| Exam Board | Edexcel |
|---|---|
| Module | M1 (Mechanics 1) |
| Year | 2016 |
| Session | October |
| Marks | 13 |
| Paper | Download PDF ↗ |
| Mark scheme | Download PDF ↗ |
| Topic | Pulley systems |
| Type | Particle on rough incline, particle hanging |
| Difficulty | Standard +0.3 This is a standard M1 pulley system question with routine application of Newton's second law and friction. Students use F=ma for both particles, apply kinematic equations (v²=u²+2as), and solve simultaneous equations. The tan α = 3/4 requiring sin α = 3/5 and cos α = 4/5 is a common M1 technique. All steps are predictable textbook methods with no novel insight required, making it slightly easier than average. |
| Spec | 1.05a Sine, cosine, tangent: definitions for all arguments3.02d Constant acceleration: SUVAT formulae3.03k Connected particles: pulleys and equilibrium3.03l Newton's third law: extend to situations requiring force resolution3.03r Friction: concept and vector form3.03t Coefficient of friction: F <= mu*R model |
| END |
| Answer | Marks | Guidance |
|---|---|---|
| Working/Answer | Marks | Guidance |
| \(1.4^2 = 2a \times 0.5 \Rightarrow a = 1.96 \text{ ms}^{-2}\) | M1 A1 | M1 for using one or more suvat formulae to produce equation in \(a\) only; A1 for 1.96 (or \(-1.96\)) |
| \(3g - T = 3a\) or \(-3a\) | M1 A1 | M1 for resolving vertically for \(Q\) (correct no. of terms, condone sign errors); A1 for correct equation |
| \(T = 23.5\text{ N}\) or \(24\text{ N}\) | A1 | Third A1 for 23.5 or 24 |
| Answer | Marks | Guidance |
|---|---|---|
| Working/Answer | Marks | Guidance |
| \(F = \mu R\) | B1 | B1 for \(F = \mu R\) seen |
| \(R = 2g\cos\alpha\) | M1 A1 | M1 for resolving perpendicular to plane (correct no. of terms with \(2g\) resolved); A1 for correct equation (M1A0 for \(R = mg\cos\alpha\)) |
| \(T - 2g\sin\alpha - F = 2a\) or \(-2a\) | M1 A1 A1 | M1 for resolving parallel to plane (condone sign errors); A1 A1 for correct equation (A1A0 for one error); neither \(T\) nor \(F\) nor \(a\) need substituting |
| \(\mu = 0.5\) | DM1 A1 | DM1 dependent on both previous M marks for solving for \(\mu\) (numerical value); A1 for \(\mu = 0.5\) (A0 for 0.499) |
# Question 8:
## Part (a):
| Working/Answer | Marks | Guidance |
|---|---|---|
| $1.4^2 = 2a \times 0.5 \Rightarrow a = 1.96 \text{ ms}^{-2}$ | M1 A1 | M1 for using one or more suvat formulae to produce equation in $a$ only; A1 for 1.96 (or $-1.96$) |
| $3g - T = 3a$ or $-3a$ | M1 A1 | M1 for resolving vertically for $Q$ (correct no. of terms, condone sign errors); A1 for correct equation |
| $T = 23.5\text{ N}$ or $24\text{ N}$ | A1 | Third A1 for 23.5 or 24 |
## Part (b):
| Working/Answer | Marks | Guidance |
|---|---|---|
| $F = \mu R$ | B1 | B1 for $F = \mu R$ seen |
| $R = 2g\cos\alpha$ | M1 A1 | M1 for resolving perpendicular to plane (correct no. of terms with $2g$ resolved); A1 for correct equation (M1A0 for $R = mg\cos\alpha$) |
| $T - 2g\sin\alpha - F = 2a$ or $-2a$ | M1 A1 A1 | M1 for resolving parallel to plane (condone sign errors); A1 A1 for correct equation (A1A0 for one error); neither $T$ nor $F$ nor $a$ need substituting |
| $\mu = 0.5$ | DM1 A1 | DM1 dependent on both previous M marks for solving for $\mu$ (numerical value); A1 for $\mu = 0.5$ (A0 for 0.499) |
8.
\begin{figure}[h]
\begin{center}
\includegraphics[alt={},max width=\textwidth]{6978be48-561b-49a0-a297-c8886ca66c19-20_312_1068_230_438}
\captionsetup{labelformat=empty}
\caption{Figure 3}
\end{center}
\end{figure}
Two particles $P$ and $Q$ have masses 2 kg and 3 kg respectively. The particles are attached to the ends of a light inextensible string. The string passes over a smooth light pulley which is fixed at the top of a rough plane. The plane is inclined to horizontal ground at an angle $\alpha$, where tan $\alpha = \frac { 3 } { 4 }$. Initially $P$ is held at rest on the inclined plane with the part of the string from $P$ to the pulley parallel to a line of greatest slope of the plane. The particle $Q$ hangs freely below the pulley at a height of 0.5 m above the ground, as shown in Figure 3. The coefficient of friction between $P$ and the plane is $\mu$. The system is released from rest, with the string taut, and $Q$ strikes the ground before $P$ reaches the pulley. The speed of $Q$ at the instant when it strikes the ground is $1.4 \mathrm {~m} \mathrm {~s} ^ { - 1 }$.
\begin{enumerate}[label=(\alph*)]
\item For the motion before $Q$ strikes the ground, find the tension in the string.
\item Find the value of $\mu$.
\begin{center}
\begin{tabular}{|l|l|}
\hline
\hline
END & \\
\hline
\end{tabular}
\end{center}
\end{enumerate}
\hfill \mbox{\textit{Edexcel M1 2016 Q8 [13]}}