OCR MEI M2 2005 June — Question 3 17 marks

Exam BoardOCR MEI
ModuleM2 (Mechanics 2)
Year2005
SessionJune
Marks17
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicCentre of Mass 1
TypeFrame with straight rod/wire components only
DifficultyStandard +0.3 This is a systematic centre of mass calculation requiring careful bookkeeping of multiple components (lamina + 6 rods) in both 2D and 3D configurations. While it involves several steps and coordinate systems, the techniques are entirely standard for M2: finding individual centres of mass, using the formula $\bar{x} = \frac{\sum m_i x_i}{\sum m_i}$, and applying equilibrium conditions. The 3D extension in part (ii) and the suspension angle in part (iii) add length but not conceptual difficulty beyond typical M2 questions.
Spec6.04b Find centre of mass: using symmetry6.04c Composite bodies: centre of mass6.04d Integration: for centre of mass of laminas/solids

3 Fig. 3.1 shows an object made up as follows. ABCD is a uniform lamina of mass \(16 \mathrm {~kg} . \mathrm { BE } , \mathrm { EF }\), FG, HI, IJ and JD are each uniform rods of mass 2 kg . ABCD, BEFG and HIJD are squares lying in the same plane. The dimensions in metres are shown in the figure. \begin{figure}[h]
\includegraphics[alt={},max width=\textwidth]{43d5bbfb-8726-4bcd-a73d-01728d532e98-4_627_648_429_735} \captionsetup{labelformat=empty} \caption{Fig. 3.1}
\end{figure}
  1. Find the coordinates of the centre of mass of the object, referred to the axes shown in Fig.3.1. The rods are now re-positioned so that BEFG and HIJD are perpendicular to the lamina, as shown in Fig. 3.2. \begin{figure}[h]
    \includegraphics[alt={},max width=\textwidth]{43d5bbfb-8726-4bcd-a73d-01728d532e98-4_442_666_1510_722} \captionsetup{labelformat=empty} \caption{Fig. 3.2}
    \end{figure}
  2. Find the \(x\)-, \(y\)-and \(z\)-coordinates of the centre of mass of the object, referred to the axes shown in Fig. 3.2. Calculate the distance of the centre of mass from A . The object is now freely suspended from A and hangs in equilibrium with AC at \(\alpha ^ { \circ }\) to the vertical.
  3. Calculate \(\alpha\).

Question 3:
Part (i):
AnswerMarks Guidance
WorkingMark Guidance
\(28\begin{pmatrix}\bar{x}\\\bar{y}\end{pmatrix} = 16\begin{pmatrix}2\\2\end{pmatrix} + 2\begin{pmatrix}5\\0\end{pmatrix} + 2\begin{pmatrix}6\\1\end{pmatrix} + 2\begin{pmatrix}5\\2\end{pmatrix} + 2\begin{pmatrix}0\\5\end{pmatrix} + 2\begin{pmatrix}1\\6\end{pmatrix} + 2\begin{pmatrix}2\\5\end{pmatrix}\)M1 Complete method
B1Total mass correct
B13 c.m. correct (or 4 \(x\)- or \(y\)-values correct)
\(\bar{x} = 2.5\)A1
\(\bar{y} = 2.5\)A1 [Allow A0 A1 if only error is in total mass]. [If \(\bar{x} = \bar{y}\) claimed by symmetry and only one component worked, replace final A1, A1 by B1 explicit claim of symmetry, A1 for the 2.5]
Part (ii):
AnswerMarks Guidance
WorkingMark Guidance
\(\bar{x} = \bar{y}\)B1 Or by direct calculation
\(28\bar{x} = 16 \times 2 + 6 \times 4 + 2 \times 0 + 2 \times 1 + 2 \times 2\)M1 Dealing with 'folded' parts for \(\bar{x}\) or for \(\bar{z}\)
\(\bar{x} = \frac{31}{14}\) (2.21428...)A1 At least 3 terms correct for \(\bar{x}\)
A1
\(\bar{z} = \frac{8 \times (-1) + 4 \times (-2)}{28} = -\frac{4}{7}\) (-0.57142...)A1 All terms correct allowing sign errors
A1
Distance is \(\sqrt{\left(\frac{31}{14}\right)^2 + \left(\frac{31}{14}\right)^2 + \left(\frac{4}{7}\right)^2}\)M1 Use of Pythagoras in 3D on their c.m.
\(= 3.18318...\) so \(3.18\) m (3 s.f.)F1
Part (iii):
AnswerMarks Guidance
WorkingMark Guidance
[Diagram with A above, \(\alpha\) shown, 3.18318... and 4/7 lengths, C at base]M1 c.m. clearly directly below A
B1Diagram showing \(\alpha\) and known lengths (or equivalent). FT their values. Award if final answer follows their values
\(\sin\alpha = \frac{4}{7} / 3.18318...\)M1 Appropriate expression for \(\alpha\). FT their values
so \(\alpha = 10.3415...\) so \(10.3°\) (3 s.f.)A1 cao
# Question 3:

## Part (i):
| Working | Mark | Guidance |
|---------|------|----------|
| $28\begin{pmatrix}\bar{x}\\\bar{y}\end{pmatrix} = 16\begin{pmatrix}2\\2\end{pmatrix} + 2\begin{pmatrix}5\\0\end{pmatrix} + 2\begin{pmatrix}6\\1\end{pmatrix} + 2\begin{pmatrix}5\\2\end{pmatrix} + 2\begin{pmatrix}0\\5\end{pmatrix} + 2\begin{pmatrix}1\\6\end{pmatrix} + 2\begin{pmatrix}2\\5\end{pmatrix}$ | M1 | Complete method |
| | B1 | Total mass correct |
| | B1 | 3 c.m. correct (or 4 $x$- or $y$-values correct) |
| $\bar{x} = 2.5$ | A1 | |
| $\bar{y} = 2.5$ | A1 | [Allow A0 A1 if only error is in total mass]. [If $\bar{x} = \bar{y}$ claimed by symmetry and only one component worked, replace final A1, A1 by B1 explicit claim of symmetry, A1 for the 2.5] |

## Part (ii):
| Working | Mark | Guidance |
|---------|------|----------|
| $\bar{x} = \bar{y}$ | B1 | Or by direct calculation |
| $28\bar{x} = 16 \times 2 + 6 \times 4 + 2 \times 0 + 2 \times 1 + 2 \times 2$ | M1 | Dealing with 'folded' parts for $\bar{x}$ or for $\bar{z}$ |
| $\bar{x} = \frac{31}{14}$ (2.21428...) | A1 | At least 3 terms correct for $\bar{x}$ |
| | A1 | |
| $\bar{z} = \frac{8 \times (-1) + 4 \times (-2)}{28} = -\frac{4}{7}$ (-0.57142...) | A1 | All terms correct allowing sign errors |
| | A1 | |
| Distance is $\sqrt{\left(\frac{31}{14}\right)^2 + \left(\frac{31}{14}\right)^2 + \left(\frac{4}{7}\right)^2}$ | M1 | Use of Pythagoras in 3D on **their** c.m. |
| $= 3.18318...$ so $3.18$ m (3 s.f.) | F1 | |

## Part (iii):
| Working | Mark | Guidance |
|---------|------|----------|
| [Diagram with A above, $\alpha$ shown, 3.18318... and 4/7 lengths, C at base] | M1 | c.m. clearly directly below A |
| | B1 | Diagram showing $\alpha$ and known lengths (or equivalent). FT their values. Award if final answer follows **their** values |
| $\sin\alpha = \frac{4}{7} / 3.18318...$ | M1 | Appropriate expression for $\alpha$. FT **their** values |
| so $\alpha = 10.3415...$ so $10.3°$ (3 s.f.) | A1 | cao |

---
3 Fig. 3.1 shows an object made up as follows. ABCD is a uniform lamina of mass $16 \mathrm {~kg} . \mathrm { BE } , \mathrm { EF }$, FG, HI, IJ and JD are each uniform rods of mass 2 kg . ABCD, BEFG and HIJD are squares lying in the same plane. The dimensions in metres are shown in the figure.

\begin{figure}[h]
\begin{center}
  \includegraphics[alt={},max width=\textwidth]{43d5bbfb-8726-4bcd-a73d-01728d532e98-4_627_648_429_735}
\captionsetup{labelformat=empty}
\caption{Fig. 3.1}
\end{center}
\end{figure}

(i) Find the coordinates of the centre of mass of the object, referred to the axes shown in Fig.3.1.

The rods are now re-positioned so that BEFG and HIJD are perpendicular to the lamina, as shown in Fig. 3.2.

\begin{figure}[h]
\begin{center}
  \includegraphics[alt={},max width=\textwidth]{43d5bbfb-8726-4bcd-a73d-01728d532e98-4_442_666_1510_722}
\captionsetup{labelformat=empty}
\caption{Fig. 3.2}
\end{center}
\end{figure}

(ii) Find the $x$-, $y$-and $z$-coordinates of the centre of mass of the object, referred to the axes shown in Fig. 3.2. Calculate the distance of the centre of mass from A .

The object is now freely suspended from A and hangs in equilibrium with AC at $\alpha ^ { \circ }$ to the vertical.\\
(iii) Calculate $\alpha$.

\hfill \mbox{\textit{OCR MEI M2 2005 Q3 [17]}}