Edexcel M2 2016 January — Question 5 10 marks

Exam BoardEdexcel
ModuleM2 (Mechanics 2)
Year2016
SessionJanuary
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 finding the centroid of a composite lamina, then applying the equilibrium condition that the combined centre of mass lies vertically below the suspension point. The geometry is straightforward (two identical rectangles), and the method is routine: find individual centroids, combine with the particle using moments, then use the given angle to set up an equation for k. Slightly easier than average due to the symmetric shape and clear setup.
Spec6.04b Find centre of mass: using symmetry6.04c Composite bodies: centre of mass6.04e Rigid body equilibrium: coplanar forces

5. \begin{figure}[h]
\includegraphics[alt={},max width=\textwidth]{e6d100ff-dd4a-4591-a0a3-81761773045e-09_689_581_237_683} \captionsetup{labelformat=empty} \caption{Figure 2}
\end{figure} 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 \(k\).
(10)

Question 5:
AnswerMarks Guidance
Working/AnswerMarks Guidance
Moments about vertical axis (\(AF\)):M1 Requires all terms and dimensionally correct but condone \(g\) missing
\(\frac{Mg}{2} \times \frac{1}{2}a + \frac{Mg}{2} \times 1.5a + 3akMg = Mg(1+k)\bar{x}\)A2 \(-1\) each error. Accept with \(M\) and/or \(g\) not seen.
\(\left(\bar{x} = \frac{1+3k}{1+k}a\right)\)
Moments about horizontal axis (\(AB\) or \(FE\)):M1 Requires all terms and dimensionally correct but condone \(g\) missing
\(\frac{Mg}{2} \times 1.5a + \frac{Mg}{2} \times 3.5a + 4akMg = Mg(1+k)\bar{y}\)A2 \(-1\) each error. Accept with \(M\) and/or \(g\) not seen. Do not penalise repeated errors.
\(\left(\bar{y} = \frac{2.5+4k}{1+k}a\right)\)
Use of \(\tan\theta\) with their distances from \(AF\) & \(AB\)M1 Must be considering the whole system. Allow for inverted ratio.
\(\tan\theta = \frac{M + 3kM}{2.5M + 4kM}\left(= \frac{4}{7}\right)\)A1 or exact equivalent
Equate their \(\tan\theta\) to \(\frac{4}{7}\) and solve for \(k\): \(7M + 21kM = 10M + 16kM\)M1
\(k = \frac{3}{5}\)A1 CSO
Question (Centre of Mass / Tilting Problem):
AnswerMarks Guidance
Answer/WorkingMark Guidance
Use of \(\tan\theta\) with their distances for finding \(d_1\) or \(d_2\)M1
\(\left(\frac{5}{2}a\right)\tan\theta - a \left(=\frac{3}{7}a\right)\)A1 Correct for their centre of mass; obtain length of a side in a triangle containing \(d_1\)
\(d_1 = \left(\frac{3}{7}a\right)\cos\theta\)A1 Correct for their centre of mass
Use of \(\tan\theta\) to find second distance: \(3a - 4a\tan\theta = \frac{5}{7}a\)M1
\(d_2 = \frac{5}{7}a\cos\theta\)A1 Correct for their centre of mass
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
Total(10) Candidate may start by finding centre of mass at \(\left(a, \frac{3}{2}a\right)\) relative to \(F\); M1A2 scored
Question 6a:
AnswerMarks Guidance
Answer/WorkingMark Guidance
Taking moments about \(A\)M1 Requires all terms; condone trig confusion and sign errors
\(bF = 3mga\cos\theta + mg \times 2a\cos\theta\)A2 -1 each error
\(bF = 5mga\cos\theta \quad F = \frac{5mga}{b}\cos\theta\)A1 Given answer
Total(4)
Question 6b:
AnswerMarks Guidance
Answer/WorkingMark Guidance
Component of \(\mathbf{R}\) parallel to \(AB\): \(R\cos(\phi-\theta)\)M1 Requires all terms; condone trig confusion
\(= 3mg\sin\theta + mg\sin\theta = 4mg\sin\theta\)A1 Correct unsimplified
Component of \(\mathbf{R}\) perpendicular to \(AB\)M1 Requires all terms; condone consistent trig confusion and sign errors
\(R\sin(\phi-\theta) + F = 4mg\cos\theta\)A1 Correct unsimplified
\(R\sin(\phi-\theta) = 4mg\cos\theta - \frac{5mga}{b}\cos\theta\)A1 Correct with \(F\) substituted
Total(5) ISW for incorrect work after correct components seen
Alternatives via \(M(B)\): \(2aR\sin(\phi-\theta) + 3mga\cos\theta = F(2a-b)\)
Via \(M(C)\): \(bR\sin(\phi-\theta) + (2a-b)mg\cos\theta = 3mg(b-a)\cos\theta\)
Special Case (misread of directions in 6b):
AnswerMarks Guidance
Answer/WorkingMark Guidance
\(X = F\sin\theta = \frac{5mga}{b}\cos\theta\sin\theta\)M1 Allow with \(F\); requires all terms
A1\(F\) substituted
\(Y = 4mg - F\cos\theta = 4mg - \frac{5mga}{b}\cos^2\theta\)M1 Allow with \(F\); requires all terms
A1Correct unsimplified
A1Correct substituted
Question 6c:
AnswerMarks Guidance
Answer/WorkingMark Guidance
Use of \(R\sin(\phi-\theta) > 0\)M1
\(4 > \frac{5a}{b}\), \(\quad (2a\geq)b > \frac{5}{4}a\)A1 \(2a\) not required; CSO
Total(2)
Alternative (from SC misread):
AnswerMarks Guidance
Answer/WorkingMark Guidance
For \(\varphi > \theta\), \(\tan\phi > \tan\theta\)
\(\tan\varphi = \frac{Y}{X} = \dfrac{4 - \frac{5a}{b}\cos^2\theta}{\frac{5a}{b}\cos\theta\sin\theta} > \tan\theta\)M1
\(4 - \frac{5a}{b}\cos^2\theta > \frac{5a}{b}\sin^2\theta\)
\(4 > \frac{5a}{b}(\cos^2\theta + \sin^2\theta) \Rightarrow b > \frac{5}{4}a\)A1 CSO
Question 7a:
AnswerMarks Guidance
Answer/WorkingMark Guidance
Equate horizontal components of speedsM1
\(u\cos\theta^\circ = 6\cos 45^\circ \left(= 3\sqrt{2}\right)\) (4.24...)A1 Correct unsimplified
Use suvat for vertical speeds: \(u\sin\theta^\circ - 2g = -6\sin 45^\circ\)M1 Condone sign errors
\(u\sin\theta = 2g - 3\sqrt{2}\)A1 Correct unsimplified
Divide to find \(\tan\theta\): \(\tan\theta = \dfrac{2g - 6\sin 45}{6\cos 45}\)DM1 Dependent on previous 2 Ms; follow their components
\(\left(= \dfrac{2g - 3\sqrt{2}}{3\sqrt{2}} = 3.61..\right) \Rightarrow \theta = 74.6\ (75)\)A1 \((u = 15.93...)\)
Total(6)
Question 7b:
AnswerMarks Guidance
Answer/WorkingMark Guidance
At max height, speed \(= u\cos\theta \left(= 3\sqrt{2}\ \text{ms}^{-1}\right)\)B1
\(KE = \frac{1}{2} \times 0.7 \times \left(3\sqrt{2}\right)^2\) (J)M1 Correct for their \(v\) at the top, \(v\neq 0\)
\(= 6.3\) (J)A1 Accept awrt 6.30; CSO
Total(3)
Question 7c:
AnswerMarks Guidance
Answer/WorkingMark Guidance
When P is moving upwards at \(6\ \text{ms}^{-1}\)M1 Use suvat to find first time \(v=6\)
\(u\sin\theta - gt = 3\sqrt{2}\)A1
\(2g - 3\sqrt{2} - gt = 3\sqrt{2}\)M1 Solve for \(t\)
\(t = \dfrac{2g - 6\sqrt{2}}{g} = 1.13...\)A1 Sensitive to premature approximation; allow 1.14
\(T = 2 - 1.13... = 0.87\)A1 CAO accept awrt 0.87
Total(5)
Alternative 7c (Method 1):
AnswerMarks Guidance
Answer/WorkingMark Guidance
\(6\sin 45 = 0 + gt\)M1A1 Find time from top to \(A\)
\(T = 2t = \dfrac{12\sqrt{2}/2}{g} = 0.87\)M1, A1, A1 Correct strategy; correct unsimplified
Alternative 7c (Method 2):
AnswerMarks Guidance
Answer/WorkingMark Guidance
\(u\sin\theta = gt\) (their \(u,\theta\))M1 Time to top
\(t = 1.567...\)A1
\(T = 2(2 - 1.567...)\)M1A1
\(= 0.87\)A1
Alternative 7c (Method 3):
AnswerMarks Guidance
Answer/WorkingMark Guidance
Vertical speed at \(A = -(\text{vertical speed at }B) = \sqrt{36-(3\sqrt{2})^2} = 3\sqrt{2}\)M1, A1 Or use the \(45°\) angle
Use \(v = u + at\) for \(A\to B\): \(-3\sqrt{2} = 3\sqrt{2} - gT\)M1, A1 Correct use for their values
\(T = 0.87\)A1
Question Alt 7d:
AnswerMarks Guidance
Answer/WorkingMark Guidance
\(v^2 = \left(3\sqrt{2}\right)^2 + \left(u\sin\theta - gt\right)^2 \leq 36\)M1 Form expression for \(v^2\); inequality not needed at this stage
A1Correct inequality for \(v^2\)
\(-\sqrt{18} \leq u\sin\theta - gt \leq \sqrt{18}\)M1
\(\dfrac{u\sin\theta - \sqrt{18}}{g} \leq t \leq \dfrac{u\sin\theta + \sqrt{18}}{g}\)A1
\(T = \dfrac{u\sin\theta + \sqrt{18}}{g} - \dfrac{u\sin\theta - \sqrt{18}}{g} = \dfrac{2\sqrt{18}}{g} = 0.866\)A1
Total(5)
# Question 5:

| Working/Answer | Marks | Guidance |
|---|---|---|
| Moments about **vertical** axis ($AF$): | M1 | Requires all terms and dimensionally correct but condone $g$ missing |
| $\frac{Mg}{2} \times \frac{1}{2}a + \frac{Mg}{2} \times 1.5a + 3akMg = Mg(1+k)\bar{x}$ | A2 | $-1$ each error. Accept with $M$ and/or $g$ not seen. |
| $\left(\bar{x} = \frac{1+3k}{1+k}a\right)$ | | |
| Moments about **horizontal** axis ($AB$ or $FE$): | M1 | Requires all terms and dimensionally correct but condone $g$ missing |
| $\frac{Mg}{2} \times 1.5a + \frac{Mg}{2} \times 3.5a + 4akMg = Mg(1+k)\bar{y}$ | A2 | $-1$ each error. Accept with $M$ and/or $g$ not seen. Do not penalise repeated errors. |
| $\left(\bar{y} = \frac{2.5+4k}{1+k}a\right)$ | | |
| Use of $\tan\theta$ with their distances from $AF$ & $AB$ | M1 | Must be considering the whole system. Allow for inverted ratio. |
| $\tan\theta = \frac{M + 3kM}{2.5M + 4kM}\left(= \frac{4}{7}\right)$ | A1 | or exact equivalent |
| Equate their $\tan\theta$ to $\frac{4}{7}$ and solve for $k$: $7M + 21kM = 10M + 16kM$ | M1 | |
| $k = \frac{3}{5}$ | A1 | CSO |

# Question (Centre of Mass / Tilting Problem):

| Answer/Working | Mark | Guidance |
|---|---|---|
| Use of $\tan\theta$ with their distances for finding $d_1$ or $d_2$ | M1 | |
| $\left(\frac{5}{2}a\right)\tan\theta - a \left(=\frac{3}{7}a\right)$ | A1 | Correct for their centre of mass; obtain length of a side in a triangle containing $d_1$ |
| $d_1 = \left(\frac{3}{7}a\right)\cos\theta$ | A1 | Correct for their centre of mass |
| Use of $\tan\theta$ to find second distance: $3a - 4a\tan\theta = \frac{5}{7}a$ | M1 | |
| $d_2 = \frac{5}{7}a\cos\theta$ | A1 | Correct for their centre of mass |
| 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 | |
| **Total** | **(10)** | Candidate may start by finding centre of mass at $\left(a, \frac{3}{2}a\right)$ relative to $F$; M1A2 scored |

---

# Question 6a:

| Answer/Working | Mark | Guidance |
|---|---|---|
| Taking moments about $A$ | M1 | Requires all terms; condone trig confusion and sign errors |
| $bF = 3mga\cos\theta + mg \times 2a\cos\theta$ | A2 | -1 each error |
| $bF = 5mga\cos\theta \quad F = \frac{5mga}{b}\cos\theta$ | A1 | **Given answer** |
| **Total** | **(4)** | |

---

# Question 6b:

| Answer/Working | Mark | Guidance |
|---|---|---|
| Component of $\mathbf{R}$ parallel to $AB$: $R\cos(\phi-\theta)$ | M1 | Requires all terms; condone trig confusion |
| $= 3mg\sin\theta + mg\sin\theta = 4mg\sin\theta$ | A1 | Correct unsimplified |
| Component of $\mathbf{R}$ perpendicular to $AB$ | M1 | Requires all terms; condone consistent trig confusion and sign errors |
| $R\sin(\phi-\theta) + F = 4mg\cos\theta$ | A1 | Correct unsimplified |
| $R\sin(\phi-\theta) = 4mg\cos\theta - \frac{5mga}{b}\cos\theta$ | A1 | Correct with $F$ substituted |
| **Total** | **(5)** | ISW for incorrect work after correct components seen |

Alternatives via $M(B)$: $2aR\sin(\phi-\theta) + 3mga\cos\theta = F(2a-b)$

Via $M(C)$: $bR\sin(\phi-\theta) + (2a-b)mg\cos\theta = 3mg(b-a)\cos\theta$

**Special Case (misread of directions in 6b):**

| Answer/Working | Mark | Guidance |
|---|---|---|
| $X = F\sin\theta = \frac{5mga}{b}\cos\theta\sin\theta$ | M1 | Allow with $F$; requires all terms |
| | A1 | $F$ substituted |
| $Y = 4mg - F\cos\theta = 4mg - \frac{5mga}{b}\cos^2\theta$ | M1 | Allow with $F$; requires all terms |
| | A1 | Correct unsimplified |
| | A1 | Correct substituted |

---

# Question 6c:

| Answer/Working | Mark | Guidance |
|---|---|---|
| Use of $R\sin(\phi-\theta) > 0$ | M1 | |
| $4 > \frac{5a}{b}$, $\quad (2a\geq)b > \frac{5}{4}a$ | A1 | $2a$ not required; CSO |
| **Total** | **(2)** | |

**Alternative (from SC misread):**

| Answer/Working | Mark | Guidance |
|---|---|---|
| For $\varphi > \theta$, $\tan\phi > \tan\theta$ | | |
| $\tan\varphi = \frac{Y}{X} = \dfrac{4 - \frac{5a}{b}\cos^2\theta}{\frac{5a}{b}\cos\theta\sin\theta} > \tan\theta$ | M1 | |
| $4 - \frac{5a}{b}\cos^2\theta > \frac{5a}{b}\sin^2\theta$ | | |
| $4 > \frac{5a}{b}(\cos^2\theta + \sin^2\theta) \Rightarrow b > \frac{5}{4}a$ | A1 | CSO |

---

# Question 7a:

| Answer/Working | Mark | Guidance |
|---|---|---|
| Equate horizontal components of speeds | M1 | |
| $u\cos\theta^\circ = 6\cos 45^\circ \left(= 3\sqrt{2}\right)$ (4.24...) | A1 | Correct unsimplified |
| Use suvat for vertical speeds: $u\sin\theta^\circ - 2g = -6\sin 45^\circ$ | M1 | Condone sign errors |
| $u\sin\theta = 2g - 3\sqrt{2}$ | A1 | Correct unsimplified |
| Divide to find $\tan\theta$: $\tan\theta = \dfrac{2g - 6\sin 45}{6\cos 45}$ | DM1 | Dependent on previous 2 Ms; follow their components |
| $\left(= \dfrac{2g - 3\sqrt{2}}{3\sqrt{2}} = 3.61..\right) \Rightarrow \theta = 74.6\ (75)$ | A1 | $(u = 15.93...)$ |
| **Total** | **(6)** | |

---

# Question 7b:

| Answer/Working | Mark | Guidance |
|---|---|---|
| At max height, speed $= u\cos\theta \left(= 3\sqrt{2}\ \text{ms}^{-1}\right)$ | B1 | |
| $KE = \frac{1}{2} \times 0.7 \times \left(3\sqrt{2}\right)^2$ (J) | M1 | Correct for their $v$ at the top, $v\neq 0$ |
| $= 6.3$ (J) | A1 | Accept awrt 6.30; CSO |
| **Total** | **(3)** | |

---

# Question 7c:

| Answer/Working | Mark | Guidance |
|---|---|---|
| When P is moving upwards at $6\ \text{ms}^{-1}$ | M1 | Use suvat to find first time $v=6$ |
| $u\sin\theta - gt = 3\sqrt{2}$ | A1 | |
| $2g - 3\sqrt{2} - gt = 3\sqrt{2}$ | M1 | Solve for $t$ |
| $t = \dfrac{2g - 6\sqrt{2}}{g} = 1.13...$ | A1 | Sensitive to premature approximation; allow 1.14 |
| $T = 2 - 1.13... = 0.87$ | A1 | CAO accept awrt 0.87 |
| **Total** | **(5)** | |

**Alternative 7c (Method 1):**

| Answer/Working | Mark | Guidance |
|---|---|---|
| $6\sin 45 = 0 + gt$ | M1A1 | Find time from top to $A$ |
| $T = 2t = \dfrac{12\sqrt{2}/2}{g} = 0.87$ | M1, A1, A1 | Correct strategy; correct unsimplified |

**Alternative 7c (Method 2):**

| Answer/Working | Mark | Guidance |
|---|---|---|
| $u\sin\theta = gt$ (their $u,\theta$) | M1 | Time to top |
| $t = 1.567...$ | A1 | |
| $T = 2(2 - 1.567...)$ | M1A1 | |
| $= 0.87$ | A1 | |

**Alternative 7c (Method 3):**

| Answer/Working | Mark | Guidance |
|---|---|---|
| Vertical speed at $A = -(\text{vertical speed at }B) = \sqrt{36-(3\sqrt{2})^2} = 3\sqrt{2}$ | M1, A1 | Or use the $45°$ angle |
| Use $v = u + at$ for $A\to B$: $-3\sqrt{2} = 3\sqrt{2} - gT$ | M1, A1 | Correct use for their values |
| $T = 0.87$ | A1 | |

---

# Question Alt 7d:

| Answer/Working | Mark | Guidance |
|---|---|---|
| $v^2 = \left(3\sqrt{2}\right)^2 + \left(u\sin\theta - gt\right)^2 \leq 36$ | M1 | Form expression for $v^2$; inequality not needed at this stage |
| | A1 | Correct inequality for $v^2$ |
| $-\sqrt{18} \leq u\sin\theta - gt \leq \sqrt{18}$ | M1 | |
| $\dfrac{u\sin\theta - \sqrt{18}}{g} \leq t \leq \dfrac{u\sin\theta + \sqrt{18}}{g}$ | A1 | |
| $T = \dfrac{u\sin\theta + \sqrt{18}}{g} - \dfrac{u\sin\theta - \sqrt{18}}{g} = \dfrac{2\sqrt{18}}{g} = 0.866$ | A1 | |
| **Total** | **(5)** | |
5.

\begin{figure}[h]
\begin{center}
  \includegraphics[alt={},max width=\textwidth]{e6d100ff-dd4a-4591-a0a3-81761773045e-09_689_581_237_683}
\captionsetup{labelformat=empty}
\caption{Figure 2}
\end{center}
\end{figure}

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 $k$.\\
(10)

\hfill \mbox{\textit{Edexcel M2 2016 Q5 [10]}}