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VICSpecialist Mathematics2022Exam 2

VCE Specialist Mathematics 2022 Exam 2

Worked solutions to the 2022 VCE Specialist Mathematics Examination 2 (80 marks, CAS allowed): the 18 published multiple-choice answers with reasons and every published Section B part, checked against the VCAA external assessment report, with study design changes flagged.

Marks
80
Time
120 min
Authority
VCAA
Updated

Every published question from the 2022 VCE Specialist Mathematics Examination 2, the technology-active (CAS) paper. Multiple-choice answers come with a one-line reason; Section B solutions sit behind a Show worked solution toggle. For the no-calculator paper, see the 2022 Examination 1 walkthrough.

How to use this page

  • Questions are from the 2022 VCE Specialist Mathematics Examination 2, copyright Victorian Curriculum and Assessment Authority (VCAA). Each question is summarised briefly here; open the official examination PDF for the full wording, diagrams and answer options.
  • Answers are original ExamExplained working. Every multiple-choice answer matches the key in the 2022 Specialist Mathematics Examination 2 external assessment report (Word document), and every Section B result was recomputed and compared with the report. Both files are listed on the VCAA Specialist Mathematics examinations page.
  • Redacted questions. VCAA has redacted multiple-choice Questions 4 and 19 and Section B Question 6f from the published paper and report, following the Independent Review into its examination-setting policies, processes and procedures. They are not covered here.
  • Study design. This was the last Examination 2 set on the previous Specialist Mathematics study design (2016 to 2022); the current one began in 2023. Most of the paper is still on the course. The exceptions, flagged where they appear, are the mechanics questions. Momentum is not in the current study design, so multiple-choice Question 17 and Question 5b are outside it. Forces and Newton's second law are covered only in Specialist Mathematics Unit 2 (vectors applied to statics and motion under a constant force), which Units 3 and 4 assume but do not list as a topic, so multiple-choice Questions 15, 16 and 20 and Questions 5a and 5e are partly outside it; the formula sheet also no longer lists the Mechanics formulas (momentum and the equation of motion) that it gave in 2022. Anything not flagged is still examinable.

Structure and timing

Examination 2 is 80 marks in 120 minutes (plus 15 minutes reading time), with a CAS calculator and one bound reference allowed. In 2022 the multiple-choice questions had five options (A to E). Take g=9.8 m s−2g = 9.8 \text{ m s}^{-2}.

  • Section A (20 marks): 20 multiple-choice questions. Aim for about 25 minutes.
  • Section B (60 marks): 6 extended-response questions (11, 9, 10, 11, 10 and 9 marks).

According to the report, students did well at finding asymptotes and sketching rational functions, working with velocity and speed from vector functions of time, resolving forces and solving equations of motion, related rates, hypothesis testing and using CAS. Weaker areas were answering every part of a multi-part question (the ray in 2c, the point in 3b.ii and the time in 4b.ii were often left out), how a function involving inverse tangent behaves in the limit, and random variables that are functions of other random variables.

Section A: Multiple choice

Q1
For 12≤x≤3\tfrac12 \le x \le 3, which line matches y=∣2x−1∣−∣x−3∣y = |2x - 1| - |x - 3|? Answer: B - on this interval 2x−1≥02x - 1 \ge 0 and x−3≤0x - 3 \le 0, so y=(2x−1)−(3−x)=3x−4y = (2x - 1) - (3 - x) = 3x - 4.
Q2
Simplify 1−4sin⁡2(x)tan⁡2(x)+11 - \dfrac{4\sin^2(x)}{\tan^2(x) + 1}. Answer: E - tan⁡2x+1=sec⁡2x\tan^2x + 1 = \sec^2x, so the expression is 1−4sin⁡2xcos⁡2x=1−sin⁡2(2x)=cos⁡2(2x)1 - 4\sin^2x\cos^2x = 1 - \sin^2(2x) = \cos^2(2x).
Q3
What must the graph of y=x2+2x+cx2−4y = \dfrac{x^2 + 2x + c}{x^2 - 4} always have? Answer: E - the degrees match, so y=1y = 1 is always a horizontal asymptote, but a factor can cancel: with c=0c = 0 the function reduces to 1+2x−21 + \tfrac{2}{x - 2}, leaving only x=2x = 2. So there is at least one vertical asymptote. (38% correct; 41% chose A, which fails when a factor cancels.)
Q4
Redacted by VCAA from the published paper and report; not covered here.
Q5
If Arg(z−i)=3π4\text{Arg}(z - i) = \tfrac{3\pi}{4}, which is true? Answer: A - this is a ray from (0,1)(0, 1) heading up and to the left at gradient −1-1, with the endpoint excluded: y=1−xy = 1 - x, x<0x < 0.
Q6
Which graph meets the circle ∣z−5∣=2|z - 5| = 2 in two points? Answer: E - ∣z−5−5i∣=4|z - 5 - 5i| = 4 is a circle centred at (5,5)(5, 5) of radius 4; the centres are 5 apart and 4−2<5<4+24 - 2 < 5 < 4 + 2, so the circles cross twice. Options B and C touch the circle once, D misses it, and the ray in A only reaches its excluded endpoint (3,0)(3, 0).
Q7
Rewrite ∫0log⁡e211+ex dx\displaystyle\int_0^{\log_e 2}\frac{1}{1 + e^x}\,dx using u=1+exu = 1 + e^x. Answer: D - du=(u−1) dxdu = (u - 1)\,dx and the terminals become u=2u = 2 and u=3u = 3, giving ∫23duu(u−1)=∫23(1u−1−1u)du\displaystyle\int_2^3\frac{du}{u(u - 1)} = \int_2^3\left(\frac{1}{u - 1} - \frac{1}{u}\right)du.
Q8
Which differential equation matches the direction field? Answer: C - the slopes are negative in the first and third quadrants and positive in the second and fourth, and they are steep near the xx-axis: dydx=−2xy\dfrac{dy}{dx} = -\dfrac{2x}{y} gives slope −2-2 at (1,1)(1, 1), while option B would give only −12-\tfrac12.
Q9
Euler's method on dydx=2x2\dfrac{dy}{dx} = 2x^2 with x0=1x_0 = 1, y0=2y_0 = 2 gives y2=2.976y_2 = 2.976. Find hh. Answer: B - y1=2+2hy_1 = 2 + 2h and y2=y1+2h(1+h)2y_2 = y_1 + 2h(1 + h)^2; with h=0.2h = 0.2 this is 2.4+0.576=2.9762.4 + 0.576 = 2.976.
Q10
When is the tangent to 5x2y−3xy+y2=105x^2y - 3xy + y^2 = 10 at (1,m)(1, m) negatively sloped? Answer: E - at x=1x = 1 the curve gives m2+2m=10m^2 + 2m = 10, so m=−1±11m = -1 \pm \sqrt{11}. Implicit differentiation gives dydx=−7m2m+2\tfrac{dy}{dx} = \tfrac{-7m}{2m + 2} at x=1x = 1, which is about −2.44-2.44 and −4.56-4.56 for the two values: both negative. (21% correct; 38% chose A.)
Q11
a=2i−3j+pk\mathbf a = 2\mathbf i - 3\mathbf j + p\mathbf k, b=i+2j−qk\mathbf b = \mathbf i + 2\mathbf j - q\mathbf k and c=−3i+2j+5k\mathbf c = -3\mathbf i + 2\mathbf j + 5\mathbf k are linearly dependent. Then? Answer: A - the determinant of the three vectors is 8p−5q+358p - 5q + 35, which must be zero, so 8p=5q−358p = 5q - 35.
Q12
When is u(x)=−cosec(x)i+3j\mathbf u(x) = -\text{cosec}(x)\mathbf i + \sqrt3\mathbf j perpendicular to v(x)=cos⁡(x)i+j\mathbf v(x) = \cos(x)\mathbf i + \mathbf j? Answer: A - u⋅v=−cot⁡x+3=0\mathbf u\cdot\mathbf v = -\cot x + \sqrt3 = 0 gives tan⁡x=13\tan x = \tfrac{1}{\sqrt3}, so x=π6x = \tfrac{\pi}{6} or 7π6\tfrac{7\pi}{6}.
Q13
r¨(t)=sin⁡(t)i+2cos⁡(t)j\ddot{\mathbf r}(t) = \sin(t)\mathbf i + 2\cos(t)\mathbf j and r˙(0)=2i+j\dot{\mathbf r}(0) = 2\mathbf i + \mathbf j. Find r˙(t)\dot{\mathbf r}(t). Answer: B - antidifferentiating gives (−cos⁡t+c1)i+(2sin⁡t+c2)j(-\cos t + c_1)\mathbf i + (2\sin t + c_2)\mathbf j; the initial velocity forces c1=3c_1 = 3 and c2=1c_2 = 1.
Q14
Constant acceleration, 7 m/s at AA and 17 m/s at BB. Velocity at the midpoint of ABAB? Answer: D - 172=72+2as17^2 = 7^2 + 2as gives as=120as = 120, and at the midpoint v2=72+2a⋅s2=49+120=169v^2 = 7^2 + 2a\cdot\tfrac{s}{2} = 49 + 120 = 169, so v=13v = 13. (28% correct; 49% chose C, the average of the two velocities, which applies at the time midpoint, not the distance midpoint.)
Q15
A mass on a smooth incline is acted on by N\mathbf N, T\mathbf T (at angle α\alpha to the slope) and W\mathbf W, and accelerates at a\mathbf a. What is necessarily true? Answer: E - Newton's second law in vector form, N+W+T=ma\mathbf N + \mathbf W + \mathbf T = m\mathbf a, holds whatever the direction of motion. Option C assumes the object accelerates down the slope, but it could be accelerating up it. (26% correct; 49% chose C.)

Study design: partly outside the current course. Resolving forces and Newton's second law on an inclined plane are covered only in Specialist Mathematics Unit 2 (vectors applied to statics and motion under a constant force), which Units 3 and 4 assume.

Q16. Forces of 5 N, 7 N and 10 N keep a particle in equilibrium. Which equation gives the angle θ\theta between the 5 N and 7 N forces? Answer: A - the 5 N and 7 N forces must add to a resultant of magnitude 10, so ∣F5+F7∣2=25+49+2×5×7cos⁡θ=100|\mathbf F_5 + \mathbf F_7|^2 = 25 + 49 + 2 \times 5 \times 7\cos\theta = 100. In the triangle of forces the interior angle is π−θ\pi - \theta, which is why the cosine rule there carries a minus sign. (17% correct; 63% chose B.)

Study design: partly outside the current course. Equilibrium of coplanar forces is covered only in Specialist Mathematics Unit 2 (vectors applied to statics and motion under a constant force), which Units 3 and 4 assume.

Q17. A 7 kg particle with constant acceleration starts at 3 m/s and covers 30 m in 6 s. Change in momentum? Answer: C - 30=3(6)+12a(36)30 = 3(6) + \tfrac12a(36) gives a=23a = \tfrac23, so the final velocity is 3+4=73 + 4 = 7 m/s and the change in momentum is 7(7−3)=287(7 - 3) = 28 kg m/s.

Study design: outside the current course, which does not include momentum.

Q18
Travel times are N(30,2.52)N(30, 2.5^2) and independent. Probability that two consecutive times differ by more than 6 minutes? Answer: B - the difference D=T1−T2D = T_1 - T_2 has mean 0 and variance 2×2.52=12.52 \times 2.5^2 = 12.5, so 1−Pr⁡(−6<D<6)≈0.08971 - \Pr(-6 < D < 6) \approx 0.0897. (42% correct.)
Q19
Redacted by VCAA from the published paper and report; not covered here.
Q20
A 4 kg mass hangs on one side of a pulley and two 2 kg masses on the other; the actual masses are normal with means 1.980 and 3.940 and standard deviations 0.015 and 0.002. Probability the 4 kg mass moves up? Answer: C - it rises when the two 2 kg masses together outweigh it. X=M1+M2−M4X = M_1 + M_2 - M_4 has mean 0.020.02 and standard deviation 2(0.015)2+0.0022≈0.0213\sqrt{2(0.015)^2 + 0.002^2} \approx 0.0213, so Pr⁡(X>0)≈0.826\Pr(X > 0) \approx 0.826. (41% correct; 24% chose B.)

Study design: partly outside the current course. The probability step (a linear combination of independent normal variables) is on the course, but deciding the direction of motion of a connected-particle pulley system relies on forces and Newton's second law, covered only in Specialist Mathematics Unit 2 (vectors applied to statics and motion under a constant force), which Units 3 and 4 assume.

Section B: Extended response

Question 1 (11 marks)

The family f(x)=x2x−kf(x) = \dfrac{x^2}{x - k}, k∈R∖{0}k \in R \setminus \{0\}.

a
State the equations of the two asymptotes when k=1k = 1. (2 marks)
b
Sketch y=f(x)y = f(x) for k=1k = 1 on the grid (about −4.5≤x≤4.5-4.5 \le x \le 4.5, −8≤y≤8-8 \le y \le 8), labelling turning points with coordinates and asymptotes with equations. (3 marks)
c. i
Find the asymptotes in terms of kk. (1 mark)
ii
Find, in terms of kk, the distance between the two turning points. (2 marks)

Now let h(x)=x+3h(x) = x + 3 and g(x)=∣x2x−1∣g(x) = \left|\dfrac{x^2}{x - 1}\right|. The region bounded by their graphs is rotated about the xx-axis.

d. i. Write a definite integral for the volume of the solid. (2 marks)

ii. Find the volume, correct to two decimal places. (1 mark)

Show worked solution

a. [2 marks]. Dividing, x2x−1=x+1+1x−1\dfrac{x^2}{x - 1} = x + 1 + \dfrac{1}{x - 1}. The asymptotes are

x=1andy=x+1.x = 1 \quad\text{and}\quad y = x + 1.

b. [3 marks]. f′(x)=x(x−2)(x−1)2=0f'(x) = \dfrac{x(x - 2)}{(x - 1)^2} = 0 at x=0x = 0 and x=2x = 2, giving a local maximum at (0,0)(0, 0) and a local minimum at (2,4)(2, 4). The left branch lies below y=x+1y = x + 1 and drops to −∞-\infty as x→1−x \to 1^-; the right branch lies above y=x+1y = x + 1 and rises to ∞\infty as x→1+x \to 1^+.

Graph of y = x squared over (x - 1) Two branches separated by the vertical asymptote x = 1. The left branch comes up from below close to the oblique asymptote y = x + 1, reaches a local maximum at the origin, then falls steeply towards negative infinity as x approaches 1 from the left. The right branch comes down from positive infinity just right of x = 1 to a local minimum at (2, 4) and then rises, approaching y = x + 1 from above. x y -4 -2 2 4 -5 5 (0, 0) (2, 4) x = 1 y = x + 1

c. i. [1 mark]. x2x−k=x+k+k2x−k\dfrac{x^2}{x - k} = x + k + \dfrac{k^2}{x - k}, so the asymptotes are x=kx = k and y=x+ky = x + k.

ii. [2 marks]. f′(x)=x(x−2k)(x−k)2=0f'(x) = \dfrac{x(x - 2k)}{(x - k)^2} = 0 at x=0x = 0 and x=2kx = 2k, so the turning points are (0,0)(0, 0) and (2k,4k)(2k, 4k). The distance between them is

(2k)2+(4k)2=20k2=25 ∣k∣.\sqrt{(2k)^2 + (4k)^2} = \sqrt{20k^2} = 2\sqrt{5}\,|k|.

d. i. [2 marks]. For x<1x < 1, g(x)=x21−xg(x) = \dfrac{x^2}{1 - x}. Setting x+3=x21−xx + 3 = \dfrac{x^2}{1 - x} gives 2x2+2x−3=02x^2 + 2x - 3 = 0, so x=−1±72x = \dfrac{-1 \pm \sqrt{7}}{2}. (For x>1x > 1 the graphs meet only at x=32x = \tfrac32, and beyond that gg stays below hh, so that region is unbounded.) Between the two roots h(x)≥g(x)≥0h(x) \ge g(x) \ge 0, so the solid is a washer with outer radius hh and inner radius gg:

V=π∫−1−72−1+72((h(x))2−(g(x))2)dx=π∫−1−72−1+72((x+3)2−x4(x−1)2)dx.V = \pi\int_{\frac{-1 - \sqrt{7}}{2}}^{\frac{-1 + \sqrt{7}}{2}}\left(\big(h(x)\big)^2 - \big(g(x)\big)^2\right)dx = \pi\int_{\frac{-1 - \sqrt{7}}{2}}^{\frac{-1 + \sqrt{7}}{2}}\left((x + 3)^2 - \frac{x^4}{(x - 1)^2}\right)dx.

ii. [1 mark]. By CAS, V≈51.42V \approx 51.42 cubic units.

From the report. Parts a and c.i were done well (average 1.8 out of 2 for a; 76% correct for c.i). In the sketch, weaker answers did not show the curve approaching its asymptotes, or drew the oblique asymptote carelessly out of position; matching the calculator window to the grid helps. In c.ii many gave the distance without making it positive, which needs ∣k∣|k|. In d.i a frequent error was squaring the difference, (h(x)−g(x))2\big(h(x) - g(x)\big)^2, instead of taking the difference of the squares. Only 37% got d.ii, and some who had written π\pi in the integral left it out when evaluating.

Question 2 (9 marks)

Let u=a+iu = a + i and v=b−2 iv = b - \sqrt{2}\,i, where a,b∈Ra, b \in R.

a. i
Given uv=(2+6)+(2−6)iuv = \left(\sqrt{2} + \sqrt{6}\right) + \left(\sqrt{2} - \sqrt{6}\right)i, show that a2+(1−3)a−3=0a^2 + \left(1 - \sqrt{3}\right)a - \sqrt{3} = 0. (2 marks)
ii
One solution is a=3a = \sqrt{3}, b=2b = \sqrt{2}. Find the other pair of values. (1 mark)
b
Plot and label u=3+iu = \sqrt{3} + i and v=2−2 iv = \sqrt{2} - \sqrt{2}\,i on the polar-grid Argand diagram. (2 marks)
c
The ray Arg(z)=θ\text{Arg}(z) = \theta passes through the midpoint of the interval joining uu and vv. Find θ\theta in radians and draw the ray on the diagram. (2 marks)
d
The interval joining uu and vv divides the circle ∣z∣=2|z| = 2 into a major and a minor segment. Find the area of the minor segment, correct to two decimal places. (2 marks)
Show worked solution

a. i. [2 marks]. Expanding,

(a+i)(b−2 i)=(ab+2)+(b−2 a)i.(a + i)\left(b - \sqrt{2}\,i\right) = \left(ab + \sqrt{2}\right) + \left(b - \sqrt{2}\,a\right)i.

Equating real and imaginary parts with the given product: ab=6ab = \sqrt{6} and b−2 a=2−6b - \sqrt{2}\,a = \sqrt{2} - \sqrt{6}. Multiply the second equation by aa and substitute ab=6ab = \sqrt{6}:

6−2 a2=(2−6)a.\sqrt{6} - \sqrt{2}\,a^2 = \left(\sqrt{2} - \sqrt{6}\right)a.

Dividing by −2-\sqrt{2} gives a2−3=−(1−3)aa^2 - \sqrt{3} = -\left(1 - \sqrt{3}\right)a, that is

a2+(1−3)a−3=0.a^2 + \left(1 - \sqrt{3}\right)a - \sqrt{3} = 0.

ii. [1 mark]
The quadratic factorises as (a+1)(a−3)=0(a + 1)\left(a - \sqrt{3}\right) = 0, so the other root is a=−1a = -1, and then b=6a=−6b = \dfrac{\sqrt{6}}{a} = -\sqrt{6}.
b. [2 marks]
In polar form u=2 cis(π6)u = 2\,\text{cis}\left(\tfrac{\pi}{6}\right) and v=2 cis(−π4)v = 2\,\text{cis}\left(-\tfrac{\pi}{4}\right), so both points lie on the circle of radius 2, on the spokes at π6\tfrac{\pi}{6} and −π4-\tfrac{\pi}{4}.
c. [2 marks]
Since ∣u∣=∣v∣=2|u| = |v| = 2, the triangle OuvOuv is isosceles and the midpoint of uvuv lies on the bisector of the angle at OO:

θ=12(π6−π4)=−π24.\theta = \frac{1}{2}\left(\frac{\pi}{6} - \frac{\pi}{4}\right) = -\frac{\pi}{24}.

The ray starts at (but excludes) the origin and passes through the midpoint (orange below).

Points u and v on the circle |z| = 2 and the ray through their midpoint An Argand diagram with the circle of radius 2 about the origin. The point u = root 3 + i lies on the circle at argument pi/6 and v = root 2 - root 2 i lies on the circle at argument -pi/4. The chord joining them is drawn, and a ray from the origin at argument -pi/24 passes through the midpoint of the chord. Re(z) Im(z) 2 2 u v Arg(z) = -π/24

d. [2 marks]. Both uu and vv lie on ∣z∣=2|z| = 2, and the angle they subtend at OO is π6+π4=5π12\tfrac{\pi}{6} + \tfrac{\pi}{4} = \tfrac{5\pi}{12}. The minor segment has area

A=12×22×(5π12−sin⁡5π12)≈0.69 square units.A = \frac{1}{2} \times 2^2 \times \left(\frac{5\pi}{12} - \sin\frac{5\pi}{12}\right) \approx 0.69 \text{ square units}.

From the report. In a.i many solved the given quadratic on CAS and substituted back, which does not show the result; the steps had to be set out. In a.ii some gave the negatives of the given values. In b the polar grid lets the points be placed exactly, and plotting from rough Cartesian values was less accurate. Part c averaged 0.8 out of 2: −π12-\tfrac{\pi}{12} was a common wrong angle, and many did not draw the ray, some of them after finding a correct angle. In d about half scored zero; most successful answers used the segment area formula, while attempts by integration usually went wrong.

Question 3 (10 marks)

A particle moves in a straight line with dxdt=2e−x1+4t2\dfrac{dx}{dt} = \dfrac{2e^{-x}}{1 + 4t^2}, where xx metres is its distance from OO at time tt seconds and x=0x = 0 when t=0t = 0.

a. i
Write the differential equation in the form ∫g(x) dx=∫f(t) dt\displaystyle\int g(x)\,dx = \int f(t)\,dt. (1 mark)
ii
Hence show that x=log⁡e(tan⁡−1(2t)+1)x = \log_e\left(\tan^{-1}(2t) + 1\right). (2 marks)
b. i
State the equation of the horizontal asymptote of this graph. (1 mark)
ii
Sketch the graph and the asymptote for 0≤t≤100 \le t \le 10, and plot and label the point where t=10t = 10, with xx correct to two decimal places. (2 marks)
c
Find the speed when t=3t = 3, in m/s correct to two decimal places. (1 mark)

A second particle passes through OO two seconds after the first, and its distance is x=log⁡e(tan⁡−1(3t−6)+1)x = \log_e\left(\tan^{-1}(3t - 6) + 1\right), with tt measured from when the first particle passed OO.

d. Verify that the particles are the same distance from OO when t=6t = 6. (1 mark)

e. Find the ratio of the first particle's speed to the second's at that moment, as ab\dfrac{a}{b} in simplest form, where aa and bb are positive integers. (2 marks)

Show worked solution

a. i. [1 mark]. Multiply both sides by exe^{x} and separate:

∫ex dx=∫21+4t2 dt.\int e^{x}\,dx = \int \frac{2}{1 + 4t^2}\,dt.

ii. [2 marks]. Since 21+(2t)2\dfrac{2}{1 + (2t)^2} is the derivative of tan⁡−1(2t)\tan^{-1}(2t),

ex=tan⁡−1(2t)+c.e^{x} = \tan^{-1}(2t) + c.

At t=0t = 0, x=0x = 0: 1=0+c1 = 0 + c, so c=1c = 1. Then ex=tan⁡−1(2t)+1e^{x} = \tan^{-1}(2t) + 1 and x=log⁡e(tan⁡−1(2t)+1)x = \log_e\left(\tan^{-1}(2t) + 1\right).

b. i. [1 mark]. As t→∞t \to \infty, tan⁡−1(2t)→π2\tan^{-1}(2t) \to \tfrac{\pi}{2}, so the asymptote is

x=log⁡e(π2+1)  (≈0.94).x = \log_e\left(\frac{\pi}{2} + 1\right) \;(\approx 0.94).

ii. [2 marks]. The graph starts at the origin, rises steeply, then flattens and stays just below the asymptote. At t=10t = 10, x=log⁡e(tan⁡−1(20)+1)≈0.92x = \log_e\left(\tan^{-1}(20) + 1\right) \approx 0.92, so the labelled point is (10,0.92)(10, 0.92).

Graph of x = log_e(arctan(2t) + 1) for t from 0 to 10 The curve starts at the origin, rises steeply, bends over by about t = 2 and then increases slowly, staying below the dashed horizontal asymptote x = log_e(pi/2 + 1), about 0.94. The point (10, 0.92) is marked on the curve. t x O 2 4 6 8 10 0.2 0.4 0.6 0.8 1.0 (10, 0.92) x = loge(π/2 + 1)

c. [1 mark]. dxdt=2e−x1+4t2=2(tan⁡−1(2t)+1)(1+4t2)\dfrac{dx}{dt} = \dfrac{2e^{-x}}{1 + 4t^2} = \dfrac{2}{\left(\tan^{-1}(2t) + 1\right)(1 + 4t^2)}. At t=3t = 3:

dxdt=237(tan⁡−1(6)+1)≈0.02 m/s.\frac{dx}{dt} = \frac{2}{37\left(\tan^{-1}(6) + 1\right)} \approx 0.02 \text{ m/s}.

d. [1 mark]. At t=6t = 6, 2t=122t = 12 and 3t−6=123t - 6 = 12, so both distances equal log⁡e(tan⁡−1(12)+1)\log_e\left(\tan^{-1}(12) + 1\right) (≈0.91\approx 0.91 m). (Equivalently, setting the two expressions equal gives 2t=3t−62t = 3t - 6, so t=6t = 6.)

e. [2 marks]. Differentiating each position at t=6t = 6 (where both inner arguments equal 12, so 1+122=1451 + 12^2 = 145):

v1=2(tan⁡−1(12)+1)(1+144)=2145(tan⁡−1(12)+1),v2=3(tan⁡−1(12)+1)(1+(3×6−6)2)=3145(tan⁡−1(12)+1).v_1 = \frac{2}{\left(\tan^{-1}(12) + 1\right)(1 + 144)} = \frac{2}{145\left(\tan^{-1}(12) + 1\right)}, \qquad v_2 = \frac{3}{\left(\tan^{-1}(12) + 1\right)\left(1 + (3 \times 6 - 6)^2\right)} = \frac{3}{145\left(\tan^{-1}(12) + 1\right)}.

Both speeds are positive, and the ratio of the first to the second is

v1v2=23.\frac{v_1}{v_2} = \frac{2}{3}.

From the report. Parts a.i (85% correct) and a.ii were answered well, although fraction errors in the integration cost some marks. Only 23% got b.i: x=1x = 1 was a common wrong answer, as was writing the asymptote as y=…y = \dots when the vertical axis is xx. In b.ii many sketches were not drawn precisely enough. In d, many simply substituted t=6t = 6 into both expressions, which was accepted. In e, correct answers came in several equivalent forms, depending on the CAS used.

Question 4 (11 marks)

A minigolf ball is blown off course by a strong wind. It passes through the origin OO at t=0t = 0 and the hole is at (0,7)(0, 7), 7 m from OO in the forward (j\mathbf j) direction. Its path is r(t)=12sin⁡(πt4)i+2t j\mathbf r(t) = \dfrac{1}{2}\sin\left(\dfrac{\pi t}{4}\right)\mathbf i + 2t\,\mathbf j for t∈[0,5]t \in [0, 5], in metres, where i\mathbf i points to the right. At OO the path makes an angle of θ\theta degrees with the forward direction.

a
Find θ\theta, correct to one decimal place. (2 marks)
b. i
Find the speed of the ball as it passes through OO, in m/s correct to two decimal places. (2 marks)
ii
Find the minimum speed of the ball and the time at which it occurs. (2 marks)
c
Find the minimum distance from the ball to the hole, in metres correct to three decimal places. (3 marks)
d
How far does the ball travel in the first four seconds after passing through OO? Answer in metres correct to three decimal places. (2 marks)
Show worked solution

a. [2 marks]. Differentiate:

r˙(t)=π8cos⁡(πt4)i+2 j,r˙(0)=π8i+2 j.\dot{\mathbf r}(t) = \frac{\pi}{8}\cos\left(\frac{\pi t}{4}\right)\mathbf i + 2\,\mathbf j, \qquad \dot{\mathbf r}(0) = \frac{\pi}{8}\mathbf i + 2\,\mathbf j.

The angle between this velocity and the forward direction j\mathbf j satisfies tan⁡θ=π/82=π16\tan\theta = \dfrac{\pi/8}{2} = \dfrac{\pi}{16}, so θ≈11.1\theta \approx 11.1.

b. i. [2 marks].

∣r˙(0)∣=π264+4≈2.04 m/s.|\dot{\mathbf r}(0)| = \sqrt{\frac{\pi^2}{64} + 4} \approx 2.04 \text{ m/s}.

ii. [2 marks]. Speed =π264cos⁡2(πt4)+4= \sqrt{\dfrac{\pi^2}{64}\cos^2\left(\dfrac{\pi t}{4}\right) + 4}. This is least when cos⁡(πt4)=0\cos\left(\dfrac{\pi t}{4}\right) = 0, which in [0,5][0, 5] happens only at t=2t = 2. The minimum speed is 4=2\sqrt{4} = 2 m/s, at t=2t = 2 seconds.

c. [3 marks]. The vector from the hole to the ball is r(t)−7j\mathbf r(t) - 7\mathbf j, so the distance is

d(t)=14sin⁡2(πt4)+(2t−7)2.d(t) = \sqrt{\frac{1}{4}\sin^2\left(\frac{\pi t}{4}\right) + (2t - 7)^2}.

Minimising with CAS on [0,5][0, 5] gives a minimum at t≈3.517t \approx 3.517, and the minimum distance is d≈0.188d \approx 0.188 m.

d. [2 marks]. The distance travelled is the arc length, the integral of the speed:

∫04π264cos⁡2(πt4)+4  dt≈8.077 m.\int_0^4 \sqrt{\frac{\pi^2}{64}\cos^2\left(\frac{\pi t}{4}\right) + 4}\;dt \approx 8.077 \text{ m}.

From the report. Part a averaged 0.9 out of 2: the most common error was giving the complementary angle, 78.9∘78.9^\circ, measured from the i\mathbf i direction instead of the forward direction. Using dydx\tfrac{dy}{dx} from the parametric equations, or a scalar product with j\mathbf j, also worked. Part b.i was well answered (73% full marks). In b.ii some students with the right minimum speed also gave wrong values of tt. Part c was answered fully by 38%; approaches using perpendicularity succeeded less often. In part d a number of students found the straight-line distance between the start and end points instead of the arc length, and those who used the Cartesian equation often kept the tt values as terminals.

Question 5 (10 marks)

An object of mass 5 kg moves to the right along a horizontal surface. Forces of 20320\sqrt{3} N (at 30∘30^\circ above the horizontal) and 10210\sqrt{2} N (at a further 15∘15^\circ above that force, so 45∘45^\circ to the horizontal) act on it, with a horizontal resistance of 5k5k N, k∈Rk \in R. At point OO its speed is 0.5 m s−1^{-1}.

a. Show that the acceleration of the object is (8−k)(8 - k) m s−2^{-2}. (2 marks)

After 5 seconds the object reaches point PP with speed 2 m s−1^{-1}.

b
Find the change in momentum, in kg m s−1^{-1}, from t=0t = 0 to t=5t = 5. (1 mark)
c
Show that k=7.7k = 7.7. (2 marks)
d
Find the distance, in metres, from OO to PP. (2 marks)
e
At PP the two slanting forces stop acting and the object moves up a plane PQPQ, inclined at θ∘\theta^\circ to the horizontal, at a reduced speed of 1.95 m s−1^{-1}. A resistance of 38.5 N acts parallel to the plane, and the object comes to rest 0.2 m up the plane from PP. Find θ\theta, correct to one decimal place. (3 marks)

Study design: part b is outside the current course, which does not include momentum. Parts a and e, which resolve forces and apply Newton's second law (on a horizontal surface and on an inclined plane with resistance), are partly outside: the current study design covers forces only in Specialist Mathematics Unit 2 (vectors applied to statics and motion under a constant force), which Units 3 and 4 assume but do not list as a topic. Parts c and d use only the constant acceleration formulas with the acceleration from part a, which is on the current course.

Show worked solution

a. [2 marks]. Resolve horizontally (to the right positive). The 10210\sqrt{2} N force is at 30∘+15∘=45∘30^\circ + 15^\circ = 45^\circ to the horizontal. By Newton's second law:

102cos⁡45∘+203cos⁡30∘−5k=5a10\sqrt{2}\cos 45^\circ + 20\sqrt{3}\cos 30^\circ - 5k = 5a

102×12+203×32−5k=5a  ⇒  10+30−5k=5a  ⇒  a=8−k.10\sqrt{2} \times \frac{1}{\sqrt{2}} + 20\sqrt{3} \times \frac{\sqrt{3}}{2} - 5k = 5a \;\Rightarrow\; 10 + 30 - 5k = 5a \;\Rightarrow\; a = 8 - k.

b. [1 mark]. Δp=m(v−u)=5(2−0.5)=7.5\Delta p = m(v - u) = 5(2 - 0.5) = 7.5 kg m s−1^{-1}.

c. [2 marks]. The acceleration is constant, so with v=u+atv = u + at:

2=0.5+(8−k)×5  ⇒  8−k=0.3  ⇒  k=7.7.2 = 0.5 + (8 - k) \times 5 \;\Rightarrow\; 8 - k = 0.3 \;\Rightarrow\; k = 7.7.

d. [2 marks]. With a=0.3a = 0.3 m s−2^{-2}:

s=ut+12at2=0.5×5+12×0.3×52=6.25 m.s = ut + \frac{1}{2}at^2 = 0.5 \times 5 + \frac{1}{2} \times 0.3 \times 5^2 = 6.25 \text{ m}.

e. [3 marks]. Up the plane, the only forces along the slope are the resistance 38.5 N and the weight component 5gsin⁡θ5g\sin\theta, both acting down the slope (on the plane the only resistance is the stated 38.5 N, and the two slanting forces no longer act):

−38.5−5×9.8sin⁡θ=5a  ⇒  a=−7.7−9.8sin⁡θ.-38.5 - 5 \times 9.8\sin\theta = 5a \;\Rightarrow\; a = -7.7 - 9.8\sin\theta.

The object slows from 1.95 m s−1^{-1} to rest in 0.2 m, so with v2=u2+2asv^2 = u^2 + 2as:

0=1.952+2(−7.7−9.8sin⁡θ)(0.2).0 = 1.95^2 + 2(-7.7 - 9.8\sin\theta)(0.2).

This gives a=−9.50625a = -9.50625 m s−2^{-2}, so sin⁡θ=9.50625−7.79.8≈0.1843\sin\theta = \dfrac{9.50625 - 7.7}{9.8} \approx 0.1843 and θ≈10.6\theta \approx 10.6.

From the report. Part a was quite well done (72% full marks), but as a "show that" question it needed every step set out; some responses mixed up sine and cosine. In part b (71% correct) some students wrongly took the initial velocity as zero, and the same error appeared in part d. In part c, students who integrated the acceleration often forgot the constants of integration. Part e was answered fully by only 35%: a number of students did not recognise that the two slanting forces had stopped acting once the object passed PP.

Question 6 (9 marks)

A supplier claims the mass of aluminium in each empty can is normally distributed with mean 15 g and standard deviation 0.25 g. A random sample of 64 cans has mean mass 14.94 g. The company conducts a one-tailed test at the 5% level of significance, taking the standard deviation as 0.25 g.

a
Write down suitable hypotheses H0H_0 and H1H_1. (1 mark)
b
Find the pp value for the test, correct to three decimal places. (1 mark)
c
Does the sample mean support the supplier's claim at the 5% level for a one-tailed test? Justify your answer. (1 mark)
d
What is the smallest value of the sample mean of 64 cans for which H0H_0 is not rejected? Answer correct to two decimal places. (1 mark)

Filled cans have masses normally distributed with mean 406 g and standard deviation 5 g.

e. Find the probability that the masses of two randomly selected filled cans differ by no more than 3 g, correct to three decimal places. (2 marks)

Part f was redacted by VCAA from the paper and the report (following the Independent Review into VCAA's examination-setting policies, processes and procedures), so it is not covered here.

Show worked solution

a. [1 mark]. H0:μ=15H_0: \mu = 15 and H1:μ<15H_1: \mu < 15 (the sample mean is below 15, so the test is lower-tailed).

b. [1 mark]. Under H0H_0, Xˉ∼N(15,(0.2564)2)\bar X \sim N\left(15, \left(\tfrac{0.25}{\sqrt{64}}\right)^2\right), with standard deviation 0.258=0.03125\tfrac{0.25}{8} = 0.03125.

p=Pr⁡(Xˉ<14.94)=Pr⁡(Z<−1.92)≈0.027.p = \Pr(\bar X < 14.94) = \Pr(Z < -1.92) \approx 0.027.

c. [1 mark]. No. Since p≈0.027<0.05p \approx 0.027 < 0.05, H0H_0 is rejected at the 5% level, so the sample does not support the supplier's claim that the mean is 15 g.

d. [1 mark]. H0H_0 is not rejected when Pr⁡(Xˉ<xˉ)≥0.05\Pr(\bar X < \bar x) \geq 0.05. The critical value satisfies

xˉ=15+z0.05×0.03125=15−1.6449×0.03125≈14.9486,\bar x = 15 + z_{0.05} \times 0.03125 = 15 - 1.6449 \times 0.03125 \approx 14.9486,

so the smallest sample mean is 14.95 g (to two decimal places).

e. [2 marks]. Let D=X1−X2D = X_1 - X_2 be the difference in masses of two independent cans. Then E(D)=406−406=0E(D) = 406 - 406 = 0 and Var⁡(D)=52+52=50\operatorname{Var}(D) = 5^2 + 5^2 = 50, so D∼N(0,50)D \sim N(0, 50).

Pr⁡(∣D∣≤3)=Pr⁡(−3≤D≤3)≈0.329.\Pr(|D| \leq 3) = \Pr(-3 \leq D \leq 3) \approx 0.329.

From the report. Part a was well done (85% correct); the usual error was writing hypotheses for a two-tailed test. In part c (71% correct) some students did not justify their answer by referring to the pp value. Part d was answered correctly by 60%; some students miscopied the answer as 14.59. Part e was harder (48% scored zero, 40% full marks); most students did see that the condition is −3<D<3-3 < D < 3 for the difference DD.

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