| Exam Board | Edexcel |
|---|---|
| Module | FM2 (Further Mechanics 2) |
| Year | 2022 |
| Session | June |
| Marks | 14 |
| Paper | Download PDF ↗ |
| Mark scheme | Download PDF ↗ |
| Topic | Simple Harmonic Motion |
| Type | String becomes slack timing |
| Difficulty | Challenging +1.2 This is a standard Further Maths SHM question requiring equilibrium analysis, SHM equation setup, energy methods, and understanding of slack string motion. While it involves multiple parts and careful reasoning about when the string becomes slack, the techniques are all standard FM2 material with no novel insights required. The 'show that' structure guides students through the solution, making it moderately above average difficulty but not exceptional. |
| Spec | 4.10f Simple harmonic motion: x'' = -omega^2 x6.02g Hooke's law: T = k*x or T = lambda*x/l6.02i Conservation of energy: mechanical energy principle |
| Answer | Marks | Guidance |
|---|---|---|
| Answer/Working | Mark | Guidance |
| At equilibrium: \(0.5g = \frac{25e}{1.25}\), \(e = \frac{0.5\times10\times1.25}{25} = \frac{1}{4}\) | B1 | Correct only. Award if \(mg = \frac{\lambda e}{l}\) used in equation of motion |
| For taut string, equation of motion with \(x\) from equilibrium: \(\frac{25(e+x)}{1.25} - 0.5g = -0.5\ddot{x}\) | M1, A1ft | Need all terms, dimensionally correct. Allow with their \(e \neq 0\). Condone sign errors. Correct unsimplified equation |
| \(\ddot{x} = -40x\), hence SHM | A1* | Reach given conclusion from correct working |
| Periodic time: \(T = \frac{2\pi}{\sqrt{40}} = \frac{\pi}{\sqrt{10}}\) | M1, A1* | Use \(T = \frac{2\pi}{\omega}\) from \(\ddot{x} = -\omega^2 x\). Obtain given answer from correct working |
| Answer | Marks | Guidance |
|---|---|---|
| Answer/Working | Mark | Guidance |
| Max KE \(= 2.5 = \frac{1}{2}\times\frac{1}{2}\times\max v^2 \Rightarrow \max v^2 = 10\) | B1 | Use KE to find max \(v\) or max \(v^2\) |
| Max speed \(= a\omega\): \(\sqrt{10} = a\sqrt{40}\) | M1 | Use model to find amplitude |
| \(AB = 1.25 + \frac{1}{4} + \frac{1}{2} = 2\ (\text{m})\) | A1* | Obtain given answer from correct working |
| Answer | Marks | Guidance |
|---|---|---|
| Answer/Working | Mark | Guidance |
| Energy: \(\frac{25e^2}{2.5} + 2.5 + 0.5ga = \frac{25(e+a)^2}{2.5}\) | B1 | Using correct \(\lambda\) and \(l\) and \(e\) or their \(e\) |
| Solve for \(a\) | M1 | Requires energy equation with all right terms |
| \(AB = 1.25 + \frac{1}{4} + \frac{1}{2} = 2\ (\text{m})\) | A1* | Obtain given answer from correct working |
| Answer | Marks | Guidance |
|---|---|---|
| Answer/Working | Mark | Guidance |
| \(a = 0.5\), \(x = 0.5\cos\sqrt{40}t\) | B1 | Correct equation for SHM seen or implied |
| \(-0.25 = 0.5\cos\sqrt{40}t \Rightarrow t = 0.3311\ldots\) | M1 | Find time until string goes slack. If working from \(x = 0.5\sin\sqrt{40}t\) need \(\frac{T}{4} + \frac{1}{\sqrt{40}}\sin^{-1}\frac{1}{2}\) |
| \(v^2 = 40\left(0.5^2 - 0.25^2\right) = \frac{15}{2}\) | M1 | Use model to find \(v\) or \(v^2\) at instant string goes slack (\(v = 2.738\ldots\)). Using SHM formula or conservation of energy |
| Total time \(= 2\times0.3311\ldots + \frac{2\times\sqrt{7.5}}{10}\) | DM1 | Complete method to find total time until return to \(B\). Requires preceding M marks |
| \(= 1.2\ (\text{s})\) or better | A1 |
| Answer | Marks | Guidance |
|---|---|---|
| Answer/Working | Mark | Guidance |
| \(\sqrt{\dfrac{15}{2}} = -\sqrt{\dfrac{15}{2}} + gt\) or a combination of \(v^2 = u^2 + 2as\) and \(s = ut + \dfrac{1}{2}at^2\) | M1 | If they use suvat to find the time as a projectile it must be a complete method |
| \(= 1.2\) (s) or better | A1 | Condone an answer to \(> 2\) s.f. Not scored if they have used \(9.8\) |
# Question 8:
## Part (a):
| Answer/Working | Mark | Guidance |
|---|---|---|
| At equilibrium: $0.5g = \frac{25e}{1.25}$, $e = \frac{0.5\times10\times1.25}{25} = \frac{1}{4}$ | B1 | Correct only. Award if $mg = \frac{\lambda e}{l}$ used in equation of motion |
| For taut string, equation of motion with $x$ from equilibrium: $\frac{25(e+x)}{1.25} - 0.5g = -0.5\ddot{x}$ | M1, A1ft | Need all terms, dimensionally correct. Allow with their $e \neq 0$. Condone sign errors. Correct unsimplified equation |
| $\ddot{x} = -40x$, hence SHM | A1* | Reach given conclusion from correct working |
| Periodic time: $T = \frac{2\pi}{\sqrt{40}} = \frac{\pi}{\sqrt{10}}$ | M1, A1* | Use $T = \frac{2\pi}{\omega}$ from $\ddot{x} = -\omega^2 x$. Obtain given answer from correct working |
## Part (b):
| Answer/Working | Mark | Guidance |
|---|---|---|
| Max KE $= 2.5 = \frac{1}{2}\times\frac{1}{2}\times\max v^2 \Rightarrow \max v^2 = 10$ | B1 | Use KE to find max $v$ or max $v^2$ |
| Max speed $= a\omega$: $\sqrt{10} = a\sqrt{40}$ | M1 | Use model to find amplitude |
| $AB = 1.25 + \frac{1}{4} + \frac{1}{2} = 2\ (\text{m})$ | A1* | Obtain given answer from correct working |
## Part (b) alt:
| Answer/Working | Mark | Guidance |
|---|---|---|
| Energy: $\frac{25e^2}{2.5} + 2.5 + 0.5ga = \frac{25(e+a)^2}{2.5}$ | B1 | Using correct $\lambda$ and $l$ and $e$ or their $e$ |
| Solve for $a$ | M1 | Requires energy equation with all right terms |
| $AB = 1.25 + \frac{1}{4} + \frac{1}{2} = 2\ (\text{m})$ | A1* | Obtain given answer from correct working |
## Part (c):
| Answer/Working | Mark | Guidance |
|---|---|---|
| $a = 0.5$, $x = 0.5\cos\sqrt{40}t$ | B1 | Correct equation for SHM seen or implied |
| $-0.25 = 0.5\cos\sqrt{40}t \Rightarrow t = 0.3311\ldots$ | M1 | Find time until string goes slack. If working from $x = 0.5\sin\sqrt{40}t$ need $\frac{T}{4} + \frac{1}{\sqrt{40}}\sin^{-1}\frac{1}{2}$ |
| $v^2 = 40\left(0.5^2 - 0.25^2\right) = \frac{15}{2}$ | M1 | Use model to find $v$ or $v^2$ at instant string goes slack ($v = 2.738\ldots$). Using SHM formula or conservation of energy |
| Total time $= 2\times0.3311\ldots + \frac{2\times\sqrt{7.5}}{10}$ | DM1 | Complete method to find total time until return to $B$. Requires preceding M marks |
| $= 1.2\ (\text{s})$ or better | A1 | |
## Mark Scheme Content
**Question (Projectile time calculation):**
| Answer/Working | Mark | Guidance |
|---|---|---|
| $\sqrt{\dfrac{15}{2}} = -\sqrt{\dfrac{15}{2}} + gt$ or a combination of $v^2 = u^2 + 2as$ and $s = ut + \dfrac{1}{2}at^2$ | M1 | If they use suvat to find the time as a projectile it must be a complete method |
| $= 1.2$ (s) or better | A1 | Condone an answer to $> 2$ s.f. Not scored if they have used $9.8$ |
\begin{enumerate}
\item Throughout this question, use $\boldsymbol { g } = \mathbf { 1 0 m ~ s } ^ { \mathbf { - 2 } }$
\end{enumerate}
A light elastic string has natural length 1.25 m and modulus of elasticity 25 N .\\
A particle $P$ of mass 0.5 kg is attached to one end of the string. The other end of the string is attached to a fixed point $A$. Particle $P$ hangs freely in equilibrium with $P$ vertically below $A$
The particle is then pulled vertically down to a point $B$ and released from rest.\\
(a) Show that, while the string is taut, $P$ moves with simple harmonic motion with period $\frac { \pi } { \sqrt { 10 } }$ seconds.
The maximum kinetic energy of $P$ during the subsequent motion is 2.5 J .\\
(b) Show that $A B = 2 \mathrm {~m}$
The particle returns to $B$ for the first time $T$ seconds after it was released from rest at $B$\\
(c) Find the value of $T$
\hfill \mbox{\textit{Edexcel FM2 2022 Q8 [14]}}