| Exam Board | Edexcel |
|---|---|
| Module | FM2 (Further Mechanics 2) |
| Year | 2022 |
| Session | June |
| Marks | 12 |
| Paper | Download PDF ↗ |
| Mark scheme | Download PDF ↗ |
| Topic | Circular Motion 2 |
| Type | Vertical circle: complete revolution conditions |
| Difficulty | Standard +0.3 This is a standard Further Mechanics 2 vertical circle problem with typical parts: (a) deriving tension using energy conservation and circular motion equations (structured 'show that'), (b) finding minimum speed for complete revolution (standard condition T≥0 at top), (c) calculating acceleration at a specific point, (d) model refinement. While it requires multiple techniques (energy, circular motion, vectors), these are routine applications of well-practiced FM2 methods with no novel insight required. Slightly easier than average A-level due to the guided structure. |
| Spec | 6.02i Conservation of energy: mechanical energy principle6.05d Variable speed circles: energy methods6.05e Radial/tangential acceleration |
| Answer | Marks | Guidance |
|---|---|---|
| Answer/Working | Mark | Guidance |
| Conservation of energy: \(\frac{1}{2}mu^2 = \frac{1}{2}mv^2 + mg \times \frac{2a}{5}(1-\cos\theta)\) | M1, A1 | Need all terms, dimensionally correct. Condone sign errors and sin/cos confusion. Allow with \(\frac{2a}{5}\cos\theta\) in place of \(\frac{2a}{5}(1-\cos\theta)\) |
| Equation of motion towards \(O\): \(T - mg\cos\theta = \frac{5mv^2}{2a}\) | M1, A1 | Need all terms, dimensionally correct. Condone sign errors and sin/cos confusion |
| Complete method to find \(T\) in terms of \(u\), \(a\) and \(\theta\) | DM1 | Complete method using conservation of energy and circular motion to eliminate \(v\). Requires two preceding M marks |
| \(T = mg\cos\theta + \frac{5m}{2a}\left(u^2 - \frac{4a}{5}g(1-\cos\theta)\right) = 3mg\cos\theta - 2mg + \frac{5mu^2}{2a}\) | A1* | Obtain given result from correct working |
| Answer | Marks | Guidance |
|---|---|---|
| Answer/Working | Mark | Guidance |
| Require \(T \geq 0\) when \(\theta = \pi\): \(\frac{5mu^2}{2a} \geq mg(2+3)\) | M1 | Identify correct condition for complete circle, solve for \(u\). Condone working from \(T=0\) |
| \(u^2 \geq 2ag\), minimum \(u = \sqrt{2ag}\) | A1 | Allow \(u \geq \sqrt{2ag}\). Condone \(u > \sqrt{2ag}\) and \(u = \sqrt{2ag}\) |
| Answer | Marks | Guidance |
|---|---|---|
| Answer/Working | Mark | Guidance |
| \(\theta = \frac{\pi}{2}, u = 2\sqrt{ag} \Rightarrow T = -2mg + \frac{5m}{2a}\times 4ag = 8mg\) | B1 | Correct \(T\) or \(v^2\) seen or implied |
| Magnitude of acceleration \(= g\sqrt{64+1} = \sqrt{65}g\) | M1, A1 | Use Pythagoras with horizontal component of acceleration. Correct only, or \(8.1g\) (\(8.062\ldots g\)) or better |
| Answer | Marks | Guidance |
|---|---|---|
| Answer/Working | Mark | Guidance |
| Consider the uniformity/dimensions of the package; string might be extensible; include the weight of the string | B1 | Any valid suggestion relating to the model. Allow negatives of statements within the model. B0 if multiple suggestions including one incorrect. B0 for accuracy of \(g\) |
# Question 7:
## Part (a):
| Answer/Working | Mark | Guidance |
|---|---|---|
| Conservation of energy: $\frac{1}{2}mu^2 = \frac{1}{2}mv^2 + mg \times \frac{2a}{5}(1-\cos\theta)$ | M1, A1 | Need all terms, dimensionally correct. Condone sign errors and sin/cos confusion. Allow with $\frac{2a}{5}\cos\theta$ in place of $\frac{2a}{5}(1-\cos\theta)$ |
| Equation of motion towards $O$: $T - mg\cos\theta = \frac{5mv^2}{2a}$ | M1, A1 | Need all terms, dimensionally correct. Condone sign errors and sin/cos confusion |
| Complete method to find $T$ in terms of $u$, $a$ and $\theta$ | DM1 | Complete method using conservation of energy and circular motion to eliminate $v$. Requires two preceding M marks |
| $T = mg\cos\theta + \frac{5m}{2a}\left(u^2 - \frac{4a}{5}g(1-\cos\theta)\right) = 3mg\cos\theta - 2mg + \frac{5mu^2}{2a}$ | A1* | Obtain given result from correct working |
## Part (b):
| Answer/Working | Mark | Guidance |
|---|---|---|
| Require $T \geq 0$ when $\theta = \pi$: $\frac{5mu^2}{2a} \geq mg(2+3)$ | M1 | Identify correct condition for complete circle, solve for $u$. Condone working from $T=0$ |
| $u^2 \geq 2ag$, minimum $u = \sqrt{2ag}$ | A1 | Allow $u \geq \sqrt{2ag}$. Condone $u > \sqrt{2ag}$ and $u = \sqrt{2ag}$ |
## Part (c):
| Answer/Working | Mark | Guidance |
|---|---|---|
| $\theta = \frac{\pi}{2}, u = 2\sqrt{ag} \Rightarrow T = -2mg + \frac{5m}{2a}\times 4ag = 8mg$ | B1 | Correct $T$ or $v^2$ seen or implied |
| Magnitude of acceleration $= g\sqrt{64+1} = \sqrt{65}g$ | M1, A1 | Use Pythagoras with horizontal component of acceleration. Correct only, or $8.1g$ ($8.062\ldots g$) or better |
## Part (d):
| Answer/Working | Mark | Guidance |
|---|---|---|
| Consider the uniformity/dimensions of the package; string might be extensible; include the weight of the string | B1 | Any valid suggestion **relating to the model**. Allow negatives of statements within the model. B0 if multiple suggestions including one incorrect. B0 for accuracy of $g$ |
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7.
\begin{figure}[h]
\begin{center}
\includegraphics[alt={},max width=\textwidth]{1f39620e-c10f-4344-89f1-626fff36d187-24_639_593_246_737}
\captionsetup{labelformat=empty}
\caption{Figure 5}
\end{center}
\end{figure}
A package $P$ of mass $m$ is attached to one end of a string of length $\frac { 2 a } { 5 }$. The other end of the string is attached to a fixed point $O$. The package hangs at rest vertically below $O$ with the string taut and is then projected horizontally with speed $u$, as shown in Figure 5.
When $O P$ has turned through an angle $\theta$ and the string is still taut, the tension in the string is $T$
The package is modelled as a particle and the string as being light and inextensible.
\begin{enumerate}[label=(\alph*)]
\item Show that $T = 3 m g \cos \theta - 2 m g + \frac { 5 m u ^ { 2 } } { 2 a }$
Given that $P$ moves in a complete vertical circle with centre $O$
\item find, in terms of $a$ and $g$, the minimum possible value of $u$
Given that $u = 2 \sqrt { a g }$
\item find, in terms of $g$, the magnitude of the acceleration of $P$ at the instant when $O P$ is horizontal.
\item Apart from including air resistance, suggest one way in which the model could be refined to make it more realistic.
\end{enumerate}
\hfill \mbox{\textit{Edexcel FM2 2022 Q7 [12]}}