Edexcel M2 2018 June — Question 2 9 marks

Exam BoardEdexcel
ModuleM2 (Mechanics 2)
Year2018
SessionJune
Marks9
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicMoments
TypeRod with end on ground or wall supported by string
DifficultyStandard +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.
Spec6.04e Rigid body equilibrium: coplanar forces

2. \begin{figure}[h]
\includegraphics[alt={},max width=\textwidth]{a3f28425-4acf-4878-b0e3-15b5bc8a92d7-04_494_1116_226_415} \captionsetup{labelformat=empty} \caption{Figure 1}
\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 \(\mu\).
  1. Show that, to 3 significant figures, \(T = 27.1\)
  2. 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}

2a.
AnswerMarks
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.
AnswerMarks
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 \(\mu\)
## 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]}}