VCAA Specialist Mathematics Calculus

15 sample questions with marking guides and sample answers

Q6
2025
VCAA
Paper 1
4 marks
Q6
4 marks

Find the volume of the solid of revolution formed when the area between the curve

y=arctan(x)1+x2y = \sqrt{\frac{\arctan(x)}{1+x^2}}

and the xx-axis from x=1x = 1 to x=3x = \sqrt{3} is rotated about the xx-axis.

Give your answer in the form aπbc\frac{a\pi^b}{c}, where a,b,cZ+a, b, c \in Z^+.

Reveal Answer

V=π13arctan(x)1+x2dxV = \pi \int_1^{\sqrt{3}} \frac{\arctan(x)}{1+x^2} dx

Method 1 (substitution)
u=arctan(x), du=dx1+x2u = \arctan(x), \ du = \frac{dx}{1+x^2}.

V=ππ4π3u du=π[u22]π4π3=π32(19116)=7π3288\begin{align*} V &= \pi \int_{\frac{\pi}{4}}^{\frac{\pi}{3}} u \ du\\ &= \pi \left[ \frac{u^2}{2} \right]_{\frac{\pi}{4}}^{\frac{\pi}{3}}\\ &= \frac{\pi^3}{2} \left( \frac{1}{9} - \frac{1}{16} \right)\\ &= \frac{7\pi^3}{288} \end{align*}
Marking Criteria
DescriptorMarks

Sets up the correct definite integral for the volume of revolution, including the factor of π\pi

1

Identifies the correct substitution u=arctan(x)u = \arctan(x) and corresponding du=dx1+x2du = \frac{dx}{1+x^2}

1

Correctly changes the limits of integration to π4\frac{\pi}{4} and π3\frac{\pi}{3} and finds the antiderivative

1

Evaluates the integral to obtain the correct final answer 7π3288\frac{7\pi^3}{288}

1
Q3
2025
VCAA
Paper 2
10 marks
Q3

A tank initially contains 5 kg5 \text{ kg} of salt dissolved in 3000 litres3000 \text{ litres} of water. Salty water that contains 0.1 kg0.1 \text{ kg} of salt per litre of water enters the tank at a rate of 20 litres per minute20 \text{ litres per minute}. The solution is kept thoroughly mixed and drains from the tank via a tap at the same rate of 20 litres per minute20 \text{ litres per minute}.

Q3a
1 mark

By considering concentration, explain whether the quantity of salt in the tank increases with time.

Reveal Answer

The initial concentration =53000=1600= \frac{5}{3000} = \frac{1}{600} which is smaller than the incoming concentration
=0.1 kg/litre= 0.1 \text{ kg/litre}; hence, the quantity of salt increases.

Marking Criteria
DescriptorMarks

Explains that the quantity of salt increases by correctly comparing the initial concentration (1600 kg/L\frac{1}{600} \text{ kg/L}) to the incoming concentration (0.1 kg/L0.1 \text{ kg/L})

1
Q3b
1 mark

Let QQ denote the quantity of salt, in kilograms, in the tank at time t minutest \text{ minutes}.

Show that QQ satisfies the differential equation dQdt=300Q150\frac{dQ}{dt} = \frac{300 - Q}{150}.

Reveal Answer

dQdt=0.1×20Q3000×20=300150Q150\frac{dQ}{dt} = 0.1 \times 20 - \frac{Q}{3000} \times 20 = \frac{300}{150} - \frac{Q}{150}

Marking Criteria
DescriptorMarks

Shows the correct development of the differential equation by subtracting the rate out (Q3000×20\frac{Q}{3000} \times 20) from the rate in (0.1×200.1 \times 20)

1
Q3c
2 marks

Using Euler's method with a step size of 15 minutes15 \text{ minutes}, find Q(30)Q(30), the approximate quantity of salt in the tank after 30 minutes30 \text{ minutes}.

Give your answer in kilograms, correct to two decimal places.

Reveal Answer

61.05

Qn+1=Qn+15×300Qn150Q_{n+1} = Q_n + 15 \times \frac{300 - Q_n}{150}
Q(15)=692Q(15) = \frac{69}{2}
Q(30)=61.05Q(30) = 61.05

Marking Criteria
DescriptorMarks

Calculates the correct value for Q(15)Q(15) (692\frac{69}{2}) or demonstrates correct application of Euler's method

1

Calculates the correct final answer of 61.0561.05

1
Q3d
3 marks

Use calculus to solve the differential equation dQdt=300Q150\frac{dQ}{dt} = \frac{300 - Q}{150}, expressing QQ in terms of tt.

Reveal Answer

dQdt=300Q150t=150300QdQt=150loge(300Q)+cc=150loge(295)t=150loge(295300Q)Q=300295et150\begin{align*} \frac{dQ}{dt} &= \frac{300 - Q}{150}\\ t &= \int \frac{150}{300 - Q} dQ\\ t &= -150 \log_e(|300 - Q|) + c\\ c &= 150 \log_e(295)\\ t &= 150 \log_e\left(\frac{295}{300 - Q}\right)\\ Q &= 300 - 295 e^{-\frac{t}{150}} \end{align*}
Marking Criteria
DescriptorMarks

Correctly integrates the differential equation to find an expression involving a constant of integration (e.g., t=150loge(300Q)+ct = -150 \log_e(|300 - Q|) + c)

1

Correctly uses the initial condition to evaluate the constant of integration

1

Correctly expresses QQ in terms of tt as Q=300295et150Q = 300 - 295 e^{-\frac{t}{150}}

1
Q3e
1 mark

What value does the quantity of salt in the tank approach as time approaches infinity?

Give your answer in kilograms.

Reveal Answer

300 kg

Marking Criteria
DescriptorMarks

States the correct limiting value of 300300

1
Q3f
1 mark

Find the time taken for the quantity of salt in the tank to reach 100 kg100 \text{ kg}.

Reveal Answer

t=150loge(5940)t = 150 \log_e\left(\frac{59}{40}\right)

Marking Criteria
DescriptorMarks

Calculates the correct exact time of 150loge(5940)150 \log_e\left(\frac{59}{40}\right)

1
Q3g
1 mark

When the quantity of salt in the tank reaches 100 kg100 \text{ kg}, the tap draining the tank is turned off. Assume that the tank does not overflow and there is no change to the inflow rate.

After the tap is turned off, how many minutes does it take for the concentration of salt in the tank to reach 120 kg L1\frac{1}{20} \text{ kg L}^{-1}?

Reveal Answer

50

This can be found by equating the concentration to the given value 2t+1003000+20t=120\frac{2t + 100}{3000 + 20t} = \frac{1}{20}.

Marking Criteria
DescriptorMarks

Calculates the correct time of 5050 minutes

1
Q12
2021
SCSA
Paper 2
6 marks
Q12

The horizontal displacement of a Ferris wheel cabin exhibits simple harmonic motion. The maximum horizontal speed is π2\frac{\pi}{2} metres per second and its period of motion is exactly 60 seconds.

Let x(t)=Acos(nt)x(t) = A\cos(nt) be the horizontal displacement after tt seconds.

Q12a
3 marks

Determine the values of AA and nn.

Reveal Answer

Period T=60=2πn    n=π30(0.1047....)T = 60 = \frac{2\pi}{n} \implies \therefore n = \frac{\pi}{30} \quad (0.1047....)

v(t)=A(π30)sin(πt30)v(t) = -A\left(\frac{\pi}{30}\right)\sin\left(\frac{\pi t}{30}\right)

Max v=A(π30)=π2    A=15\therefore \text{Max } v = A\left(\frac{\pi}{30}\right) = \frac{\pi}{2} \implies \therefore A = 15

Hence x(t)=15cos(πt30)x(t) = 15\cos\left(\frac{\pi t}{30}\right)

Marking Criteria
DescriptorMarks

determines nn correctly

1

differentiates and forms the correct expression for the maximum speed

1

determines AA correctly

1
Q12b
3 marks

Determine the horizontal acceleration, correct to the nearest 0.001 m/s20.001\text{ m/s}^2, when the horizontal displacement is 10 metres.

Reveal Answer

Condition for S.H.M. is a=(π30)2xa = -\left(\frac{\pi}{30}\right)^2 x

\therefore When x=10a=(π2900)(10)=0.10966... metres/sec2x = 10 \quad a = -\left(\frac{\pi^2}{900}\right)(10) = -0.10966 ... \text{ metres/sec}^2

i.e. acceleration is 0.110 m/sec2-0.110 \text{ m/sec}^2 (3 d.p.)

Marking Criteria
DescriptorMarks

applies the condition for S.H.M. correctly

1

substitutes x=10x = 10 correctly

1

determines the acceleration correct to 0.001 m/sec20.001 \text{ m/sec}^2

1
Q6
2025
QCAA
Paper 2
1 mark
Q6
1 mark

Determine the gradient of the tangent to y2=4xy^2 = 4x when y=1y = 1.

A

4

B

2

C

0.5

D

0.25

Reveal Answer
A

4

Incorrect. This is the derivative of the right side (4x4x) with respect to xx, but it fails to apply implicit differentiation to the y2y^2 term.

B

2

Correct Answer

Correct. Using implicit differentiation, 2ydydx=42y \frac{dy}{dx} = 4, which simplifies to dydx=2y\frac{dy}{dx} = \frac{2}{y}. Substituting y=1y = 1 gives a gradient of 2.

C

0.5

Incorrect. This calculates dxdy=y2=0.5\frac{dx}{dy} = \frac{y}{2} = 0.5, which is the reciprocal of the gradient. The gradient of the tangent must be dydx\frac{dy}{dx}.

D

0.25

Incorrect. This is the xx-coordinate of the point on the curve when y=1y = 1 (since 12=4x    x=0.251^2 = 4x \implies x = 0.25), not the gradient of the tangent line.

Q3
2024
VCAA
Paper 2
10 marks
Q3

A pollutant, at time t=0t = 0 days, begins to enter a pond of still, unpolluted water at a rate of dVdt=8t240+5t4\frac{dV}{dt} = \frac{8t}{240 + 5t^4}, where VV is the volume of pollutant, in cubic metres, in the pond after tt days.

The pollutant does not dissolve or mix, and spreads across the pond, maintaining the shape of a thin circular disc of radius r(t)r(t) metres and constant depth of 11 millimetre.

Q3a
1 mark

What is the maximum rate, in cubic metres per day, at which the pollutant will enter the pond, and for what value of tt will this rate occur?

Reveal Answer

The maximum rate occurs when d2Vdt2=1920120t4(240+5t4)2=0\frac{d^2V}{dt^2} = \frac{1920 - 120t^4}{(240+5t^4)^2} = 0, so 1920120t4=120(16t4)=01920 - 120t^4 = 120(16-t^4) = 0, so as t>0t > 0 then t=2t = 2, at which time dVdt=16240+524=16320=120\frac{dV}{dt} = \frac{16}{240+5 \cdot 2^4} = \frac{16}{320} = \frac{1}{20} cubic metres per day.

0.05=1200.05 = \frac{1}{20} (cubic metres per day) when t=2t = 2

Marking Criteria
DescriptorMarks

Calculates the correct maximum rate of 120\frac{1}{20} (or 0.050.05) cubic metres per day and the correct time t=2t = 2

1
Q3b
3 marks

At what rate is the radius of the disc increasing after t=4t = 4 days, where it may be assumed that the radius of the disc is 6.546.54 m?

Give your answer in metres per day correct to two decimal places.

Reveal Answer

Let rr be the radius in metres, so V=πr21000V = \frac{\pi r^2}{1000} and hence dVdt=π10002rdrdt=π500rdrdt\frac{dV}{dt} = \frac{\pi}{1000} 2r \frac{dr}{dt} = \frac{\pi}{500} r \frac{dr}{dt}.

When t=4t = 4 we have dVdt=48240+544=321520=295\frac{dV}{dt} = \frac{4 \cdot 8}{240 + 5 \cdot 4^4} = \frac{32}{1520} = \frac{2}{95}.

Also substituting r=6.54r = 6.54 we obtain 295=π5006.54drdt\frac{2}{95} = \frac{\pi}{500} 6.54 \frac{dr}{dt} which yields drdt=100095π×6.540.51\frac{dr}{dt} = \frac{1000}{95\pi \times 6.54} \approx 0.51
drdt=0.51\frac{dr}{dt} = 0.51

Marking Criteria
DescriptorMarks

Establishes a correct relationship between the rates of change, such as dVdt=π500rdrdt\frac{dV}{dt} = \frac{\pi}{500} r \frac{dr}{dt}

1

Calculates the correct rate of change of volume at t=4t = 4, dVdt=295\frac{dV}{dt} = \frac{2}{95}

1

Calculates the correct rate of change of the radius, 0.510.51

1
Q3c (i)
1 mark

Use the substitution u=5t2u = \sqrt{5} t^2 to express 8t240+5t4dt\int \frac{8t}{240 + 5t^4} \, dt as an integral involving only the variable uu.

Reveal Answer

We have dudt=25t\frac{du}{dt} = 2\sqrt{5} t and u2=5t4u^2 = 5t^4, so t dt=du25t \ dt = \frac{du}{2\sqrt{5}} and 8t240+5t4dt=8240+u2du25=45du240+u2\int \frac{8t}{240+5t^4} dt = \int \frac{8}{240+u^2} \frac{du}{2\sqrt{5}} = \frac{4}{\sqrt{5}} \int \frac{du}{240+u^2}

Marking Criteria
DescriptorMarks

Correctly expresses the integral in terms of uu, 451240+u2du\frac{4}{\sqrt{5}} \int \frac{1}{240+u^2} du

1
Q3c (ii)
1 mark

Hence, or otherwise, find, in terms of tt, the total volume V m3V \text{ m}^3 of pollutant that has entered the pond after tt days.

Give your answer in the form 1abarctan(tcdb)\frac{1}{a\sqrt{b}} \arctan\left(\frac{t^c}{d\sqrt{b}}\right), where a,b,c,dZ+a, b, c, d \in Z^+.

Reveal Answer

V=0t8t240+5t4dt=4505t21240+u2du=4524005t2240240+u2du=175[arctan(u240)]05t2=153arctan(5t2240)\begin{align*} V &= \int_0^t \frac{8t'}{240+5t'^4} dt'\\ &= \frac{4}{\sqrt{5}} \int_0^{\sqrt{5}t^2} \frac{1}{240+u^2} du\\ &= \frac{4}{\sqrt{5 \cdot 240}} \int_0^{\sqrt{5}t^2} \frac{\sqrt{240}}{240+u^2} du \\ &= \frac{1}{\sqrt{75}} \left[ \arctan\left(\frac{u}{\sqrt{240}}\right) \right]_0^{\sqrt{5}t^2}\\ &= \frac{1}{5\sqrt{3}} \arctan\left(\frac{\sqrt{5}t^2}{\sqrt{240}}\right) \end{align*}
Marking Criteria
DescriptorMarks

Correctly evaluates the integral and expresses the volume in the required form, 153arctan(t243)\frac{1}{5\sqrt{3}} \arctan\left(\frac{t^2}{4\sqrt{3}}\right)

1
Q3d
2 marks

What surface area of the pond would the coverage of the pollutant approach?

Give your answer in square metres correct to two decimal places.

Reveal Answer

Since volume = surface area ×11000\times \frac{1}{1000}, surface area is given by 1000V=2003arctan(t243)1000 V = \frac{200}{\sqrt{3}} \arctan\left(\frac{t^2}{4\sqrt{3}}\right).

As tt \to \infty the surface area approaches 2003π2=100π3=181.38\frac{200}{\sqrt{3}} \cdot \frac{\pi}{2} = \frac{100\pi}{\sqrt{3}} = 181.38

Marking Criteria
DescriptorMarks

Correctly identifies the limit of the arctan function as tt \to \infty is π2\frac{\pi}{2} to find the limiting surface area

1

Calculates the correct limiting surface area, 181.38181.38

1
Q3e
2 marks

The clean-up of the pond begins after five days, where the pollutant is removed at a constant rate of 0.050.05 cubic metres per day until the pond is free of pollutant. However, efforts to stem the flow are unsuccessful and the pollutant continues to enter the pond at a rate of 8t240+5t4\frac{8t}{240 + 5t^4} cubic metres per day.

After how many days, from the start of the clean-up, will the pond be free of pollutant?
Give your answer in days correct to one decimal place.

Reveal Answer

The volume of the pollutant after 5 days is V(5)V(5)

To find the number of days needed for the pond to be free of pollutant solve

0=5t+5(8x240+5x40.05)dx+V(5)t=3.40 = \int_5^{t+5} \left(\frac{8x}{240+5x^4} - 0.05\right) dx + V(5) \Rightarrow t = 3.4 days

Marking Criteria
DescriptorMarks

Sets up a correct equation to solve for the time, accounting for the 5-day delay and the constant removal rate, such as 0=5t+5(8x240+5x40.05)dx+V(5)0 = \int_5^{t+5} \left(\frac{8x}{240+5x^4} - 0.05\right) dx + V(5)

1

Calculates the correct number of days, 3.43.4

1
Q13
2025
VCAA
Paper 2
1 mark
Q13
1 mark

From an open window, a person projects a ball vertically up using an outstretched arm so the ball does not strike any part of the building. The point of projection of the ball is 50 m50 \text{ m} above the ground and its velocity of projection is 20 m s120 \text{ m s}^{-1}.

The time, in seconds, it takes for the ball to reach the tray of a truck that is 1 m1 \text{ m} above the ground directly below the point of projection is closest to

A

1.721.72

B

5.805.80

C

5.835.83

D

1.751.75

Reveal Answer
A

1.721.72

This is the magnitude of the negative root of the kinematic equation, which represents the time if the trajectory was extended backwards before projection.

B

5.805.80

Correct Answer

Using the kinematic equation Δy=ut+12at2\Delta y = ut + \frac{1}{2}at^2 with a displacement of Δy=49 m\Delta y = -49 \text{ m} (since the tray is 1 m1 \text{ m} above the ground), u=20 m s1u = 20 \text{ m s}^{-1}, and a=9.8 m s2a = -9.8 \text{ m s}^{-2} yields t5.80 st \approx 5.80 \text{ s}.

C

5.835.83

This is the time it would take for the ball to reach the ground (Δy=50 m\Delta y = -50 \text{ m}), failing to account for the truck tray being 1 m1 \text{ m} above the ground.

D

1.751.75

This is the magnitude of the negative root if the displacement was incorrectly set to 50 m-50 \text{ m} (reaching the ground instead of the truck tray).

Q13
2020
QCAA
Paper 1
4 marks
Q13
4 marks

The expected value of an exponential random variable XX with parameter λ>0\lambda > 0 can be determined using the rule

E(X)=0xλeλxdxE(X) = \int_0^\infty x\lambda e^{-\lambda x} dx

Use integration by parts to determine E(X)E(X).
Express your answer in simplest form.

Reveal Answer

E(X)=0xλeλxdxE(X) = \int_0^\infty x \lambda e^{-\lambda x} dx
udvdxdx=uvvdudxdx\int u \frac{dv}{dx} dx = uv - \int v \frac{du}{dx} dx

u=xdudx=1u = x \quad \frac{du}{dx} = 1
dvdx=λeλxv=eλx\frac{dv}{dx} = \lambda e^{-\lambda x} \quad v = -e^{-\lambda x}

E(X)=xeλx0+0eλxdxE(X) = -xe^{-\lambda x}|_0^\infty + \int_0^\infty e^{-\lambda x} dx
=0+0eλxdx= 0 + \int_0^\infty e^{-\lambda x} dx
=eλxλ0= \frac{e^{-\lambda x}}{-\lambda}|_0^\infty
=01λ= 0 - \frac{1}{-\lambda}
=1λ= \frac{1}{\lambda}

Marking Criteria
DescriptorMarks

correctly determines dudx\frac{du}{dx} and vv

1

substitutes into the integration by parts rule

1

calculates xeλx0-xe^{-\lambda x}|_0^\infty to equal 0

1

shows that E(X)=1λE(X) = \frac{1}{\lambda}

1
Q18
2021
QCAA
Paper 1
6 marks
Q18
6 marks

This differential equation can be used to determine the current II (amperes) at time tt (seconds) with voltage VV (volts) in an electric circuit containing a resistance RR (ohms):

kdIdt+RI=Vk \frac{dI}{dt} + RI = V

where kk, RR and VV are positive constants and t0t \geq 0.

Assuming that there is no current in the electric circuit initially, show that the size of the current can never be greater than VR\frac{V}{R}.

Reveal Answer

kdIdt+RI=VkdIdt=VRIk \frac{dI}{dt} + RI = V \Rightarrow k \frac{dI}{dt} = V - RI
kVRIdI=1dt\int \frac{k}{V - RI} dI = \int 1 dt
kRlnVRI=t+c-\frac{k}{R} \ln|V - RI| = t + c
Given I=0I = 0 when t=0t = 0
c=kRln(V)c = -\frac{k}{R} \ln(V) (as V>0V > 0)
kRlnVRI=tkRln(V)-\frac{k}{R} \ln|V - RI| = t - \frac{k}{R} \ln(V)
lnVRI=Rkt+ln(V)\ln|V - RI| = -\frac{R}{k}t + \ln(V)
VRI=eRkt+ln(V)V - RI = e^{-\frac{R}{k}t + \ln(V)}
VRI=VeRktV - RI = V e^{-\frac{R}{k}t}
For all t,eRkt>0VRI>0V>RII<VRt, e^{-\frac{R}{k}t} > 0 \Rightarrow V - RI > 0 \Rightarrow V > RI \Rightarrow I < \frac{V}{R}
So, the size of the current can never be greater than VR\frac{V}{R}.

Marking Criteria
DescriptorMarks

correctly uses the separation of variables method to set up indefinite integrals

1

develops a general solution of the differential equation

1

uses the given condition to determine expression for the constant of integration

1

rearranges relationship to express lnVRI\ln|V - RI| as the subject of the equation

1

expresses relationship as an exponential function

1

considers value of II over time to determine the required limit

1
Q12
2024
VCAA
Paper 2
1 mark
Q12
1 mark

The position, xx metres, of a particle moving in a straight line from a fixed origin OO at time, tt seconds, is given by x=e(k1)tx = e^{(k - 1)t}, where k>1k > 1.

The acceleration of the particle, in m s2\text{m s}^{-2}, when x=k+1x = k + 1 is

A

k21k^2 - 1

B

(k21)(k+1)(k^2 - 1)(k + 1)

C

(k21)(k1)(k^2 - 1)(k - 1)

D

(k1)2(k - 1)^2

Reveal Answer
A

k21k^2 - 1

Incorrect. This represents the velocity of the particle when x=k+1x = k + 1, found by taking the first derivative v=(k1)xv = (k - 1)x, rather than the acceleration.

B

(k21)(k+1)(k^2 - 1)(k + 1)

Incorrect. This expression does not match the acceleration formula a=(k1)2xa = (k - 1)^2 x. It incorrectly multiplies the velocity by xx instead of taking the second derivative.

C

(k21)(k1)(k^2 - 1)(k - 1)

Correct Answer

Correct. The acceleration is the second derivative of position, a=(k1)2xa = (k - 1)^2 x. Substituting x=k+1x = k + 1 gives $a = (k - 1)^2(k + 1) = (k - 1)(k^2 - 1).

D

(k1)2(k - 1)^2

Incorrect. This is the coefficient of xx in the acceleration equation a=(k1)2xa = (k - 1)^2 x, but it fails to substitute the given value x=k+1x = k + 1.

Q5
2024
VCAA
Paper 1
3 marks
Q5
3 marks

The curve with equation y=k1x2y = \sqrt{k - \frac{1}{x^2}}, for 1xk21 \le x \le \frac{k}{2} where k>2k > 2, is rotated about the xx-axis to form a solid of revolution that has volume 7π2\frac{7\pi}{2} units3^3.

Show that kk satisfies the equation k32k29k+4=0k^3 - 2k^2 - 9k + 4 = 0.

Reveal Answer

The volume VV is given by V=π1k(k1x2)dxV = \pi \int_1^k \left(k - \frac{1}{x^2}\right) dx.

V=π1k(k1x2)dx=π[kx+1x]1k=π(12k2+2kk1)V = \pi \int_1^k \left(k - \frac{1}{x^2}\right) dx= \pi \left[kx + \frac{1}{x}\right]_1^k= \pi \left(\frac{1}{2}k^2 + \frac{2}{k} - k - 1\right)

π(12k2+2kk1)=7π2    k32k29k+4=0\pi \left(\frac{1}{2}k^2 + \frac{2}{k} - k - 1\right) = \frac{7\pi}{2}\implies k^3 - 2k^2 - 9k + 4 = 0

Marking Criteria
DescriptorMarks

Sets up the correct definite integral for the volume

1

Correctly integrates the expression and substitutes the limits

1

Equates the evaluated integral to 7π2\frac{7\pi}{2} and correctly rearranges to show k32k29k+4=0k^3 - 2k^2 - 9k + 4 = 0

1
Q17
2020
QCAA
Paper 2
7 marks
Q17
7 marks

An object is released from rest at a height of 100 m above the ground.
The motion of the vertical descent of the object is modelled by

vdvdx=9.80.004v2(v0)v\frac{dv}{dx} = 9.8 - 0.004v^2 \quad (v \ge 0)

where vv is the velocity (m s1^{-1}) and xx is the displacement from the ground (m).
Determine the velocity of the object when it strikes the ground.

Reveal Answer

vdvdx=9.80.004v2,v>0v\frac{dv}{dx} = 9.8 - 0.004v^2, v > 0
v9.80.004v2dv=dx\int \frac{v}{9.8 - 0.004v^2} dv = \int dx
10.0080.008v9.80.004v2dv=dx\frac{-1}{0.008} \int \frac{-0.008v}{9.8 - 0.004v^2} dv = \int dx
125ln9.80.004v2=x+c-125 \ln|9.8 - 0.004v^2| = x + c

Given v=0v = 0 when x=100x = -100
125ln9.8=100+c-125 \ln|9.8| = -100 + c
c185.298c \approx -185.298

125ln9.80.004v2=x185.298-125 \ln|9.8 - 0.004v^2| = x - 185.298
Determining vv when x=0x = 0
125ln9.80.004v2=185.298-125 \ln|9.8 - 0.004v^2| = -185.298

Using graph facility of GDC
v36.7 ms1v \approx -36.7 \text{ ms}^{-1} or v36.7 ms1v \approx 36.7 \text{ ms}^{-1}
As v>0v > 0, the negative solution is rejected
v36.7 ms1\therefore v \approx 36.7 \text{ ms}^{-1}

Marking Criteria
DescriptorMarks

correctly uses separation of variables

1

correctly develops the general solution of the differential equation

1

correctly uses the given position of the origin

1

uses the given condition to determine value for c

1

substitutes the displacement at impact to form an equation in terms of v

1

determines one reasonable solution of v

1

shows logical organisation communicating key steps

1
Q1
2020
QCAA
Paper 2
1 mark
Q1
1 mark

The position xx (m) at time tt (s) of a 7 kg particle moving in a straight line is given by

x=3t35t2+2t4 for 0t10x = 3t^3 - 5t^2 + 2t - 4 \text{ for } 0 \le t \le 10

Determine the time when the particle has a momentum of 620 kg m s1^{-1}.

A

1.73 s

B

2.60 s

C

3.66 s

D

3.71 s

Reveal Answer
A

1.73 s

This time value is incorrect. It may result from a calculation error or solving an incorrect kinematic equation.

B

2.60 s

This is an incorrect answer. Substituting t=2.60t = 2.60 s into the derived momentum equation yields a value significantly lower than 620 kg m s1^{-1}.

C

3.66 s

This value is close but incorrect. Using t=3.66t = 3.66 s results in a momentum of approximately 602 kg m s1^{-1}, which is less than the required value.

D

3.71 s

Correct Answer

First, find the velocity function by differentiating the position: v(t)=dxdt=9t210t+2v(t) = \frac{dx}{dt} = 9t^2 - 10t + 2. Then, use the momentum formula p=mvp = mv to set up 620=7(9t210t+2)620 = 7(9t^2 - 10t + 2). Solving this quadratic equation for tt yields t3.71t \approx 3.71 s.

Q17
2025
QCAA
Paper 1
7 marks
Q17
7 marks

The radius of a cylinder decreases at a constant rate of 0.5 m s10.5 \text{ m s}^{-1}, while maintaining a constant height of four metres.

Given that the cylinder has an initial volume of 100π m3100\pi \text{ m}^3, determine the rate of change of the volume (m3 s1\text{m}^3 \text{ s}^{-1}) of the cylinder after four seconds.

Reveal Answer

Given V=πr2hV=4πr2V = \pi r^2 h \Rightarrow V = 4\pi r^2

Given drdt=0.5 m s1\frac{dr}{dt} = -0.5 \text{ m s}^{-1}

V=4πr2dVdt=8πrdrdtV = 4\pi r^2 \Rightarrow \frac{dV}{dt} = 8\pi r \frac{dr}{dt}

At t=0t = 0, V=100πV = 100\pi (given)

100π=4πr2r=5 m(as r>0)100\pi = 4\pi r^2 \Rightarrow r = 5 \text{ m} (\text{as } r > 0)

At t=4t = 4,

r=54×0.5=3 mr = 5 - 4 \times 0.5 = 3 \text{ m}

When r=3r = 3:

dVdt=8π×3×(0.5)=12π m3 s1\frac{dV}{dt} = 8\pi \times 3 \times (-0.5) = -12\pi \text{ m}^3 \text{ s}^{-1}
Marking Criteria
DescriptorMarks

correctly determines the rule for the volume of cylinder in terms of rr

1

correctly expresses the rate of change of the radius as a mathematical expression

1

determines a general expression for dVdt\frac{dV}{dt}

1

determines initial value of rr

1

determines value of rr after 4 seconds

1

determines value of dVdt\frac{dV}{dt} when t=4t = 4

1

shows logical organisation, having fully attempted the question

1
Q18
2023
QCAA
Paper 1
6 marks
Q18
6 marks

A particular solution to the differential equation dydx=x(x2+1)tan(y)\frac{dy}{dx} = \frac{x}{(x^2+1)\tan(y)}, where x0x \ge 0 and π2<y0-\frac{\pi}{2} < y \le 0, passes through the origin.

Determine this solution in the form x=f(y)x = f(y). Leave your answer in simplified form.

Reveal Answer

dydx=x(x2+1)tan(y)\frac{dy}{dx} = \frac{x}{(x^2+1)\tan(y)}

tan(y)dy=xx2+1dx\int \tan(y) dy = \int \frac{x}{x^2+1} dx

sin(y)cos(y)dy=122xx2+1dx-\int \frac{-\sin(y)}{\cos(y)} dy = \frac{1}{2} \int \frac{2x}{x^2+1} dx

lncos(y)=12lnx2+1+c-\ln|\cos(y)| = \frac{1}{2}\ln|x^2+1| + c

Given y=0y=0 when x=0x=0,
lncos(0)=12ln1+c    c=0-\ln|\cos(0)| = \frac{1}{2}\ln|1| + c \implies c=0

12lnx2+1=lncos(y)\therefore \frac{1}{2}\ln|x^2+1| = -\ln|\cos(y)|

lnx2+1=ln1cos(y)\ln\sqrt{x^2+1} = \ln\left|\frac{1}{\cos(y)}\right|

x2+1=sec(y)\sqrt{x^2+1} = |\sec(y)|
x2+1=sec2(y)x^2+1 = \sec^2(y)
x2=tan2(y)x^2 = \tan^2(y)
x=±tan(y)x = \pm \tan(y)

As x0,π2<y0x \ge 0, -\frac{\pi}{2} < y \le 0
x=tan(y)x = -\tan(y)

Marking Criteria
DescriptorMarks

Correctly separates the variables

1

Applies suitable integration methods

1

Determines a value for the constant of integration

1

Determines an expression for a solution that does not contain logarithms

1

Expresses xx in terms of yy

1

Evaluates the reasonableness of the results and expresses the solution in the form of x=f(y)x = f(y) in simplified form

1
Q17
2024
QCAA
Paper 1
6 marks
Q17
6 marks

The acceleration (m s2\text{m s}^{-2}) of an object that moves in a straight line in an easterly direction over time tt for 0tπ60 \le t \le \frac{\pi}{6} seconds is given by a=2(1+v2)a = 2(1+v^2), where vv is its velocity (m s1\text{m s}^{-1}).

The object is initially at rest at a position that is ln(2)\ln(\sqrt{2}) metres west of the origin.

A student uses this information to calculate that the object is positioned at the origin when t=π6t = \frac{\pi}{6} seconds.

Evaluate the reasonableness of the student's calculation.

Reveal Answer

Method 1

a=2(1+v2)a = 2(1+v^2)
dvdt=2(1+v2)\frac{dv}{dt} = 2(1+v^2)

11+v2dv=2dt\int \frac{1}{1+v^2} dv = \int 2 dt
tan1(v)=2t+c\tan^{-1}(v) = 2t + c

At t=0,v=0:tan1(0)=0+ct=0, v=0: \tan^{-1}(0) = 0 + c
c=0\therefore c = 0

tan1(v)=2t\therefore \tan^{-1}(v) = 2t
v=tan(2t)v = \tan(2t)
x=vdtx = \int v dt
=tan(2t)dt= \int \tan(2t) dt
=12ln(cos(2t))+c= -\frac{1}{2} \ln(\cos(2t)) + c
=12ln(cos(2t))+c= -\frac{1}{2} \ln(\cos(2t)) + c

Given x=ln(2)x = -\ln(\sqrt{2}) when t=0t=0
ln(2)=12ln(cos(0))+c-\ln(\sqrt{2}) = -\frac{1}{2} \ln(\cos(0)) + c
c=ln(2)c = -\ln(\sqrt{2})

x=12ln(cos(2t))ln(2)x = -\frac{1}{2} \ln(\cos(2t)) - \ln(\sqrt{2})

When t=π6t = \frac{\pi}{6}
x=12ln(cos(π3))ln(2)x = -\frac{1}{2} \ln(\cos(\frac{\pi}{3})) - \ln(\sqrt{2})
=12ln(12)ln(2)= -\frac{1}{2} \ln(\frac{1}{2}) - \ln(\sqrt{2})

x=ln((12)12)ln(2)x = \ln((\frac{1}{2})^{-\frac{1}{2}}) - \ln(\sqrt{2})
=ln(2)ln(2)= \ln(\sqrt{2}) - \ln(\sqrt{2})
=0= 0
So the calculation is reasonable.

Marking Criteria
DescriptorMarks

correctly determines a general solution to the differential equation in terms of v and time

1

determines an appropriate constant of integration

1

determines a general solution for displacement in terms of time

1

determines an appropriate constant of integration

1

determines a result for displacement when t=π6t = \frac{\pi}{6} without a trigonometric term

1

provides an appropriate statement of reasonableness based on mathematical reasoning

1

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