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VICSpecialist Mathematics2022Exam 1

VCE Specialist Mathematics 2022 Exam 1

Worked solutions to every question in the 2022 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 2022 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 2022 Examination 2 walkthrough.

How to use this page

  • Questions are from the 2022 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 2022 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.
  • Redacted part. VCAA has redacted Question 3b from the published paper and report, following the Independent Review into its examination-setting policies, processes and procedures. It is not covered here.
  • Study design. This was the last Examination 1 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 exception, flagged where it appears, is Question 5, which resolves forces on an inclined plane and uses 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. Everything else, including the kinematics in Question 8, 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 2022 it had 10 questions worth 3 to 6 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 highest-scoring questions were 1, 2, 5a and 6a, while comparatively few students gained full marks on 3a, 4, 7, 9 and 10a. There were no show-that questions, but 1a, 7 and 10b asked for the answer in a given form, which both guides the working and confirms the result. Integration (Questions 2, 4, 8, 9 and 10b), basic vectors (Question 6) and kinematics and mechanics (Questions 5 and 8) were strengths. Weaknesses were the probability in 3a, poor handling of the integrand in Question 4, and, in Question 7, expanding cos⁡(x+y)\cos(x + y) with an identity before differentiating, which made the algebra much heavier. The report also noted that students who solved Questions 2 and 9 by setting up definite integrals needed a dummy variable of integration; most successful students used the usual indefinite-integral method.

Questions and worked solutions

Question 1 (3 marks)

Consider p(z)=z2+6iz−25p(z) = z^2 + 6iz - 25, z∈Cz \in C.

a. Express p(z)p(z) in the form (z+ai)2+b(z + ai)^2 + b, where a,b∈Ra, b \in R. (1 mark)

b. Hence, or otherwise, solve p(z)=0p(z) = 0. (2 marks)

Show worked solution

a. [1 mark]. Complete the square. Half the coefficient of zz is 3i3i, and (3i)2=−9(3i)^2 = -9:

p(z)=(z+3i)2−(3i)2−25=(z+3i)2+9−25=(z+3i)2−16.p(z) = (z + 3i)^2 - (3i)^2 - 25 = (z + 3i)^2 + 9 - 25 = (z + 3i)^2 - 16.

So a=3a = 3 and b=−16b = -16.

b. [2 marks]. From part a, p(z)=0p(z) = 0 when (z+3i)2=16(z + 3i)^2 = 16, so z+3i=±4z + 3i = \pm 4 and

z=4−3iorz=−4−3i.z = 4 - 3i \quad\text{or}\quad z = -4 - 3i.

The quadratic formula gives the same result: z=−6i±(6i)2+1002=−6i±642=−3i±4z = \dfrac{-6i \pm \sqrt{(6i)^2 + 100}}{2} = \dfrac{-6i \pm \sqrt{64}}{2} = -3i \pm 4.

From the report. Part a was answered well (79% correct): most students saw that completing the square was needed, though there were some arithmetic slips. In part b (70% full marks) students could use part a, as above, or the quadratic formula.

Question 2 (3 marks)

Solve the differential equation dydx=−x4−y2\dfrac{dy}{dx} = -x\sqrt{4 - y^2}, given that y(2)=0y(2) = 0. Give your answer in the form y=f(x)y = f(x). (3 marks)

Show worked solution

[3 marks]. The equation is separable:

∫14−y2 dy=∫−x dx  ⟹  arcsin⁡(y2)=−x22+c.\int\frac{1}{\sqrt{4 - y^2}}\,dy = \int -x\,dx \implies \arcsin\left(\frac{y}{2}\right) = -\frac{x^2}{2} + c.

At x=2x = 2, y=0y = 0: arcsin⁡(0)=0=−2+c\arcsin(0) = 0 = -2 + c, so c=2c = 2. Taking the sine of both sides,

y2=sin⁡(2−x22)  ⟹  y=2sin⁡(2−x22).\frac{y}{2} = \sin\left(2 - \frac{x^2}{2}\right) \implies y = 2\sin\left(2 - \frac{x^2}{2}\right).

(The step from arcsin⁡\arcsin to sin⁡\sin holds while 2−x222 - \tfrac{x^2}{2} stays between −π2-\tfrac{\pi}{2} and π2\tfrac{\pi}{2}, which includes the initial point x=2x = 2.)

From the report. Well answered (60% full marks): most students recognised the separable differential equation and tried to solve it. A few worked correctly through to an inverse cosine version of the solution, which gives the equivalent form y=2cos⁡(x22+π2−2)y = 2\cos\left(\tfrac{x^2}{2} + \tfrac{\pi}{2} - 2\right).

Question 3 (4 marks)

The time a coffee machine takes to dispense a cup of coffee is normally distributed with mean 10 seconds and standard deviation 1.5 seconds.

a. Find the probability that more than 34 seconds is needed to dispense a total of four cups of coffee, correct to two decimal places. (2 marks)

b. Redacted by VCAA (see above).

Show worked solution

a. [2 marks]. Let T=X1+X2+X3+X4T = X_1 + X_2 + X_3 + X_4 be the total time for four cups, where the XiX_i are independent, each normal with mean 10 and variance 1.52=2.251.5^2 = 2.25. Then TT is normal with

E⁡(T)=4×10=40,var⁡(T)=4×2.25=9,sd⁡(T)=3.\operatorname{E}(T) = 4 \times 10 = 40, \qquad \operatorname{var}(T) = 4 \times 2.25 = 9, \qquad \operatorname{sd}(T) = 3.

(This is a sum of four separate cups, not 4X4X for one cup, which would have variance 16×2.25=3616 \times 2.25 = 36.) So

Pr⁡(T>34)=Pr⁡(Z>34−403)=Pr⁡(Z>−2).\Pr(T > 34) = \Pr\left(Z > \frac{34 - 40}{3}\right) = \Pr(Z > -2).

About 95% of a normal distribution lies within 2 standard deviations of the mean, so Pr⁡(Z<−2)≈0.025\Pr(Z < -2) \approx 0.025 and

Pr⁡(Z>−2)≈1−0.025=0.975≈0.98.\Pr(Z > -2) \approx 1 - 0.025 = 0.975 \approx 0.98.

From the report. Only 31% scored full marks and 59% scored zero. Many students got the standard deviation of the total wrong, so could not reduce the problem to Pr⁡(Z>−2)\Pr(Z > -2); others reached Pr⁡(Z>−2)\Pr(Z > -2) but could not evaluate it. Students who got it right often sketched the normal curve and knew the approximate probabilities within 1, 2 and 3 standard deviations of the mean.

Question 4 (4 marks)

Find ∫3x2+4x+12x(x2+4) dx\displaystyle\int\frac{3x^2 + 4x + 12}{x\left(x^2 + 4\right)}\,dx. (4 marks)

Show worked solution

[4 marks]. Use partial fractions with a linear and an irreducible quadratic factor:

3x2+4x+12x(x2+4)=Ax+Bx+Cx2+4  ⟹  3x2+4x+12=A(x2+4)+(Bx+C)x.\frac{3x^2 + 4x + 12}{x\left(x^2 + 4\right)} = \frac{A}{x} + \frac{Bx + C}{x^2 + 4} \implies 3x^2 + 4x + 12 = A\left(x^2 + 4\right) + (Bx + C)x.

Putting x=0x = 0 gives 4A=124A = 12, so A=3A = 3. Comparing coefficients of x2x^2: A+B=3A + B = 3, so B=0B = 0; of xx: C=4C = 4. So

∫(3x+4x2+4)dx=3log⁡e∣x∣+2arctan⁡(x2)+c.\int\left(\frac{3}{x} + \frac{4}{x^2 + 4}\right)dx = 3\log_e|x| + 2\arctan\left(\frac{x}{2}\right) + c.

A shortcut avoids partial fractions: split the numerator as (3x2+12)+4x=3(x2+4)+4x\left(3x^2 + 12\right) + 4x = 3\left(x^2 + 4\right) + 4x, so the integrand is 3x+4x2+4\dfrac{3}{x} + \dfrac{4}{x^2 + 4} straight away.

From the report. 36% scored full marks. The shortcut above was spotted by only a small number of students. Many mixed some initial algebra with one or more rounds of partial fractions, which was inefficient and often much longer than needed. Some omitted the absolute value in the logarithm or the constant of integration, and a few integrated 4x2+4\tfrac{4}{x^2 + 4} incorrectly.

Question 5 (3 marks)

A body of mass 10 kg, initially at rest, slides down a smooth plane inclined at θ\theta to the horizontal, where tan⁡(θ)=13\tan(\theta) = \tfrac13 (diagram in the paper). Take g=9.8g = 9.8.

a. Find the speed of the body after it has been in motion for two seconds. (2 marks)

b. After two seconds, a constant braking force of RR newtons is applied parallel to the plane so that the body then moves with constant velocity. Find RR. (1 mark)

Study design: partly outside the current course. Resolving forces on an inclined plane and using Newton's second law are covered in the current study design 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 equation of motion that it gave in 2022. The constant acceleration step in part a is still on the course.

Show worked solution

a. [2 marks]. From tan⁡(θ)=13\tan(\theta) = \tfrac13, draw a right triangle with opposite side 1 and adjacent side 3; the hypotenuse is 10\sqrt{10}, so sin⁡(θ)=110\sin(\theta) = \dfrac{1}{\sqrt{10}}.

The plane is smooth, so the only force with a component along the plane is the weight, whose component down the plane is mgsin⁡(θ)mg\sin(\theta). By Newton's second law the acceleration down the plane is

a=gsin⁡(θ)=g10 m s−2.a = g\sin(\theta) = \frac{g}{\sqrt{10}} \text{ m s}^{-2}.

The acceleration is constant and u=0u = 0, so v=u+atv = u + at gives

v=0+g10×2=2g10=10 g5 m s−1 (≈6.2 m s−1).v = 0 + \frac{g}{\sqrt{10}} \times 2 = \frac{2g}{\sqrt{10}} = \frac{\sqrt{10}\,g}{5} \text{ m s}^{-1} \ (\approx 6.2 \text{ m s}^{-1}).

b. [1 mark]. Constant velocity means zero acceleration, so the net force along the plane is zero: mgsin⁡(θ)−R=0mg\sin(\theta) - R = 0 and

R=10g×110=10 g (≈31 newtons).R = 10g \times \frac{1}{\sqrt{10}} = \sqrt{10}\,g \ (\approx 31 \text{ newtons}).

From the report. Part a was answered well (55% full marks), with several equivalent forms of the answer accepted; successful students often marked the forces on the diagram before resolving them. In part b (48% correct) equivalent answers were also accepted.

Question 6 (6 marks)

a
Find the cosine of the acute angle between a=2i−3j+6k\mathbf a = 2\mathbf i - 3\mathbf j + 6\mathbf k and b=i+2j+2k\mathbf b = \mathbf i + 2\mathbf j + 2\mathbf k. (2 marks)
b
OPQOPQ is a semicircle of radius aa with equation y=a2−(x−a)2y = \sqrt{a^2 - (x - a)^2}, where OO is the origin and QQ is the other end of the diameter on the positive xx-axis. P(x,y)P(x, y) is a point on the semicircle.
i
Express OP→\overrightarrow{OP} and QP→\overrightarrow{QP} in terms of aa, xx, yy, i\mathbf i and j\mathbf j. (1 mark)
ii
Hence, using the scalar (dot) product, determine whether OP→\overrightarrow{OP} is perpendicular to QP→\overrightarrow{QP}. (3 marks)
Show worked solution

a. [2 marks]. a⋅b=2−6+12=8\mathbf a \cdot \mathbf b = 2 - 6 + 12 = 8, ∣a∣=4+9+36=7|\mathbf a| = \sqrt{4 + 9 + 36} = 7 and ∣b∣=1+4+4=3|\mathbf b| = \sqrt{1 + 4 + 4} = 3, so

cos⁡(θ)=a⋅b∣a∣∣b∣=87×3=821.\cos(\theta) = \frac{\mathbf a \cdot \mathbf b}{|\mathbf a||\mathbf b|} = \frac{8}{7 \times 3} = \frac{8}{21}.

The dot product is positive, so this angle is already acute.

b. i. [1 mark]. The semicircle has centre (a,0)(a, 0) and radius aa, so QQ is the point (2a,0)(2a, 0). Then

OP→=xi+yj,QP→=OP→−OQ→=(x−2a)i+yj,\overrightarrow{OP} = x\mathbf i + y\mathbf j, \qquad \overrightarrow{QP} = \overrightarrow{OP} - \overrightarrow{OQ} = (x - 2a)\mathbf i + y\mathbf j,

where y=a2−(x−a)2y = \sqrt{a^2 - (x - a)^2}.

ii. [3 marks]. Using y2=a2−(x−a)2y^2 = a^2 - (x - a)^2,

OP→⋅QP→=x(x−2a)+y2=x2−2ax+a2−(x2−2ax+a2)=0.\overrightarrow{OP} \cdot \overrightarrow{QP} = x(x - 2a) + y^2 = x^2 - 2ax + a^2 - \left(x^2 - 2ax + a^2\right) = 0.

The dot product is zero, so OP→\overrightarrow{OP} is perpendicular to QP→\overrightarrow{QP} for every point PP on the semicircle other than OO and QQ (where one of the vectors is zero). This is the vector proof that the angle in a semicircle is a right angle.

From the report. Part a was answered very well (76% full marks), mostly by the method above, with some arithmetic errors. Part b.i (61%) was answered well apart from occasional sign errors. In b.ii (47% full marks) students had to use the dot product; some made algebraic errors or drew the wrong conclusion.

Question 7 (3 marks)

A curve has equation xcos⁡(x+y)=π48x\cos(x + y) = \dfrac{\pi}{48}. Find the gradient of the curve at the point (π24,7π24)\left(\dfrac{\pi}{24}, \dfrac{7\pi}{24}\right), in the form ab−ππ\dfrac{a\sqrt b - \pi}{\pi}, where a,b∈Za, b \in Z. (3 marks)

Show worked solution

[3 marks]. Differentiate implicitly with respect to xx, using the product rule and then the chain rule on cos⁡(x+y)\cos(x + y). Keep cos⁡(x+y)\cos(x + y) as it is rather than expanding it:

cos⁡(x+y)−xsin⁡(x+y)(1+dydx)=0.\cos(x + y) - x\sin(x + y)\left(1 + \frac{dy}{dx}\right) = 0.

At the point, x+y=8π24=π3x + y = \tfrac{8\pi}{24} = \tfrac{\pi}{3}, so cos⁡(x+y)=12\cos(x + y) = \tfrac12 and sin⁡(x+y)=32\sin(x + y) = \tfrac{\sqrt3}{2}:

12−π24×32(1+dydx)=0  ⟹  1+dydx=243 π=83π.\frac12 - \frac{\pi}{24} \times \frac{\sqrt3}{2}\left(1 + \frac{dy}{dx}\right) = 0 \implies 1 + \frac{dy}{dx} = \frac{24}{\sqrt3\,\pi} = \frac{8\sqrt3}{\pi}.

So

dydx=83π−1=83−ππ,\frac{dy}{dx} = \frac{8\sqrt3}{\pi} - 1 = \frac{8\sqrt3 - \pi}{\pi},

with a=8a = 8 and b=3b = 3. (The point is on the curve: π24cos⁡(π3)=π48\tfrac{\pi}{24}\cos\left(\tfrac{\pi}{3}\right) = \tfrac{\pi}{48}.)

From the report. 34% scored full marks and 33% scored zero. Many students expanded cos⁡(x+y)\cos(x + y) with the compound angle formula before differentiating; few of them reached the right answer, as the number of terms became unmanageable.

Question 8 (4 marks)

A body moves in a straight line so that at displacement xx metres from a fixed origin OO its acceleration is −4x-4x m s−2^{-2}. It accelerates from rest, has velocity v=−2v = -2 m s−1^{-1} as it passes through the origin, and then comes to rest again. Find vv in terms of xx for this interval. (4 marks)

Show worked solution

[4 marks]. Acceleration is given in terms of xx, so write it as ddx(12v2)\dfrac{d}{dx}\left(\dfrac12v^2\right):

ddx(12v2)=−4x  ⟹  12v2=−2x2+c.\frac{d}{dx}\left(\frac12v^2\right) = -4x \implies \frac12v^2 = -2x^2 + c.

At x=0x = 0, v=−2v = -2: 12×4=c\tfrac12 \times 4 = c, so c=2c = 2. Then

v2=4−4x2=4(1−x2).v^2 = 4 - 4x^2 = 4\left(1 - x^2\right).

The body is at rest when v=0v = 0, that is at x=±1x = \pm1. It starts from rest at x=1x = 1, moves in the negative direction through the origin (where v=−2<0v = -2 < 0) and comes to rest at x=−1x = -1, so v≤0v \le 0 throughout. Take the negative square root:

v=−21−x2,−1≤x≤1.v = -2\sqrt{1 - x^2}, \quad -1 \le x \le 1.

From the report. 37% scored full marks. Many students used a suitable form of acceleration, either ddx(12v2)\tfrac{d}{dx}\left(\tfrac12v^2\right) or vdvdxv\tfrac{dv}{dx}. A common error was the wrong sign in the final answer: the negative root is needed because v=−2v = -2 at x=0x = 0.

Question 9 (4 marks)

Given that f′(x)=cos⁡(2x)sin⁡3(2x)f'(x) = \dfrac{\cos(2x)}{\sin^3(2x)} and f(π8)=34f\left(\dfrac{\pi}{8}\right) = \dfrac34, find f(x)f(x). (4 marks)

Show worked solution

[4 marks]. Substitute u=sin⁡(2x)u = \sin(2x), so dudx=2cos⁡(2x)\dfrac{du}{dx} = 2\cos(2x) and cos⁡(2x) dx=12 du\cos(2x)\,dx = \tfrac12\,du:

f(x)=∫cos⁡(2x)sin⁡3(2x) dx=12∫u−3 du=12×u−2−2+c=−14sin⁡2(2x)+c.f(x) = \int\frac{\cos(2x)}{\sin^3(2x)}\,dx = \frac12\int u^{-3}\,du = \frac12 \times \frac{u^{-2}}{-2} + c = -\frac{1}{4\sin^2(2x)} + c.

At x=π8x = \tfrac{\pi}{8}, sin⁡(2x)=sin⁡(π4)=12\sin(2x) = \sin\left(\tfrac{\pi}{4}\right) = \tfrac{1}{\sqrt2}, so sin⁡2(2x)=12\sin^2(2x) = \tfrac12 and

−14×12+c=34  ⟹  −12+c=34  ⟹  c=54.-\frac{1}{4 \times \frac12} + c = \frac34 \implies -\frac12 + c = \frac34 \implies c = \frac54.

Hence

f(x)=54−14sin⁡2(2x)=54−14cosec⁡2(2x).f(x) = \frac54 - \frac{1}{4\sin^2(2x)} = \frac54 - \frac14\operatorname{cosec}^2(2x).

From the report. 34% scored full marks and 32% scored zero; other correct forms were accepted. Some students tried to rewrite the integrand with trigonometric identities before integrating, usually without success. Among those who chose a suitable substitution, a frequent slip was antidifferentiating u−3u^{-3} as −2u−2-2u^{-2} or −2u−4-2u^{-4} instead of −12u−2-\tfrac12u^{-2}.

Question 10 (6 marks)

Let f(x)=sec⁡(4x)f(x) = \sec(4x).

a. Sketch the graph of ff for x∈[−π4,π4]x \in \left[-\dfrac{\pi}{4}, \dfrac{\pi}{4}\right] on the axes provided, labelling any asymptotes with their equations, and any turning points and the endpoints with their coordinates. (3 marks)

b. The graph of y=f(x)y = f(x) for x∈[−π24,π48]x \in \left[-\dfrac{\pi}{24}, \dfrac{\pi}{48}\right] is rotated about the xx-axis to form a solid of revolution. Find its volume in the form (a−b)πc\dfrac{\left(a - \sqrt b\right)\pi}{c}, where a,b,c∈Ra, b, c \in R. (3 marks)

Show worked solution

a. [3 marks]. sec⁡(4x)=1cos⁡(4x)\sec(4x) = \dfrac{1}{\cos(4x)}, whose period is 2π4=π2\dfrac{2\pi}{4} = \dfrac{\pi}{2}, so the interval covers exactly one period.

  • Asymptotes where cos⁡(4x)=0\cos(4x) = 0: 4x=±π24x = \pm\tfrac{\pi}{2}, so x=−π8x = -\tfrac{\pi}{8} and x=π8x = \tfrac{\pi}{8}.
  • Turning point where cos⁡(4x)=1\cos(4x) = 1: the local minimum (0,1)(0, 1).
  • Endpoints: cos⁡(±π)=−1\cos(\pm\pi) = -1, so (−π4,−1)\left(-\tfrac{\pi}{4}, -1\right) and (π4,−1)\left(\tfrac{\pi}{4}, -1\right), both included.

Between the asymptotes the graph is a U shape above y=1y = 1; outside them it lies on or below y=−1y = -1, falling from each endpoint towards −∞-\infty as it approaches the nearer asymptote. The graph is symmetric about the yy-axis and has no horizontal asymptote.

Graph of y = sec(4x) for x from -pi/4 to pi/4 Three branches with vertical asymptotes x = -pi/8 and x = pi/8. The middle branch is U-shaped, opening upwards, with a minimum turning point at (0, 1) and rising towards positive infinity near each asymptote. The left branch starts at the closed endpoint (-pi/4, -1) and falls towards negative infinity as x approaches -pi/8; the right branch rises from negative infinity just after x = pi/8 to the closed endpoint (pi/4, -1). x y -10 -5 5 10 x = -π/8 x = π/8 (0, 1) (-π/4, -1) (π/4, -1)

b. [3 marks]. V=π∫y2 dxV = \pi\displaystyle\int y^2\,dx, and sec⁡2(4x)\sec^2(4x) has antiderivative 14tan⁡(4x)\tfrac14\tan(4x):

V=π∫−π/24π/48sec⁡2(4x) dx=π4[tan⁡(4x)]−π/24π/48=π4(tan⁡(π12)−tan⁡(−π6)).V = \pi\int_{-\pi/24}^{\pi/48}\sec^2(4x)\,dx = \frac{\pi}{4}\Big[\tan(4x)\Big]_{-\pi/24}^{\pi/48} = \frac{\pi}{4}\left(\tan\left(\frac{\pi}{12}\right) - \tan\left(-\frac{\pi}{6}\right)\right).

Here tan⁡(−π6)=−13\tan\left(-\tfrac{\pi}{6}\right) = -\tfrac{1}{\sqrt3}. For tan⁡(π12)\tan\left(\tfrac{\pi}{12}\right) use the difference formula:

tan⁡(π12)=tan⁡(π3−π4)=3−11+3=(3−1)23−1=4−232=2−3.\tan\left(\frac{\pi}{12}\right) = \tan\left(\frac{\pi}{3} - \frac{\pi}{4}\right) = \frac{\sqrt3 - 1}{1 + \sqrt3} = \frac{\left(\sqrt3 - 1\right)^2}{3 - 1} = \frac{4 - 2\sqrt3}{2} = 2 - \sqrt3.

(Alternatively, with t=tan⁡(π12)t = \tan\left(\tfrac{\pi}{12}\right) the double angle formula gives 2t1−t2=13\tfrac{2t}{1 - t^2} = \tfrac{1}{\sqrt3}, so t2+23 t−1=0t^2 + 2\sqrt3\,t - 1 = 0 and t=−3±2t = -\sqrt3 \pm 2; take the positive root, 2−32 - \sqrt3.) So

V=π4(2−3+33)=π4×6−233=(6−23)π12=(3−3)π6.V = \frac{\pi}{4}\left(2 - \sqrt3 + \frac{\sqrt3}{3}\right) = \frac{\pi}{4} \times \frac{6 - 2\sqrt3}{3} = \frac{\left(6 - 2\sqrt3\right)\pi}{12} = \frac{\left(3 - \sqrt3\right)\pi}{6}.

So a=3a = 3, b=3b = 3 and c=6c = 6 (other forms such as (6−12)π12\tfrac{\left(6 - \sqrt{12}\right)\pi}{12} are equivalent).

From the report. In part a (13% full marks) many students found the vertical asymptotes, the turning point and the endpoints correctly, but some implied a horizontal asymptote, and some graphs had the wrong shape or were not symmetric about the yy-axis. In part b (25% full marks) most wrote a correct volume integral and many recognised 14tan⁡(4x)\tfrac14\tan(4x) as an antiderivative of sec⁡2(4x)\sec^2(4x). The sticking point was finding tan⁡(π12)\tan\left(\tfrac{\pi}{12}\right): those using the double angle formula sometimes could not solve the resulting quadratic or kept the wrong root, and those using the difference formula often made arithmetic errors.

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