| Exam Board | Edexcel |
|---|---|
| Module | Paper 3 (Paper 3) |
| Year | 2018 |
| Session | June |
| Marks | 13 |
| Paper | Download PDF ↗ |
| Mark scheme | Download PDF ↗ |
| Topic | Moments |
| Type | Rod hinged to wall with rough contact at free end |
| Difficulty | Standard +0.3 This is a standard A-level mechanics problem on moments with a horizontal rod. It requires taking moments about point A, resolving forces horizontally and vertically, and using given information systematically. The multi-part structure guides students through the solution, and the techniques (moments, resolution, trigonometry with tan α = 3/4) are all routine for this topic. Slightly easier than average due to the scaffolding and standard setup. |
| Spec | 3.04a Calculate moments: about a point3.04b Equilibrium: zero resultant moment and force |
| Answer | Marks | Guidance |
|---|---|---|
| Working/Answer | Mark | Guidance |
| Moments about \(A\) (or any other complete method) | M1 | 3.3 |
| \(T \cdot 2a\sin\alpha = Mga + 3Mgx\) | A1 | 1.1b |
| \(T = \frac{Mg(a+3x)}{2a \times \frac{3}{5}} = \frac{5Mg(3x+a)}{6a}\) * GIVEN ANSWER | A1* | 2.1 |
| Answer | Marks | Guidance |
|---|---|---|
| Working/Answer | Mark | Guidance |
| \(\frac{5Mg(3x+a)}{6a}\cos\alpha = 2Mg\) OR \(2Mg \cdot 2a\tan\alpha = Mga + 3Mgx\) | M1 | 3.1b |
| \(x = \frac{2a}{3}\) | A1 | 2.2a |
| Answer | Marks | Guidance |
|---|---|---|
| Working/Answer | Mark | Guidance |
| Resolve vertically OR Moments about \(B\) | M1 | 3.1b |
| \(Y = 3Mg + Mg - \frac{5Mg(3\cdot\frac{2a}{3}+a)}{6a}\sin\alpha\) or \(2aY = Mga + 3Mg(2a - \frac{2a}{3})\) Or: \(Y = 3Mg + Mg - \left(\frac{2Mg}{\cos\alpha}\right)\sin\alpha\) | A1ft | 1.1b |
| \(Y = \frac{5Mg}{2}\) | A1 | 1.1b |
| \(\tan\beta = \frac{Y}{X}\) or \(\frac{R\sin\beta}{R\cos\beta} = \frac{\frac{5Mg}{2}}{2Mg}\) | M1 | 3.4 |
| \(= \frac{5}{4}\) | A1 | 2.2a |
| Answer | Marks | Guidance |
|---|---|---|
| Working/Answer | Mark | Guidance |
| \(\frac{5Mg(3x+a)}{6a} \leq 5Mg\) and solve for \(x\) | M1 | 2.4 |
| \(x \leq \frac{5a}{3}\) | A1 | 2.4 |
| For rope not to break, block can't be more than \(\frac{5a}{3}\) from \(A\) | B1 A1 | 2.4 |
| Answer | Marks | Guidance |
|---|---|---|
| \(\sin\alpha = \frac{3}{5}\) used to obtain correct equation in \(a\), \(M\), \(x\) and \(T\) only | M1 | Using M(A) with usual rules or any other complete method |
| Correct equation | A1 | |
| Correct printed answer, correctly obtained, need to see \(\sin\alpha = \frac{3}{5}\) used | A1* | Given answer |
| Answer | Marks | Guidance |
|---|---|---|
| Accept \(0.67a\) or better | A1 | Using appropriate strategy e.g. resolve horizontally OR moments about \(C\); must use given expression for \(T\) |
| Answer | Marks | Guidance |
|---|---|---|
| \(Y\) (or \(R\sin\beta\)) \(= \frac{5Mg}{2}\) or \(2.5Mg\) or \(2.50Mg\) | A1 | Correct equation with \(x\) substituted in \(T\) expression or using \(T = \frac{2Mg}{\cos\alpha}\) |
| Equation in \(\tan\beta\) only using \(\tan\beta = \frac{Y}{X}\) or \(\tan\beta = \frac{X}{Y}\) | M1 | Independent but must have found a \(Y\) |
| Accept \(\frac{-5}{4}\) if it follows from working | A1 |
| Answer | Marks | Guidance |
|---|---|---|
| Allow \(x = \frac{5a}{3}\) or \(x < \frac{5a}{3}\); accept \(1.7a\) or better | A1 | Allow \(T = 5Mg\) or \(T < 5Mg\), solve for \(x\) showing all steps; M0 for \(T > 5Mg\) |
| Maximum value of \(x\) is \(\frac{5a}{3}\) | B1 | Treat as A1; any appropriate equivalent fully correct statement |
## Question 9:
### Part (a):
| Working/Answer | Mark | Guidance |
|---|---|---|
| Moments about $A$ (or any other complete method) | M1 | 3.3 |
| $T \cdot 2a\sin\alpha = Mga + 3Mgx$ | A1 | 1.1b |
| $T = \frac{Mg(a+3x)}{2a \times \frac{3}{5}} = \frac{5Mg(3x+a)}{6a}$ * GIVEN ANSWER | A1* | 2.1 |
### Part (b):
| Working/Answer | Mark | Guidance |
|---|---|---|
| $\frac{5Mg(3x+a)}{6a}\cos\alpha = 2Mg$ **OR** $2Mg \cdot 2a\tan\alpha = Mga + 3Mgx$ | M1 | 3.1b |
| $x = \frac{2a}{3}$ | A1 | 2.2a |
### Part (c):
| Working/Answer | Mark | Guidance |
|---|---|---|
| Resolve vertically **OR** Moments about $B$ | M1 | 3.1b |
| $Y = 3Mg + Mg - \frac{5Mg(3\cdot\frac{2a}{3}+a)}{6a}\sin\alpha$ or $2aY = Mga + 3Mg(2a - \frac{2a}{3})$ **Or:** $Y = 3Mg + Mg - \left(\frac{2Mg}{\cos\alpha}\right)\sin\alpha$ | A1ft | 1.1b |
| $Y = \frac{5Mg}{2}$ | A1 | 1.1b |
| $\tan\beta = \frac{Y}{X}$ or $\frac{R\sin\beta}{R\cos\beta} = \frac{\frac{5Mg}{2}}{2Mg}$ | M1 | 3.4 |
| $= \frac{5}{4}$ | A1 | 2.2a |
**Notes:**
- N.B. May use $R\sin\beta$ for $Y$ and/or $R\cos\beta$ for $X$ throughout
### Part (d):
| Working/Answer | Mark | Guidance |
|---|---|---|
| $\frac{5Mg(3x+a)}{6a} \leq 5Mg$ and solve for $x$ | M1 | 2.4 |
| $x \leq \frac{5a}{3}$ | A1 | 2.4 |
| For rope not to break, block can't be more than $\frac{5a}{3}$ from $A$ | B1 A1 | 2.4 |
**Notes:**
- N.B. If the correct inequality is not found, their comment must mention 'distance from $A$'
- Or just: $x \leq \frac{5a}{3}$, if no incorrect statement seen
# Question (from first page - appears to be Q9 based on context):
## Part (a):
| $\sin\alpha = \frac{3}{5}$ used to obtain correct equation in $a$, $M$, $x$ and $T$ only | M1 | Using M(A) with usual rules or any other complete method |
|---|---|---|
| Correct equation | A1 | |
| Correct printed answer, correctly obtained, need to see $\sin\alpha = \frac{3}{5}$ used | A1* | Given answer |
## Part (b):
| Accept $0.67a$ or better | A1 | Using appropriate strategy e.g. resolve horizontally OR moments about $C$; must use given expression for $T$ |
## Part (c):
| $Y$ (or $R\sin\beta$) $= \frac{5Mg}{2}$ or $2.5Mg$ or $2.50Mg$ | A1 | Correct equation with $x$ substituted in $T$ expression or using $T = \frac{2Mg}{\cos\alpha}$ |
| Equation in $\tan\beta$ only using $\tan\beta = \frac{Y}{X}$ or $\tan\beta = \frac{X}{Y}$ | M1 | Independent but must have found a $Y$ |
| Accept $\frac{-5}{4}$ if it follows from working | A1 | |
## Part (d):
| Allow $x = \frac{5a}{3}$ or $x < \frac{5a}{3}$; accept $1.7a$ or better | A1 | Allow $T = 5Mg$ or $T < 5Mg$, solve for $x$ showing all steps; M0 for $T > 5Mg$ |
| Maximum value of $x$ is $\frac{5a}{3}$ | B1 | Treat as A1; any appropriate equivalent fully correct statement |
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9.
\begin{figure}[h]
\begin{center}
\includegraphics[alt={},max width=\textwidth]{65e4b254-fb7b-45c2-9702-32f034018193-28_684_908_246_580}
\captionsetup{labelformat=empty}
\caption{Figure 3}
\end{center}
\end{figure}
A plank, $A B$, of mass $M$ and length $2 a$, rests with its end $A$ against a rough vertical wall. The plank is held in a horizontal position by a rope. One end of the rope is attached to the plank at $B$ and the other end is attached to the wall at the point $C$, which is vertically above $A$.
A small block of mass $3 M$ is placed on the plank at the point $P$, where $A P = x$. The plank is in equilibrium in a vertical plane which is perpendicular to the wall.
The angle between the rope and the plank is $\alpha$, where $\tan \alpha = \frac { 3 } { 4 }$, as shown in Figure 3 .\\
The plank is modelled as a uniform rod, the block is modelled as a particle and the rope is modelled as a light inextensible string.
\begin{enumerate}[label=(\alph*)]
\item Using the model, show that the tension in the rope is $\frac { 5 M g ( 3 x + a ) } { 6 a }$
The magnitude of the horizontal component of the force exerted on the plank at $A$ by the wall is $2 M g$.
\item Find $x$ in terms of $a$.
The force exerted on the plank at $A$ by the wall acts in a direction which makes an angle $\beta$ with the horizontal.
\item Find the value of $\tan \beta$
The rope will break if the tension in it exceeds $5 M g$.
\item Explain how this will restrict the possible positions of $P$. You must justify your answer carefully.
\end{enumerate}
\hfill \mbox{\textit{Edexcel Paper 3 2018 Q9 [13]}}