Edexcel M2 2018 Specimen — Question 5 10 marks

Exam BoardEdexcel
ModuleM2 (Mechanics 2)
Year2018
SessionSpecimen
Marks10
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 problem requiring students to find the COM of a composite lamina, add a particle, then use equilibrium conditions with a given angle. It involves routine techniques (composite COM, moments about suspension point) with straightforward algebra, making it slightly easier than average for M2 level.
Spec6.04b Find centre of mass: using symmetry6.04c Composite bodies: centre of mass6.04e Rigid body equilibrium: coplanar forces

5. Figure 2 The uniform lamina \(A B C D E F\), shown in Figure 2, consists of two identical rectangles with sides of length \(a\) and \(3 a\). The mass of the lamina is \(M\). A particle of mass \(k M\) is attached to the lamina at \(E\). The lamina, with the attached particle, is freely suspended from \(A\) and hangs in equilibrium with \(A F\) at an angle \(\theta\) to the downward vertical. Given that \(\tan \theta = \frac { 4 } { 7 }\), find the value of \(k\). \includegraphics[max width=\textwidth, alt={}, center]{f30ed5b8-880e-42de-860e-d1538fa68f11-16_677_677_244_580}
VIIIV SIHI NI JIIIM ION OCVIIV SIHI NI JAHAM ION OOVI4V SIHIL NI JIIIM ION OC

Question 5:
Moments about vertical axis (AF):
AnswerMarks Guidance
WorkingMark Guidance
\(\frac{Mg}{2}\times\frac{1}{2}a+\frac{Mg}{2}\times 1.5a+3akMg=Mg(1+k)\bar{x}\)M1 Requires all terms, dimensionally correct but condone \(g\) missing
Above equation correctA2 -1 each error; accept with \(M\) and/or \(g\) not seen
\(\bar{x}=\frac{1+3k}{1+k}a\)
Moments about horizontal axis (AB or FE):
AnswerMarks Guidance
WorkingMark Guidance
\(\frac{Mg}{2}\times 1.5a+\frac{Mg}{2}\times 3.5a+4akMg=Mg(1+k)\bar{y}\)M1 Requires all terms, dimensionally correct but condone \(g\) missing
Above equation correctA2 -1 each error; accept with \(M\) and/or \(g\) not seen; do not penalise repeated errors
\(\bar{y}=\frac{2.5+4k}{1+k}a\)
*Note: Working with axes through F gives \(\bar{x}=\frac{1+3k}{1+k}a\) and \(\bar{y}=\frac{1.5}{1+k}a\)*
*SR: A candidate working with a mixture of mass and mass ratio can score 4/6: M1A0A0M1A2*
Finding \(\tan\theta\):
AnswerMarks Guidance
WorkingMark Guidance
Use of \(\tan\theta\) with their distances from \(AF\) and \(AB\)M1 Must be considering whole system; allow for inverted ratio
\(\tan\theta=\frac{M+3kM}{2.5M+4kM}\left(=\frac{4}{7}\right)\)A1 Or exact equivalent
Solving for k:
AnswerMarks Guidance
WorkingMark Guidance
Equate their \(\tan\theta\) to \(\frac{4}{7}\) and solve for \(k\)M1
\(7M+21kM=10M+16kM\)
\(k=\frac{3}{5}\)A1 cso
(10)
Alternative (L-shape first):
AnswerMarks Guidance
WorkingMark Guidance
\(\bar{x}=a\) and \(\bar{y}=\frac{5}{2}a\) or \(\frac{3}{2}a\)M1A2 M1 requires all terms, dimensionally correct, condone \(g/M\) missing; A1 for each correct
Combine with the particleM1A2 M1 requires all terms, dimensionally correct, condone \(g\) missing; A1 for each correct
Geometrical approach:
AnswerMarks Guidance
WorkingMark Guidance
Centre of mass at \(\left(a,\frac{3}{2}a\right)\) relative to \(F\)M1A2
Use of \(\tan\theta\) to find \(d_1\) or \(d_2\)M1
\(\left(\frac{5}{2}a\right)\tan\theta - a = \frac{3}{7}a\)A1 Correct for their centre of mass
\(d_1=\left(\frac{3}{7}a\right)\cos\theta\)A1 Correct for their centre of mass
\(3a-4a\tan\theta=\frac{5}{7}a\)M1 Use of \(\tan\theta\) to find second distance
\(d_2=\frac{5}{7}a\cos\theta\)A1
Moments about \(A\): \(Md_1=kMd_2\)M1
\(\frac{3}{7}a\cos\theta=k\times\frac{5}{7}a\cos\theta\Rightarrow k=\frac{3}{5}\)A1
(10)
## Question 5:

**Moments about vertical axis (AF):**

| Working | Mark | Guidance |
|---------|------|----------|
| $\frac{Mg}{2}\times\frac{1}{2}a+\frac{Mg}{2}\times 1.5a+3akMg=Mg(1+k)\bar{x}$ | M1 | Requires all terms, dimensionally correct but condone $g$ missing |
| Above equation correct | A2 | -1 each error; accept with $M$ and/or $g$ not seen |
| $\bar{x}=\frac{1+3k}{1+k}a$ | — | — |

**Moments about horizontal axis (AB or FE):**

| Working | Mark | Guidance |
|---------|------|----------|
| $\frac{Mg}{2}\times 1.5a+\frac{Mg}{2}\times 3.5a+4akMg=Mg(1+k)\bar{y}$ | M1 | Requires all terms, dimensionally correct but condone $g$ missing |
| Above equation correct | A2 | -1 each error; accept with $M$ and/or $g$ not seen; do not penalise repeated errors |
| $\bar{y}=\frac{2.5+4k}{1+k}a$ | — | — |

*Note: Working with axes through F gives $\bar{x}=\frac{1+3k}{1+k}a$ and $\bar{y}=\frac{1.5}{1+k}a$*

*SR: A candidate working with a mixture of mass and mass ratio can score 4/6: M1A0A0M1A2*

**Finding $\tan\theta$:**

| Working | Mark | Guidance |
|---------|------|----------|
| Use of $\tan\theta$ with their distances from $AF$ and $AB$ | M1 | Must be considering whole system; allow for inverted ratio |
| $\tan\theta=\frac{M+3kM}{2.5M+4kM}\left(=\frac{4}{7}\right)$ | A1 | Or exact equivalent |

**Solving for k:**

| Working | Mark | Guidance |
|---------|------|----------|
| Equate their $\tan\theta$ to $\frac{4}{7}$ and solve for $k$ | M1 | — |
| $7M+21kM=10M+16kM$ | — | — |
| $k=\frac{3}{5}$ | A1 | cso |
| | **(10)** | |

**Alternative (L-shape first):**

| Working | Mark | Guidance |
|---------|------|----------|
| $\bar{x}=a$ and $\bar{y}=\frac{5}{2}a$ or $\frac{3}{2}a$ | M1A2 | M1 requires all terms, dimensionally correct, condone $g/M$ missing; A1 for each correct |
| Combine with the particle | M1A2 | M1 requires all terms, dimensionally correct, condone $g$ missing; A1 for each correct |

**Geometrical approach:**

| Working | Mark | Guidance |
|---------|------|----------|
| Centre of mass at $\left(a,\frac{3}{2}a\right)$ relative to $F$ | M1A2 | — |
| Use of $\tan\theta$ to find $d_1$ or $d_2$ | M1 | — |
| $\left(\frac{5}{2}a\right)\tan\theta - a = \frac{3}{7}a$ | A1 | Correct for their centre of mass |
| $d_1=\left(\frac{3}{7}a\right)\cos\theta$ | A1 | Correct for their centre of mass |
| $3a-4a\tan\theta=\frac{5}{7}a$ | M1 | Use of $\tan\theta$ to find second distance |
| $d_2=\frac{5}{7}a\cos\theta$ | A1 | — |
| Moments about $A$: $Md_1=kMd_2$ | M1 | — |
| $\frac{3}{7}a\cos\theta=k\times\frac{5}{7}a\cos\theta\Rightarrow k=\frac{3}{5}$ | A1 | |
| | **(10)** | |

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5.

Figure 2

The uniform lamina $A B C D E F$, shown in Figure 2, consists of two identical rectangles with sides of length $a$ and $3 a$. The mass of the lamina is $M$. A particle of mass $k M$ is attached to the lamina at $E$. The lamina, with the attached particle, is freely suspended from $A$ and hangs in equilibrium with $A F$ at an angle $\theta$ to the downward vertical.

Given that $\tan \theta = \frac { 4 } { 7 }$, find the value of $k$.\\
\includegraphics[max width=\textwidth, alt={}, center]{f30ed5b8-880e-42de-860e-d1538fa68f11-16_677_677_244_580}

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VIIIV SIHI NI JIIIM ION OC & VIIV SIHI NI JAHAM ION OO & VI4V SIHIL NI JIIIM ION OC \\
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\hfill \mbox{\textit{Edexcel M2 2018 Q5 [10]}}