motion of either C or D and include: component of weight, resistance and $T$. No extra forces. Condone sign errors and $s \leftrightarrow c$. Do not condone inconsistent value of mass.

$T$ gives | | |

For D: $10 \times 9.8 \times \sin 5 - 15 - T = 10a$ | | |

(For C: $8 \times 9.8 \times \sin 5 - 5 + T = 8a$) | F1 | FT only applies to $a$, and only if direction is consistent. '+T' if $T$ taken as a thrust. '-T' if $T$ taken as a thrust

$T = -3.888\ldots = -3.89 \text{ N}$ (3 s.f.) | A1 | If $T$ taken as thrust, then $T = +3.89$. Dependent on $T$ correct

The force is a thrust | A1 |

**or**

Newton's 2nd Law down slope. Force in rod can be taken as tension or thrust. Taking it as tension | M1 | $F = ma$. Must consider the motion of C and include: component of weight, resistance and $T$. No extra forces. Condone sign errors and $s \leftrightarrow c$. Do not condone inconsistent value of mass.

$T$ gives | | |

For C: $8 \times 9.8 \times \sin 5 - 5 + T = 8a$ | | |

$a = -0.2569\ldots$, $T = -3.888\ldots = -3.89 \text{ N}$ (3s.f.) | A1 | First of $a$ and $T$ found is correct. If $T$ taken as thrust, then $T = +3.89$.

| F1 | The second of $a$ and $T$ found is FT. Award for either the equation for C or the equation for D correct. '-T' if $T$ taken as a thrust. '+T' if $T$ taken as a thrust

| A1 | Dependent on $T$ correct

**then**

After 2 s: $v = 3 + 2 \times a$ | M1 | Allow sign of $a$ not followed. FT their value of $a$. Allow change to correct sign of $a$ at this stage.

$v = 2.4860303\ldots$ so $2.49 \text{ m s}^{-1}$ (3 s.f.) | F1 | FT from magnitude of their $a$ but must be consistent with its direction.

| | 9 |

| | 18 |
8 A trolley C of mass 8 kg with rusty axle bearings is initially at rest on a horizontal floor.\\
The trolley stays at rest when it is pulled by a horizontal string with tension 25 N , as shown in Fig. 8.1.

\begin{figure}[h]
\begin{center}
  \includegraphics[alt={},max width=\textwidth]{2efbb554-fe60-42ce-9213-8c66bfdb1d85-5_255_1097_397_523}
\captionsetup{labelformat=empty}
\caption{Fig. 8.1}
\end{center}
\end{figure}

(i) State the magnitude of the horizontal resistance opposing the pull.

A second trolley D of mass 10 kg is connected to trolley C by means of a light, horizontal rod.\\
The string now has tension 50 N , and is at an angle of $25 ^ { \circ }$ to the horizontal, as shown in Fig. 8.2. The two trolleys stay at rest.

\begin{figure}[h]
\begin{center}
  \includegraphics[alt={},max width=\textwidth]{2efbb554-fe60-42ce-9213-8c66bfdb1d85-5_305_1191_1050_701}
\captionsetup{labelformat=empty}
\caption{Fig. 8.2}
\end{center}
\end{figure}

(ii) Calculate the magnitude of the total horizontal resistance acting on the two trolleys opposing the pull.\\
(iii) Calculate the normal reaction of the floor on trolley C .

The axle bearings of the trolleys are oiled and the total horizontal resistance to the motion of the two trolleys is now 20 N . The two trolleys are still pulled by the string with tension 50 N , as shown in Fig. 8.2.\\
(iv) Calculate the acceleration of the trolleys.

In a new situation, the trolleys are on a slope at $5 ^ { \circ }$ to the horizontal and are initially travelling down the slope at $3 \mathrm {~m} \mathrm {~s} ^ { - 1 }$. The resistances are 15 N to the motion of D and 5 N to the motion of C . There is no string attached. The rod connecting the trolleys is parallel to the slope. This situation is shown in Fig. 8.3.

\begin{figure}[h]
\begin{center}
  \includegraphics[alt={},max width=\textwidth]{2efbb554-fe60-42ce-9213-8c66bfdb1d85-5_355_1294_2156_429}
\captionsetup{labelformat=empty}
\caption{Fig. 8.3}
\end{center}
\end{figure}

(v) Calculate the speed of the trolleys after 2 seconds and also the force in the rod connecting the trolleys, stating whether this rod is in tension or thrust (compression).

\hfill \mbox{\textit{OCR MEI M1 2011 Q8 [18]}}