| Exam Board | Edexcel |
|---|---|
| Module | M5 (Mechanics 5) |
| Year | 2018 |
| Session | June |
| Marks | 16 |
| Paper | Download PDF ↗ |
| Mark scheme | Download PDF ↗ |
| Topic | Moments of inertia |
| Type | Detachment or peg impact mid-motion |
| Difficulty | Challenging +1.8 This is a challenging Further Maths mechanics question requiring multiple advanced techniques: moment of inertia about a parallel axis, SHM period formula for compound pendulum, energy conservation from inverted position, impulse-momentum with angular motion, and energy methods for finding angle after rebound. However, the question provides the moment of inertia and guides students through structured parts with standard methods, making it demanding but accessible to well-prepared FM students. |
| Spec | 6.03f Impulse-momentum: relation6.03g Impulse in 2D: vector form6.04c Composite bodies: centre of mass6.04d Integration: for centre of mass of laminas/solids6.05f Vertical circle: motion including free fall |
| Answer | Marks | Guidance |
|---|---|---|
| Working/Answer | Marks | Guidance |
| \(3mg\cdot 2l\sin\theta+4mg\cdot 4l\sin\theta=-2m(a^2+40l^2)\ddot{\theta}\) | M1 A1 | M1 for equation of motion about \(A\) with usual rules; A1 for correct equation |
| For small \(\theta\), \(\sin\theta\approx\theta\): \(-\frac{11gl}{(a^2+40l^2)}\theta=\ddot{\theta}\) | M1 | M1 for using small angle approx. and putting into appropriate form (with \(-\) sign) |
| SHM; \(T=2\pi\sqrt{\dfrac{(a^2+40l^2)}{11gl}}\) | M1 A1 | M1 for SHM and use of correct formula for period; A1 for correct answer |
| Answer | Marks | Guidance |
|---|---|---|
| Working/Answer | Marks | Guidance |
| \(4mg\cdot 4l+3mg\cdot 2l=\frac{1}{2}\cdot 2m(a^2+40l^2)\omega^2\) | M1 A1 | M1 for conservation of energy equation with usual rules; A1 for correct equation |
| \(\omega^2=\dfrac{22gl}{(a^2+40l^2)}\) | A1 | A1 for correct GIVEN ANSWER |
| Answer | Marks | Guidance |
|---|---|---|
| Working/Answer | Marks | Guidance |
| \(J\cdot 2l=2m(a^2+40l^2)\!\left(\tfrac{1}{2}\omega-(-\omega)\right)\) | M1 A2 | M1A2 for angular impulse-momentum equation |
| \(J=\dfrac{3m}{2}\sqrt{\dfrac{22g(a^2+40l^2)}{l}}\) | A1 | A1 for correct answer |
| Answer | Marks | Guidance |
|---|---|---|
| Working/Answer | Marks | Guidance |
| \(\frac{1}{2}\cdot 2m(a^2+40l^2)\!\left(\tfrac{1}{2}\omega\right)^2=3mg\cdot 2l\sin\theta+4mg\cdot 4l\sin\theta\) | M1 A1 | M1A1 for energy equation |
| \(\frac{1}{8}\cdot 2m(a^2+40l^2)\cdot\dfrac{22gl}{(a^2+40l^2)}=22mgl\sin\theta\) | DM1 | DM1 for substituting \(\omega^2\) |
| \(\sin\theta=\dfrac{1}{4}\Rightarrow\theta=\sin^{-1}\!\dfrac{1}{4}\) | A1 | A1 for GIVEN ANSWER correctly obtained |
| Answer | Marks | Guidance |
|---|---|---|
| Answer/Working | Marks | Guidance |
| Impulse-momentum equation (general form, \(I\) and \(\omega\) not yet substituted) | M1 | \(I\) and \(\omega\) do not need to be substituted at this stage |
| Correct equation without \(I\) and \(\omega\) substituted | A1 | First correct equation |
| Correct equation with \(I\) and \(\omega\) substituted | A1 | Second correct equation |
| Correct final answer (must be positive) | A1 | Third mark |
| Answer | Marks | Guidance |
|---|---|---|
| Answer/Working | Marks | Guidance |
| Conservation of energy equation (general form) | M1 | First M1, usual rules apply |
| Correct equation without \(\omega\) substituted | A1 | First A1 |
| Substituting for \(\omega\) | DM1 | Dependent on first M1 |
| Correctly obtaining the given answer | A1 | Second A1, must arrive at GIVEN ANSWER |
# Question 7:
## Part 7(a):
| Working/Answer | Marks | Guidance |
|---|---|---|
| $3mg\cdot 2l\sin\theta+4mg\cdot 4l\sin\theta=-2m(a^2+40l^2)\ddot{\theta}$ | M1 A1 | M1 for equation of motion about $A$ with usual rules; A1 for correct equation |
| For small $\theta$, $\sin\theta\approx\theta$: $-\frac{11gl}{(a^2+40l^2)}\theta=\ddot{\theta}$ | M1 | M1 for using small angle approx. and putting into appropriate form (with $-$ sign) |
| SHM; $T=2\pi\sqrt{\dfrac{(a^2+40l^2)}{11gl}}$ | M1 A1 | M1 for SHM and use of correct formula for period; A1 for correct answer |
## Part 7(b):
| Working/Answer | Marks | Guidance |
|---|---|---|
| $4mg\cdot 4l+3mg\cdot 2l=\frac{1}{2}\cdot 2m(a^2+40l^2)\omega^2$ | M1 A1 | M1 for conservation of energy equation with usual rules; A1 for correct equation |
| $\omega^2=\dfrac{22gl}{(a^2+40l^2)}$ | A1 | A1 for correct GIVEN ANSWER |
## Part 7(c):
| Working/Answer | Marks | Guidance |
|---|---|---|
| $J\cdot 2l=2m(a^2+40l^2)\!\left(\tfrac{1}{2}\omega-(-\omega)\right)$ | M1 A2 | M1A2 for angular impulse-momentum equation |
| $J=\dfrac{3m}{2}\sqrt{\dfrac{22g(a^2+40l^2)}{l}}$ | A1 | A1 for correct answer |
## Part 7(d):
| Working/Answer | Marks | Guidance |
|---|---|---|
| $\frac{1}{2}\cdot 2m(a^2+40l^2)\!\left(\tfrac{1}{2}\omega\right)^2=3mg\cdot 2l\sin\theta+4mg\cdot 4l\sin\theta$ | M1 A1 | M1A1 for energy equation |
| $\frac{1}{8}\cdot 2m(a^2+40l^2)\cdot\dfrac{22gl}{(a^2+40l^2)}=22mgl\sin\theta$ | DM1 | DM1 for substituting $\omega^2$ |
| $\sin\theta=\dfrac{1}{4}\Rightarrow\theta=\sin^{-1}\!\dfrac{1}{4}$ | A1 | A1 for GIVEN ANSWER correctly obtained |
## Question 7:
### Part 7(c):
| Answer/Working | Marks | Guidance |
|---|---|---|
| Impulse-momentum equation (general form, $I$ and $\omega$ not yet substituted) | M1 | $I$ and $\omega$ do not need to be substituted at this stage |
| Correct equation without $I$ and $\omega$ substituted | A1 | First correct equation |
| Correct equation with $I$ and $\omega$ substituted | A1 | Second correct equation |
| Correct final answer (must be positive) | A1 | Third mark |
---
### Part 7(d):
| Answer/Working | Marks | Guidance |
|---|---|---|
| Conservation of energy equation (general form) | M1 | First M1, usual rules apply |
| Correct equation without $\omega$ substituted | A1 | First A1 |
| Substituting for $\omega$ | DM1 | Dependent on first M1 |
| Correctly obtaining the given answer | A1 | Second A1, must arrive at GIVEN ANSWER |
7. A pendulum consists of a uniform circular disc, of radius $a$ and mass $4 m$, whose centre is fixed to the end $B$ of a uniform $\operatorname { rod } A B$. The rod has mass $3 m$ and length $4 l$, where $2 l > a$. The rod lies in the same plane as the disc. The pendulum is free to rotate about a fixed smooth horizontal axis $L$ which passes through $A$ and is perpendicular to the plane of the disc. The moment of inertia of the pendulum about $L$ is $2 m \left( a ^ { 2 } + 40 l ^ { 2 } \right)$.
\begin{enumerate}[label=(\alph*)]
\item Find the approximate period of small oscillations of the pendulum about its position of stable equilibrium.
The pendulum is held with $B$ vertically above $A$ and is then slightly displaced from rest. In the subsequent motion the midpoint of $A B$ strikes a small peg, which is fixed at the same horizontal level as $A$, and the pendulum rebounds upwards. Immediately before it strikes the peg, the angular speed of the pendulum is $\omega$.
\item Show that $\omega ^ { 2 } = \frac { 22 g l } { \left( a ^ { 2 } + 40 l ^ { 2 } \right) }$
Immediately after it strikes the peg, the angular speed of the pendulum is $\frac { 1 } { 2 } \omega$.
\item Find, in terms of $m , g , a$ and $l$, the magnitude of the impulse exerted on the peg by the pendulum.
\item Show that the size of the angle turned through by the pendulum, between it hitting the peg and it next coming to rest, is $\arcsin \frac { 1 } { 4 }$.
\begin{center}
\includegraphics[max width=\textwidth, alt={}]{1242d28a-a4bd-4754-ac49-9b48de95b880-24_2632_1830_121_121}
\end{center}
\end{enumerate}
\hfill \mbox{\textit{Edexcel M5 2018 Q7 [16]}}