| Exam Board | OCR |
|---|---|
| Module | PURE |
| Marks | 16 |
| Paper | Download PDF ↗ |
| Topic | Pulley systems |
| Type | Applied force in addition to weights |
| Difficulty | Standard +0.3 This is a standard A-level mechanics pulley problem with connected particles. While it has multiple parts (a-f), each step follows routine procedures: applying F=ma to find acceleration, calculating tension, then using SUVAT equations after the string breaks. The calculations are straightforward with no conceptual surprises, making it slightly easier than average. |
| Spec | 3.02d Constant acceleration: SUVAT formulae3.02h Motion under gravity: vector form3.03l Newton's third law: extend to situations requiring force resolution3.03o Advanced connected particles: and pulleys |
| Answer | Marks | Guidance |
|---|---|---|
| For \(P\): \(40 - T - 8 = 3a\) | A1 | — |
| For \(Q\): \(T - 2g = 2a\) | A1 | — |
| \(32 - 2g = 5a \Rightarrow a = \ldots\) | Dep\*M1 | Attempt to solve simultaneous equations; M1\* attempt N2L for \(P\) or \(Q\) (must include correct number of terms — use of weight for mass is M0) |
| \(a = 2.48 \text{ m s}^{-2}\) | A1 | AG — must show sufficient working to justify the given answer; M1 A2 for \(40 - 8 - 2g = 5a\) for M1 must have correct number of terms and mass must be \(5\) not \(5g\) |
| Answer | Marks | Guidance |
|---|---|---|
| \(T - 2g = 2(2.48)\) | M1 | Substitute given value of \(a\) into either equation; must include correct number of terms — use of weight for mass is M0 |
| \(T = 24.56 \text{ N}\) | A1 | cao; allow 24.6 |
| Answer | Marks | Guidance |
|---|---|---|
| \(v = 2.48(0.5)\) | B1 | Speed after 0.5 seconds \(= 1.24\) |
| \(s = 0.5(2.48)(0.5)^2\) | B1 | Distance travelled in this time \(= 0.31\) |
| \(-(2 + 0.31) = 1.24t - 0.5(9.8)t^2\) | M1 | Applying \(s = ut + 0.5at^2\) correctly — allow sign errors; M0 if not using relevant displacement |
| \(t = 0.825 \text{ s}\) | A1 | BC; \(0.8246986\ldots\) |
| ALT: \(0 = 1.24^2 - 2(9.8)s \Rightarrow s = 0.0784\); \(2 + 0.31 + 0.0784 = 0.5(9.8)t_1^2\); \(t_1 = 0.698\); \(t = 0.825\) | M1, A1, A1 | Complete method to calculate time down; correct value for time down |
| Answer | Marks | Guidance |
|---|---|---|
| \(v^2 = 1.24^2 + 2(-9.8)(-2.31)\) | M1 | Applying \(v^2 = u^2 + 2as\) correctly with their 1.24 and 2.31 or any other complete method; M0 if not using total time or relevant displacement |
| \(v = 6.84 \text{ m s}^{-1}\) | A1 | Allow 6.85; \(6.8420464\ldots\) |
| Answer | Marks | Guidance |
|---|---|---|
| \(19.6 \text{ N}\) | B1 | Accept \(2g\) |
| Answer | Marks | Guidance |
|---|---|---|
| e.g. include a more accurate value for \(g\); e.g. include a variable resistance in the model rather than a constant; e.g. include the dimension of the pulley in the model so that the string is not parallel to the table; e.g. include a frictional force at the pulley | B1 | AO 3.5c |
## Question 11(a):
For $P$: $40 - T - 8 = 3a$ | **A1** | —
For $Q$: $T - 2g = 2a$ | **A1** | —
$32 - 2g = 5a \Rightarrow a = \ldots$ | **Dep\*M1** | Attempt to solve simultaneous equations; M1\* attempt N2L for $P$ or $Q$ (must include correct number of terms — use of weight for mass is **M0**)
$a = 2.48 \text{ m s}^{-2}$ | **A1** | AG — must show sufficient working to justify the given answer; M1 A2 for $40 - 8 - 2g = 5a$ for M1 must have correct number of terms and mass must be $5$ not $5g$
---
## Question 11(b):
$T - 2g = 2(2.48)$ | **M1** | Substitute given value of $a$ into either equation; must include correct number of terms — use of weight for mass is **M0**
$T = 24.56 \text{ N}$ | **A1** | cao; allow 24.6
---
## Question 11(c):
$v = 2.48(0.5)$ | **B1** | Speed after 0.5 seconds $= 1.24$
$s = 0.5(2.48)(0.5)^2$ | **B1** | Distance travelled in this time $= 0.31$
$-(2 + 0.31) = 1.24t - 0.5(9.8)t^2$ | **M1** | Applying $s = ut + 0.5at^2$ correctly — allow sign errors; **M0** if not using relevant displacement
$t = 0.825 \text{ s}$ | **A1** | BC; $0.8246986\ldots$
**ALT:** $0 = 1.24^2 - 2(9.8)s \Rightarrow s = 0.0784$; $2 + 0.31 + 0.0784 = 0.5(9.8)t_1^2$; $t_1 = 0.698$; $t = 0.825$ | **M1, A1, A1** | Complete method to calculate time down; correct value for time down
---
## Question 11(d):
$v^2 = 1.24^2 + 2(-9.8)(-2.31)$ | **M1** | Applying $v^2 = u^2 + 2as$ correctly with their 1.24 and 2.31 or any other complete method; **M0** if not using total time or relevant displacement
$v = 6.84 \text{ m s}^{-1}$ | **A1** | Allow 6.85; $6.8420464\ldots$
---
## Question 11(e):
$19.6 \text{ N}$ | **B1** | Accept $2g$
---
## Question 11(f):
e.g. include a more accurate value for $g$; e.g. include a variable resistance in the model rather than a constant; e.g. include the dimension of the pulley in the model so that the string is not parallel to the table; e.g. include a frictional force at the pulley | **B1** | AO 3.5c
11 Two small balls $P$ and $Q$ have masses 3 kg and 2 kg respectively. The balls are attached to the ends of a string. $P$ is held at rest on a rough horizontal surface. The string passes over a pulley which is fixed at the edge of the surface. $Q$ hangs vertically below the pulley at a height of 2 m above a horizontal floor.\\
\includegraphics[max width=\textwidth, alt={}, center]{d6430776-0b87-4e5e-8f78-c6228ee163d5-7_346_906_445_255}
The system is initially at rest with the string taut. A horizontal force of magnitude 40 N acts on $P$ as shown in the diagram.\\
$P$ is released and moves directly away from the pulley. A constant frictional force of magnitude 8 N opposes the motion of $P$. It is given that $P$ does not leave the horizontal surface and that $Q$ does not reach the pulley in the subsequent motion.
The balls are modelled as particles, the pulley is modelled as being small and smooth, and the string is modelled as being light and inextensible.
\begin{enumerate}[label=(\alph*)]
\item Show that the magnitude of the acceleration of each particle is $2.48 \mathrm {~ms} ^ { - 2 }$.
\item Find the tension in the string.
When the balls have been in motion for 0.5 seconds, the string breaks.
\item Find the additional time that elapses until $Q$ hits the floor.
\item Find the speed of $Q$ as it hits the floor.
\item Write down the magnitude of the normal reaction force acting on $Q$ when $Q$ has come to rest on the floor.
\item State one improvement that could be made to the model.
\section*{OCR}
Oxford Cambridge and RSA
\end{enumerate}
\hfill \mbox{\textit{OCR PURE Q11 [16]}}