Edexcel FM2 2022 June — Question 7 12 marks

Exam BoardEdexcel
ModuleFM2 (Further Mechanics 2)
Year2022
SessionJune
Marks12
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicCircular Motion 2
TypeVertical circle: complete revolution conditions
DifficultyStandard +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.
Spec6.02i Conservation of energy: mechanical energy principle6.05d Variable speed circles: energy methods6.05e Radial/tangential acceleration

7. \begin{figure}[h]
\includegraphics[alt={},max width=\textwidth]{1f39620e-c10f-4344-89f1-626fff36d187-24_639_593_246_737} \captionsetup{labelformat=empty} \caption{Figure 5}
\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.
  1. 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 \(O\)
  2. find, in terms of \(a\) and \(g\), the minimum possible value of \(u\) Given that \(u = 2 \sqrt { a g }\)
  3. find, in terms of \(g\), the magnitude of the acceleration of \(P\) at the instant when \(O P\) is horizontal.
  4. Apart from including air resistance, suggest one way in which the model could be refined to make it more realistic.

Question 7:
Part (a):
AnswerMarks Guidance
Answer/WorkingMark 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):
AnswerMarks Guidance
Answer/WorkingMark 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):
AnswerMarks Guidance
Answer/WorkingMark 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):
AnswerMarks Guidance
Answer/WorkingMark Guidance
Consider the uniformity/dimensions of the package; string might be extensible; include the weight of the stringB1 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 $g$ |

---
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]}}