CAIE M2 2010 November — Question 6 10 marks

Exam BoardCAIE
ModuleM2 (Mechanics 2)
Year2010
SessionNovember
Marks10
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicVariable acceleration (1D)
TypeAcceleration as function of velocity (separation of variables)
DifficultyStandard +0.3 This is a standard M2 variable acceleration question following a well-established template: apply Newton's second law to get a differential equation, separate variables and integrate, then integrate velocity for distance. The resistance being proportional to velocity (leading to exponential approach to terminal velocity) is a classic setup. All three parts follow routine procedures with no novel problem-solving required, though it does require competent algebraic manipulation and integration skills across multiple steps.
Spec4.10c Integrating factor: first order equations6.06a Variable force: dv/dt or v*dv/dx methods

A cyclist and his bicycle have a total mass of \(81 \text{ kg}\). The cyclist starts from rest and rides in a straight line. The cyclist exerts a constant force of \(135 \text{ N}\) and the motion is opposed by a resistance of magnitude \(9v \text{ N}\), where \(v \text{ m s}^{-1}\) is the cyclist's speed at time \(t \text{ s}\) after starting.
  1. Show that \(\frac{9}{15-v} \frac{dv}{dt} = 1\). [2]
  2. Solve this differential equation to show that \(v = 15(1-e^{-\frac{t}{9}})\). [4]
  3. Find the distance travelled by the cyclist in the first \(9 \text{ s}\) of the motion. [4]

Question 6:
AnswerMarks Guidance
6(i) 81a = 135 – 9v M1
9 dv/dt = 1 AG
AnswerMarks
15−vA1
[2]
(ii) ∫ 1 dv = ∫1dt
AnswerMarks
15−v 9M1
–ln(15 – v) = t/9 (+ c)A1
t = 0, v = 0, hence c = –ln15M1
ln( 15 ) = t/9
15−v
–t/9
15e = 15 – v
–t/9
AnswerMarks
v = 15(1 – e ) AGA1
[4]
AnswerMarks
(iii) x = ∫ 15(1 – e –t/9 )dtM1
–t/9
AnswerMarks
x = 15t + 15e /(1/9) (+ c)A1
t = 0, x=0, hence c = –135
–9/9
AnswerMarks
x(9) = 15x9 + 15x9e – 135M1
x(9) = 49.7 mA1
[4]
Question 6:
6 | (i) 81a = 135 – 9v | M1
9 dv/dt = 1 AG
15−v | A1
[2]
(ii) ∫ 1 dv = ∫1dt
15−v 9 | M1
–ln(15 – v) = t/9 (+ c) | A1
t = 0, v = 0, hence c = –ln15 | M1
ln( 15 ) = t/9
15−v
–t/9
15e = 15 – v
–t/9
v = 15(1 – e ) AG | A1
[4]
(iii) x = ∫ 15(1 – e –t/9 )dt | M1
–t/9
x = 15t + 15e /(1/9) (+ c) | A1
t = 0, x=0, hence c = –135
–9/9
x(9) = 15x9 + 15x9e – 135 | M1
x(9) = 49.7 m | A1
[4]
A cyclist and his bicycle have a total mass of $81 \text{ kg}$. The cyclist starts from rest and rides in a straight line. The cyclist exerts a constant force of $135 \text{ N}$ and the motion is opposed by a resistance of magnitude $9v \text{ N}$, where $v \text{ m s}^{-1}$ is the cyclist's speed at time $t \text{ s}$ after starting.

\begin{enumerate}[label=(\roman*)]
\item Show that $\frac{9}{15-v} \frac{dv}{dt} = 1$. [2]
\item Solve this differential equation to show that $v = 15(1-e^{-\frac{t}{9}})$. [4]
\item Find the distance travelled by the cyclist in the first $9 \text{ s}$ of the motion. [4]
\end{enumerate}

\hfill \mbox{\textit{CAIE M2 2010 Q6 [10]}}