| Exam Board | Edexcel |
|---|---|
| Module | M2 (Mechanics 2) |
| Year | 2018 |
| Session | June |
| Marks | 9 |
| Paper | Download PDF ↗ |
| Mark scheme | Download PDF ↗ |
| Topic | Moments |
| Type | Rod with end on ground or wall supported by string |
| Difficulty | Standard +0.3 This is a standard M2 ladder/rod equilibrium problem requiring resolution of forces in two directions and taking moments about one point. The geometry is straightforward with given angles, and part (a) is a 'show that' which guides students to the tension value. Part (b) requires finding the friction coefficient range, which is a routine extension involving the friction inequality F ≤ μR. While it requires multiple steps and careful angle work, it follows a well-practiced template that M2 students drill extensively. |
| Spec | 6.04e Rigid body equilibrium: coplanar forces |
| Answer | Marks |
|---|---|
| Moments about \(A: T \times 1.6\sin 70° = 6g \times 0.8\cos 30°\) | M1 A2 |
| \(T = 27.1\) | A1 |
| (4) | |
| Given Answer |
| Answer | Marks |
|---|---|
| Resolve \(\leftrightarrow: F = T\cos 40\) | B1 |
| Resolve \(\updownarrow: R + T\cos 50 = 6g\) | M1 A1 |
| Use of \(F \leq \mu R\) and solve for \(\mu: \mu \geq \frac{20.76}{41.38} = 0.50\) (0.502) | DM1 A1 |
| (5) | |
| [9] |
## 2a.
Moments about $A: T \times 1.6\sin 70° = 6g \times 0.8\cos 30°$ | M1 A2 |
$T = 27.1$ | A1 |
(4) | |
**Given Answer** | |
## 2b.
Resolve $\leftrightarrow: F = T\cos 40$ | B1 |
Resolve $\updownarrow: R + T\cos 50 = 6g$ | M1 A1 |
Use of $F \leq \mu R$ and solve for $\mu: \mu \geq \frac{20.76}{41.38} = 0.50$ (0.502) | DM1 A1 |
(5) | |
[9] | |
**Notes for Q2:**
2(a)
- M1 for a complete method to obtain an equation in $T$ only, with usual rules (applied to all equations if more than one is used)
- N.B. Treat wrong angle(s) as A error(s)
- A2 for a correct equation (or equations) A1 A0 if one error (Allow use of $a$ and $2a$ for lengths)
- A1 for 27.1 correctly obtained (and no incorrect work seen)
- N.B. GIVEN ANSWER
Other equations:
- $\swarrow: R\cos 60 + F\cos 30 = 6g\cos 60 + T\cos 70$
- $\nwarrow: R\sin 60 + T\sin 70 = F\sin 30 + 6g\sin 60$
- $M(B): 6gl\cos 30 + F 2l\sin 30 = R 2l\cos 30$
- $M(G): Fl\sin 30 + Tl\sin 70 = Rl\cos 30$
2(b)
- B1 for $F = T\cos 40$ seen
- First M1 for a complete method, with usual rules applied to all equations used, to find $R$
- N.B. Treat wrong angle(s) as A error(s)
- First A1 for a correct equation
- Second DM1, dependent on first M1, for use of $F \leq \mu R$, and solve for $\mu$
- (Allow this M if they use $F = \mu R$ or $F < \mu R$ but final A1 not then available but M0 if they use $F \geq \mu R$ or $F > \mu R$)
- Second A1 for either $\mu \geq 0.5(0)$ or $\mu \geq 0.502$
- A0 if they also give an upper bound for $\mu$
---
2.
\begin{figure}[h]
\begin{center}
\includegraphics[alt={},max width=\textwidth]{a3f28425-4acf-4878-b0e3-15b5bc8a92d7-04_494_1116_226_415}
\captionsetup{labelformat=empty}
\caption{Figure 1}
\end{center}
\end{figure}
A uniform rod $A B$, of mass 6 kg and length 1.6 m , rests with its end $A$ on rough horizontal ground. The rod is held in equilibrium at $30 ^ { \circ }$ to the horizontal by a light string attached to the rod at $B$. The string is at $40 ^ { \circ }$ to the horizontal and lies in the same vertical plane as the rod, as shown in Figure 1. The tension in the string is $T$ newtons. The coefficient of friction between the ground and the rod is $\mu$.
\begin{enumerate}[label=(\alph*)]
\item Show that, to 3 significant figures, $T = 27.1$
\item Find the set of values of $\mu$ for which equilibrium is possible.
\includegraphics[max width=\textwidth, alt={}, center]{a3f28425-4acf-4878-b0e3-15b5bc8a92d7-07_27_40_2802_1893}
\end{enumerate}
\hfill \mbox{\textit{Edexcel M2 2018 Q2 [9]}}