| Exam Board | Edexcel |
|---|---|
| Module | M1 (Mechanics 1) |
| Year | 2011 |
| Session | June |
| Marks | 16 |
| Paper | Download PDF ↗ |
| Mark scheme | Download PDF ↗ |
| Topic | Pulley systems |
| Type | Particle on rough incline, particle hanging |
| Difficulty | Standard +0.8 This is a substantial M1 pulley problem requiring resolution of forces on an incline (with given tan α needing sin/cos conversion), friction calculations, connected particles equations with given acceleration, and post-string-break kinematics. The 16 total marks and three-part structure with the final part requiring careful consideration of friction direction change makes this harder than average, though all techniques are standard M1 content. |
| Spec | 3.02d Constant acceleration: SUVAT formulae3.03d Newton's second law: 2D vectors3.03k Connected particles: pulleys and equilibrium3.03r Friction: concept and vector form3.03v Motion on rough surface: including inclined planes |
| Answer | Marks |
|---|---|
| \(R = 0.3g\cos\alpha\) | M1 |
| \(= 0.24g = 2.35\) (3sf)\(= 2.4\) (2sf) | A1 |
| (2) |
| Answer | Marks |
|---|---|
| \(mg - T = 1.4m\) | M1 A1 |
| \(T - 0.3g\sin\alpha - F = 0.3 \times 1.4\) | M1 A2 |
| \(F = 0.5R\) | M1 |
| Eliminating \(R\) and \(T\) | DM1 |
| \(m = 0.4\) | A1 |
| (8) |
| Answer | Marks |
|---|---|
| \(v = 1.4 \times 0.5\) | B1 |
| \(-0.3g\sin\alpha - F = 0.3a\) | M1 A1 |
| \(a = -9.8\) | A1 |
| \(0 = 0.7 - 9.8t\) | M1 |
| \(t = 0.071 \text{ s or } 0.0714 \text{ s } (1/14 \text{ A0})\) | A1 |
| (6) | |
| 16 |
## (a)
$R = 0.3g\cos\alpha$ | M1 |
$= 0.24g = 2.35$ (3sf)$= 2.4$ (2sf) | A1 |
| (2) |
## (b)
$mg - T = 1.4m$ | M1 A1 |
$T - 0.3g\sin\alpha - F = 0.3 \times 1.4$ | M1 A2 |
$F = 0.5R$ | M1 |
Eliminating $R$ and $T$ | **DM1** |
$m = 0.4$ | A1 |
| (8) |
## (c)
$v = 1.4 \times 0.5$ | B1 |
$-0.3g\sin\alpha - F = 0.3a$ | M1 A1 |
$a = -9.8$ | A1 |
$0 = 0.7 - 9.8t$ | M1 |
$t = 0.071 \text{ s or } 0.0714 \text{ s } (1/14 \text{ A0})$ | A1 |
| (6) |
| **16** |
---
\includegraphics{figure_2}
Two particles $P$ and $Q$ have masses 0.3 kg and $m$ kg respectively. The particles are attached to the ends of a light inextensible string. The string passes over a small smooth pulley which is fixed at the top of a fixed rough plane. The plane is inclined to the horizontal at an angle $\alpha$, where $\tan \alpha = \frac{3}{4}$. The coefficient of friction between $P$ and the plane is $\frac{1}{2}$.
The string lies in a vertical plane through a line of greatest slope of the inclined plane. The particle $P$ is held at rest on the inclined plane and the particle $Q$ hangs freely below the pulley with the string taut, as shown in Figure 2.
The system is released from rest and $Q$ accelerates vertically downwards at 1.4 m s$^{-2}$. Find
\begin{enumerate}[label=(\alph*)]
\item the magnitude of the normal reaction of the inclined plane on $P$, [2]
\item the value of $m$. [8]
\end{enumerate}
When the particles have been moving for 0.5 s, the string breaks. Assuming that $P$ does not reach the pulley,
\begin{enumerate}[label=(\alph*)]
\setcounter{enumi}{2}
\item find the further time that elapses until $P$ comes to instantaneous rest. [6]
\end{enumerate}
\hfill \mbox{\textit{Edexcel M1 2011 Q6 [16]}}