Edexcel Paper 3 2018 June — Question 9 13 marks

Exam BoardEdexcel
ModulePaper 3 (Paper 3)
Year2018
SessionJune
Marks13
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicMoments
TypeRod hinged to wall with rough contact at free end
DifficultyStandard +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.
Spec3.04a Calculate moments: about a point3.04b Equilibrium: zero resultant moment and force

9. \begin{figure}[h]
\includegraphics[alt={},max width=\textwidth]{65e4b254-fb7b-45c2-9702-32f034018193-28_684_908_246_580} \captionsetup{labelformat=empty} \caption{Figure 3}
\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.
  1. 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 \(2 M g\).
  2. 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.
  3. Find the value of \(\tan \beta\) The rope will break if the tension in it exceeds \(5 M g\).
  4. Explain how this will restrict the possible positions of \(P\). You must justify your answer carefully.

Question 9:
Part (a):
AnswerMarks Guidance
Working/AnswerMark 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 ANSWERA1* 2.1
Part (b):
AnswerMarks Guidance
Working/AnswerMark 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):
AnswerMarks Guidance
Working/AnswerMark 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):
AnswerMarks Guidance
Working/AnswerMark 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):
AnswerMarks Guidance
\(\sin\alpha = \frac{3}{5}\) used to obtain correct equation in \(a\), \(M\), \(x\) and \(T\) onlyM1 Using M(A) with usual rules or any other complete method
Correct equationA1
Correct printed answer, correctly obtained, need to see \(\sin\alpha = \frac{3}{5}\) usedA1* Given answer
Part (b):
AnswerMarks Guidance
Accept \(0.67a\) or betterA1 Using appropriate strategy e.g. resolve horizontally OR moments about \(C\); must use given expression for \(T\)
Part (c):
AnswerMarks 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 workingA1
Part (d):
AnswerMarks Guidance
Allow \(x = \frac{5a}{3}\) or \(x < \frac{5a}{3}\); accept \(1.7a\) or betterA1 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 |

---
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]}}