Edexcel M2 2015 January — Question 4 9 marks

Exam BoardEdexcel
ModuleM2 (Mechanics 2)
Year2015
SessionJanuary
Marks9
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicCentre of Mass 1
TypeParticle attached to lamina - find mass/position
DifficultyStandard +0.3 This is a standard M2 centre of mass question with two straightforward parts: (a) uses symmetry and the given centre of mass distance to find cos θ through basic coordinate geometry, and (b) applies the equilibrium condition for a suspended lamina with an attached particle. Both parts follow routine M2 procedures with no novel insight required, making it slightly easier than average.
Spec6.04c Composite bodies: centre of mass6.04e Rigid body equilibrium: coplanar forces

4. \begin{figure}[h]
\captionsetup{labelformat=empty} \caption{Figure 1}
\end{figure} The uniform plane lamina \(A B C D E F\) shown in Figure 1 is made from two identical rhombuses. Each rhombus has sides of length \(a\) and angle \(B A D =\) angle \(D A F = \theta\). The centre of mass of the lamina is \(0.9 a\) from \(A\).
  1. Show that \(\cos \theta = 0.8\) The weight of the lamina is \(W\). A particle of weight \(k W\) is fixed to the lamina at the point \(A\). The lamina is freely suspended from \(B\) and hangs in equilibrium with \(D A\) horizontal.
  2. Find the value of \(k\).

Question 4:
Part (a):
AnswerMarks Guidance
Answer/WorkingMark Guidance
Use total height \(A\) to \(C\); \(a + a\cos\theta\) seenB1
The centres of mass of the rhombuses lie on a straight line passing through the centre of massM1 Using symmetry of figure; condone sin/cos confusion
\(0.9a = \frac{1}{2}(a + a\cos\theta)\)A2 \(-1\) each error
\(\cos\theta = 0.8\)A1 Given answer
Alternative 1:
AnswerMarks Guidance
Answer/WorkingMark Guidance
Distance from \(A\) to centre of rhombus \(= a\cos\frac{\theta}{2}\)B1
\(\lambda\cdot a\cos\frac{\theta}{2}\cdot\cos\frac{\theta}{2} + \lambda\cdot a\cos\frac{\theta}{2}\cos\frac{\theta}{2} = 2\lambda\times0.9a\)M1, A2 Taking moments about axis through \(A\) parallel to \(FB\); condone sin/cos confusion; \(-1\) each error
\(\cos^2\frac{\theta}{2} = 0.9\)
\(\cos\theta = 2\cos^2\frac{\theta}{2} - 1 = 0.8\)A1 Given answer — from exact working
Alternative 2:
AnswerMarks Guidance
Answer/WorkingMark Guidance
Distance from \(A\) to centre of rhombus \(= a\cos\frac{\theta}{2}\)B1
The centres of mass of the rhombuses lie on a straight line through the centre of massM1 Using symmetry; condone sin/cos confusion
\(a\cos\frac{\theta}{2}\times\cos\frac{\theta}{2} = 0.9a\)A2 \(-1\) each error
\(\cos^2\frac{\theta}{2} = 0.9\)
\(\cos\theta = 2\cos^2\frac{\theta}{2} - 1 = 0.8\)A1 Given answer — from exact working
> Working backwards from \(\cos\theta = 0.8\) to deduce that the distance is \(0.9a\) is acceptable for 5/5.
Question Alt 3:
AnswerMarks Guidance
Answer/WorkingMarks Guidance
Correct division of lamina with correct mass ratios (table with EFBC, EDC, FAB, lamina rows showing \(2a^2\sin\theta\), \(a^2\sin\theta\cos\theta\), \(a^2\sin\theta\cos\theta\), \(2a^2\sin\theta\) and positions \(a\cos\theta+\frac{a}{2}\), \(a+\frac{2}{3}a\cos\theta\), \(\frac{2}{3}a\cos\theta\), \(0.9a\))B1 Correct division of lamina with correct mass ratios
\(2a^2\sin\theta\left(a\cos\theta+\frac{a}{2}\right)-a^2\sin\theta\cos\theta\left(\frac{2}{3}a\cos\theta+a-\frac{2}{3}a\cos\theta\right)=2a^2\sin\theta\times0.9a\)M1 A2 Moments equation – addition and subtraction of terms consistent with their division. -1 each error
\(\cos\theta=0.8\)A1 *Given answer*
Question Alt 4:
AnswerMarks Guidance
Answer/WorkingMarks Guidance
Correct division with EDF & BCD, AFD & ADB, lamina: masses \(2\times\frac{1}{2}a^2\sin\theta\), \(2\times\frac{1}{2}a^2\sin\theta\), \(2a^2\sin\theta\); positions \(\frac{2}{3}a(1+\cos\theta)\), \(\frac{1}{3}a(1+\cos\theta)\), \(0.9a\)B1 Correct division of lamina with correct mass ratios
\(2\times\frac{1}{3}a(1+\cos\theta)\times\frac{1}{2}a^2\sin\theta+2\times\frac{2}{3}a(1+\cos\theta)\times\frac{1}{2}a^2\sin\theta=2a^2\sin\theta\times0.9a\)M1 A2 Moments equation addition and subtraction of terms consistent with their division. -1 each error
\(\cos\theta=0.8\)A1 *Given answer*
Question Alt 5:
AnswerMarks Guidance
Answer/WorkingMarks Guidance
\(AM=a\cos\theta\)B1 Let M be the midpoint of FB. Centre of mass lies at the midpoint of DM
\(DM=a-a\cos\theta\)
\(0.9a=a\cos\theta+\frac{1}{2}(a-a\cos\theta)\)M1 A2
\(0.4a=\frac{1}{2}a\cos\theta\), \(\cos\theta=0.8\)A1 *Given answer*
Question Alt 6:
AnswerMarks Guidance
Answer/WorkingMarks Guidance
\(0.4a\) seen or implied (from diagram with measurements \(0.1a\), \(0.4a\), \(0.5a\))B1 \(0.4a\) seen or implied
\(\cos\theta=\frac{0.4a}{0.5a}\)M1 A2 Trig ratio for \(\theta\). Condone sin/cos confusion. Correct unsimplified expression
\(=0.8\)A1
Question 4(b):
AnswerMarks Guidance
Answer/WorkingMarks Guidance
\(kW(a\cos\theta)=W(0.9a-a\cos\theta)\)M1 A2 Taking moments about \(B\). Must have both terms. Condone trig & sign errors. -1 each error
\(0.8kW=0.1W\), \(k=\frac{1}{8}\)A1
Alt 4(b):
AnswerMarks Guidance
Answer/WorkingMarks Guidance
Centre of mass is on \(BF\)M1 Taking moments about A
\(0.9aW=(k+1)W\times a\cos\theta=(k+1)\times0.8aW\)A2 -1 each error
\(k=\frac{1}{8}\)A1
## Question 4:

### Part (a):

| Answer/Working | Mark | Guidance |
|---|---|---|
| Use total height $A$ to $C$; $a + a\cos\theta$ seen | B1 | |
| The centres of mass of the rhombuses lie on a straight line passing through the centre of mass | M1 | Using symmetry of figure; condone sin/cos confusion |
| $0.9a = \frac{1}{2}(a + a\cos\theta)$ | A2 | $-1$ each error |
| $\cos\theta = 0.8$ | A1 | **Given answer** |

**Alternative 1:**

| Answer/Working | Mark | Guidance |
|---|---|---|
| Distance from $A$ to centre of rhombus $= a\cos\frac{\theta}{2}$ | B1 | |
| $\lambda\cdot a\cos\frac{\theta}{2}\cdot\cos\frac{\theta}{2} + \lambda\cdot a\cos\frac{\theta}{2}\cos\frac{\theta}{2} = 2\lambda\times0.9a$ | M1, A2 | Taking moments about axis through $A$ parallel to $FB$; condone sin/cos confusion; $-1$ each error |
| $\cos^2\frac{\theta}{2} = 0.9$ | | |
| $\cos\theta = 2\cos^2\frac{\theta}{2} - 1 = 0.8$ | A1 | **Given answer** — from exact working |

**Alternative 2:**

| Answer/Working | Mark | Guidance |
|---|---|---|
| Distance from $A$ to centre of rhombus $= a\cos\frac{\theta}{2}$ | B1 | |
| The centres of mass of the rhombuses lie on a straight line through the centre of mass | M1 | Using symmetry; condone sin/cos confusion |
| $a\cos\frac{\theta}{2}\times\cos\frac{\theta}{2} = 0.9a$ | A2 | $-1$ each error |
| $\cos^2\frac{\theta}{2} = 0.9$ | | |
| $\cos\theta = 2\cos^2\frac{\theta}{2} - 1 = 0.8$ | A1 | **Given answer** — from exact working |

> Working backwards from $\cos\theta = 0.8$ to deduce that the distance is $0.9a$ is acceptable for 5/5.

## Question Alt 3:

| Answer/Working | Marks | Guidance |
|---|---|---|
| Correct division of lamina with correct mass ratios (table with EFBC, EDC, FAB, lamina rows showing $2a^2\sin\theta$, $a^2\sin\theta\cos\theta$, $a^2\sin\theta\cos\theta$, $2a^2\sin\theta$ and positions $a\cos\theta+\frac{a}{2}$, $a+\frac{2}{3}a\cos\theta$, $\frac{2}{3}a\cos\theta$, $0.9a$) | B1 | Correct division of lamina with correct mass ratios |
| $2a^2\sin\theta\left(a\cos\theta+\frac{a}{2}\right)-a^2\sin\theta\cos\theta\left(\frac{2}{3}a\cos\theta+a-\frac{2}{3}a\cos\theta\right)=2a^2\sin\theta\times0.9a$ | M1 A2 | Moments equation – addition and subtraction of terms consistent with their division. -1 each error |
| $\cos\theta=0.8$ | A1 | *Given answer* |

---

## Question Alt 4:

| Answer/Working | Marks | Guidance |
|---|---|---|
| Correct division with EDF & BCD, AFD & ADB, lamina: masses $2\times\frac{1}{2}a^2\sin\theta$, $2\times\frac{1}{2}a^2\sin\theta$, $2a^2\sin\theta$; positions $\frac{2}{3}a(1+\cos\theta)$, $\frac{1}{3}a(1+\cos\theta)$, $0.9a$ | B1 | Correct division of lamina with correct mass ratios |
| $2\times\frac{1}{3}a(1+\cos\theta)\times\frac{1}{2}a^2\sin\theta+2\times\frac{2}{3}a(1+\cos\theta)\times\frac{1}{2}a^2\sin\theta=2a^2\sin\theta\times0.9a$ | M1 A2 | Moments equation addition and subtraction of terms consistent with their division. -1 each error |
| $\cos\theta=0.8$ | A1 | *Given answer* |

---

## Question Alt 5:

| Answer/Working | Marks | Guidance |
|---|---|---|
| $AM=a\cos\theta$ | B1 | Let M be the midpoint of FB. Centre of mass lies at the midpoint of DM |
| $DM=a-a\cos\theta$ | | |
| $0.9a=a\cos\theta+\frac{1}{2}(a-a\cos\theta)$ | M1 A2 | |
| $0.4a=\frac{1}{2}a\cos\theta$, $\cos\theta=0.8$ | A1 | *Given answer* |

---

## Question Alt 6:

| Answer/Working | Marks | Guidance |
|---|---|---|
| $0.4a$ seen or implied (from diagram with measurements $0.1a$, $0.4a$, $0.5a$) | B1 | $0.4a$ seen or implied |
| $\cos\theta=\frac{0.4a}{0.5a}$ | M1 A2 | Trig ratio for $\theta$. Condone sin/cos confusion. Correct unsimplified expression |
| $=0.8$ | A1 | |

---

## Question 4(b):

| Answer/Working | Marks | Guidance |
|---|---|---|
| $kW(a\cos\theta)=W(0.9a-a\cos\theta)$ | M1 A2 | Taking moments about $B$. Must have both terms. Condone trig & sign errors. -1 each error |
| $0.8kW=0.1W$, $k=\frac{1}{8}$ | A1 | |

**Alt 4(b):**

| Answer/Working | Marks | Guidance |
|---|---|---|
| Centre of mass is on $BF$ | M1 | Taking moments about A |
| $0.9aW=(k+1)W\times a\cos\theta=(k+1)\times0.8aW$ | A2 | -1 each error |
| $k=\frac{1}{8}$ | A1 | |

---
4.

\begin{figure}[h]
\begin{center}
  \begin{tikzpicture}[line cap=round, line join=round]

    % Define parameters for the shape
    \def\a{4}           % Length of the side 'a'
    \def\thetaAngle{40} % Angle \theta from the vertical axis

    % Define coordinates based on the geometric properties
    % A is the origin
    \coordinate (A) at (0,0);
    
    % D is straight up from A, at distance 'a'
    \coordinate (D) at (0,\a);
    
    % B is rotated from the vertical by -\theta, at distance 'a' from A
    \coordinate (B) at (90-\thetaAngle:\a);
    
    % F is rotated from the vertical by \theta, at distance 'a' from A
    \coordinate (F) at (90+\thetaAngle:\a);
    
    % C is vertically above B by distance 'a'
    \coordinate (C) at ($(B)+(0,\a)$);
    
    % E is vertically above F by distance 'a'
    \coordinate (E) at ($(F)+(0,\a)$);

    % Draw the main solid boundary lines
    \draw[thick] (A) -- (B) -- (C) -- (D) -- (E) -- (F) -- cycle;

    % Draw the dashed line of symmetry
    \draw[thick, dashed] (A) -- (D);

    % Add vertex labels
    \node[below, yshift=-2pt] at (A) {$A$};
    \node[right, xshift=2pt]  at (B) {$B$};
    \node[above right]        at (C) {$C$};
    \node[above, yshift=2pt]  at (D) {$D$};
    \node[above left]         at (E) {$E$};
    \node[left, xshift=-2pt]  at (F) {$F$};

    % Add side length labels 'a'
    % The positions are chosen to match the reference image visually
    \path (A) -- (B) node[midway, below right=1pt] {$a$};
    \path (B) -- (C) node[midway, right=2pt]       {$a$};
    \path (D) -- (C) node[midway, above left=1pt]  {$a$};
    \path (D) -- (E) node[midway, above right=1pt] {$a$};
    \path (E) -- (F) node[midway, left=2pt]        {$a$};
    \path (F) -- (A) node[midway, below left=1pt]  {$a$};

    % Add angle arcs and labels for \theta
    \def\arcRad{0.6} % Radius for the angle arcs
    
    % Right angle \theta
    \draw (90-\thetaAngle:\arcRad) arc (90-\thetaAngle:90:\arcRad);
    \node at (90-\thetaAngle/2:\arcRad+0.25) {$\theta$};
    
    % Left angle \theta
    \draw (90:\arcRad) arc (90:90+\thetaAngle:\arcRad);
    \node at (90+\thetaAngle/2:\arcRad+0.25) {$\theta$};

\end{tikzpicture}
\captionsetup{labelformat=empty}
\caption{Figure 1}
\end{center}
\end{figure}

The uniform plane lamina $A B C D E F$ shown in Figure 1 is made from two identical rhombuses. Each rhombus has sides of length $a$ and angle $B A D =$ angle $D A F = \theta$. The centre of mass of the lamina is $0.9 a$ from $A$.
\begin{enumerate}[label=(\alph*)]
\item Show that $\cos \theta = 0.8$

The weight of the lamina is $W$. A particle of weight $k W$ is fixed to the lamina at the point $A$. The lamina is freely suspended from $B$ and hangs in equilibrium with $D A$ horizontal.
\item Find the value of $k$.
\end{enumerate}

\hfill \mbox{\textit{Edexcel M2 2015 Q4 [9]}}