· H2 Mathematics — Ten-Year Series, worked ← All 11 questions

2017 A-Level · Paper 1 · Question 11

2017 H2 Maths Paper 1, Question 11

Differential equations 13 marks motion under gravity
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Part (i)(a)

1 mark
dvdt=c\frac{dv}{dt} = c

Part (i)(b)

3 marks

Approach

With dvdt=c\frac{dv}{dt} = c constant, integrating directly gives vv as a linear function of tt; the initial condition and the value after 2.5 s2.5\ s then pin down the two constants.

dvdt=c\frac{dv}{dt} = c
∫dv=∫c dt\int dv = \int c\, dt
v=ct+Dv = ct + D

Since v=4v = 4 when t=0t = 0, D=4D = 4, so v=ct+4v = ct + 4.

Using the given value v=29v = 29 when t=2.5t = 2.5:

29=2.5c+429 = 2.5c + 4
c=10c = 10

∴\therefore v=10t+4v = 10t + 4, with c=10c = 10.

Part (ii)

5 marks

Approach

The new rate of change is dvdt=10−kv\frac{dv}{dt} = 10 - kv, a first-order equation with vv and tt separable. We integrate both sides, using the initial condition v=0v = 0 at t=0t = 0 to fix the constant, then rearrange to make vv the subject.

dvdt=10−kv\frac{dv}{dt} = 10 - kv

Separating variables,

∫110−kv dv=∫dt\int\frac{1}{10 - kv}\, dv = \int dt
−1kln⁡∣10−kv∣=t+D- \frac{1}{k}\ln|10 - kv| = t + D

Since v=0v = 0 when t=0t = 0:

−1kln⁡10=D- \frac{1}{k}\ln 10 = D

Substituting back:

−1kln⁡∣10−kv∣=t−1kln⁡10- \frac{1}{k}\ln|10 - kv| = t - \frac{1}{k}\ln 10

Multiplying throughout by −k- k:

ln⁡∣10−kv∣=−kt+ln⁡10\ln|10 - kv| = - kt + \ln 10
ln⁡∣10−kv10∣=−kt\ln\left| \frac{10 - kv}{10} \right| = - kt

Note: while the terminal velocity has not yet been reached, v<10kv < \frac{10}{k}, so 10−kv>010 - kv > 0 and the modulus can be dropped.

10−kv10=e−kt\frac{10 - kv}{10} = e^{- kt}
10−kv=10e−kt10 - kv = 10e^{- kt}
v=10k(1−e−kt)v = \frac{10}{k}\left( 1 - e^{- kt} \right)
To check your answer: at t=0t = 0, v=10k(1−1)=0v = \frac{10}{k}(1 - 1) = 0, which matches the given initial condition. ✓

∴\therefore v=10k(1−e−kt)v = \frac{10}{k}\left( 1 - e^{- kt} \right).

Part (iii)

4 marks

Approach

The terminal velocity is the limit of vv as t→∞t \rightarrow \infty. As t→∞t \rightarrow \infty, e−kt→0e^{- kt} \rightarrow 0 (since k>0k > 0), so this limit is 10k\frac{10}{k}, which lets us find kk from the given terminal velocity before solving for tt.

As t→∞t \rightarrow \infty, e−kt→0e^{- kt} \rightarrow 0, so the terminal velocity is

lim⁡t→∞v=10k\lim_{t \rightarrow \infty}v = \frac{10}{k}

Since the terminal velocity is 40 m s−140\ m\, s^{- 1}:

10k=40\frac{10}{k} = 40
k=14k = \frac{1}{4}

So v=40(1−e−t/4)v = 40\left( 1 - e^{- t/4} \right). We require tt such that v=0.9(40)=36v = 0.9(40) = 36:

36=40(1−e−t/4)36 = 40\left( 1 - e^{- t/4} \right)
1−e−t/4=0.91 - e^{- t/4} = 0.9
e−t/4=0.1e^{- t/4} = 0.1
−t4=ln⁡0.1- \frac{t}{4} = \ln 0.1
t=−4ln⁡0.1=4ln⁡10t = - 4\ln 0.1 = 4\ln 10

∴\therefore t=4ln⁡10=9.21 st = 4\ln 10 = 9.21\ s (3 s.f.).

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