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VICSpecialist Mathematics2021Exam 2

VCE Specialist Mathematics 2021 Exam 2

Worked solutions to the 2021 VCE Specialist Mathematics Examination 2 (80 marks, CAS allowed): all 20 multiple-choice answers with reasons and every Section B part, checked against the VCAA external assessment report, with the questions on forces flagged against the current study design.

Marks
80
Time
120 min
Authority
VCAA
Updated

Every question from the 2021 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 2021 Examination 1 walkthrough.

How to use this page

  • Questions are from the 2021 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 2021 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.
  • Percentages after multiple-choice answers are the share of students who chose the correct option. In Section B, the From the report notes summarise what the assessors said, with the share of students who gained full marks.
  • Study design. This paper was 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 as partly outside where they appear, are the questions about forces: Section A Questions 14 (Newton's second law), 15 (forces in equilibrium) and 16 (an object sliding down a smooth slope), and all of Section B Question 5 (connected masses on a rough inclined plane). The current 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, and the formula sheet no longer lists the Mechanics formulas (momentum and the equation of motion) that it gave in 2021. Everything else, including Question 4 (the stunt car, which is kinematics and vector calculus with no forces), 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 2021 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 (10, 9, 10, 11, 10 and 10 marks).

The report named these strengths: sketching in the complex plane, setting up a volume-of-revolution integral, using the chain rule for related rates, drawing a force diagram and CAS use. The weaknesses were answering every part of a multi-part question (1c, 3b.ii and 6d were singled out), using the right angle for the gradient of a line, justifying an answer when asked to, and noticing when the conditions change part-way through a mechanics problem. Three parts (3b.i, 4a and 4d) ask you to show a given result, so every step must be set out.

Section A: Multiple choice

Q1
How many asymptotes does the graph of f(x)=1sec⁡(3x)+32f(x) = \dfrac{1}{\sec(3x) + \frac32} have on [−π6,π]\left[-\tfrac{\pi}{6}, \pi\right]? Answer: B - f(x)=2cos⁡(3x)2+3cos⁡(3x)f(x) = \dfrac{2\cos(3x)}{2 + 3\cos(3x)} has a vertical asymptote wherever cos⁡(3x)=−23\cos(3x) = -\tfrac23. For 3x∈[−π2,3π]3x \in \left[-\tfrac{\pi}{2}, 3\pi\right] this happens three times (3x≈2.303x \approx 2.30, 3.983.98 and 8.588.58). Where cos⁡(3x)=0\cos(3x) = 0 the rule is undefined but f(x)→0f(x) \to 0, so those points are holes, not asymptotes. (66% correct; 20% chose C.)
Q2
Implied domain of f(x)=cos⁡−1(log⁡e(bx))f(x) = \cos^{-1}\big(\log_e(bx)\big), b>0b > 0. Answer: E - need −1≤log⁡e(bx)≤1-1 \le \log_e(bx) \le 1, so e−1≤bx≤ee^{-1} \le bx \le e and x∈[1be,eb]x \in \left[\tfrac{1}{be}, \tfrac{e}{b}\right]. (76% correct.)
Q3
Local maxima of y=1(cos⁡(ax)+1)2+3y = \dfrac{1}{\big(\cos(ax) + 1\big)^2 + 3}, a≠0a \ne 0. Answer: E - yy is largest when the denominator is smallest, which is 3 when cos⁡(ax)=−1\cos(ax) = -1, that is ax=(1+2k)πax = (1 + 2k)\pi: the points (π(1+2k)a,13)\left(\tfrac{\pi(1 + 2k)}{a}, \tfrac13\right), k∈Zk \in Z. (51% correct.)
Q4
For Im(z)>0\text{Im}(z) > 0, find Arg(zzˉz−zˉ)\text{Arg}\left(\dfrac{z\bar z}{z - \bar z}\right). Answer: A - with z=a+biz = a + bi and b>0b > 0, zzˉ=a2+b2z\bar z = a^2 + b^2 and z−zˉ=2biz - \bar z = 2bi, so the quotient is a2+b22bi=−a2+b22bi\dfrac{a^2 + b^2}{2bi} = -\dfrac{a^2 + b^2}{2b}i, on the negative imaginary axis: −π2-\tfrac{\pi}{2}. (35% correct; 29% chose D, the wrong sign.)
Q5
Maximum of ∣z∣|z| on the circle ∣z−2−3i∣=1\left|z - 2 - \sqrt3i\right| = 1. Answer: D - the farthest point from the origin lies on the line through the centre: ∣2+3i∣+1=4+3+1=7+1\left|2 + \sqrt3i\right| + 1 = \sqrt{4 + 3} + 1 = \sqrt7 + 1. (32% correct; 42% chose A, 3+1\sqrt3 + 1.)
Q6
z≠0z \ne 0 and z2∈Rz^2 \in R. Possible values of arg⁡(z)\arg(z)? Answer: A - if arg⁡(z)=θ\arg(z) = \theta, then z2=∣z∣2cis(2θ)z^2 = |z|^2\text{cis}(2\theta) is real exactly when 2θ=kπ2\theta = k\pi, so θ=kπ2\theta = \tfrac{k\pi}{2}, k∈Zk \in Z: real and purely imaginary zz both work. (23% correct; 30% chose C, which leaves out the real values of zz.)
Q7
x=5cos⁡(2t)+1x = 5\cos(2t) + 1, y=5sin⁡(2t)−1y = 5\sin(2t) - 1. Shortest distance along the graph from A(6,−1)A(6, -1) to B(1,4)B(1, 4). Answer: E - the graph is the circle with centre (1,−1)(1, -1) and radius 5. AA is due east of the centre and BB due north, a quarter-turn apart, so the shorter arc is 14×2π×5=5π2\tfrac14 \times 2\pi \times 5 = \tfrac{5\pi}{2}. (39% correct; 23% chose D.)
Q8
Euler's method, step 0.1, for dydx=ysin⁡(x)\dfrac{dy}{dx} = y\sin(x) with y=2y = 2 at x=1x = 1. Estimate yy at x=1.2x = 1.2. Answer: C - y1=2+0.1×2sin⁡(1)≈2.1683y_1 = 2 + 0.1 \times 2\sin(1) \approx 2.1683, then y2=2.1683+0.1×2.1683sin⁡(1.1)≈2.362y_2 = 2.1683 + 0.1 \times 2.1683\sin(1.1) \approx 2.362. (72% correct.)
Q9
Which f′(x)f'(x) gives a graph of ff with no points of inflection? Answer: B - for f′(x)=2(x−3)3+5f'(x) = 2(x - 3)^3 + 5, f′′(x)=6(x−3)2≥0f''(x) = 6(x - 3)^2 \ge 0 never changes sign. In A, C and D, f′′f'' is linear and changes sign at x=3x = 3; in E, f′′(x)=3(x−3)2−12f''(x) = 3(x - 3)^2 - 12 changes sign at x=1x = 1 and x=5x = 5. (38% correct; 22% chose E.)
Q10
Which differential equation has the given direction field? Answer: D - dydx=y−2x\dfrac{dy}{dx} = y - 2x. The slopes are zero along the line y=2xy = 2x (for example at (0.5,1)(0.5, 1) and (−0.5,−1)(-0.5, -1)), negative on the positive xx-axis and positive on the negative xx-axis. Only B and D are zero along y=2xy = 2x, and B has the opposite signs. (68% correct.)
Q11
With i\mathbf i east and j\mathbf j north, hikers walk 5 km in the direction south 30∘30^\circ west, then 10 km north. Their position vector? Answer: B - the first leg is 5(−sin⁡30∘ i−cos⁡30∘ j)=−52i−532j5\left(-\sin 30^\circ\,\mathbf i - \cos 30^\circ\,\mathbf j\right) = -\tfrac52\mathbf i - \tfrac{5\sqrt3}{2}\mathbf j; adding 10j10\mathbf j gives −52i+(10−532)j-\tfrac52\mathbf i + \left(10 - \tfrac{5\sqrt3}{2}\right)\mathbf j. (69% correct.)
Q12
a=xi+j\mathbf a = x\mathbf i + \mathbf j, b=i−j\mathbf b = \mathbf i - \mathbf j, c=i+xj\mathbf c = \mathbf i + x\mathbf j; θ\theta is the angle between a\mathbf a and b\mathbf b, and ϕ\phi the angle between b\mathbf b and c\mathbf c. Find cos⁡(θ)cos⁡(ϕ)\cos(\theta)\cos(\phi). Answer: D - cos⁡θ=x−12x2+1\cos\theta = \dfrac{x - 1}{\sqrt2\sqrt{x^2 + 1}} and cos⁡ϕ=1−x2x2+1\cos\phi = \dfrac{1 - x}{\sqrt2\sqrt{x^2 + 1}}, so the product is −(x−1)22(1+x2)-\dfrac{(x - 1)^2}{2(1 + x^2)}. (60% correct.)
Q13
The scalar resolute of a\mathbf a in the direction of b=−3 i\mathbf b = -\sqrt3\,\mathbf i is −4-4. The vector resolute? Answer: E - multiply the scalar resolute by the unit vector b^=−i\hat{\mathbf b} = -\mathbf i: −4(−i)=4i-4(-\mathbf i) = 4\mathbf i. (46% correct; 22% chose A, −4i-4\mathbf i.)
Q14
A 5 kg body moves in a straight line with v=3+2xv = 3 + 2x. Find the net force FF when x=2x = 2. Answer: D - a=vdvdx=(3+2x)(2)=14a = v\dfrac{dv}{dx} = (3 + 2x)(2) = 14 at x=2x = 2, so F=ma=5×14=70F = ma = 5 \times 14 = 70 N. (56% correct.) Study design: partly outside. Finding a=vdvdxa = v\frac{dv}{dx} is on the course, but F=maF = ma is not listed in Units 3 and 4: 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, and the formula sheet no longer lists the Mechanics formulas (momentum and the equation of motion) that it gave in 2021.
Q15
A stationary body is acted on by 8 N to the right, F1F_1 to the left, F2F_2 at 60∘60^\circ above the horizontal (on the 8 N side) and 6 N at 30∘30^\circ below the horizontal (on the F1F_1 side). Find F1F_1. Answer: A - vertically, F2sin⁡60∘=6sin⁡30∘F_2\sin 60^\circ = 6\sin 30^\circ, so F2=23F_2 = 2\sqrt3. Horizontally, F1=8+F2cos⁡60∘−6cos⁡30∘=8+3−33=8−23F_1 = 8 + F_2\cos 60^\circ - 6\cos 30^\circ = 8 + \sqrt3 - 3\sqrt3 = 8 - 2\sqrt3. (53% correct.) Study design: partly outside. Resolving vectors into components is on the course, but forces in equilibrium (statics) are now Specialist Mathematics Unit 2 content, which Units 3 and 4 assume but do not list as a topic.
Q16
An object slides down a smooth slope inclined at θ∘\theta^\circ (0∘<θ∘<45∘0^\circ < \theta^\circ < 45^\circ) with acceleration aa. Its acceleration when the angle is doubled? Answer: B - on a smooth slope a=gsin⁡θa = g\sin\theta, so cos⁡θ=g2−a2g\cos\theta = \dfrac{\sqrt{g^2 - a^2}}{g} and gsin⁡2θ=2gsin⁡θcos⁡θ=2agg2−a2g\sin 2\theta = 2g\sin\theta\cos\theta = \dfrac{2a}{g}\sqrt{g^2 - a^2}. (48% correct.) Study design: partly outside. The result a=gsin⁡θa = g\sin\theta comes from resolving the forces on the object, and the current study design covers forces only in Specialist Mathematics Unit 2 (motion under a constant force), which Units 3 and 4 assume. The trigonometry is still needed.
Q17
Fill volumes are normal with mean 1.26 L and standard deviation 0.01 L. Probability the mean of six bottles is at least 1.25 L? Answer: E - Xˉ\bar X has mean 1.26 and standard deviation 0.016\tfrac{0.01}{\sqrt6}, so Pr⁡(Xˉ≥1.25)=Pr⁡(Z≥−6)≈0.9928\Pr(\bar X \ge 1.25) = \Pr\left(Z \ge -\sqrt6\right) \approx 0.9928. (50% correct; 20% chose B, 0.8413, which is the probability for a single bottle.)
Q18
A 95% confidence interval from a sample of 100 fish is (70.2,75.8)(70.2, 75.8) g. The sample mean divided by the population standard deviation? Answer: C - xˉ=73\bar x = 73 and the margin is 2.8=1.96×σ102.8 = 1.96 \times \tfrac{\sigma}{10}, so σ≈14.29\sigma \approx 14.29 and 7314.29≈5.1\tfrac{73}{14.29} \approx 5.1. (65% correct.)
Q19
Scores with mean 25 and variance 36 are scaled by S=mX+nS = mX + n (m>0m > 0) to mean 30 and variance 49, with SS rounded to the nearest integer. What does 32 scale to? Answer: D - m2=4936m^2 = \tfrac{49}{36} gives m=76m = \tfrac76, and 30=76×25+n30 = \tfrac76 \times 25 + n gives n=56n = \tfrac56. Then S=76×32+56≈38.2S = \tfrac76 \times 32 + \tfrac56 \approx 38.2, which rounds to 38. (51% correct; 24% chose C.)
Q20
Two independent machines each take a normally distributed time with mean 30 s and standard deviation 5 s to make a cup of coffee. Probability their times differ by less than 3 seconds? Answer: C - T1−T2T_1 - T_2 has mean 0 and variance 25+25=5025 + 25 = 50, so Pr⁡(∣T1−T2∣<3)=Pr⁡(∣Z∣<350)≈0.329\Pr\left(|T_1 - T_2| < 3\right) = \Pr\left(|Z| < \tfrac{3}{\sqrt{50}}\right) \approx 0.329. (43% correct.)

Section B: Extended response

Question 1 (10 marks)

Let f(x)=(2x−3)(x+5)(x−1)(x+2)f(x) = \dfrac{(2x - 3)(x + 5)}{(x - 1)(x + 2)}.

a
Express f(x)f(x) in the form A+Bx+C(x−1)(x+2)A + \dfrac{Bx + C}{(x - 1)(x + 2)}. (1 mark)
b
State the equations of the asymptotes of the graph of ff. (2 marks)
c
Sketch the graph of ff, labelling the asymptotes, the maximum turning point and the point of inflection (coordinates to two decimal places), and the axis intercepts. (3 marks)

Let gk(x)=(2x−3)(x+5)(x−k)(x+2)g_k(x) = \dfrac{(2x - 3)(x + 5)}{(x - k)(x + 2)}, where kk is a real constant.

d. i. For what values of kk does the graph of gkg_k have two asymptotes? (2 marks)

ii. Given that the graph of gkg_k has more than two asymptotes, for what values of kk does it have no stationary points? (2 marks)

Show worked solution

a. [1 mark]. (2x−3)(x+5)=2x2+7x−15=2(x2+x−2)+5x−11(2x - 3)(x + 5) = 2x^2 + 7x - 15 = 2\left(x^2 + x - 2\right) + 5x - 11 and (x−1)(x+2)=x2+x−2(x - 1)(x + 2) = x^2 + x - 2, so

f(x)=2+5x−11(x−1)(x+2).f(x) = 2 + \frac{5x - 11}{(x - 1)(x + 2)}.

That is A=2A = 2, B=5B = 5 and C=−11C = -11.

b. [2 marks]. Vertical asymptotes x=1x = 1 and x=−2x = -2 (the numerator is not zero there), and the horizontal asymptote y=2y = 2, since the fraction in part a tends to 0 as x→±∞x \to \pm\infty.

c. [3 marks]. The intercepts are (−5,0)(-5, 0), (1.5,0)(1.5, 0) and (0,7.5)(0, 7.5). Differentiating,

f′(x)=−5x2+22x+1(x−1)2(x+2)2,f'(x) = \frac{-5x^2 + 22x + 1}{(x - 1)^2(x + 2)^2},

which is zero at x=11±3145x = \dfrac{11 \pm 3\sqrt{14}}{5}. The root x≈4.44x \approx 4.44 gives the maximum turning point (4.44,2.51)(4.44, 2.51); the other root, x≈−0.04x \approx -0.04, is the minimum of the middle branch, just left of the yy-intercept. Solving f′′(x)=0f''(x) = 0 with CAS gives one point of inflection, (6.79,2.45)(6.79, 2.45). The right branch crosses y=2y = 2 at x=2.2x = 2.2 (where 5x−11=05x - 11 = 0), rises to the maximum, then falls back towards y=2y = 2 from above.

Graph of y = (2x - 3)(x + 5) / ((x - 1)(x + 2)) Vertical asymptotes x = -2 and x = 1 and horizontal asymptote y = 2. The left branch comes in just below y = 2, crosses the x-axis at (-5, 0) and falls to negative infinity at x = -2. The middle branch is a U shape between the asymptotes, crossing the y-axis at (0, 7.5), very close to its lowest point. The right branch rises from negative infinity at x = 1, crosses the x-axis at (1.5, 0) and the line y = 2 at x = 2.2, reaches a maximum at (4.44, 2.51), passes a point of inflection at (6.79, 2.45) and then decreases towards y = 2. x y -10 5 10 -5 5 15 (-5, 0) (1.5, 0) (0, 7.5) (4.44, 2.51) (6.79, 2.45) x = -2 x = 1 y = 2

d. i. [2 marks]. Usually gkg_k has three asymptotes: x=kx = k, x=−2x = -2 and y=2y = 2. It has only two when one of the vertical asymptotes disappears:

  • k=−2k = -2: the denominator is (x+2)2(x + 2)^2, leaving x=−2x = -2 and y=2y = 2.
  • k=−5k = -5 or k=32k = \tfrac32: the factor x−kx - k cancels with a factor of the numerator, leaving a hole instead of an asymptote.

So k=−5k = -5, k=−2k = -2 or k=32k = \tfrac32.

ii. [2 marks]. The numerator of gk′(x)g_k'(x) is the quadratic

−(2k+3)x2+(30−8k)x+(30−29k),-(2k + 3)x^2 + (30 - 8k)x + (30 - 29k),

whose discriminant simplifies to −84(k+5)(2k−3)-84(k + 5)(2k - 3). There are no stationary points when the discriminant is negative, that is when (k+5)(2k−3)>0(k + 5)(2k - 3) > 0:

k<−5ork>32.k < -5 \quad\text{or}\quad k > \tfrac32.

(For −5<k<32-5 < k < \tfrac32 with k≠−2k \ne -2, the numerator has real roots, none of them at x=kx = k or x=−2x = -2, so stationary points exist. At k=−32k = -\tfrac32 the x2x^2 term vanishes, leaving one stationary point.)

From the report. Part a was well answered (79% correct). In part b (67% full marks) the usual slip was leaving out the horizontal asymptote y=2y = 2. Part c had 22% full marks: a significant number of graphs had no middle branch (matching the CAS window to the given axes avoids this), and many were missing a required label, such as the point of inflection or an axis intercept. In d.i (6% full marks) very few gave all three values, and many gave just k=−2k = -2. In d.ii (13% full marks, 82% scored zero) some added incorrect values of kk, and many did not attempt it.

Question 2 (9 marks)

The polynomial p(z)=z3+αz2+βz+γp(z) = z^3 + \alpha z^2 + \beta z + \gamma, with α,β,γ∈R\alpha, \beta, \gamma \in R, can also be written p(z)=(z−z1)(z−z2)(z−z3)p(z) = (z - z_1)(z - z_2)(z - z_3), where z1∈Rz_1 \in R and z2,z3∈Cz_2, z_3 \in C.

a. i. State the relationship between z2z_2 and z3z_3. (1 mark)

ii. Find α\alpha, β\beta and γ\gamma, given that p(2)=−13p(2) = -13, ∣z2+z3∣=0|z_2 + z_3| = 0 and ∣z2−z3∣=6|z_2 - z_3| = 6. (3 marks)

Let z4=3+iz_4 = \sqrt3 + i.

b. Sketch the ray Arg(z−z4)=5π6\text{Arg}(z - z_4) = \dfrac{5\pi}{6} on an Argand diagram. (2 marks)

The ray meets the circle ∣z−3i∣=1|z - 3i| = 1, dividing it into a major and a minor segment.

c. i. Sketch the circle ∣z−3i∣=1|z - 3i| = 1 on the same diagram. (1 mark)

ii. Find the area of the minor segment. (2 marks)

Show worked solution

a. i. [1 mark]. The coefficients are real, so the non-real roots are a conjugate pair: z3=zˉ2z_3 = \bar z_2 (equivalently z2=zˉ3z_2 = \bar z_3).

ii. [3 marks]. Write z2=a+biz_2 = a + bi and z3=a−biz_3 = a - bi. Then ∣z2+z3∣=∣2a∣=0|z_2 + z_3| = |2a| = 0 gives a=0a = 0, and ∣z2−z3∣=∣2bi∣=6|z_2 - z_3| = |2bi| = 6 gives b=±3b = \pm3. So the complex roots are ±3i\pm3i and (z−z2)(z−z3)=z2+9(z - z_2)(z - z_3) = z^2 + 9. Using the factorised form,

p(2)=(2−z1)(4+9)=−13  ⟹  z1=3,p(2) = (2 - z_1)(4 + 9) = -13 \implies z_1 = 3,

p(z)=(z−3)(z2+9)=z3−3z2+9z−27,p(z) = (z - 3)\left(z^2 + 9\right) = z^3 - 3z^2 + 9z - 27,

so α=−3\alpha = -3, β=9\beta = 9 and γ=−27\gamma = -27. (If z2z_2 and z3z_3 are taken to be real, then z2=3z_2 = 3, z3=−3z_3 = -3 and z1=−35z_1 = -\tfrac35 also fit, giving α=35\alpha = \tfrac35, β=−9\beta = -9 and γ=−275\gamma = -\tfrac{27}{5}; the report accepted this when the working across parts a.i and a.ii was correct and complete.)

b. [2 marks]. The ray starts at z4=3+iz_4 = \sqrt3 + i, drawn as an open circle because that point is not on the ray, and heads up and to the left at 5π6\tfrac{5\pi}{6} to the positive real direction, so its gradient is tan⁡5π6=−13\tan\tfrac{5\pi}{6} = -\tfrac{1}{\sqrt3}. Moving 3\sqrt3 to the left raises it by 1, so it passes through 2i2i.

c. i. [1 mark]. The circle with centre 3i3i and radius 1, through 2i2i, 4i4i and ±1+3i\pm1 + 3i.

The ray Arg(z - (root 3 + i)) = 5pi/6 and the circle |z - 3i| = 1 A ray starts at root 3 + i (open circle) and heads up and to the left at 5pi/6 to the positive real direction, passing through 2i. The ray enters the circle of radius 1 centred at 3i at 2i, the circle's lowest point, and leaves it at -root 3/2 + 5i/2. The small shaded region between this chord and the lower-left arc of the circle is the minor segment. Re(z) Im(z) -3 -2 -1 1 2 3 1 √3 + i 3i

ii. [2 marks]. Points on the ray are (3(1−s),1+s)\left(\sqrt3(1 - s), 1 + s\right) for s≥0s \ge 0. Substituting into x2+(y−3)2=1x^2 + (y - 3)^2 = 1 gives 4s2−10s+6=04s^2 - 10s + 6 = 0, so s=1s = 1 or s=32s = \tfrac32: the ray cuts the circle at 2i2i and −32+52i-\tfrac{\sqrt3}{2} + \tfrac52i. These points are 1 apart, the same as the radius, so the chord and the two radii form an equilateral triangle and the angle at the centre is π3\tfrac{\pi}{3}:

A=12r2(θ−sin⁡θ)=12(π3−32)=π6−34=2π−3312≈0.091.A = \frac12r^2(\theta - \sin\theta) = \frac12\left(\frac{\pi}{3} - \frac{\sqrt3}{2}\right) = \frac{\pi}{6} - \frac{\sqrt3}{4} = \frac{2\pi - 3\sqrt3}{12} \approx 0.091.

From the report. Part a.i was well answered (73% correct). In a.ii (23% full marks) many students substituted p(2)=−13p(2) = -13 into the expanded cubic, when working with the factorised form was quicker. In part b (31% full marks) the angle of the ray was usually right, but its starting point must be an open circle, and it was sometimes left out or put in the wrong place. Part c.i was well done (75%). In c.ii (22% full marks) the strongest answers used the segment-area formula (a smaller number used a definite integral), and some who used an area formula had trouble finding the angle at the centre.

Question 3 (10 marks)

A thin-walled vessel is formed by rotating the graph of y=x3−8y = x^3 - 8 about the yy-axis for 0≤y≤H0 \le y \le H (lengths in centimetres).

a. i. Write a definite integral in terms of yy and HH for the volume of the vessel. (1 mark)

ii. Hence find the volume in terms of HH. (1 mark)

Water leaks out through a crack in the base at dVdt=−4h\dfrac{dV}{dt} = -4\sqrt h cm³ per minute, where hh cm is the depth of water and VV cm³ the volume of water after tt minutes.

b. i
Show that dhdt=−4hπ(h+8)2/3\dfrac{dh}{dt} = \dfrac{-4\sqrt h}{\pi(h + 8)^{2/3}}. (2 marks)
ii
Find the maximum rate at which the depth decreases, in cm per minute to two decimal places, and the depth at which it occurs. (2 marks)
iii
A vessel with H=50H = 50 is initially full and still leaking at 4h4\sqrt h cm³ per minute. Find the maximum rate at which water can be added without the vessel overflowing. (1 mark)
c
With H=50H = 50 and the vessel initially full, extra water is poured in at 40240\sqrt2 cm³ per minute once the depth has dropped to 25 cm, while the leak continues. How long does the vessel take to refill completely from a depth of 25 cm, in minutes to one decimal place? (3 marks)
Show worked solution

a. i. [1 mark]. y=x3−8y = x^3 - 8 gives x=(y+8)1/3x = (y + 8)^{1/3}, the radius at height yy, so

V=π∫0H(y+8)2/3 dy.V = \pi\int_0^H (y + 8)^{2/3}\,dy.

ii. [1 mark]. V=π[35(y+8)5/3]0H=3π5((H+8)5/3−32)V = \pi\left[\tfrac35(y + 8)^{5/3}\right]_0^H = \dfrac{3\pi}{5}\left((H + 8)^{5/3} - 32\right) cm³, since 85/3=328^{5/3} = 32.

b. i. [2 marks]. When the depth is hh, the volume of water is V=π∫0h(y+8)2/3 dyV = \pi\displaystyle\int_0^h(y + 8)^{2/3}\,dy, so dVdh=π(h+8)2/3\dfrac{dV}{dh} = \pi(h + 8)^{2/3}. By the chain rule,

dhdt=dVdt×dhdV=−4h×1π(h+8)2/3=−4hπ(h+8)2/3.\frac{dh}{dt} = \frac{dV}{dt} \times \frac{dh}{dV} = -4\sqrt h \times \frac{1}{\pi(h + 8)^{2/3}} = \frac{-4\sqrt h}{\pi(h + 8)^{2/3}}.

ii. [2 marks]. The depth falls fastest where r(h)=4hπ(h+8)2/3r(h) = \dfrac{4\sqrt h}{\pi(h + 8)^{2/3}} is largest. Setting r′(h)=0r'(h) = 0:

(h+8)2/32h=23h(h+8)−1/3  ⟹  3(h+8)=4h  ⟹  h=24.\frac{(h + 8)^{2/3}}{2\sqrt h} = \frac23\sqrt h(h + 8)^{-1/3} \implies 3(h + 8) = 4h \implies h = 24.

Then r(24)=424π×322/3≈0.62r(24) = \dfrac{4\sqrt{24}}{\pi \times 32^{2/3}} \approx 0.62. The maximum rate of decrease is 0.62 cm per minute, at a depth of 24 cm.

iii. [1 mark]. When the vessel is full, h=50h = 50 and water leaks out at 450=202≈28.34\sqrt{50} = 20\sqrt2 \approx 28.3 cm³ per minute. Adding water any faster would raise the level above the brim, so the maximum rate is 20220\sqrt2 cm³ per minute.

c. [3 marks]. While water is poured in, dVdt=402−4h\dfrac{dV}{dt} = 40\sqrt2 - 4\sqrt h, so

dhdt=402−4hπ(h+8)2/3  ⟹  t=∫2550π(h+8)2/3402−4h dh≈31.4 minutes.\frac{dh}{dt} = \frac{40\sqrt2 - 4\sqrt h}{\pi(h + 8)^{2/3}} \implies t = \int_{25}^{50}\frac{\pi(h + 8)^{2/3}}{40\sqrt2 - 4\sqrt h}\,dh \approx 31.4 \text{ minutes}.

(The inflow, 402≈56.640\sqrt2 \approx 56.6 cm³ per minute, is always more than the leak, which is at most 450≈28.34\sqrt{50} \approx 28.3, so the depth rises the whole time.)

From the report. Parts a.i (80% correct) and b.i (77% full marks) were well done, b.i by applying the chain rule. In a.ii (59% correct) the common errors were in notation, such as putting the 32 outside the brackets or writing hh for HH. In b.ii (22% full marks) a number of students gave just one of the two values asked for. In b.iii (23% correct) a number of students wrote 4h4\sqrt h and went no further; equivalent forms such as 4504\sqrt{50} were accepted. Part c (12% full marks) depended on understanding the physical set-up, solid calculus and careful CAS work: 77% scored zero, and about half of those who made a productive start reached 31.4.

Question 4 (11 marks)

A stunt car accelerates from rest at AA along a horizontal track, is launched from the ramp BOBO and lands on a second section of track, inclined at 10∘10^\circ to the horizontal (sloping down), at or beyond C(16,4)C(16, 4). Air resistance is negligible, OO is the origin and distances are in metres. At OO the car has speed uu m s−1^{-1} at an angle θ\theta to the horizontal, and its rear wheels then follow r(t)=utcos⁡(θ) i+(utsin⁡(θ)−12gt2)j\mathbf r(t) = ut\cos(\theta)\,\mathbf i + \left(ut\sin(\theta) - \tfrac12gt^2\right)\mathbf j.

a
Show that the path of the rear wheels is y=xtan⁡(θ)−4.9x2u2cos⁡2(θ)y = x\tan(\theta) - \dfrac{4.9x^2}{u^2\cos^2(\theta)}. (1 mark)
b
If θ=30∘\theta = 30^\circ, find the minimum speed at OO for the rear wheels to land at or beyond CC, to two decimal places. (2 marks)
c
For what values of θ\theta (to the nearest degree) and uu (to one decimal place) does the path join the second section of track smoothly at CC? (3 marks)

On the horizontal section ABAB, the acceleration after the car has travelled ss metres from AA is a=60va = \dfrac{60}{v}, where vv is its speed.

d. Show that v=(180s)1/3v = (180s)^{1/3}. (2 marks)

e. The car reaches 20 m s−1^{-1} at BB. If the stunt is called off, the car brakes at 9 m s−2^{-2} and must stop at or before BB; WW is the furthest point along ABAB at which the stunt can be called off. How far is WW from BB, to one decimal place? (3 marks)

Show worked solution

a. [1 mark]. From x=utcos⁡θx = ut\cos\theta, t=xucos⁡θt = \dfrac{x}{u\cos\theta}. Substituting into y=utsin⁡θ−4.9t2y = ut\sin\theta - 4.9t^2:

y=usin⁡θ×xucos⁡θ−4.9(xucos⁡θ)2=xtan⁡θ−4.9x2u2cos⁡2θ.y = u\sin\theta \times \frac{x}{u\cos\theta} - 4.9\left(\frac{x}{u\cos\theta}\right)^2 = x\tan\theta - \frac{4.9x^2}{u^2\cos^2\theta}.

b. [2 marks]. At the minimum speed the rear wheels land exactly at CC. Substituting x=16x = 16, y=4y = 4 and θ=30∘\theta = 30^\circ:

4=16tan⁡30∘−4.9×162u2cos⁡230∘  ⟹  u2=4.9×2560.75(16tan⁡30∘−4)  ⟹  u≈17.87 m s−1.4 = 16\tan 30^\circ - \frac{4.9 \times 16^2}{u^2\cos^2 30^\circ} \implies u^2 = \frac{4.9 \times 256}{0.75\left(16\tan 30^\circ - 4\right)} \implies u \approx 17.87 \text{ m s}^{-1}.

Any faster and the car is still above the track when x=16x = 16, so it lands beyond CC.

c. [3 marks]. Two conditions: the path passes through C(16,4)C(16, 4), and its gradient there matches the track, which slopes down at 10∘10^\circ, so its gradient is tan⁡(170∘)=−tan⁡10∘\tan(170^\circ) = -\tan 10^\circ. The path has dydx=tan⁡θ−9.8xu2cos⁡2θ\dfrac{dy}{dx} = \tan\theta - \dfrac{9.8x}{u^2\cos^2\theta}, so with K=9.8×16u2cos⁡2θK = \dfrac{9.8 \times 16}{u^2\cos^2\theta} (note 4.9×162=8×9.8×164.9 \times 16^2 = 8 \times 9.8 \times 16):

tan⁡θ−K=−tan⁡10∘,16tan⁡θ−8K=4.\tan\theta - K = -\tan 10^\circ, \qquad 16\tan\theta - 8K = 4.

Eliminating KK: 16tan⁡θ−8(tan⁡θ+tan⁡10∘)=416\tan\theta - 8\left(\tan\theta + \tan 10^\circ\right) = 4, so tan⁡θ=12+tan⁡10∘≈0.676\tan\theta = \tfrac12 + \tan 10^\circ \approx 0.676 and θ≈34∘\theta \approx 34^\circ. Then u2cos⁡2θ=156.8tan⁡θ+tan⁡10∘u^2\cos^2\theta = \dfrac{156.8}{\tan\theta + \tan 10^\circ} gives u≈16.4u \approx 16.4 m s−1^{-1}.

d. [2 marks]. Use a=vdvdsa = v\dfrac{dv}{ds}:

vdvds=60v  ⟹  dsdv=v260  ⟹  s=v3180+c.v\frac{dv}{ds} = \frac{60}{v} \implies \frac{ds}{dv} = \frac{v^2}{60} \implies s = \frac{v^3}{180} + c.

The car starts from rest at AA, so v=0v = 0 when s=0s = 0 and c=0c = 0. Hence v3=180sv^3 = 180s and v=(180s)1/3v = (180s)^{1/3}.

e. [3 marks]. At BB, 20=(180s)1/320 = (180s)^{1/3} gives AB=8000180=4009≈44.4AB = \tfrac{8000}{180} = \tfrac{400}{9} \approx 44.4 m. Let WW be dd metres before BB. The speed at WW is (180(4009−d))1/3\left(180\left(\tfrac{400}{9} - d\right)\right)^{1/3}, and braking at 9 m s−2^{-2} brings the car to rest in exactly dd metres when (from v2=u2+2asv^2 = u^2 + 2as) the square of that speed equals 2×9×d2 \times 9 \times d:

(180(4009−d))2/3=18d  ⟹  d≈16.4 m (CAS).\left(180\left(\tfrac{400}{9} - d\right)\right)^{2/3} = 18d \implies d \approx 16.4 \text{ m (CAS)}.

So WW is about 16.4 m from BB.

From the report. In part a (57% correct) some students used the Pythagorean identity to eliminate θ\theta, which did not help; the intended route eliminates tt. In part b (40% full marks) incorrect vector-calculus methods were common, and some substituted the coordinates of CC the wrong way round; students who could not do part a could still use its given result here and gain full marks. Part c had 6% full marks and 80% scored zero: many did not attempt it, very few set up both equations, and a common error was taking the gradient as tan⁡10∘\tan 10^\circ instead of tan⁡170∘=−tan⁡10∘\tan 170^\circ = -\tan 10^\circ. The equations can be solved for tan⁡θ\tan\theta by hand, by elimination. In part d (31% full marks) some wrongly used a constant acceleration formula, and others left out the constant of integration or did not show that it is zero. Part e was rarely done well (3% full marks, 87% scored zero).

Question 5 (10 marks)

A mass of m1m_1 kg on a plane inclined at 30∘30^\circ is connected by a light inextensible string, over a frictionless pulley at the top of the incline, to a mass of m2m_2 kg hanging vertically.

a. If the plane is smooth, find the relationship between m1m_1 and m2m_2 for m1m_1 to move down the plane at constant speed. (2 marks)

The plane is now rough. With NN the magnitude of the normal force on m1m_1, a resistance force of magnitude λN\lambda N opposes the motion of m1m_1.

b
The mass m1m_1 moves up the plane.
i
Mark and label all the forces acting on m1m_1. (1 mark)
ii
Taking up the plane as positive, find the acceleration of m1m_1 in terms of m1m_1, m2m_2 and λ\lambda. (2 marks)

Later, m2m_2 hits the ground at 4.5 m s−1^{-1} and the string becomes slack, with m1m_1 at the point PP on the plane, 2 m from the pulley. Take λ=0.1\lambda = 0.1.

c. How far from PP does m1m_1 travel before it starts to slide back down the plane, to two decimal places? (2 marks)

d. Find the time from when the string becomes slack until m1m_1 returns to PP, to the nearest tenth of a second. (3 marks)

Study design: partly outside. This question is about forces: resolving the weight on an inclined plane, the tension in a string over a pulley, a resistance force λN\lambda N and Newton's second law. 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; pulleys, connected masses and resistance forces are not named in it, and the formula sheet no longer lists the Mechanics formulas (momentum and the equation of motion) that it gave in 2021. Parts c and d finish with constant-acceleration kinematics, which is still on the course.

Show worked solution

a. [2 marks]. At constant speed the acceleration is zero, so the forces on each mass balance. For m2m_2, T=m2gT = m_2g. Along the smooth plane, m1gsin⁡30∘=Tm_1g\sin 30^\circ = T. So 12m1g=m2g\tfrac12m_1g = m_2g, that is

m1=2m2.m_1 = 2m_2.

b. i. [1 mark]. Four forces act on m1m_1: its weight m1gm_1g vertically down, the normal force NN perpendicular to the plane, the tension TT up the plane, and the resistance λN\lambda N down the plane, opposing the motion.

Forces on the mass m1 moving up the rough 30 degree plane A plane inclined at 30 degrees with a pulley at its top and the mass m2 hanging on the far side. Four forces act on the mass m1 on the plane: the normal force N perpendicular to the plane, the tension T up the plane along the string, the resistance lambda N down the plane (opposing the motion up the plane), and the weight m1 g vertically downwards. 30° m₁ m₂ N T λN m₁g

ii. [2 marks]. Perpendicular to the plane, N=m1gcos⁡30∘=32m1gN = m_1g\cos 30^\circ = \tfrac{\sqrt3}{2}m_1g. Newton's second law for each mass, with common acceleration aa:

m2g−T=m2a,T−λm1gcos⁡30∘−m1gsin⁡30∘=m1a.m_2g - T = m_2a, \qquad T - \lambda m_1g\cos 30^\circ - m_1g\sin 30^\circ = m_1a.

Adding the two equations eliminates TT:

a=gm1+m2(m2−3λm12−m12)=g(2m2−m1−3λm1)2(m1+m2).a = \frac{g}{m_1 + m_2}\left(m_2 - \frac{\sqrt3\lambda m_1}{2} - \frac{m_1}{2}\right) = \frac{g\left(2m_2 - m_1 - \sqrt3\lambda m_1\right)}{2(m_1 + m_2)}.

c. [2 marks]. Once the string is slack, only gravity and the resistance act along the plane, and both act down the slope while m1m_1 is still moving up:

a=−g(sin⁡30∘+0.1cos⁡30∘)=−g(12+320)≈−5.749 m s−2.a = -g\left(\sin 30^\circ + 0.1\cos 30^\circ\right) = -g\left(\frac12 + \frac{\sqrt3}{20}\right) \approx -5.749 \text{ m s}^{-2}.

From v2=u2+2asv^2 = u^2 + 2as with u=4.5u = 4.5 and v=0v = 0, s=4.522×5.749≈1.76s = \dfrac{4.5^2}{2 \times 5.749} \approx 1.76 m. (That is less than the 2 m to the pulley.)

d. [3 marks]. Up the plane: 0=4.5−5.749t0 = 4.5 - 5.749t gives t≈0.783t \approx 0.783 s. Coming back down, the resistance acts up the plane, so the acceleration down the slope is smaller:

g(12−320)≈4.051 m s−2,1.761=12×4.051×t2  ⟹  t≈0.932 s.g\left(\frac12 - \frac{\sqrt3}{20}\right) \approx 4.051 \text{ m s}^{-2}, \qquad 1.761 = \tfrac12 \times 4.051 \times t^2 \implies t \approx 0.932 \text{ s}.

The total time is 0.783+0.932≈1.70.783 + 0.932 \approx 1.7 s.

From the report. In part a (46% full marks) many did not see that constant speed means zero acceleration. Part b.i was generally well done (65% correct); the usual errors were drawing the resistance up the plane or leaving out a force. In b.ii (24% full marks) common errors were taking the tension to be m2gm_2g or not using N=m1gcos⁡30∘N = m_1g\cos 30^\circ. In part c (11% full marks) many answers expressed the acceleration using m1m_1, m2m_2 or TT, and some mixed up the starting and final velocities. Part d was rarely done well (3% full marks): a common error was assuming the trip down takes as long as the trip up, and only a minority reversed the direction of the resistance for the return.

Question 6 (10 marks)

A lift has a maximum load of 1000 kg. The masses of employees are normally distributed with mean 75 kg and standard deviation 8 kg, and nn employees are about to use the lift.

a. What is the maximum value of nn for there to be less than a 1% chance of the lift exceeding the maximum load? (2 marks)

The times to dispense hot drinks are independent and normally distributed with mean 2 minutes and standard deviation 0.5 minutes.

b. At 8.52 am Clare is fourth in the queue, and her meeting starts at 9.00 am. The waiting time between drinks is negligible and she needs 0.5 minutes to reach the meeting room. Find the probability, to four decimal places, that she is on time. (2 marks)

Daily sales of chocolate bars are normally distributed with mean 60 000 and standard deviation 5000. After an advertising campaign, the mean daily sales over 14 randomly selected days is 63 500. Clare performs a one-sided test at the 1% level of significance.

c. i
Write down suitable null and alternative hypotheses. (1 mark)
ii
Find the pp value, to four decimal places. (1 mark)
iii
Giving a reason, state whether there is any evidence that the campaign succeeded. (1 mark)
d
Find the range of values of the mean daily sales over another 14 days that would lead to the null hypothesis being rejected at the 1% level, to the nearest integer. (1 mark)
e
The mean daily sales is now in fact 63 000. For a test at the 5% level, find the probability that the null hypothesis would be incorrectly accepted, based on another 14 days and a standard deviation of 5000, to three decimal places. (2 marks)
Show worked solution

a. [2 marks]. The total mass of nn people is Wn∼N(75n,82n)W_n \sim N\left(75n, 8^2n\right). We need Pr⁡(Wn>1000)<0.01\Pr(W_n > 1000) < 0.01:

  • n=12n = 12: W12∼N(900,768)W_{12} \sim N(900, 768) and Pr⁡(W12>1000)≈0.0002\Pr(W_{12} > 1000) \approx 0.0002.
  • n=13n = 13: W13∼N(975,832)W_{13} \sim N(975, 832) and Pr⁡(W13>1000)≈0.19\Pr(W_{13} > 1000) \approx 0.19.

So the maximum is n=12n = 12.

b. [2 marks]. Clare needs all four drinks (the three ahead of her and her own) within 8−0.5=7.58 - 0.5 = 7.5 minutes. Their total time T4T_4 is the sum of four independent times, so T4∼N(4×2,4×0.52)=N(8,1)T_4 \sim N\left(4 \times 2, 4 \times 0.5^2\right) = N(8, 1) and

Pr⁡(T4<7.5)=Pr⁡(Z<−0.5)≈0.3085.\Pr(T_4 < 7.5) = \Pr(Z < -0.5) \approx 0.3085.

c. i. [1 mark]
H0:μ=60 000H_0: \mu = 60\,000 and H1:μ>60 000H_1: \mu > 60\,000.
ii. [1 mark]
Under H0H_0, Xˉ\bar X is normal with mean 60 000 and standard deviation 500014\tfrac{5000}{\sqrt{14}}, so p=Pr⁡(Xˉ≥63 500)≈0.0044p = \Pr\left(\bar X \ge 63\,500\right) \approx 0.0044.
iii. [1 mark]
p≈0.0044<0.01p \approx 0.0044 < 0.01, so reject H0H_0: there is evidence, at the 1% level of significance, that the campaign increased mean daily sales.
d. [1 mark]
The critical value is 60 000+2.3263×500014≈63 108.760\,000 + 2.3263 \times \tfrac{5000}{\sqrt{14}} \approx 63\,108.7, so H0H_0 is rejected when the mean daily sales is at least 63 109.
e. [2 marks]
At the 5% level the critical value is 60 000+1.6449×500014≈62 198.0360\,000 + 1.6449 \times \tfrac{5000}{\sqrt{14}} \approx 62\,198.03. The null hypothesis is incorrectly accepted (a type II error) when Xˉ<62 198.03\bar X < 62\,198.03 even though μ=63 000\mu = 63\,000:

Pr⁡(Xˉ<62 198.03∣μ=63 000)≈0.274.\Pr\left(\bar X < 62\,198.03 \mid \mu = 63\,000\right) \approx 0.274.

From the report. Part a was poorly done (14% full marks): successful students tried values of nn or solved using a standardised value, while a common error was to treat it as a sample-mean problem with standard deviation 8n\tfrac{8}{\sqrt n}. In part b (24% full marks) some confused adding four independent times with multiplying one time by 4, which gives the wrong variance. Parts c.i (75%) and c.ii (70%) were well answered; in c.iii (55%) some stated a conclusion without referring to the pp value. In part d (16% correct) some found 63 108.7 but did not give the answer as a range of values. Part e was answered correctly by only 9%, though most who found the critical value 62 198.03 went on to get the probability.

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