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    9709/33 May/June 2025 Worked Answers (A-Level Maths 9709 A2)

    16 questions · 75 marks · 110 minutes

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    Worked answers for 16 questions
    1. Step 1: ∣3x−2a∣<x+5a|3x - 2a| < x + 5a requires x+5a>0x + 5a > 0 (i.e. x>−5ax > -5a); within this region, the inequality is equivalent to −(x+5a)<3x−2a<x+5a-(x + 5a) < 3x - 2a < x + 5a. Step 2: Right inequality: 3x−2a<x+5a⇒2x<7a⇒x<7a23x - 2a < x + 5a \Rightarrow 2x < 7a \Rightarrow x < \dfrac{7a}{2}. Step 3: Left inequality: −(x+5a)<3x−2a⇒−x−5a<3x−2a⇒−3a<4x⇒x>−3a4-(x + 5a) < 3x - 2a \Rightarrow -x - 5a < 3x - 2a \Rightarrow -3a < 4x \Rightarrow x > -\dfrac{3a}{4}. Step 4: Combine: −3a4<x<7a2-\dfrac{3a}{4} < x < \dfrac{7a}{2}.
      Method:
      Convert the modulus inequality to a two-sided form, solve each linear inequality for xx in terms of aa, and intersect.
      Examiner tips
      • ∣f(x)∣<g(x)  ⟺  −g(x)<f(x)<g(x)|f(x)| < g(x) \iff -g(x) < f(x) < g(x) when g(x)>0g(x) > 0
      • When parameters appear, keep aa symbolic until the end
    2. Question 2

      4 marksLogarithm Equation
      Step 1: Use 2ln⁡u=ln⁡u22 \ln u = \ln u^2 and combine: ln⁡(2x+3)22x+5=ln⁡(3x)\ln \dfrac{(2x+3)^2}{2x+5} = \ln(3x). Step 2: Equate arguments: (2x+3)2=3x(2x+5)(2x+3)^2 = 3x(2x+5). Step 3: Expand: 4x2+12x+9=6x2+15x4x^2 + 12x + 9 = 6x^2 + 15x, so 2x2+3x−9=02x^2 + 3x - 9 = 0. Step 4: Factorise: (2x−3)(x+3)=0(2x - 3)(x + 3) = 0, so x=32x = \dfrac{3}{2} or x=−3x = -3. Step 5: Check domain: ln⁡(3x)\ln(3x) needs x>0x > 0, so reject x=−3x = -3. Final answer: x=32x = \dfrac{3}{2}.
      Method:
      Apply log laws to form a single log on each side, equate the arguments, solve the resulting quadratic, and reject solutions outside the log domain.
      Examiner tips
      • Always check the domain of each logarithm and reject extraneous solutions
      • Use aln⁡b=ln⁡baa \ln b = \ln b^a before combining
    3. Step 1: Use the identity cos⁡25x=1+cos⁡10x2\cos^2 5x = \dfrac{1 + \cos 10x}{2}, so 3cos⁡25x=32+32cos⁡10x3 \cos^2 5x = \dfrac{3}{2} + \dfrac{3}{2} \cos 10x. Step 2: Antidifferentiate: ∫(32+32cos⁡10x)dx=32x+320sin⁡10x\displaystyle \int \left(\dfrac{3}{2} + \dfrac{3}{2} \cos 10x\right) dx = \dfrac{3}{2} x + \dfrac{3}{20} \sin 10x. Step 3: Apply the upper limit x=π/4x = \pi/4: 32⋅π4+320sin⁡10π4=3π8+320sin⁡5π2=3π8+320\dfrac{3}{2} \cdot \dfrac{\pi}{4} + \dfrac{3}{20} \sin \dfrac{10\pi}{4} = \dfrac{3\pi}{8} + \dfrac{3}{20} \sin \dfrac{5\pi}{2} = \dfrac{3\pi}{8} + \dfrac{3}{20} (since sin⁡(5π/2)=1\sin(5\pi/2) = 1). Step 4: Apply the lower limit x=π/5x = \pi/5: 32⋅π5+320sin⁡2π=3π10+0\dfrac{3}{2} \cdot \dfrac{\pi}{5} + \dfrac{3}{20} \sin 2\pi = \dfrac{3\pi}{10} + 0. Step 5: Subtract: (3π8−3π10)+320=15π−12π40+320=3π40+320\left(\dfrac{3\pi}{8} - \dfrac{3\pi}{10}\right) + \dfrac{3}{20} = \dfrac{15\pi - 12\pi}{40} + \dfrac{3}{20} = \dfrac{3\pi}{40} + \dfrac{3}{20}.
      Method:
      Apply the double-angle identity, integrate term-by-term, and substitute the limits separately before subtracting.
      Examiner tips
      • cos⁡2θ\cos^2 \theta and sin⁡2θ\sin^2 \theta usually call for the double-angle identity in integration
      • Work each limit separately to avoid confusing sin⁡\sin values
    4. Step 1: Since the coefficients are real, complex roots come in conjugate pairs. The other root is zˉ=3e−iπ/4\bar{z} = 3 e^{-i\pi/4}. Step 2: For a monic quadratic with roots z,zˉz, \bar{z}: b=−(z+zˉ)b = -(z + \bar{z}) and c=zzˉc = z \bar{z}. Step 3: z+zˉ=3eiπ/4+3e−iπ/4=6cos⁡(π/4)=6⋅22=32z + \bar{z} = 3 e^{i\pi/4} + 3 e^{-i\pi/4} = 6 \cos(\pi/4) = 6 \cdot \dfrac{\sqrt{2}}{2} = 3\sqrt{2}. So b=−32b = -3\sqrt{2}. Step 4: zzˉ=3⋅3⋅eiπ/4−iπ/4=9z \bar{z} = 3 \cdot 3 \cdot e^{i\pi/4 - i\pi/4} = 9. So c=9c = 9.
      Method:
      Identify the conjugate as the other root, then use Vieta's formulas: b=−(z+zˉ)b = -(z + \bar z) and c=zzˉc = z \bar z.
      Examiner tips
      • z+zˉ=2Re⁡(z)z + \bar{z} = 2 \operatorname{Re}(z) and zzˉ=∣z∣2z \bar{z} = |z|^2
      • Real coefficients ⇒\Rightarrow conjugate pairs
    5. Step 1: At x=0x = 0, the curve equation becomes 0⋅y+y2⋅1=40 \cdot y + y^2 \cdot 1 = 4, so y2=4y^2 = 4, giving y=2y = 2 or y=−2y = -2. Step 2: At x=0x = 0, the gradient simplifies: dydx=y2−y2y=y(y−1)2y=y−12\dfrac{dy}{dx} = \dfrac{y^2 - y}{2y} = \dfrac{y(y-1)}{2y} = \dfrac{y - 1}{2}. Step 3: At y=2y = 2: 2−12=12\dfrac{2 - 1}{2} = \dfrac{1}{2}. Step 4: At y=−2y = -2: −2−12=−32\dfrac{-2 - 1}{2} = -\dfrac{3}{2}.
      Method:
      Determine the yy-values at x=0x = 0 from the curve, then evaluate the given gradient formula at each point.
      Examiner tips
      • Always find ALL points on the curve at the given xx-value
      • Simplify the gradient formula before substituting
    6. Step 1: Write z=x+iyz = x + iy. Then z+4z+4i=(x+4)+iyx+i(y+4)\dfrac{z + 4}{z + 4i} = \dfrac{(x+4) + iy}{x + i(y+4)}. Multiply numerator and denominator by x−i(y+4)x - i(y+4). Step 2: Numerator becomes (x+4)x+y(y+4)+i[xy−(y+4)(x+4)](x+4)x + y(y+4) + i\big[xy - (y+4)(x+4)\big]. Step 3: For the quotient to be real, the imaginary part vanishes: xy−(y+4)(x+4)=0⇒xy−xy−4x−4y−16=0⇒x+y=−4xy - (y+4)(x+4) = 0 \Rightarrow xy - xy - 4x - 4y - 16 = 0 \Rightarrow x + y = -4. Step 4: Use ∣z∣2=x2+y2=10|z|^2 = x^2 + y^2 = 10. With y=−x−4y = -x - 4: x2+(x+4)2=10⇒2x2+8x+6=0⇒x2+4x+3=0⇒(x+1)(x+3)=0x^2 + (x+4)^2 = 10 \Rightarrow 2x^2 + 8x + 6 = 0 \Rightarrow x^2 + 4x + 3 = 0 \Rightarrow (x+1)(x+3) = 0, so x=−1x = -1 or x=−3x = -3. Step 5: Corresponding yy: at x=−1x = -1, y=−3y = -3; at x=−3x = -3, y=−1y = -1. So z=−1−3iz = -1 - 3i or z=−3−iz = -3 - i.
      Method:
      Set z=x+iyz = x + iy, rationalise the quotient, set the imaginary part of the numerator to zero, and combine with the modulus condition to solve.
      Examiner tips
      • Realness of a quotient ⇒\Rightarrow imaginary part of numerator (after rationalising) is zero
      • Always combine with the modulus condition to get a unique pair of solutions
    7. Question 7a

      3 marksPartial Fractions
      Step 1: Set up 3a−5x(3a+2x)(2a−x)=A3a+2x+B2a−x\dfrac{3a - 5x}{(3a + 2x)(2a - x)} = \dfrac{A}{3a + 2x} + \dfrac{B}{2a - x}. Step 2: Multiply through: 3a−5x=A(2a−x)+B(3a+2x)3a - 5x = A(2a - x) + B(3a + 2x). Step 3: Substitute x=2ax = 2a: 3a−10a=B(3a+4a)⇒−7a=7aB⇒B=−13a - 10a = B(3a + 4a) \Rightarrow -7a = 7aB \Rightarrow B = -1. Step 4: Substitute x=−3a2x = -\dfrac{3a}{2}: 3a+15a2=A(2a+3a2)⇒21a2=7a2A⇒A=33a + \dfrac{15a}{2} = A\left(2a + \dfrac{3a}{2}\right) \Rightarrow \dfrac{21a}{2} = \dfrac{7a}{2} A \Rightarrow A = 3. Step 5: Therefore f(x)=33a+2x−12a−xf(x) = \dfrac{3}{3a + 2x} - \dfrac{1}{2a - x}.
      Method:
      Set up partial fraction form, multiply through, substitute the roots of each linear factor to find AA and BB.
      Examiner tips
      • Cover-up rule is fastest for distinct linear factors
      • Verify by reconstructing the numerator
    8. Step 1: 33a+2x=33a⋅11+2x3a=1a(1−2x3a+4x29a2+⋯ )=1a−2x3a2+4x29a3\dfrac{3}{3a + 2x} = \dfrac{3}{3a} \cdot \dfrac{1}{1 + \frac{2x}{3a}} = \dfrac{1}{a} \left(1 - \dfrac{2x}{3a} + \dfrac{4x^2}{9a^2} + \cdots\right) = \dfrac{1}{a} - \dfrac{2x}{3a^2} + \dfrac{4x^2}{9a^3}. Step 2: −12a−x=−12a⋅11−x2a=−12a(1+x2a+x24a2+⋯ )=−12a−x4a2−x28a3-\dfrac{1}{2a - x} = -\dfrac{1}{2a} \cdot \dfrac{1}{1 - \frac{x}{2a}} = -\dfrac{1}{2a}\left(1 + \dfrac{x}{2a} + \dfrac{x^2}{4a^2} + \cdots\right) = -\dfrac{1}{2a} - \dfrac{x}{4a^2} - \dfrac{x^2}{8a^3}. Step 3: Constant: 1a−12a=12a\dfrac{1}{a} - \dfrac{1}{2a} = \dfrac{1}{2a}. Step 4: xx-coefficient: −23a2−14a2=−8+312a2=−1112a2-\dfrac{2}{3a^2} - \dfrac{1}{4a^2} = -\dfrac{8 + 3}{12 a^2} = -\dfrac{11}{12 a^2}. Step 5: x2x^2-coefficient: 49a3−18a3=32−972a3=2372a3\dfrac{4}{9 a^3} - \dfrac{1}{8 a^3} = \dfrac{32 - 9}{72 a^3} = \dfrac{23}{72 a^3}.
      Method:
      Factor each denominator, expand each term up to x2x^2, then combine the constants, xx-, and x2x^2-coefficients.
      Examiner tips
      • Always factor the constant out of each linear factor before applying (1+u)−1(1+u)^{-1}
      • Check xx and x2x^2 coefficients separately
    9. Step 1: 11+2x/(3a)\dfrac{1}{1 + 2x/(3a)} is valid for ∣2x/(3a)∣<1|2x/(3a)| < 1, i.e. ∣x∣<3a2|x| < \dfrac{3a}{2}. Step 2: 11−x/(2a)\dfrac{1}{1 - x/(2a)} is valid for ∣x/(2a)∣<1|x/(2a)| < 1, i.e. ∣x∣<2a|x| < 2a. Step 3: Both expansions must converge simultaneously, so we need the tighter condition: ∣x∣<3a2|x| < \dfrac{3a}{2} (since 3a2<2a\dfrac{3a}{2} < 2a).
      Method:
      Identify the convergence region of each binomial expansion separately, then intersect them.
      Examiner tips
      • When two binomial expansions are added, take the smaller (tighter) convergence region
      • Always factor the constant out first to find the convergence parameter
    10. Step 1: Substitute the identity: 4cot⁡2xcosec⁡2x=5sec⁡2x4 \cot 2x \operatorname{cosec} 2x = 5 \sec 2x, i.e. 4cos⁡2xsin⁡22x=5cos⁡2x\dfrac{4 \cos 2x}{\sin^2 2x} = \dfrac{5}{\cos 2x}. Step 2: Cross-multiply: 4cos⁡22x=5sin⁡22x4 \cos^2 2x = 5 \sin^2 2x, so tan⁡22x=45\tan^2 2x = \dfrac{4}{5}. Step 3: tan⁡2x=±25≈±0.8944\tan 2x = \pm \dfrac{2}{\sqrt{5}} \approx \pm 0.8944. For 0<x<90∘0 < x < 90^\circ, 0<2x<180∘0 < 2x < 180^\circ. Step 4: 2x=arctan⁡(2/5)≈41.81∘2x = \arctan(2/\sqrt 5) \approx 41.81^\circ, so x≈20.9∘x \approx 20.9^\circ. Also 2x=180∘−41.81∘=138.19∘2x = 180^\circ - 41.81^\circ = 138.19^\circ, giving x≈69.1∘x \approx 69.1^\circ.
      Method:
      Use the given identity to reduce both sides to expressions in sin⁡2x\sin 2x and cos⁡2x\cos 2x, simplify to tan⁡22x=\tan^2 2x = constant, and find both solutions in the range.
      Examiner tips
      • When the equation reduces to tan⁡2ϕ=k\tan^2 \phi = k, expect TWO solutions in any half-revolution interval
      • Convert all to a single trig function before solving
    11. Question 9a

      2 marksVector Equation of a Line
      Step 1: Direction vector BC→=OC→−OB→=(2−1,−1−3,3−(−2))=(1,−4,5)\overrightarrow{BC} = \overrightarrow{OC} - \overrightarrow{OB} = (2-1, -1-3, 3-(-2)) = (1, -4, 5). Step 2: A vector equation is r=OB→+λBC→=(i+3j−2k)+λ(i−4j+5k)\mathbf{r} = \overrightarrow{OB} + \lambda \overrightarrow{BC} = (\mathbf{i} + 3\mathbf{j} - 2\mathbf{k}) + \lambda(\mathbf{i} - 4\mathbf{j} + 5\mathbf{k}).
      Method:
      Compute BC→\overrightarrow{BC} as the difference of position vectors, then write r=OB→+λBC→\mathbf{r} = \overrightarrow{OB} + \lambda \overrightarrow{BC}.
      Examiner tips
      • Either BB or CC can be used as the position vector
      • BC→\overrightarrow{BC} and −BC→-\overrightarrow{BC} are both valid direction vectors
    12. Step 1: A general point on ll is P=(1+λ,3−4λ,−2+5λ)P = (1 + \lambda, 3 - 4\lambda, -2 + 5\lambda). So AP→=(λ,1−4λ,−2+5λ)\overrightarrow{AP} = (\lambda, 1 - 4\lambda, -2 + 5\lambda). Step 2: Perpendicularity: AP→⋅(1,−4,5)=0\overrightarrow{AP} \cdot (1, -4, 5) = 0. Step 3: λ⋅1+(1−4λ)(−4)+(−2+5λ)(5)=0⇒λ−4+16λ−10+25λ=0⇒42λ=14⇒λ=13\lambda \cdot 1 + (1 - 4\lambda)(-4) + (-2 + 5\lambda)(5) = 0 \Rightarrow \lambda - 4 + 16\lambda - 10 + 25\lambda = 0 \Rightarrow 42\lambda = 14 \Rightarrow \lambda = \dfrac{1}{3}. Step 4: OP→=(1+13,3−43,−2+53)=(43,53,−13)\overrightarrow{OP} = \left(1 + \dfrac{1}{3}, 3 - \dfrac{4}{3}, -2 + \dfrac{5}{3}\right) = \left(\dfrac{4}{3}, \dfrac{5}{3}, -\dfrac{1}{3}\right).
      Method:
      Parameterise the foot of perpendicular on the line, set the scalar product of AP→\overrightarrow{AP} with the direction vector to zero, solve for λ\lambda, and substitute back.
      Examiner tips
      • Distinguish AP→\overrightarrow{AP} from OP→\overrightarrow{OP}
      • Don't forget to substitute λ\lambda back to find OP→\overrightarrow{OP}
    13. Step 1: PP is the midpoint of AA and its reflection DD, so OP→=OA→+OD→2\overrightarrow{OP} = \dfrac{\overrightarrow{OA} + \overrightarrow{OD}}{2}, giving OD→=2OP→−OA→\overrightarrow{OD} = 2\overrightarrow{OP} - \overrightarrow{OA}. Step 2: Compute 2OP→=(83,103,−23)2 \overrightarrow{OP} = \left(\dfrac{8}{3}, \dfrac{10}{3}, -\dfrac{2}{3}\right). Step 3: Subtract OA→=(1,2,0)\overrightarrow{OA} = (1, 2, 0): OD→=(83−1,103−2,−23)=(53,43,−23)\overrightarrow{OD} = \left(\dfrac{8}{3} - 1, \dfrac{10}{3} - 2, -\dfrac{2}{3}\right) = \left(\dfrac{5}{3}, \dfrac{4}{3}, -\dfrac{2}{3}\right).
      Method:
      Use the midpoint relation to express the reflection as OD→=2OP→−OA→\overrightarrow{OD} = 2 \overrightarrow{OP} - \overrightarrow{OA}.
      Examiner tips
      • PP is the midpoint of AA and the reflected point DD
      • OD→=2OP→−OA→\overrightarrow{OD} = 2\overrightarrow{OP} - \overrightarrow{OA} is the standard reflection formula
    14. Step 1: Use the double-angle identity sin⁡4y=2sin⁡2ycos⁡2y\sin 4y = 2 \sin 2y \cos 2y, so sin⁡4ysin⁡2y=2cos⁡2y\dfrac{\sin 4y}{\sin 2y} = 2 \cos 2y. Step 2: Separate variables: 2cos⁡2y dy=xsin⁡3x dx2 \cos 2y \, dy = x \sin 3x \, dx. Step 3: Integrate LHS: ∫2cos⁡2y dy=sin⁡2y\int 2 \cos 2y \, dy = \sin 2y. Step 4: Integrate RHS by parts with u=x,dv=sin⁡3x dxu = x, dv = \sin 3x \, dx: u=x,du=dx,v=−13cos⁡3xu = x, du = dx, v = -\dfrac{1}{3}\cos 3x. So ∫xsin⁡3x dx=−x3cos⁡3x+13∫cos⁡3x dx=−x3cos⁡3x+19sin⁡3x+C\int x \sin 3x \, dx = -\dfrac{x}{3} \cos 3x + \dfrac{1}{3} \int \cos 3x \, dx = -\dfrac{x}{3} \cos 3x + \dfrac{1}{9} \sin 3x + C. Step 5: Apply IC y=π/12,x=π/2y = \pi/12, x = \pi/2: sin⁡(π/6)=12\sin(\pi/6) = \dfrac{1}{2}. RHS at x=π/2x=\pi/2: −π/23cos⁡(3π/2)+19sin⁡(3π/2)+C=0−19+C-\dfrac{\pi/2}{3} \cos(3\pi/2) + \dfrac{1}{9} \sin(3\pi/2) + C = 0 - \dfrac{1}{9} + C. So 12=−19+C⇒C=1118\dfrac{1}{2} = -\dfrac{1}{9} + C \Rightarrow C = \dfrac{11}{18}.
      Method:
      Reduce sin⁡4y/sin⁡2y\sin 4y / \sin 2y to 2cos⁡2y2 \cos 2y using the double-angle identity, separate variables, integrate the RHS by parts, and apply the initial condition.
      Examiner tips
      • Use sin⁡4y=2sin⁡2ycos⁡2y\sin 4y = 2 \sin 2y \cos 2y to make the LHS easily separable
      • Always check signs carefully when integrating by parts
    15. Step 1: At x=0x = 0: sin⁡2y=0+0+1118≈0.6111\sin 2y = 0 + 0 + \dfrac{11}{18} \approx 0.6111. Step 2: For 0<y<π20 < y < \dfrac{\pi}{2}, we have 0<2y<π0 < 2y < \pi. Solutions of sin⁡2y=0.6111\sin 2y = 0.6111 in this range: 2y=arcsin⁡(0.6111)≈0.65872y = \arcsin(0.6111) \approx 0.6587 and 2y=π−0.6587≈2.4832y = \pi - 0.6587 \approx 2.483. Step 3: y≈0.65872=0.329y \approx \dfrac{0.6587}{2} = 0.329 (3 s.f.) and y≈2.4832=1.241≈1.24y \approx \dfrac{2.483}{2} = 1.241 \approx 1.24 (3 s.f.).
      Method:
      Substitute x=0x = 0 to reduce to sin⁡2y=c\sin 2y = c, find both solutions for 2y∈(0,π)2y \in (0, \pi), then halve.
      Examiner tips
      • sin⁡2y=c\sin 2y = c in (0,π)(0, \pi) has exactly two solutions when 0<c<10 < c < 1
      • Halve 2y2y to get yy
    16. Step 1: Starting from x0=0.9x_0 = 0.9: x1=12(π−tan⁡−1(3.6))≈12(3.14159−1.29920)≈0.920872x_1 = \tfrac{1}{2}(\pi - \tan^{-1}(3.6)) \approx \tfrac{1}{2}(3.14159 - 1.29920) \approx 0.920872. Step 2: x2=12(π−tan⁡−1(3.683...))≈0.917944x_2 = \tfrac{1}{2}(\pi - \tan^{-1}(3.683...)) \approx 0.917944. Step 3: x3≈0.918347x_3 \approx 0.918347, x4≈0.918292x_4 \approx 0.918292, x5≈0.918300x_5 \approx 0.918300. Step 4: The sequence stabilises around 0.918300.91830, which to 4 d.p. is 0.91830.9183.
      Method:
      Apply the iteration in radians from x0=0.9x_0 = 0.9, retaining at least 6 d.p., until two successive values agree to 5 d.p.
      Examiner tips
      • Always work in radians for tan⁡−1\tan^{-1} unless told otherwise
      • Keep at least 6 d.p. through the iteration

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