| Exam Board | OCR MEI |
|---|---|
| Module | Further Mechanics Major (Further Mechanics Major) |
| Year | 2022 |
| Session | June |
| Marks | 17 |
| Paper | Download PDF ↗ |
| Mark scheme | Download PDF ↗ |
| Topic | Hooke's law and elastic energy |
| Type | Simple harmonic motion with elastic string |
| Difficulty | Challenging +1.3 This is a Further Maths mechanics question involving elastic strings with damping. Part (a) is routine equilibrium (Hooke's law). Part (b) requires setting up a second-order ODE from forces, which is standard for this module. Part (c) verifies a given solution by differentiation and substitution. Part (d) requires finding when tension becomes zero. While it involves multiple techniques (differential equations, damped oscillations, verification), each step follows established procedures for Further Maths students with no novel insight required. The 'show that' and 'verify' structure reduces problem-solving demand. |
| Spec | 4.10d Second order homogeneous: auxiliary equation method6.02h Elastic PE: 1/2 k x^2 |
| Answer | Marks | Guidance |
|---|---|---|
| 13 | (a) | T =0.15g |
| Answer | Marks |
|---|---|
| OA=0.45+e=0.5(m) | M1 |
| Answer | Marks |
|---|---|
| [3] | 1.1 |
| Answer | Marks |
|---|---|
| 1.1 | Resolving vertically for P at A |
| Answer | Marks |
|---|---|
| (b) | d2x dx |
| Answer | Marks |
|---|---|
| dt2 dt | M1* |
| Answer | Marks |
|---|---|
| [3] | 2.1 |
| Answer | Marks |
|---|---|
| 2.2a | Apply N2L vertically – correct number of terms |
| Answer | Marks |
|---|---|
| (c) | 5 d2x dx |
| Answer | Marks |
|---|---|
| 7 28 56 | M1* |
| Answer | Marks |
|---|---|
| [6] | 1.1 |
| Answer | Marks |
|---|---|
| 2.2a | Differentiating x using the product rule (two terms of |
| Answer | Marks |
|---|---|
| Alternative method (solving the given differential equation) | Solving the differential equation |
| Answer | Marks | Guidance |
|---|---|---|
| m2+ 4m+ 200= 0Þ m= - 2± 14i | B1 | Correct roots of auxiliary equation – allow - 2+14i |
| Answer | Marks | Guidance |
|---|---|---|
| x= e- 2t(Acos(14t)+ Bsin(14t)) | M1* | Correct general solution from their roots of the |
| Answer | Marks | Guidance |
|---|---|---|
| t= 0,x= 0Þ A= 0 | A1 | Must follow from correct general solution |
| Answer | Marks | Guidance |
|---|---|---|
| dt | M1dep* | Differentiating using the product rule (ignore terms in |
| Answer | Marks | Guidance |
|---|---|---|
| dt 56 | A1 | Dependent on correctly differentiated terms in B |
| Answer | Marks | Guidance |
|---|---|---|
| 56 | A1 | Dependent on completely correct working |
| Answer | Marks |
|---|---|
| (d) | dx 5 |
| Answer | Marks |
|---|---|
| −0.046007... <0.05⇒string does not go slack | M1* |
| Answer | Marks |
|---|---|
| [5] | 3.1b |
| Answer | Marks |
|---|---|
| 2.2b | Setting first derivative (two terms from the product |
Question 13:
13 | (a) | T =0.15g
13.5e
=0.15g⇒e=...
0.45
OA=0.45+e=0.5(m) | M1
M1
A1
[3] | 1.1
3.3
1.1 | Resolving vertically for P at A
Apply Hooke’s law and solve for e – where e is the
extension of the string from its natural length to A
AG - if g = 9.8 used then A0
(b) | d2x dx
0.15 =0.15g−T −0.6
dt2 x dt
d2x 13.5 dx
0.15 =0.15g− (0.05+x)−0.6
dt2 0.45 dt
d2x dx
0.15 =−0.6 −30x
dt2 dt
d2x dx
⇒ +4 +200x=0
dt2 dt | M1*
M1dep*
A1
[3] | 2.1
1.1
2.2a | Apply N2L vertically – correct number of terms
Substitute correct expression for the tension when the
extension is 0.05 + x
AG if g = 9.8 used then A0
(c) | 5 d2x dx
x= e −2tsin(14t) and + 4 + 200x= 0
56 dt2 dt
dx 5 5
= e −2tcos(14t)− e −2tsin(14t)
dt 4 28
dx 5 5
t =0, = e −0cos(0)− e −0sin(0)=1.25
dt 4 28
5
t =0,x= e −0sin(0)=0
56
d2x 120
=− e −2tsin(14t)−5e −2tcos(14t)
dt2 7
2
𝑑𝑑 𝑥𝑥 𝑑𝑑𝑥𝑥
2 +4 +200𝑥𝑥
𝑑𝑑𝑡𝑡 𝑑𝑑𝑡𝑡
−2𝑡𝑡 120
= e �− 𝑠𝑠𝑠𝑠𝑠𝑠(14𝑡𝑡)−5𝑐𝑐𝑐𝑐𝑠𝑠(14𝑡𝑡)�
7
−2𝑡𝑡 5 5
+4𝑒𝑒 � 𝑐𝑐𝑐𝑐𝑠𝑠(14𝑡𝑡)− 𝑠𝑠𝑠𝑠𝑠𝑠(14𝑡𝑡)�
4 28
−2𝑡𝑡 5
=e −2tsin(14t) − 120 − 20+ + 1200000𝑒𝑒 +e �−2 5 t 6co 𝑠𝑠 s 𝑠𝑠𝑠𝑠(1 ( 4 1 t 4)𝑡𝑡() − � 5+5)=0
7 28 56 | M1*
A1
B1
A1
M1dep*
A1
[6] | 1.1
1.1
3.4
1.1
3.4
2.2a | Differentiating x using the product rule (two terms of
the form uv¢+ vu¢with sin(14t)® ± cos(14t))
dx 5
= e −2t( 14cos(14t)−2sin(14t))
dt 56
dx
Verifying that when t = 0, =1.25and x = 0 – from
dt
a correct first derivative
Correct second derivative (need not be simplified),
for example
d2x = 5 ( −2e −2t )( 14cos(14t)−2sin(14t))
dt2 56
5
+ e −2t(−196sin(14t)−28cos(14t))
56
Substitute x, and its first and second derivatives into
the correct differential equation
AG – sufficient working must be shown
Alternative method (solving the given differential equation) | Solving the differential equation
d2x dx
+ 4 + 200x= 0
dt2 dt
m2+ 4m+ 200= 0Þ m= - 2± 14i | B1 | Correct roots of auxiliary equation – allow - 2+14i
if correct general solution seen
x= e- 2t(Acos(14t)+ Bsin(14t)) | M1* | Correct general solution from their roots of the
auxiliary equation
t= 0,x= 0Þ A= 0 | A1 | Must follow from correct general solution | Must follow from correct general solution
dx
= e- 2t(14Bcos(14t))- 2e- 2t(Bsin(14t))
dt | M1dep* | Differentiating using the product rule (ignore terms in
A)
dx 5
t= 0, = 1.25Þ B=
dt 56 | A1 | Dependent on correctly differentiated terms in B
5
x= e −2tsin(14t)
56 | A1 | Dependent on completely correct working
[6]
(d) | dx 5
= (e- 2t(14cos(14t))- 2e- 2t(sin(14t)))= 0
dt 56
tan(14t)=7
t =0.10206...,0.32646...
when t = 0.32646…, x=−0.046007...
−0.046007... <0.05⇒string does not go slack | M1*
A1
M1dep*
M1
A1
[5] | 3.1b
1.1
3.1a
3.4
2.2b | Setting first derivative (two terms from the product
rule) equal to zero (to find when P is at rest)
Or equivalent 5 e −2t(7cos14t−sin14t)=0
28
Either finding the correct first two times from their
tan(14t)=k for any non-zero k or just considers the
second time (stating 0.326… is sufficient for this
mark)
Finding the displacement of P when P is at rest for the
second time – dependent on both previous M marks
Comparison and conclusion that the string does not
go slack
Differentiating using the product rule (ignore terms in
A)
In this question take $g = 10$.
A particle P of mass 0.15 kg is attached to one end of a light elastic string of modulus of elasticity 13.5 N and natural length 0.45 m. The other end of the string is attached to a fixed point O. The particle P rests in equilibrium at a point A with the string vertical.
\begin{enumerate}[label=(\alph*)]
\item Show that the distance OA is 0.5 m. [3]
\end{enumerate}
At time $t = 0$, P is projected vertically downwards from A with a speed of 1.25 m s$^{-1}$. Throughout the subsequent motion, P experiences a variable resistance $R$ newtons which is of magnitude 0.6 times its speed (in m s$^{-1}$).
\begin{enumerate}[label=(\alph*)]
\setcounter{enumi}{1}
\item Given that the downward displacement of P from A at time $t$ seconds is $x$ metres, show that, while the string remains taut, $x$ satisfies the differential equation
$$\frac{d^2x}{dt^2} + 4\frac{dx}{dt} + 200x = 0.$$ [3]
\item Verify that $x = \frac{5}{56}e^{-2t}\sin(14t)$. [6]
\item Determine whether the string becomes slack during the motion. [5]
\end{enumerate}
\hfill \mbox{\textit{OCR MEI Further Mechanics Major 2022 Q13 [17]}}