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VICSpecialist Mathematics2023Exam 1

VCE Specialist Mathematics 2023 Exam 1

Worked solutions to every question in the 2023 VCE Specialist Mathematics Examination 1 (40 marks, no calculator), checked against the VCAA external assessment report, with the common errors the report flagged.

Marks
40
Time
60 min
Authority
VCAA
Updated

Every question from the 2023 VCE Specialist Mathematics Examination 1, the technology-free paper and the first under the current study design, 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 2023 Examination 2 walkthrough.

How to use this page

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 2023 it had 10 questions. New topics tested included integration by parts (Q5), surface area of revolution (Q7), proof by induction (Q8) and planes (Q9). The report singled out the alternative form of acceleration (Q3a), simple limits (Q3b), implicit differentiation (Q4) and induction (Q8) as weaker areas.

Questions and worked solutions

Question 1 (4 marks)

Let f(x)=x2+x−6x−1f(x) = \dfrac{x^2 + x - 6}{x - 1}.

a. Show that f(x)=x+2−4x−1f(x) = x + 2 - \dfrac{4}{x - 1}. (1 mark)

b. Sketch the graph of ff, labelling any asymptotes with their equations. (3 marks)

Show worked solution

a. [1 mark]. (x+2)(x−1)=x2+x−2(x + 2)(x - 1) = x^2 + x - 2, so x2+x−6=(x+2)(x−1)−4x^2 + x - 6 = (x + 2)(x - 1) - 4 and

f(x)=(x+2)(x−1)−4x−1=x+2−4x−1.f(x) = \frac{(x + 2)(x - 1) - 4}{x - 1} = x + 2 - \frac{4}{x - 1}.

b. [3 marks]. Asymptotes x=1x = 1 and y=x+2y = x + 2. Intercepts: x2+x−6=(x+3)(x−2)x^2 + x - 6 = (x + 3)(x - 2) gives (−3,0)(-3, 0) and (2,0)(2, 0), and f(0)=6f(0) = 6 gives (0,6)(0, 6). Since f′(x)=1+4(x−1)2>0f'(x) = 1 + \tfrac{4}{(x - 1)^2} > 0 there are no turning points. For x<1x < 1 the graph is above the oblique asymptote; for x>1x > 1 it is below.

Graph of y = x + 2 - 4/(x - 1) Two branches with vertical asymptote x = 1 and oblique asymptote y = x + 2. The left branch lies above the oblique asymptote and rises through (-3, 0) and (0, 6) towards positive infinity near x = 1; the right branch lies below it, rising from negative infinity near x = 1 through (2, 0) towards the oblique asymptote. x y -4 -2 2 4 -4 -2 2 4 8 10 (-3, 0) (2, 0) (0, 6) x = 1 y = x + 2

From the report. Both asymptotes had to be correct and labelled; the oblique asymptote was sometimes missing. Some graphs moved away from their asymptotes instead of approaching them.

Question 2 (3 marks)

For z=(b−i)3z = (b - i)^3 with b>0b > 0, find bb given arg⁡(z)=−π2\arg(z) = -\dfrac{\pi}{2}. (3 marks)

Show worked solution

[3 marks]. Let θ=arg⁡(b−i)\theta = \arg(b - i). Since b>0b > 0, b−ib - i is in the fourth quadrant, so −π2<θ<0-\tfrac{\pi}{2} < \theta < 0 and −3π2<3θ<0-\tfrac{3\pi}{2} < 3\theta < 0. We need arg⁡(z)=3θ=−π2\arg(z) = 3\theta = -\tfrac{\pi}{2} (the only value in that range), so θ=−π6\theta = -\tfrac{\pi}{6}:

tan⁡θ=−1b=−13  ⟹  b=3.\tan\theta = -\frac1b = -\frac{1}{\sqrt3} \implies b = \sqrt3.

Check: 3−i=2 cis(−π6)\sqrt3 - i = 2\,\text{cis}\left(-\tfrac{\pi}{6}\right), so z=8 cis(−π2)=−8iz = 8\,\text{cis}\left(-\tfrac{\pi}{2}\right) = -8i.

Alternatively, expand: (b−i)3=(b3−3b)+(1−3b2)i(b - i)^3 = (b^3 - 3b) + (1 - 3b^2)i. For argument −π2-\tfrac{\pi}{2} the real part must be 0 and the imaginary part negative, so b2=3b^2 = 3 and b=3b = \sqrt3.

From the report. The report showed both the polar approach and expanding the cube; graphical approaches were also seen.

Question 3 (3 marks)

A particle at xx m from OO has velocity v=3x+22x−1v = \dfrac{3x + 2}{2x - 1} m/s, x≥1x \ge 1.

a. Find the acceleration when x=2x = 2. (2 marks)

b. Find the value the velocity approaches as xx becomes very large. (1 mark)

Show worked solution

a. [2 marks]. Velocity is given in terms of xx, so use a=vdvdxa = v\dfrac{dv}{dx}:

dvdx=3(2x−1)−2(3x+2)(2x−1)2=−7(2x−1)2.\frac{dv}{dx} = \frac{3(2x - 1) - 2(3x + 2)}{(2x - 1)^2} = \frac{-7}{(2x - 1)^2}.

At x=2x = 2: v=83v = \tfrac83 and dvdx=−79\tfrac{dv}{dx} = -\tfrac79, so a=83×(−79)=−5627a = \tfrac83 \times \left(-\tfrac79\right) = -\dfrac{56}{27} m s−2^{-2}.

b. [1 mark]. v=3+2/x2−1/x→32v = \dfrac{3 + 2/x}{2 - 1/x} \to \dfrac32 m/s.

From the report. Many students found dvdx\tfrac{dv}{dx} at x=2x = 2 and stopped: acceleration is vdvdxv\tfrac{dv}{dx} (or ddx(12v2)\tfrac{d}{dx}\left(\tfrac12v^2\right)), not dvdx\tfrac{dv}{dx}. Part b was answered correctly by only half the students.

Question 4 (3 marks)

Use implicit differentiation on xarcsin⁡(y2)=πx\arcsin(y^2) = \pi to find dydx\dfrac{dy}{dx} at (6,12)\left(6, \tfrac{1}{\sqrt2}\right), in the form −πab-\dfrac{\pi\sqrt a}{b}. (3 marks)

Show worked solution

[3 marks]. Product rule, with the chain rule on arcsin⁡(y2)\arcsin(y^2):

arcsin⁡(y2)+x⋅2y1−y4dydx=0.\arcsin(y^2) + x\cdot\frac{2y}{\sqrt{1 - y^4}}\frac{dy}{dx} = 0.

At (6,12)\left(6, \tfrac{1}{\sqrt2}\right): y2=12y^2 = \tfrac12, arcsin⁡12=π6\arcsin\tfrac12 = \tfrac{\pi}{6} and 1−y4=32\sqrt{1 - y^4} = \tfrac{\sqrt3}{2}:

π6+6⋅23/2dydx=0  ⟹  dydx=−π6⋅3122=−π6144.\frac{\pi}{6} + 6 \cdot \frac{\sqrt2}{\sqrt3/2}\frac{dy}{dx} = 0 \implies \frac{dy}{dx} = -\frac{\pi}{6}\cdot\frac{\sqrt3}{12\sqrt2} = -\frac{\pi\sqrt6}{144}.

So a=6a = 6 and b=144b = 144.

From the report. The product and chain rules were often applied poorly; students who differentiated correctly usually completed the question.

Question 5 (3 marks)

Evaluate ∫12x2log⁡e(x) dx\displaystyle\int_1^2 x^2\log_e(x)\,dx. (3 marks)

Show worked solution

[3 marks]. Integrate by parts, differentiating log⁡ex\log_e x and antidifferentiating x2x^2:

∫12x2log⁡ex dx=[x33log⁡ex]12−∫12x33⋅1x dx=83log⁡e2−[x39]12=83log⁡e2−79.\int_1^2 x^2\log_e x\,dx = \left[\frac{x^3}{3}\log_e x\right]_1^2 - \int_1^2\frac{x^3}{3}\cdot\frac1x\,dx = \frac83\log_e 2 - \left[\frac{x^3}{9}\right]_1^2 = \frac83\log_e 2 - \frac79.

From the report. Most did well. Some chose the parts the wrong way round, did not evaluate the definite integral consistently, or left xx in the final answer.

Question 6 (4 marks)

Josie's drive Xc∼N(20,62)X_c \sim N(20, 6^2), train wait Xw∼N(8,(3)2)X_w \sim N(8, (\sqrt3)^2) and train ride Xt∼N(12,52)X_t \sim N(12, 5^2) minutes are independent.

a. Find the mean and standard deviation of her total travel time. (2 marks)

b. For 12 independent work days, the probability that her average wait is between 7 minutes 45 seconds and 8 minutes 30 seconds equals Pr⁡(a<Z<b)\Pr(a < Z < b). Find aa and bb. (2 marks)

Show worked solution

a. [2 marks]. Mean 20+8+12=4020 + 8 + 12 = 40 minutes. Variances add: 36+3+25=6436 + 3 + 25 = 64, so the standard deviation is 88 minutes.

b. [2 marks]. The average wait Xˉw\bar X_w has mean 8 and standard deviation 312=12\tfrac{\sqrt3}{\sqrt{12}} = \tfrac12. So

Pr⁡(7.75<Xˉw<8.5)=Pr⁡(7.75−80.5<Z<8.5−80.5)=Pr⁡(−0.5<Z<1),\Pr(7.75 < \bar X_w < 8.5) = \Pr\left(\frac{7.75 - 8}{0.5} < Z < \frac{8.5 - 8}{0.5}\right) = \Pr(-0.5 < Z < 1),

giving a=−12a = -\tfrac12, b=1b = 1 (by symmetry, a=−1a = -1, b=12b = \tfrac12 is equivalent).

From the report. In part a many added the standard deviations (6+3+56 + \sqrt3 + 5) instead of the variances. Part b was not answered well; the usual error was using the wrong standard deviation for the sample mean.

Question 7 (4 marks)

The curve x=t24−1x = \tfrac{t^2}{4} - 1, y=3ty = \sqrt3t, 0≤t≤20 \le t \le 2, is rotated about the xx-axis. Find the surface area in the form π(abc−d)\pi\left(\dfrac{a\sqrt b}{c} - d\right). (4 marks)

Show worked solution

[4 marks]. x˙=t2\dot x = \tfrac t2 and y˙=3\dot y = \sqrt3, so

S=2π∫02yx˙2+y˙2 dt=2π∫023tt24+3 dt.S = 2\pi\int_0^2 y\sqrt{\dot x^2 + \dot y^2}\,dt = 2\pi\int_0^2\sqrt3t\sqrt{\frac{t^2}{4} + 3}\,dt.

Let u=t24+3u = \tfrac{t^2}{4} + 3, so du=t2 dtdu = \tfrac t2\,dt and t dt=2 dut\,dt = 2\,du; the terminals become u=3u = 3 and u=4u = 4:

S=43π∫34u du=43π⋅23(8−33)=π(6433−24).S = 4\sqrt3\pi\int_3^4\sqrt u\,du = 4\sqrt3\pi\cdot\frac23\left(8 - 3\sqrt3\right) = \pi\left(\frac{64\sqrt3}{3} - 24\right).

So a=64a = 64, b=3b = 3, c=3c = 3, d=24d = 24.

From the report. An explicit substitution was more reliable than trying to spot the antiderivative. A few students converted to Cartesian form and integrated successfully.

Question 8 (4 marks)

For f(x)=xe2xf(x) = xe^{2x}, prove by induction that f(n)(x)=(2nx+n2n−1)e2xf^{(n)}(x) = \left(2^nx + n2^{n-1}\right)e^{2x} for n∈Z+n \in Z^+. (4 marks)

Show worked solution

[4 marks]. Base case, n=1n = 1. f′(x)=e2x+2xe2x=(2x+1)e2x=(21x+1⋅20)e2xf'(x) = e^{2x} + 2xe^{2x} = (2x + 1)e^{2x} = \left(2^1x + 1 \cdot 2^0\right)e^{2x}. True.

Inductive step. Assume that for some k∈Z+k \in Z^+, f(k)(x)=(2kx+k2k−1)e2xf^{(k)}(x) = \left(2^kx + k2^{k-1}\right)e^{2x}. Differentiating with the product rule:

f(k+1)(x)=2ke2x+2(2kx+k2k−1)e2x=(2k+1x+k2k+2k)e2x=(2k+1x+(k+1)2k)e2x.f^{(k+1)}(x) = 2^ke^{2x} + 2\left(2^kx + k2^{k-1}\right)e^{2x} = \left(2^{k+1}x + k2^k + 2^k\right)e^{2x} = \left(2^{k+1}x + (k + 1)2^k\right)e^{2x}.

This is the statement for n=k+1n = k + 1. Since it is true for n=1n = 1, and truth for n=kn = k implies truth for n=k+1n = k + 1, by mathematical induction it is true for all n∈Z+n \in Z^+.

From the report. Most set up the base case and assumption. The inductive step required differentiating f(k)f^{(k)}; many did not differentiate, or differentiated incorrectly, and some misapplied index laws when simplifying the powers of 2.

Question 9 (6 marks)

A plane contains A(1,3,−2)A(1, 3, -2), B(−1,−2,4)B(-1, -2, 4) and C(a,−1,5)C(a, -1, 5), and meets the yy-axis at y=2y = 2 (point DD).

a
Write down DD. (1 mark)
b
Show that AB→=−2i−5j+6k\overrightarrow{AB} = -2\mathbf i - 5\mathbf j + 6\mathbf k and AD→=−i−j+2k\overrightarrow{AD} = -\mathbf i - \mathbf j + 2\mathbf k. (1 mark)
c
Hence find the Cartesian equation of the plane. (2 marks)
d
Find aa. (1 mark)
e
AB→\overrightarrow{AB} and AD→\overrightarrow{AD} are adjacent sides of a parallelogram. Find its area. (1 mark)
Show worked solution
a. [1 mark]
D(0,2,0)D(0, 2, 0).
b. [1 mark]
AB→=(−1−1,−2−3,4+2)=(−2,−5,6)\overrightarrow{AB} = (-1 - 1, -2 - 3, 4 + 2) = (-2, -5, 6) and AD→=(0−1,2−3,0+2)=(−1,−1,2)\overrightarrow{AD} = (0 - 1, 2 - 3, 0 + 2) = (-1, -1, 2).
c. [2 marks]
A normal is

AB→×AD→=∣ijk−2−56−1−12∣=−4i−2j−3k.\overrightarrow{AB}\times\overrightarrow{AD} = \begin{vmatrix}\mathbf i & \mathbf j & \mathbf k \\ -2 & -5 & 6 \\ -1 & -1 & 2\end{vmatrix} = -4\mathbf i - 2\mathbf j - 3\mathbf k.

Using DD: 4x+2y+3z=44x + 2y + 3z = 4. (Check AA: 4+6−6=44 + 6 - 6 = 4.)

d. [1 mark]. CC lies on the plane: 4a−2+15=44a - 2 + 15 = 4, so a=−94a = -\tfrac94.

e. [1 mark]. Area =∣AB→×AD→∣=16+4+9=29= \left|\overrightarrow{AB}\times\overrightarrow{AD}\right| = \sqrt{16 + 4 + 9} = \sqrt{29}.

From the report. Parts a and b were done very well. In part c some slipped in the cross product or in substituting a point. In part e some gave the triangle's area (half the value), and a common error was multiplying the two side lengths.

Question 10 (6 marks)

A particle has position r(t)=(5−6sin⁡2t)i+(1+6sin⁡tcos⁡t)j\mathbf r(t) = \left(5 - 6\sin^2t\right)\mathbf i + \left(1 + 6\sin t\cos t\right)\mathbf j, t≥0t \ge 0.

a
Write 5−6sin⁡2t5 - 6\sin^2t as α+βcos⁡(2t)\alpha + \beta\cos(2t) with α,β∈Z+\alpha, \beta \in Z^+. (1 mark)
b
Show that the path is (x−2)2+(y−1)2=9(x - 2)^2 + (y - 1)^2 = 9. (2 marks)
c
The particle is at AA when t=0t = 0 and at BB when t=at = a. If the distance along the curve from AA to BB is 3π4\tfrac{3\pi}{4}, find aa. (1 mark)
d
Find all tt for which r(t)\mathbf r(t) is perpendicular to r˙(t)\dot{\mathbf r}(t). (2 marks)
Show worked solution

a. [1 mark]. sin⁡2t=1−cos⁡2t2\sin^2t = \tfrac{1 - \cos 2t}{2}, so 5−6sin⁡2t=5−3+3cos⁡2t=2+3cos⁡(2t)5 - 6\sin^2t = 5 - 3 + 3\cos 2t = 2 + 3\cos(2t): α=2\alpha = 2, β=3\beta = 3.

b. [2 marks]. x=2+3cos⁡2tx = 2 + 3\cos 2t and, since 6sin⁡tcos⁡t=3sin⁡2t6\sin t\cos t = 3\sin 2t, y=1+3sin⁡2ty = 1 + 3\sin 2t. Then

(x−2)2+(y−1)2=9cos⁡22t+9sin⁡22t=9.(x - 2)^2 + (y - 1)^2 = 9\cos^2 2t + 9\sin^2 2t = 9.

c. [1 mark]. The particle moves around a circle of radius 3 with angle 2t2t, so the arc length from t=0t = 0 to t=at = a is 3×2a=6a3 \times 2a = 6a. Then 6a=3π46a = \tfrac{3\pi}{4} gives a=π8a = \tfrac{\pi}{8}.

d. [2 marks]. r˙=−6sin⁡2t i+6cos⁡2t j\dot{\mathbf r} = -6\sin 2t\,\mathbf i + 6\cos 2t\,\mathbf j. Then

r⋅r˙=−6sin⁡2t(2+3cos⁡2t)+6cos⁡2t(1+3sin⁡2t)=−12sin⁡2t+6cos⁡2t=0,\mathbf r\cdot\dot{\mathbf r} = -6\sin 2t(2 + 3\cos 2t) + 6\cos 2t(1 + 3\sin 2t) = -12\sin 2t + 6\cos 2t = 0,

so tan⁡2t=12\tan 2t = \tfrac12 and

t=12arctan⁡(12)+kπ2,k=0,1,2,…t = \frac12\arctan\left(\frac12\right) + \frac{k\pi}{2}, \quad k = 0, 1, 2, \ldots

From the report. Part b needed a double angle formula and then a Pythagorean identity. Part c (36% correct) could be done with arc length rθr\theta or by integrating the speed. In part d many set up r⋅r˙=0\mathbf r\cdot\dot{\mathbf r} = 0 but only 7% reached the full general solution.

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