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VICSpecialist Mathematics2021Exam 1

VCE Specialist Mathematics 2021 Exam 1

Worked solutions to every question in the 2021 VCE Specialist Mathematics Examination 1 (40 marks, no calculator), checked against the VCAA external assessment report, with the common errors the report flagged and notes on what has changed in the current study design.

Marks
40
Time
60 min
Authority
VCAA
Updated

Every question from the 2021 VCE Specialist Mathematics Examination 1, the technology-free paper, with a full worked solution. Solutions sit behind a Show worked solution toggle so you can attempt each question first. For the calculator paper, see the 2021 Examination 2 walkthrough.

How to use this page

  • Questions are from the 2021 VCE Specialist Mathematics Examination 1, copyright Victorian Curriculum and Assessment Authority (VCAA). Each question is summarised in a line here; open the official examination PDF for the exact wording and diagrams.
  • Solutions are original ExamExplained working, checked line by line and compared with the 2021 Specialist Mathematics Examination 1 external assessment report (Word document). Both files are listed on the VCAA Specialist Mathematics examinations page.
  • The From the report note under each solution summarises what the assessors said about that question.
  • Study design. This paper was set on the previous Specialist Mathematics study design (2016 to 2022); the current one began in 2023. Almost all of the paper is still on the course. The exceptions, flagged where they appear, are in Question 1: part c uses momentum, which is not in the current study design, and part a uses Newton's second law, while 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. Everything else, including Question 1b, is still examinable.

Structure and timing

Examination 1 is 40 marks in 60 minutes (plus 15 minutes reading time), with no calculator or notes; a formula sheet is provided. In 2021 it had 9 questions worth 3 to 8 marks each. Answers must be exact unless a question says otherwise, and working must be shown for any question worth more than 1 mark.

According to the report, among the best-answered parts were 1a, 3a, 8a and 9a.i, while comparatively few students gained full marks on 7b, 8b and both parts of 9c. Integration (Questions 2, 4 and 7a), implicit differentiation (Question 5), linear dependence of vectors (Question 6) and parametric equations (Questions 9a.i and 9b.i) were strengths. Weaknesses were poor setting out, basic arithmetic and algebra errors, and hypothesis testing and confidence intervals. The report also reminded students to give answers in the form asked (4b), to answer the whole question (7b), and to show every step in a show-that question, especially one worth only 1 mark.

Questions and worked solutions

Question 1 (4 marks)

The net force on a body of mass 10 kg is F=5i+12j\mathbf F = 5\mathbf i + 12\mathbf j newtons.

a
Find the acceleration of the body in m s−2^{-2}. (1 mark)
b
The initial velocity of the body is −3j-3\mathbf j m s−1^{-1}. Find its velocity at any time tt seconds. (2 marks)
c
Find the momentum of the body, in kg m s−1^{-1}, when t=2t = 2 seconds. (1 mark)

Study design: part c is outside the current course, which does not include momentum. Part a, which uses Newton's second law, is 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, and the formula sheet no longer lists the Mechanics formulas (momentum and the equation of motion) that it gave in 2021. Part b, antidifferentiating the acceleration vector, is on the current course.

Show worked solution

a. [1 mark]. Newton's second law, F=ma\mathbf F = m\mathbf a:

a=Fm=5i+12j10=12i+65j m s−2.\mathbf a = \frac{\mathbf F}{m} = \frac{5\mathbf i + 12\mathbf j}{10} = \frac12\mathbf i + \frac65\mathbf j \text{ m s}^{-2}.

b. [2 marks]. The acceleration is constant, so antidifferentiate with respect to tt:

v(t)=t2i+6t5j+c.\mathbf v(t) = \frac{t}{2}\mathbf i + \frac{6t}{5}\mathbf j + \mathbf c.

v(0)=−3j\mathbf v(0) = -3\mathbf j gives c=−3j\mathbf c = -3\mathbf j, so

v(t)=t2i+(6t5−3)j m s−1.\mathbf v(t) = \frac{t}{2}\mathbf i + \left(\frac{6t}{5} - 3\right)\mathbf j \text{ m s}^{-1}.

(This is v=u+at\mathbf v = \mathbf u + \mathbf a t for constant acceleration.)

c. [1 mark]. v(2)=i+(125−3)j=i−35j\mathbf v(2) = \mathbf i + \left(\tfrac{12}{5} - 3\right)\mathbf j = \mathbf i - \tfrac35\mathbf j, so the momentum is

p=mv(2)=10(i−35j)=10i−6j kg m s−1.\mathbf p = m\mathbf v(2) = 10\left(\mathbf i - \frac35\mathbf j\right) = 10\mathbf i - 6\mathbf j \text{ kg m s}^{-1}.

From the report. Part a was answered well (80% correct), though some gave the magnitude of the acceleration instead of the vector. In part b (66% full marks) most made progress by integrating or with a constant acceleration formula; a common slip was wrongly combining the j\mathbf j terms into −95t j-\tfrac95t\,\mathbf j. In part c (58% correct) there were arithmetic errors, and some students gave the momentum's magnitude instead of the vector.

Question 2 (3 marks)

Evaluate ∫012x+1x2+1 dx\displaystyle\int_0^1\frac{2x + 1}{x^2 + 1}\,dx. (3 marks)

Show worked solution

[3 marks]. Split the integrand into two fractions:

∫012x+1x2+1 dx=∫012xx2+1 dx+∫011x2+1 dx.\int_0^1\frac{2x + 1}{x^2 + 1}\,dx = \int_0^1\frac{2x}{x^2 + 1}\,dx + \int_0^1\frac{1}{x^2 + 1}\,dx.

In the first, the numerator is the derivative of the denominator; the second is the derivative of arctan⁡(x)\arctan(x):

=[log⁡e(x2+1)+arctan⁡(x)]01=log⁡e(2)+π4−(0+0)=log⁡e(2)+π4.= \Big[\log_e\left(x^2 + 1\right) + \arctan(x)\Big]_0^1 = \log_e(2) + \frac{\pi}{4} - (0 + 0) = \log_e(2) + \frac{\pi}{4}.

From the report. Well answered (63% full marks). Most students saw that the integrand splits into the sum of two rational functions. A substitution was unnecessary, and students who tried one sometimes introduced errors.

Question 3 (5 marks)

A company claims the lifetimes of its Shiny light globes are normally distributed with mean 200 weeks, and the standard deviation is known to be 10 weeks. After complaints that the globes last less than 200 weeks, a random sample of 36 globes has mean lifetime 195 weeks. Use Pr⁡(−1.96<Z<1.96)=0.95\Pr(-1.96 < Z < 1.96) = 0.95 and Pr⁡(−3<Z<3)=0.9973\Pr(-3 < Z < 3) = 0.9973.

a
Write down the null and alternative hypotheses for the one-tailed test used to investigate the complaints. (1 mark)
b. i
Find the pp value for the test, correct to three decimal places. (2 marks)
ii
What should the company be told if the test is carried out at the 1% level of significance? (1 mark)
c
A random sample of 25 of a new globe, Globeplus, has mean lifetime 250 weeks. Assuming the population standard deviation is 10 weeks, find an approximate 95% confidence interval for the mean lifetime of Globeplus globes, correct to two decimal places. (1 mark)
Show worked solution

a. [1 mark]. Let μ\mu be the mean lifetime of Shiny globes in weeks. The complaints are that globes last less than claimed, so

H0:μ=200,H1:μ<200.H_0: \mu = 200, \qquad H_1: \mu < 200.

b. i. [2 marks]. Under H0H_0, Xˉ\bar X is normal with mean 200 and standard deviation 1036=53\tfrac{10}{\sqrt{36}} = \tfrac53. So

p=Pr⁡(Xˉ<195∣μ=200)=Pr⁡(Z<195−2005/3)=Pr⁡(Z<−3).p = \Pr\left(\bar X < 195 \mid \mu = 200\right) = \Pr\left(Z < \frac{195 - 200}{5/3}\right) = \Pr(Z < -3).

By symmetry, Pr⁡(Z<−3)=1−0.99732=0.00135\Pr(Z < -3) = \dfrac{1 - 0.9973}{2} = 0.00135, so p=0.001p = 0.001 correct to three decimal places.

ii. [1 mark]. p=0.001<0.01p = 0.001 < 0.01, so reject H0H_0. The company should be told there is evidence, at the 1% level of significance, that the mean lifetime of Shiny globes is less than 200 weeks: the complaints are supported.

c. [1 mark]. Here σn=1025=2\tfrac{\sigma}{\sqrt n} = \tfrac{10}{\sqrt{25}} = 2, so the interval is

(250−1.96×2, 250+1.96×2)=(246.08,253.92).\left(250 - 1.96 \times 2,\ 250 + 1.96 \times 2\right) = (246.08, 253.92).

From the report. Part a was well answered (72%); errors were an alternative hypothesis with the wrong inequality (μ>200\mu > 200 or μ≠200\mu \ne 200) and non-standard notation. In b.i (41% full marks, 47% scored zero) students had to use the given Pr⁡(−3<Z<3)=0.9973\Pr(-3 < Z < 3) = 0.9973 to find Pr⁡(Z<−3)=0.00135\Pr(Z < -3) = 0.00135. In b.ii (49% correct) some drew the wrong conclusion, sometimes because they confused the pp value (0.001) with the significance level (0.01). In part c (56% correct) many used μ=200\mu = 200 instead of the sample mean 250, and there were also arithmetic errors and uses of z=2z = 2 instead of the given 1.96.

Question 4 (4 marks)

a. The region between y=sin⁡(x)y = \sin(x) and the xx-axis over [0,π][0, \pi] (between the first two non-negative xx-intercepts) is rotated about the xx-axis. Find the volume, VsV_s, of the solid formed. (3 marks)

b. The region between y=sin⁡(kx)y = \sin(kx), where k>0k > 0, and the xx-axis between its first two non-negative xx-intercepts is rotated about the xx-axis. Find the volume of this solid in terms of VsV_s. (1 mark)

Show worked solution

a. [3 marks]. Use V=π∫y2 dxV = \pi\displaystyle\int y^2\,dx with the double angle identity sin⁡2(x)=12(1−cos⁡(2x))\sin^2(x) = \tfrac12\big(1 - \cos(2x)\big):

Vs=π∫0πsin⁡2(x) dx=π2∫0π(1−cos⁡(2x)) dx=π2[x−12sin⁡(2x)]0π=π2×π=π22.V_s = \pi\int_0^\pi\sin^2(x)\,dx = \frac{\pi}{2}\int_0^\pi\big(1 - \cos(2x)\big)\,dx = \frac{\pi}{2}\left[x - \frac12\sin(2x)\right]_0^\pi = \frac{\pi}{2} \times \pi = \frac{\pi^2}{2}.

b. [1 mark]. The graph of y=sin⁡(kx)y = \sin(kx) is the graph of y=sin⁡(x)y = \sin(x) dilated by a factor of 1k\tfrac1k from the yy-axis. Its first two non-negative xx-intercepts are 00 and πk\tfrac{\pi}{k}, and the solid is the part a solid scaled by 1k\tfrac1k along the xx-axis, with the same circular cross-sections. So its volume is

1kVs.\frac{1}{k}V_s.

Check by integration: π∫0π/ksin⁡2(kx) dx=π×π2k=π22k=1kVs\pi\displaystyle\int_0^{\pi/k}\sin^2(kx)\,dx = \pi \times \frac{\pi}{2k} = \frac{\pi^2}{2k} = \frac1k V_s.

From the report. In part a (58% full marks) most wrote a correct integral for the volume, but some could not go further and incorrect attempts at integration were common; the double angle formula was the most effective method. Part b was poorly answered (30% correct): very few saw that the part b graph and solid are those of part a dilated by a factor of 1k\tfrac1k, and many of those who did still did not write the answer in terms of VsV_s as instructed.

Question 5 (3 marks)

Find the gradient of the curve exe2y+e4y2=2e4e^xe^{2y} + e^{4y^2} = 2e^4 at the point (2,1)(2, 1). (3 marks)

Show worked solution

[3 marks]. Write exe2y=ex+2ye^xe^{2y} = e^{x + 2y} and differentiate implicitly with respect to xx. The right side is a constant, so its derivative is 0:

ex+2y(1+2dydx)+8ye4y2dydx=0.e^{x + 2y}\left(1 + 2\frac{dy}{dx}\right) + 8ye^{4y^2}\frac{dy}{dx} = 0.

Substitute the point straight away. At (2,1)(2, 1), ex+2y=e4e^{x + 2y} = e^4 and e4y2=e4e^{4y^2} = e^4, so

e4(1+2dydx)+8e4dydx=0  ⟹  1+10dydx=0  ⟹  dydx=−110.e^4\left(1 + 2\frac{dy}{dx}\right) + 8e^4\frac{dy}{dx} = 0 \implies 1 + 10\frac{dy}{dx} = 0 \implies \frac{dy}{dx} = -\frac{1}{10}.

(The point is on the curve: e2e2+e4=2e4e^2e^2 + e^4 = 2e^4.)

From the report. Answered well (53% full marks). Common errors were not differentiating the constant 2e42e^4 to zero and substituting x=2x = 2, y=1y = 1 incorrectly. When dydx\tfrac{dy}{dx} is not needed in terms of xx and yy, it can be easier to substitute the values of xx and yy straight after differentiating.

Question 6 (4 marks)

For a=−i+6j−3k\mathbf a = -\mathbf i + 6\mathbf j - 3\mathbf k, b=2i−8j+5k\mathbf b = 2\mathbf i - 8\mathbf j + 5\mathbf k and c=3i+2j+∣1−p2∣k\mathbf c = 3\mathbf i + 2\mathbf j + \left|1 - p^2\right|\mathbf k, where pp is a real constant, find the values of pp for which the three vectors are linearly independent. (4 marks)

Show worked solution

[4 marks]. First find when the vectors are linearly dependent. Since a\mathbf a and b\mathbf b are not parallel, the set is dependent exactly when c=αa+βb\mathbf c = \alpha\mathbf a + \beta\mathbf b for some real α\alpha and β\beta:

  • i\mathbf i: −α+2β=3-\alpha + 2\beta = 3
  • j\mathbf j: 6α−8β=26\alpha - 8\beta = 2
  • k\mathbf k: −3α+5β=∣1−p2∣-3\alpha + 5\beta = \left|1 - p^2\right|

From the first equation α=2β−3\alpha = 2\beta - 3; substituting into the second gives 12β−18−8β=212\beta - 18 - 8\beta = 2, so β=5\beta = 5 and α=7\alpha = 7. The third equation then needs

∣1−p2∣=−21+25=4  ⟹  1−p2=4  or  1−p2=−4.\left|1 - p^2\right| = -21 + 25 = 4 \implies 1 - p^2 = 4 \ \text{ or } \ 1 - p^2 = -4.

The first gives p2=−3p^2 = -3 (no real solution) and the second gives p2=5p^2 = 5, so the vectors are dependent only when p=±5p = \pm\sqrt5. They are linearly independent for

p∈R∖{−5,5}.p \in R \setminus \left\{-\sqrt5, \sqrt5\right\}.

Equivalently, a⋅(b×c)=16−4∣1−p2∣\mathbf a \cdot (\mathbf b \times \mathbf c) = 16 - 4\left|1 - p^2\right|, which is zero exactly when ∣1−p2∣=4\left|1 - p^2\right| = 4.

From the report. Most students realised they had to set up and solve a system of linear equations to find when the vectors are dependent (average 2.5 out of 4; 26% full marks). Many found p=±5p = \pm\sqrt5 for dependence but did not go on to conclude p∈R∖{−5,5}p \in R \setminus \left\{-\sqrt5, \sqrt5\right\} (or equivalent) for independence.

Question 7 (5 marks)

A particle's displacement xx cm from a fixed point OO at time tt seconds satisfies dxdt=xsin⁡(t)\dfrac{dx}{dt} = x\sin(t). Initially the displacement is 1 cm.

a. Find an expression for xx in terms of tt. (3 marks)

b. Find the maximum displacement of the particle and the times at which this occurs. (2 marks)

Show worked solution

a. [3 marks]. Separate the variables:

∫1x dx=∫sin⁡(t) dt  ⟹  log⁡e∣x∣=−cos⁡(t)+c.\int\frac{1}{x}\,dx = \int\sin(t)\,dt \implies \log_e|x| = -\cos(t) + c.

At t=0t = 0, x=1x = 1: 0=−1+c0 = -1 + c, so c=1c = 1. Since x=1>0x = 1 > 0 initially, log⁡e(x)=1−cos⁡(t)\log_e(x) = 1 - \cos(t) and

x=e1−cos⁡(t).x = e^{1 - \cos(t)}.

b. [2 marks]. e1−cos⁡(t)e^{1 - \cos(t)} is largest when cos⁡(t)\cos(t) is smallest, that is when cos⁡(t)=−1\cos(t) = -1. The maximum displacement is e1−(−1)=e2e^{1 - (-1)} = e^2 cm, and it occurs when

t=(2k+1)π,k∈N∪{0},t = (2k + 1)\pi, \quad k \in N \cup \{0\},

that is at t=π,3π,5π,…t = \pi, 3\pi, 5\pi, \ldots seconds.

From the report. Part a was well answered (66% full marks); most separated the variables correctly, though there were sign errors when integrating the trigonometric function. Part b was poorly answered (8% full marks, 58% scored zero): the maximum could be found by inspection, but most students did not attempt, or could not give, the correct times at which it occurs.

Question 8 (4 marks)

a. Solve z2+2z+2=0z^2 + 2z + 2 = 0 for z∈Cz \in C. (1 mark)

b. Solve z2+2zˉ+2=0z^2 + 2\bar z + 2 = 0 for z∈Cz \in C. (3 marks)

Show worked solution

a. [1 mark]. Complete the square: (z+1)2+1=0(z + 1)^2 + 1 = 0, so (z+1)2=−1=i2(z + 1)^2 = -1 = i^2 and

z=−1±i.z = -1 \pm i.

b. [3 marks]. The equation involves zˉ\bar z, so it is not a polynomial equation in zz: the quadratic formula does not apply, and the solutions to part a do not carry over. Let z=x+iyz = x + iy with x,y∈Rx, y \in R, so zˉ=x−iy\bar z = x - iy:

x2−y2+2xyi+2(x−iy)+2=0.x^2 - y^2 + 2xyi + 2(x - iy) + 2 = 0.

Equate real and imaginary parts:

  • Real: x2−y2+2x+2=0x^2 - y^2 + 2x + 2 = 0
  • Imaginary: 2xy−2y=02xy - 2y = 0, so 2y(x−1)=02y(x - 1) = 0 and y=0y = 0 or x=1x = 1.

If y=0y = 0, then x2+2x+2=0x^2 + 2x + 2 = 0, which has no real solutions (its discriminant is 4−8<04 - 8 < 0). If x=1x = 1, then 1−y2+2+2=01 - y^2 + 2 + 2 = 0, so y2=5y^2 = 5 and y=±5y = \pm\sqrt5. Hence

z=1+5 iorz=1−5 i.z = 1 + \sqrt5\,i \quad\text{or}\quad z = 1 - \sqrt5\,i.

Check: (1+5 i)2=−4+25 i\left(1 + \sqrt5\,i\right)^2 = -4 + 2\sqrt5\,i and 2zˉ=2−25 i2\bar z = 2 - 2\sqrt5\,i, and −4+25 i+2−25 i+2=0-4 + 2\sqrt5\,i + 2 - 2\sqrt5\,i + 2 = 0.

From the report. Part a was answered well (70%); completing the square or the quadratic formula both work. Part b was not (10% full marks, 50% scored zero). Successful students let z=x+iyz = x + iy and equated real and imaginary parts, but algebraic errors were common in solving the resulting equations. Some assumed the solutions to part a also solved part b, and some confused the conjugate with the reciprocal. Starting from the polar form z=r cis(θ)z = r\,\text{cis}(\theta) is possible, but few took that approach and those who did rarely made significant progress.

Question 9 (8 marks)

Particles AA and BB have position vectors r(t)=(−1+4cos⁡(t))i+23sin⁡(t) j\mathbf r(t) = \big(-1 + 4\cos(t)\big)\mathbf i + \dfrac{2}{\sqrt3}\sin(t)\,\mathbf j and s(t)=(3sec⁡(t)−1)i+tan⁡(t) j\mathbf s(t) = \big(3\sec(t) - 1\big)\mathbf i + \tan(t)\,\mathbf j respectively, for 0≤t≤c0 \le t \le c, where cc is a positive real constant.

a. i
Show that the Cartesian equation of the path of AA is (x+1)216+3y24=1\dfrac{(x + 1)^2}{16} + \dfrac{3y^2}{4} = 1. (1 mark)
ii
Show that the path of AA in the first quadrant can be written as y=36−x2−2x+15y = \dfrac{\sqrt3}{6}\sqrt{-x^2 - 2x + 15}. (1 mark)
b. i
Show that the particles collide. (1 mark)
ii
Hence find the coordinates of the point of collision. (1 mark)
c. i
Show that ddx(8arcsin⁡(x+14)+(x+1)−x2−2x+152)=−x2−2x+15\dfrac{d}{dx}\left(8\arcsin\left(\dfrac{x + 1}{4}\right) + \dfrac{(x + 1)\sqrt{-x^2 - 2x + 15}}{2}\right) = \sqrt{-x^2 - 2x + 15}. (2 marks)
ii
Hence find the area bounded by y=36−x2−2x+15y = \dfrac{\sqrt3}{6}\sqrt{-x^2 - 2x + 15}, the xx-axis and the lines x=1x = 1 and x=23−1x = 2\sqrt3 - 1 (shaded in a diagram), in the form a3πb\dfrac{a\sqrt3\pi}{b}, where aa and bb are positive integers. (2 marks)
Show worked solution

a. i. [1 mark]. From x=−1+4cos⁡(t)x = -1 + 4\cos(t) and y=23sin⁡(t)y = \tfrac{2}{\sqrt3}\sin(t), cos⁡(t)=x+14\cos(t) = \tfrac{x + 1}{4} and sin⁡(t)=3y2\sin(t) = \tfrac{\sqrt3y}{2}. Since cos⁡2(t)+sin⁡2(t)=1\cos^2(t) + \sin^2(t) = 1:

(x+14)2+(3y2)2=1  ⟹  (x+1)216+3y24=1.\left(\frac{x + 1}{4}\right)^2 + \left(\frac{\sqrt3y}{2}\right)^2 = 1 \implies \frac{(x + 1)^2}{16} + \frac{3y^2}{4} = 1.

ii. [1 mark]. Multiply by 16: (x+1)2+12y2=16(x + 1)^2 + 12y^2 = 16, so

12y2=16−(x2+2x+1)=−x2−2x+15  ⟹  y2=−x2−2x+1512.12y^2 = 16 - \left(x^2 + 2x + 1\right) = -x^2 - 2x + 15 \implies y^2 = \frac{-x^2 - 2x + 15}{12}.

In the first quadrant y≥0y \ge 0, so take the positive square root:

y=−x2−2x+1512=−x2−2x+1523=36−x2−2x+15.y = \frac{\sqrt{-x^2 - 2x + 15}}{\sqrt{12}} = \frac{\sqrt{-x^2 - 2x + 15}}{2\sqrt3} = \frac{\sqrt3}{6}\sqrt{-x^2 - 2x + 15}.

b. i. [1 mark]. The particles collide if they are at the same point at the same time. Equate the i\mathbf i components:

−1+4cos⁡(t)=3sec⁡(t)−1  ⟹  4cos⁡2(t)=3  ⟹  cos⁡2(t)=34.-1 + 4\cos(t) = 3\sec(t) - 1 \implies 4\cos^2(t) = 3 \implies \cos^2(t) = \frac34.

s(t)\mathbf s(t) is only defined where sec⁡(t)\sec(t) is, so on 0≤t≤c0 \le t \le c we have t<π2t < \tfrac{\pi}{2} and cos⁡(t)>0\cos(t) > 0. So cos⁡(t)=32\cos(t) = \tfrac{\sqrt3}{2} and t=π6t = \tfrac{\pi}{6}. Check the j\mathbf j components at t=π6t = \tfrac{\pi}{6}:

23sin⁡(π6)=13=tan⁡(π6).\frac{2}{\sqrt3}\sin\left(\frac{\pi}{6}\right) = \frac{1}{\sqrt3} = \tan\left(\frac{\pi}{6}\right).

Both components agree at the same time, t=π6t = \tfrac{\pi}{6}, so the particles collide.

ii. [1 mark]. At t=π6t = \tfrac{\pi}{6}, x=−1+4×32=23−1x = -1 + 4 \times \tfrac{\sqrt3}{2} = 2\sqrt3 - 1 and y=13y = \tfrac{1}{\sqrt3}. The point of collision is

(23−1,13).\left(2\sqrt3 - 1, \frac{1}{\sqrt3}\right).

c. i. [2 marks]. Let Q=−x2−2x+15Q = -x^2 - 2x + 15 and note that 16−(x+1)2=Q16 - (x + 1)^2 = Q. By the chain rule,

ddx(8arcsin⁡(x+14))=8×14×11−(x+14)2=816−(x+1)2=8Q.\frac{d}{dx}\left(8\arcsin\left(\frac{x + 1}{4}\right)\right) = 8 \times \frac14 \times \frac{1}{\sqrt{1 - \left(\frac{x + 1}{4}\right)^2}} = \frac{8}{\sqrt{16 - (x + 1)^2}} = \frac{8}{\sqrt Q}.

By the product rule, with ddxQ=−2x−22Q=−x+1Q\dfrac{d}{dx}\sqrt Q = \dfrac{-2x - 2}{2\sqrt Q} = -\dfrac{x + 1}{\sqrt Q},

ddx((x+1)Q2)=Q2−(x+1)22Q.\frac{d}{dx}\left(\frac{(x + 1)\sqrt Q}{2}\right) = \frac{\sqrt Q}{2} - \frac{(x + 1)^2}{2\sqrt Q}.

Add the two, using (x+1)2=16−Q(x + 1)^2 = 16 - Q:

8Q+Q2−16−Q2Q=16+Q−16+Q2Q=2Q2Q=Q=−x2−2x+15.\frac{8}{\sqrt Q} + \frac{\sqrt Q}{2} - \frac{16 - Q}{2\sqrt Q} = \frac{16 + Q - 16 + Q}{2\sqrt Q} = \frac{2Q}{2\sqrt Q} = \sqrt Q = \sqrt{-x^2 - 2x + 15}.

ii. [2 marks]. By part c.i, 8arcsin⁡(x+14)+(x+1)−x2−2x+1528\arcsin\left(\tfrac{x + 1}{4}\right) + \tfrac{(x + 1)\sqrt{-x^2 - 2x + 15}}{2} is an antiderivative of −x2−2x+15\sqrt{-x^2 - 2x + 15}, so

A=36[8arcsin⁡(x+14)+(x+1)−x2−2x+152]123−1.A = \frac{\sqrt3}{6}\left[8\arcsin\left(\frac{x + 1}{4}\right) + \frac{(x + 1)\sqrt{-x^2 - 2x + 15}}{2}\right]_1^{2\sqrt3 - 1}.

  • At x=23−1x = 2\sqrt3 - 1: x+14=32\tfrac{x + 1}{4} = \tfrac{\sqrt3}{2} and −x2−2x+15=16−(x+1)2=16−12=4-x^2 - 2x + 15 = 16 - (x + 1)^2 = 16 - 12 = 4, giving 8×π3+23×22=8π3+238 \times \tfrac{\pi}{3} + \tfrac{2\sqrt3 \times 2}{2} = \tfrac{8\pi}{3} + 2\sqrt3.
  • At x=1x = 1: x+14=12\tfrac{x + 1}{4} = \tfrac12 and −x2−2x+15=12-x^2 - 2x + 15 = 12, giving 8×π6+2×232=4π3+238 \times \tfrac{\pi}{6} + \tfrac{2 \times 2\sqrt3}{2} = \tfrac{4\pi}{3} + 2\sqrt3.

The 232\sqrt3 terms cancel:

A=36(8π3−4π3)=36×4π3=23π9.A = \frac{\sqrt3}{6}\left(\frac{8\pi}{3} - \frac{4\pi}{3}\right) = \frac{\sqrt3}{6} \times \frac{4\pi}{3} = \frac{2\sqrt3\pi}{9}.

So a=2a = 2 and b=9b = 9.

From the report. Part a.i was very well answered (83%), using sin⁡2(θ)+cos⁡2(θ)=1\sin^2(\theta) + \cos^2(\theta) = 1. In a.ii (41% correct) a common error was not justifying the choice of the positive square root (y≥0y \ge 0 in the first quadrant). Part b.i (62%) was answered well by showing that both components agree when cos⁡(t)=32\cos(t) = \tfrac{\sqrt3}{2}; in b.ii (52%) some gave the point as (π6,13)\left(\tfrac{\pi}{6}, \tfrac{1}{\sqrt3}\right), confusing the parameter tt with the xx-coordinate. Few students scored full marks on either part of c (15% and 22%). In c.i the product and chain rules had to be applied and the result simplified with every step shown, since it is a show-that question; many missed steps or made algebraic errors. In c.ii most realised part c.i should be used, but many could not finish the arithmetic.

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