| Exam Board | Edexcel |
|---|---|
| Module | M2 (Mechanics 2) |
| Year | 2016 |
| Session | January |
| Marks | 10 |
| 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 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. |
| Spec | 6.04b Find centre of mass: using symmetry6.04c Composite bodies: centre of mass6.04e Rigid body equilibrium: coplanar forces |
| Answer | Marks | Guidance |
|---|---|---|
| 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 |
| Answer | Marks | Guidance |
|---|---|---|
| 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 |
| Answer | Marks | Guidance |
|---|---|---|
| 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) |
| Answer | Marks | Guidance |
|---|---|---|
| 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 |
| Answer | Marks | Guidance |
|---|---|---|
| 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 |
| Answer | Marks | Guidance |
|---|---|---|
| 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) |
| Answer | Marks | Guidance |
|---|---|---|
| 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 |
| Answer | Marks | Guidance |
|---|---|---|
| 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) |
| Answer | Marks | Guidance |
|---|---|---|
| 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) |
| Answer | Marks | Guidance |
|---|---|---|
| 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) |
| Answer | Marks | Guidance |
|---|---|---|
| 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 |
| Answer | Marks | Guidance |
|---|---|---|
| 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 |
| Answer | Marks | Guidance |
|---|---|---|
| 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 |
| Answer | Marks | Guidance |
|---|---|---|
| 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) |
# 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]}}