A2 June 2021 Paper 1 Q15
15 In this question use \(g = 9.8\) m s−2
A particle \(P\) of mass \(m\) is attached to two light elastic strings, \(AP\) and \(BP\).
The other ends of the strings, \(A\) and \(B\), are attached to fixed points which are 4 metres apart on a rough horizontal surface at the bottom of a container.
The coefficient of friction between \(P\) and the surface is 0.68
- When the extension of string \(AP\) is \(e_A\) metres, the tension in \(AP\) is \(24me_A\)
- When the extension of string \(BP\) is \(e_B\) metres, the tension in \(BP\) is \(10me_B\)
- The natural length of string \(AP\) is 1 metre
- The natural length of string \(BP\) is 1.3 metres

At time \(t\) seconds after \(P\) is released, \(AP = (1.5 + x)\) metres.

Show that when \(P\) is moving towards \(A\),
\[\frac{\mathrm{d}^2x}{\mathrm{d}t^2} + 34x = 6.664\][3 marks]
At time \(t\) seconds after \(P\) is released, the oil causes a resistive force of magnitude \(10mv\) newtons to act on the particle, where \(v\) m s−1 is the speed of the particle.
Find \(x\) in terms of \(t\) when \(P\) is moving towards \(A\). [9 marks]
| Scheme | Marks | AO |
|---|---|---|
| Uses a rigorous argument to obtain the required result | R1 | 2.1 |
| (1) |
Typical solution
Tension in \(AP = 24m(0.5) = 12m\)
Tension in \(BP = 10m(1.2) = 12m\)
So tensions are equal
| Scheme | Marks | AO |
|---|---|---|
| Obtains one correct tension | B1 | 1.1a |
| Uses Newton’s second law to form a four term differential equation with at least two terms correct (allow equivalent notation for derivatives) Condone sign errors on the terms | M1 | 3.1b |
| Completes a rigorous argument to give the required differential equation | R1 | 2.1 |
| (3) |
Typical solution
\[m\frac{\mathrm{d}^2x}{\mathrm{d}t^2} = 10m(1.2 - x) - 24m(0.5 + x) + 6.664m\]\[\frac{\mathrm{d}^2x}{\mathrm{d}t^2} + 34x = 6.664\]| Scheme | Marks | AO |
|---|---|---|
| Obtains correct 2nd order DE | B1 | 2.2a |
| Obtains correct solution to their three term Auxiliary Equation | M1 | 1.1a |
| Obtains their correct Complementary Function | A1F | 1.1b |
| Obtains correct Particular Integral ACF | B1 | 1.1b |
| Obtains correct general solution (ft their CF, but must have two unknowns) | A1F | 2.2a |
| Uses \(x = 0.4\) when \(t = 0\) to obtain correct \(A\) ACF | B1 | 3.3 |
| Sets their correct \(\dot{x} = 0\) when \(t = 0\) | M1 | 1.1a |
| Obtains correct \(B\) ACF | A1 | 1.1b |
| Obtains correct final equation ACF | R1 | 2.1 |
| (9) | ||
| (13 marks) |
Typical solution
\[m\ddot{x} = 10mv + 6.664m - 34mx\]But \(v = -\dot{x}\)
So
\[\ddot{x} + 10\dot{x} + 34x = 6.664\]\[\lambda^2 + 10\lambda + 34 = 0\]\[\lambda = -5 \pm 3\mathrm{i}\]CF:
\[x = A\mathrm{e}^{-5t}\cos 3t + B\mathrm{e}^{-5t}\sin 3t\]PI: \(x = 0.196\)
General Solution:
\[x = A\mathrm{e}^{-5t}\cos 3t + B\mathrm{e}^{-5t}\sin 3t + 0.196\]\[t = 0,\ x = 0.4 \Rightarrow A = 0.204\]\[\begin{aligned} \dot{x} = {} & -5A\mathrm{e}^{-5t}\cos 3t - 3A\mathrm{e}^{-5t}\sin 3t \\ & -5B\mathrm{e}^{-5t}\sin 3t + 3B\mathrm{e}^{-5t}\cos 3t \end{aligned}\]\[0 = -5A + 3B\]\[B = 0.34\]\[x = 0.204\mathrm{e}^{-5t}\cos 3t + 0.34\mathrm{e}^{-5t}\sin 3t + 0.196\]