Edexcel CP2 2019 June — Question 5 12 marks

Exam BoardEdexcel
ModuleCP2 (Core Pure 2)
Year2019
SessionJune
Marks12
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicSecond order differential equations
TypeParticular solution with initial conditions
DifficultyStandard +0.3 This is a standard second-order differential equation with constant coefficients requiring the auxiliary equation method to find complex roots, leading to the form e^(αt)(A cos βt + B sin βt). Applying initial conditions and finding the maximum displacement are routine procedures covered in Core Pure 2. The question is slightly easier than average because it follows a predictable template with no novel insights required, though it does require careful algebraic manipulation.
Spec4.10d Second order homogeneous: auxiliary equation method4.10g Damped oscillations: model and interpret

  1. An engineer is investigating the motion of a sprung diving board at a swimming pool.
Let \(E\) be the position of the end of the diving board when it is at rest in its equilibrium position and when there is no diver standing on the diving board.
A diver jumps from the diving board.
The vertical displacement, \(h \mathrm {~cm}\), of the end of the diving board above \(E\) is modelled by the differential equation $$4 \frac { \mathrm {~d} ^ { 2 } h } { \mathrm {~d} t ^ { 2 } } + 4 \frac { \mathrm {~d} h } { \mathrm {~d} t } + 37 h = 0$$ where \(t\) seconds is the time after the diver jumps.
  1. Find a general solution of the differential equation. When \(t = 0\), the end of the diving board is 20 cm below \(E\) and is moving upwards with a speed of \(55 \mathrm {~cm} \mathrm {~s} ^ { - 1 }\).
  2. Find, according to the model, the maximum vertical displacement of the end of the diving board above \(E\).
  3. Comment on the suitability of the model for large values of \(t\).

Question 5(a):
AnswerMarks Guidance
Answer/WorkingMark Guidance
\(4m^2+4m+37=0 \Rightarrow m = -\frac{1}{2}\pm 3i\)M1 Uses model to form and solve auxiliary equation \(4m^2+4m+37=0\)
\(h = e^{-0.5t}(A\cos3t+B\sin3t)\)A1 Correct general solution including \(h=\)
Question 5(b):
AnswerMarks Guidance
Answer/WorkingMark Guidance
\(t=0\), \(h=-20 \Rightarrow A=-20\)M1 Applies initial condition
\(\frac{dh}{dt} = -0.5e^{-0.5t}(A\cos3t+B\sin3t)+e^{-0.5t}(-3A\sin3t+3B\cos3t)\); \(t=0\), \(\frac{dh}{dt}=55 \Rightarrow B=15\)M1 Differentiates and applies second condition
\(h = e^{-0.5t}(15\sin3t-20\cos3t)\)A1 Correct particular solution
\(-0.5e^{-0.5t}(15\sin3t-20\cos3t)+e^{-0.5t}(60\sin3t+45\cos3t)=0\)M1 Sets \(\frac{dh}{dt}=0\) and attempts to solve
\(\tan3t = -\frac{22}{21}\) or \(3t+\tan^{-1}\frac{22}{21}=0\)A1, M1 on ePEN Correct equation for \(t\)
\(t = 0.778\) sA1 Correct value of \(t\)
\(h = e^{-0.5\times0.778}(15\sin(3\times0.778)-20\cos(3\times0.778))\)dM1 Substitutes \(t\) value into \(h\)
\(= 16.7\) cmA1 Correct value of \(h\)
Question 5(c):
AnswerMarks Guidance
Answer/WorkingMark Guidance
Considers large values of \(t\) in model for \(h\), or states for large \(t\), \(h\) becomes smaller/zeroM1 Must reference behaviour of model for large \(t\)
E.g. \(h\) is very small for large \(t\), suggesting model suitable as displacement gets smaller; board tends to equilibrium; but \(h\) never exactly zero so not fully appropriate for large \(t\)A1, B1 on ePEN Credit for valid comment about suitability; B1 for additional qualifying remark about limitation
# Question 5(a):

| Answer/Working | Mark | Guidance |
|---|---|---|
| $4m^2+4m+37=0 \Rightarrow m = -\frac{1}{2}\pm 3i$ | M1 | Uses model to form and solve auxiliary equation $4m^2+4m+37=0$ |
| $h = e^{-0.5t}(A\cos3t+B\sin3t)$ | A1 | Correct general solution including $h=$ |

# Question 5(b):

| Answer/Working | Mark | Guidance |
|---|---|---|
| $t=0$, $h=-20 \Rightarrow A=-20$ | M1 | Applies initial condition |
| $\frac{dh}{dt} = -0.5e^{-0.5t}(A\cos3t+B\sin3t)+e^{-0.5t}(-3A\sin3t+3B\cos3t)$; $t=0$, $\frac{dh}{dt}=55 \Rightarrow B=15$ | M1 | Differentiates and applies second condition |
| $h = e^{-0.5t}(15\sin3t-20\cos3t)$ | A1 | Correct particular solution |
| $-0.5e^{-0.5t}(15\sin3t-20\cos3t)+e^{-0.5t}(60\sin3t+45\cos3t)=0$ | M1 | Sets $\frac{dh}{dt}=0$ and attempts to solve |
| $\tan3t = -\frac{22}{21}$ or $3t+\tan^{-1}\frac{22}{21}=0$ | A1, M1 on ePEN | Correct equation for $t$ |
| $t = 0.778$ s | A1 | Correct value of $t$ |
| $h = e^{-0.5\times0.778}(15\sin(3\times0.778)-20\cos(3\times0.778))$ | dM1 | Substitutes $t$ value into $h$ |
| $= 16.7$ cm | A1 | Correct value of $h$ |

# Question 5(c):

| Answer/Working | Mark | Guidance |
|---|---|---|
| Considers large values of $t$ in model for $h$, or states for large $t$, $h$ becomes smaller/zero | M1 | Must reference behaviour of model for large $t$ |
| E.g. $h$ is very small for large $t$, suggesting model suitable as displacement gets smaller; board tends to equilibrium; but $h$ never exactly zero so not fully appropriate for large $t$ | A1, B1 on ePEN | Credit for valid comment about suitability; B1 for additional qualifying remark about limitation |
\begin{enumerate}
  \item An engineer is investigating the motion of a sprung diving board at a swimming pool.
\end{enumerate}

Let $E$ be the position of the end of the diving board when it is at rest in its equilibrium position and when there is no diver standing on the diving board.\\
A diver jumps from the diving board.\\
The vertical displacement, $h \mathrm {~cm}$, of the end of the diving board above $E$ is modelled by the differential equation

$$4 \frac { \mathrm {~d} ^ { 2 } h } { \mathrm {~d} t ^ { 2 } } + 4 \frac { \mathrm {~d} h } { \mathrm {~d} t } + 37 h = 0$$

where $t$ seconds is the time after the diver jumps.\\
(a) Find a general solution of the differential equation.

When $t = 0$, the end of the diving board is 20 cm below $E$ and is moving upwards with a speed of $55 \mathrm {~cm} \mathrm {~s} ^ { - 1 }$.\\
(b) Find, according to the model, the maximum vertical displacement of the end of the diving board above $E$.\\
(c) Comment on the suitability of the model for large values of $t$.

\hfill \mbox{\textit{Edexcel CP2 2019 Q5 [12]}}