| Exam Board | Edexcel |
|---|---|
| Module | FM2 AS (Further Mechanics 2 AS) |
| Year | 2020 |
| Session | June |
| Marks | 15 |
| Paper | Download PDF ↗ |
| Mark scheme | Download PDF ↗ |
| Topic | Centre of Mass 1 |
| Type | Particle attached to lamina - find mass/position |
| Difficulty | Standard +0.3 This is a standard Further Maths centre of mass question with straightforward application of formulas. Part (a) uses symmetry, parts (b) and (c) involve routine moment calculations, and part (d) requires basic trigonometry with the suspension condition. While it's a multi-part question requiring several steps, each part follows predictable patterns typical of FM2 centre of mass problems with no novel insights required. |
| Spec | 6.04b Find centre of mass: using symmetry6.04c Composite bodies: centre of mass6.04e Rigid body equilibrium: coplanar forces |
| Answer | Marks | Guidance |
|---|---|---|
| Answer/Working | Mark | Guidance |
| \(\frac{1}{2}a\) | B1 | 1.1b |
| Loaded lamina has a mass distribution which is symmetrical about the perpendicular bisector of \(AD\) | B1 | 2.4 |
| (2 marks) |
| Answer | Marks | Guidance |
|---|---|---|
| Answer/Working | Mark | Guidance |
| Moments about \(AD\) | M1 | 3.1a |
| \(6ma + m.2a = 12m\bar{x}\) | A1 | 1.1b |
| \(\bar{x} = \frac{2a}{3}\) * | A1* | 2.2a |
| (3 marks) |
| Answer | Marks | Guidance |
|---|---|---|
| Answer/Working | Mark | Guidance |
| Moments about \(AB\) | M1 | 3.1a |
| \(kma + 12m.\frac{1}{2}a = (k+12)m\bar{y}\) | A1 | 1.1b |
| A1 | 1.1b | |
| \(\bar{y} = \frac{(k+6)a}{(k+12)}\) * | A1* | 2.2a |
| (4 marks) |
| Answer | Marks | Guidance |
|---|---|---|
| Answer/Working | Mark | Guidance |
| Moments about \(AD\) | M1 | 3.1a |
| \(\bar{x}_1 = \frac{8a}{(k+12)}\) | A1 | 1.1b |
| Use of \(\tan\alpha = \frac{\bar{y}}{\bar{x}_1}\) | M1 | 1.1b |
| \(\frac{3}{2} = \dfrac{\dfrac{(k+6)a}{(k+12)}}{\dfrac{8a}{(k+12)}}\) | A1 | 1.1b |
| Solve for \(k\) | M1 | 1.1b |
| \(k = 6\) | A1 | 1.1b |
| SC: For use of \((\tan\alpha =)\frac{\text{their } \bar{y}}{\text{their } \bar{x}} = \frac{3}{2}\), M1A1M0A0M0A0 | ||
| (6 marks) |
## Question 1:
### Part (a):
| Answer/Working | Mark | Guidance |
|---|---|---|
| $\frac{1}{2}a$ | B1 | 1.1b |
| Loaded lamina has a mass distribution which is symmetrical about the perpendicular bisector of $AD$ | B1 | 2.4 |
| **(2 marks)** | | |
---
### Part (b):
| Answer/Working | Mark | Guidance |
|---|---|---|
| Moments about $AD$ | M1 | 3.1a |
| $6ma + m.2a = 12m\bar{x}$ | A1 | 1.1b |
| $\bar{x} = \frac{2a}{3}$ * | A1* | 2.2a |
| **(3 marks)** | | |
---
### Part (c):
| Answer/Working | Mark | Guidance |
|---|---|---|
| Moments about $AB$ | M1 | 3.1a |
| $kma + 12m.\frac{1}{2}a = (k+12)m\bar{y}$ | A1 | 1.1b |
| | A1 | 1.1b |
| $\bar{y} = \frac{(k+6)a}{(k+12)}$ * | A1* | 2.2a |
| **(4 marks)** | | |
---
### Part (d):
| Answer/Working | Mark | Guidance |
|---|---|---|
| Moments about $AD$ | M1 | 3.1a |
| $\bar{x}_1 = \frac{8a}{(k+12)}$ | A1 | 1.1b |
| Use of $\tan\alpha = \frac{\bar{y}}{\bar{x}_1}$ | M1 | 1.1b |
| $\frac{3}{2} = \dfrac{\dfrac{(k+6)a}{(k+12)}}{\dfrac{8a}{(k+12)}}$ | A1 | 1.1b |
| Solve for $k$ | M1 | 1.1b |
| $k = 6$ | A1 | 1.1b |
| **SC:** For use of $(\tan\alpha =)\frac{\text{their } \bar{y}}{\text{their } \bar{x}} = \frac{3}{2}$, M1A1M0A0M0A0 | | |
| **(6 marks)** | | |
---
**(15 marks total)**
1.
\begin{figure}[h]
\begin{center}
\includegraphics[alt={},max width=\textwidth]{0567d068-e23c-446e-9e11-f0c292972093-02_490_824_253_588}
\captionsetup{labelformat=empty}
\caption{Figure 1}
\end{center}
\end{figure}
Figure 1 shows a uniform rectangular lamina $A B C D$ with $A B = 2 a$ and $A D = a$ The mass of the lamina is $6 m$.
A particle of mass $2 m$ is attached to the lamina at $A$, a particle of mass $m$ is attached to the lamina at $B$ and a particle of mass $3 m$ is attached to the lamina at $D$, to form a loaded lamina $L$ of total mass $12 m$.
\begin{enumerate}[label=(\alph*)]
\item Write down the distance of the centre of mass of $L$ from $A B$. You must give a reason for your answer.
\item Show that the distance of the centre of mass of $L$ from $A D$ is $\frac { 2 a } { 3 }$
A particle of mass $k m$ is now also attached to $L$ at $D$ to form a new loaded lamina $N$.
\item Show that the distance of the centre of mass of $N$ from $A B$ is $\frac { ( k + 6 ) a } { ( k + 12 ) }$
When $N$ is freely suspended from $A$ and is hanging in equilibrium, the side $A B$ makes an angle $\alpha$ with the vertical, where $\tan \alpha = \frac { 3 } { 2 }$
\item Find the value of $k$.
\end{enumerate}
\hfill \mbox{\textit{Edexcel FM2 AS 2020 Q1 [15]}}