Edexcel M2 2014 June — Question 7 12 marks

Exam BoardEdexcel
ModuleM2 (Mechanics 2)
Year2014
SessionJune
Marks12
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicMoments
TypeRod hinged to wall with string support
DifficultyStandard +0.3 This is a standard M2 moments problem with a hinged rod in equilibrium. Part (a) requires taking moments about A and resolving vertically—routine techniques for this topic. Part (b) adds a simple step of finding the resultant force at a specific angle. The algebra is straightforward and the problem follows a familiar template for rod equilibrium questions.
Spec3.04b Equilibrium: zero resultant moment and force6.04e Rigid body equilibrium: coplanar forces

7. \begin{figure}[h]
\includegraphics[alt={},max width=\textwidth]{47420c50-c232-41e9-8c4d-a890d86ea933-12_837_565_226_694} \captionsetup{labelformat=empty} \caption{Figure 3}
\end{figure} A uniform rod \(A B\) of weight \(W\) has its end \(A\) freely hinged to a point on a fixed vertical wall. The rod is held in equilibrium, at angle \(\theta\) to the horizontal, by a force of magnitude \(P\). The force acts perpendicular to the rod at \(B\) and in the same vertical plane as the rod, as shown in Figure 3. The rod is in a vertical plane perpendicular to the wall. The magnitude of the vertical component of the force exerted on the rod by the wall at \(A\) is \(Y\).
  1. Show that \(Y = \frac { W } { 2 } \left( 2 - \cos ^ { 2 } \theta \right)\). Given that \(\theta = 45 ^ { \circ }\)
  2. find the magnitude of the force exerted on the rod by the wall at \(A\), giving your answer in terms of \(W\).

Question 7:
Part (a):
AnswerMarks Guidance
Answer/WorkingMarks Guidance
Resolving vertically: \(Y + P\cos\theta = W\)M1, A1 Needs all 3 terms. Condone sign errors and sin/cos confusion. Condone \(Wg\)
Moments about \(A\): \(Wl\cos\theta = 2lP\)M1, A1 Terms need to be correct structure, condone \(l\) implied if not seen
\(P = \frac{W\cos\theta}{2} \Rightarrow Y = W - \frac{W\cos^2\theta}{2} = \frac{W}{2}(2 - \cos^2\theta)\) \(\star\star\)DM1, A1 Substitute for \(P\) to obtain simplified \(Y\). Requires both preceding M marks. Obtain given result correctly
Part (b):
AnswerMarks Guidance
Answer/WorkingMarks Guidance
\(\theta = 45° \Rightarrow Y = \frac{3W}{4}\)B1
\(X = P\sin 45\)M1 Resolving horizontally. Accept in terms of \(\theta\)
\(= \frac{W\cos 45}{2} \cdot \sin 45 = \frac{W}{4}\)DM1, A1 Express \(X\) in terms of \(W\). Requires preceding M mark. Correct unsimplified but substituted
Resultant at \(A = \frac{W}{4}\sqrt{3^2 + 1^2} = \frac{W\sqrt{10}}{4}\) (\(0.79W\))DM1, A1 Use of Pythagoras with \(X\), \(Y\) in terms of \(W\) only. Dependent on first M1. Or equivalent (0.79\(W\) or better)
## Question 7:

### Part (a):

| Answer/Working | Marks | Guidance |
|---|---|---|
| Resolving vertically: $Y + P\cos\theta = W$ | M1, A1 | Needs all 3 terms. Condone sign errors and sin/cos confusion. Condone $Wg$ |
| Moments about $A$: $Wl\cos\theta = 2lP$ | M1, A1 | Terms need to be correct structure, condone $l$ implied if not seen |
| $P = \frac{W\cos\theta}{2} \Rightarrow Y = W - \frac{W\cos^2\theta}{2} = \frac{W}{2}(2 - \cos^2\theta)$ $\star\star$ | DM1, A1 | Substitute for $P$ to obtain simplified $Y$. Requires both preceding M marks. Obtain **given result** correctly |

### Part (b):

| Answer/Working | Marks | Guidance |
|---|---|---|
| $\theta = 45° \Rightarrow Y = \frac{3W}{4}$ | B1 | |
| $X = P\sin 45$ | M1 | Resolving horizontally. Accept in terms of $\theta$ |
| $= \frac{W\cos 45}{2} \cdot \sin 45 = \frac{W}{4}$ | DM1, A1 | Express $X$ in terms of $W$. Requires preceding M mark. Correct unsimplified but substituted |
| Resultant at $A = \frac{W}{4}\sqrt{3^2 + 1^2} = \frac{W\sqrt{10}}{4}$ ($0.79W$) | DM1, A1 | Use of Pythagoras with $X$, $Y$ in terms of $W$ only. Dependent on first M1. Or equivalent (0.79$W$ or better) |

---
7.

\begin{figure}[h]
\begin{center}
  \includegraphics[alt={},max width=\textwidth]{47420c50-c232-41e9-8c4d-a890d86ea933-12_837_565_226_694}
\captionsetup{labelformat=empty}
\caption{Figure 3}
\end{center}
\end{figure}

A uniform rod $A B$ of weight $W$ has its end $A$ freely hinged to a point on a fixed vertical wall. The rod is held in equilibrium, at angle $\theta$ to the horizontal, by a force of magnitude $P$. The force acts perpendicular to the rod at $B$ and in the same vertical plane as the rod, as shown in Figure 3. The rod is in a vertical plane perpendicular to the wall. The magnitude of the vertical component of the force exerted on the rod by the wall at $A$ is $Y$.
\begin{enumerate}[label=(\alph*)]
\item Show that $Y = \frac { W } { 2 } \left( 2 - \cos ^ { 2 } \theta \right)$.

Given that $\theta = 45 ^ { \circ }$
\item find the magnitude of the force exerted on the rod by the wall at $A$, giving your answer in terms of $W$.
\end{enumerate}

\hfill \mbox{\textit{Edexcel M2 2014 Q7 [12]}}