Edexcel C4 2008 January — Question 8 13 marks

Exam BoardEdexcel
ModuleC4 (Core Mathematics 4)
Year2008
SessionJanuary
Marks13
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicDifferential equations
TypeSubstitution method
DifficultyStandard +0.3 This is a structured multi-part C4 differential equations question with clear scaffolding. Parts (a) and (b) involve straightforward modeling and substitution. Part (c) requires standard separation of variables. Part (d) provides the substitution needed for integration. While it requires multiple techniques (modeling, separation, substitution integration), each step is guided and uses standard C4 methods, making it slightly easier than average.
Spec1.07t Construct differential equations: in context1.08k Separable differential equations: dy/dx = f(x)g(y)

8. Liquid is pouring into a large vertical circular cylinder at a constant rate of \(1600 \mathrm {~cm} ^ { 3 } \mathrm {~s} ^ { - 1 }\) and is leaking out of a hole in the base, at a rate proportional to the square root of the height of the liquid already in the cylinder. The area of the circular cross section of the cylinder is \(4000 \mathrm {~cm} ^ { 2 }\).
  1. Show that at time \(t\) seconds, the height \(h \mathrm {~cm}\) of liquid in the cylinder satisfies the differential equation $$\frac { \mathrm { d } h } { \mathrm {~d} t } = 0.4 - k \sqrt { } h \text {, where } k \text { is a positive constant. }$$ When \(h = 25\), water is leaking out of the hole at \(400 \mathrm {~cm} ^ { 3 } \mathrm {~s} ^ { - 1 }\).
  2. Show that \(k = 0.02\)
  3. Separate the variables of the differential equation $$\frac { \mathrm { d } h } { \mathrm {~d} t } = 0.4 - 0.02 \sqrt { } h$$ to show that the time taken to fill the cylinder from empty to a height of 100 cm is given by $$\int _ { 0 } ^ { 100 } \frac { 50 } { 20 - \sqrt { } h } \mathrm {~d} h$$ Using the substitution \(h = ( 20 - x ) ^ { 2 }\), or otherwise,
  4. find the exact value of \(\int _ { 0 } ^ { 100 } \frac { 50 } { 20 - \sqrt { h } } \mathrm {~d} h\).
  5. Hence find the time taken to fill the cylinder from empty to a height of 100 cm , giving your answer in minutes and seconds to the nearest second.

Question 8:
Part (a):
AnswerMarks Guidance
WorkingMark Guidance
\(\frac{dV}{dt} = 1600 - c\sqrt{h}\) or \(\frac{dV}{dt}=1600-k\sqrt{h}\)M1 Either of these statements
\((V=4000h) \Rightarrow \frac{dV}{dh}=4000\)M1 \(\frac{dV}{dh}=4000\) or \(\frac{dh}{dV}=\frac{1}{4000}\)
\(\frac{dh}{dt}=\frac{dh}{dV}\times\frac{dV}{dt} = \frac{\frac{dV}{dt}}{\frac{dV}{dh}}\)
\(\frac{dh}{dt}=\frac{1600-c\sqrt{h}}{4000}=\frac{1600}{4000}-\frac{c\sqrt{h}}{4000}=0.4-k\sqrt{h}\)A1 AG Convincing proof of \(\frac{dh}{dt}\) [3]
Part (b):
AnswerMarks Guidance
WorkingMark Guidance
When \(h=25\), \(\frac{dV}{dt}=400\): \(400=c\sqrt{25}=c(5) \Rightarrow c=80\)
\(k=\frac{c}{4000}=\frac{80}{4000}=0.02\)B1 AG Proof that \(k=0.02\) [1]
Aliter Way 2:
AnswerMarks Guidance
WorkingMark Guidance
\(400=4000k\sqrt{25} \Rightarrow 400=k(20000) \Rightarrow k=\frac{400}{20000}=0.02\)B1 AG Using 400, 4000 and \(h=25\) or \(\sqrt{h}=5\). Proof that \(k=0.02\) [1]
Part (c):
AnswerMarks Guidance
WorkingMark Guidance
\(\frac{dh}{dt}=0.4-k\sqrt{h} \Rightarrow \int\frac{dh}{0.4-k\sqrt{h}}=\int dt\)M1 oe Separates the variables with \(\int\frac{dh}{0.4-k\sqrt{h}}\) and \(\int dt\) on either side, integral signs not necessary
\(\therefore \text{time required} = \int_0^{100}\frac{1}{0.4-0.02\sqrt{h}}dh\ (\div 0.02)\)
\(\text{time required} = \int_0^{100}\frac{50}{20-\sqrt{h}}dh\)A1 AG Correct proof [2]
Part (d):
AnswerMarks Guidance
WorkingMark Guidance
\(\int_0^{100}\frac{50}{20-\sqrt{h}}dh\) with substitution \(h=(20-x)^2\)
\(\frac{dh}{dx}=2(20-x)(-1)\) or \(\frac{dh}{dx}=-2(20-x)\)B1 aef Correct \(\frac{dh}{dx}\)
\(h=(20-x)^2 \Rightarrow \sqrt{h}=20-x \Rightarrow x=20-\sqrt{h}\)
\(\int\frac{50}{20-\sqrt{h}}dh = \int\frac{50}{x}\cdot -2(20-x)dx\)M1 \(\pm\lambda\int\frac{20-x}{x}dx\) or \(\pm\lambda\int\frac{20-x}{20-(20-x)}dx\) where \(\lambda\) is a constant
\(= 100\int\frac{x-20}{x}dx = 100\int\left(1-\frac{20}{x}\right)dx\)
\(= 100(x-20\ln x)\ (+c)\)M1 \(\pm\alpha x \pm \beta\ln x;\ \alpha,\beta\neq 0\)
A1\(100x - 2000\ln x\)
Change limits: \(h=0\Rightarrow x=20\); \(h=100\Rightarrow x=10\)
\(\int_0^{100}\frac{50}{20-\sqrt{h}}dh = \left[100x-2000\ln x\right]_{20}^{10}\)ddM1 Correct use of limits, putting them in the correct way round. Either \(x=10\) and \(x=20\) or \(h=100\) and \(h=0\)
\(= (1000-2000\ln 10)-(2000-2000\ln 20)\)
\(= 2000\ln 20 - 2000\ln 10 - 1000\) Combining logs to give \(2000\ln 2 - 1000\)
\(= 2000\ln 2 - 1000\)A1 aef or \(-2000\ln\left(\frac{1}{2}\right)-1000\) [6]
Part (e):
AnswerMarks Guidance
WorkingMark Guidance
Time required \(= 2000\ln 2 - 1000 = 386.2943611\ldots\) sec \(= 386\) seconds (nearest second) \(= 6\) minutes and 26 secondsB1 6 minutes, 26 seconds [1]
Total: 13 marks
# Question 8:

## Part (a):

| Working | Mark | Guidance |
|---------|------|----------|
| $\frac{dV}{dt} = 1600 - c\sqrt{h}$ or $\frac{dV}{dt}=1600-k\sqrt{h}$ | M1 | Either of these statements |
| $(V=4000h) \Rightarrow \frac{dV}{dh}=4000$ | M1 | $\frac{dV}{dh}=4000$ or $\frac{dh}{dV}=\frac{1}{4000}$ |
| $\frac{dh}{dt}=\frac{dh}{dV}\times\frac{dV}{dt} = \frac{\frac{dV}{dt}}{\frac{dV}{dh}}$ | | |
| $\frac{dh}{dt}=\frac{1600-c\sqrt{h}}{4000}=\frac{1600}{4000}-\frac{c\sqrt{h}}{4000}=0.4-k\sqrt{h}$ | A1 AG | Convincing proof of $\frac{dh}{dt}$ **[3]** |

## Part (b):

| Working | Mark | Guidance |
|---------|------|----------|
| When $h=25$, $\frac{dV}{dt}=400$: $400=c\sqrt{25}=c(5) \Rightarrow c=80$ | | |
| $k=\frac{c}{4000}=\frac{80}{4000}=0.02$ | B1 AG | Proof that $k=0.02$ **[1]** |

**Aliter Way 2:**

| Working | Mark | Guidance |
|---------|------|----------|
| $400=4000k\sqrt{25} \Rightarrow 400=k(20000) \Rightarrow k=\frac{400}{20000}=0.02$ | B1 AG | Using 400, 4000 and $h=25$ or $\sqrt{h}=5$. Proof that $k=0.02$ **[1]** |

## Part (c):

| Working | Mark | Guidance |
|---------|------|----------|
| $\frac{dh}{dt}=0.4-k\sqrt{h} \Rightarrow \int\frac{dh}{0.4-k\sqrt{h}}=\int dt$ | M1 oe | Separates the variables with $\int\frac{dh}{0.4-k\sqrt{h}}$ and $\int dt$ on either side, integral signs not necessary |
| $\therefore \text{time required} = \int_0^{100}\frac{1}{0.4-0.02\sqrt{h}}dh\ (\div 0.02)$ | | |
| $\text{time required} = \int_0^{100}\frac{50}{20-\sqrt{h}}dh$ | A1 AG | Correct proof **[2]** |

## Part (d):

| Working | Mark | Guidance |
|---------|------|----------|
| $\int_0^{100}\frac{50}{20-\sqrt{h}}dh$ with substitution $h=(20-x)^2$ | | |
| $\frac{dh}{dx}=2(20-x)(-1)$ or $\frac{dh}{dx}=-2(20-x)$ | B1 aef | Correct $\frac{dh}{dx}$ |
| $h=(20-x)^2 \Rightarrow \sqrt{h}=20-x \Rightarrow x=20-\sqrt{h}$ | | |
| $\int\frac{50}{20-\sqrt{h}}dh = \int\frac{50}{x}\cdot -2(20-x)dx$ | M1 | $\pm\lambda\int\frac{20-x}{x}dx$ or $\pm\lambda\int\frac{20-x}{20-(20-x)}dx$ where $\lambda$ is a constant |
| $= 100\int\frac{x-20}{x}dx = 100\int\left(1-\frac{20}{x}\right)dx$ | | |
| $= 100(x-20\ln x)\ (+c)$ | M1 | $\pm\alpha x \pm \beta\ln x;\ \alpha,\beta\neq 0$ |
| | A1 | $100x - 2000\ln x$ |
| Change limits: $h=0\Rightarrow x=20$; $h=100\Rightarrow x=10$ | | |
| $\int_0^{100}\frac{50}{20-\sqrt{h}}dh = \left[100x-2000\ln x\right]_{20}^{10}$ | ddM1 | Correct use of limits, putting them in the correct way round. Either $x=10$ and $x=20$ or $h=100$ and $h=0$ |
| $= (1000-2000\ln 10)-(2000-2000\ln 20)$ | | |
| $= 2000\ln 20 - 2000\ln 10 - 1000$ | | Combining logs to give $2000\ln 2 - 1000$ |
| $= 2000\ln 2 - 1000$ | A1 aef | or $-2000\ln\left(\frac{1}{2}\right)-1000$ **[6]** |

## Part (e):

| Working | Mark | Guidance |
|---------|------|----------|
| Time required $= 2000\ln 2 - 1000 = 386.2943611\ldots$ sec $= 386$ seconds (nearest second) $= 6$ minutes and 26 seconds | B1 | 6 minutes, 26 seconds **[1]** |

**Total: 13 marks**
8. Liquid is pouring into a large vertical circular cylinder at a constant rate of $1600 \mathrm {~cm} ^ { 3 } \mathrm {~s} ^ { - 1 }$ and is leaking out of a hole in the base, at a rate proportional to the square root of the height of the liquid already in the cylinder. The area of the circular cross section of the cylinder is $4000 \mathrm {~cm} ^ { 2 }$.
\begin{enumerate}[label=(\alph*)]
\item Show that at time $t$ seconds, the height $h \mathrm {~cm}$ of liquid in the cylinder satisfies the differential equation

$$\frac { \mathrm { d } h } { \mathrm {~d} t } = 0.4 - k \sqrt { } h \text {, where } k \text { is a positive constant. }$$

When $h = 25$, water is leaking out of the hole at $400 \mathrm {~cm} ^ { 3 } \mathrm {~s} ^ { - 1 }$.
\item Show that $k = 0.02$
\item Separate the variables of the differential equation

$$\frac { \mathrm { d } h } { \mathrm {~d} t } = 0.4 - 0.02 \sqrt { } h$$

to show that the time taken to fill the cylinder from empty to a height of 100 cm is given by

$$\int _ { 0 } ^ { 100 } \frac { 50 } { 20 - \sqrt { } h } \mathrm {~d} h$$

Using the substitution $h = ( 20 - x ) ^ { 2 }$, or otherwise,
\item find the exact value of $\int _ { 0 } ^ { 100 } \frac { 50 } { 20 - \sqrt { h } } \mathrm {~d} h$.
\item Hence find the time taken to fill the cylinder from empty to a height of 100 cm , giving your answer in minutes and seconds to the nearest second.
\end{enumerate}

\hfill \mbox{\textit{Edexcel C4 2008 Q8 [13]}}