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    9709/33 Oct/Nov 2025 Worked Answers (A-Level Maths 9709 A2)

    14 questions · 75 marks · 110 minutes

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    Worked answers for 13 questions
    1. Step 1: Square both sides: (3x+2)2<9(2x−1)2(3x + 2)^2 < 9(2x - 1)^2, valid because both are non-negative. Step 2: Expand: 9x2+12x+4<9(4x2−4x+1)=36x2−36x+99x^2 + 12x + 4 < 9(4x^2 - 4x + 1) = 36x^2 - 36x + 9, giving 27x2−48x+5>027x^2 - 48x + 5 > 0. Step 3: Factorise: (9x−1)(3x−5)>0(9x - 1)(3x - 5) > 0. Critical values x=19x = \dfrac{1}{9} and x=53x = \dfrac{5}{3}. Step 4: Sign chart: the upward-opening quadratic is positive outside its roots. Hence x<19x < \dfrac{1}{9} or x>53x > \dfrac{5}{3}.
      Method:
      Square both sides, form the quadratic inequality, factorise, and select the correct sign regions.
      Examiner tips
      • ∣f(x)∣<∣g(x)∣  ⟺  f(x)2<g(x)2|f(x)| < |g(x)| \iff f(x)^2 < g(x)^2
      • Sketch a sign chart for the factorised quadratic
    2. Question 2

      3 marksPolynomial Long Division
      Step 1: Use the remainder theorem: remainder =f(−1)=3(−1)4−2(−1)2=3−2=1= f(-1) = 3(-1)^4 - 2(-1)^2 = 3 - 2 = 1. Step 2: Long division: 3x4/x=3x33x^4 / x = 3x^3. Multiply: 3x3(x+1)=3x4+3x33x^3(x+1) = 3x^4 + 3x^3. Subtract: −3x3−2x2-3x^3 - 2x^2. Step 3: −3x3/x=−3x2-3x^3/x = -3x^2. Multiply: −3x3−3x2-3x^3 - 3x^2. Subtract: x2x^2. Step 4: x2/x=xx^2/x = x. Multiply: x2+xx^2 + x. Subtract: −x-x. Step 5: −x/x=−1-x/x = -1. Multiply: −x−1-x - 1. Subtract: 11. So quotient =3x3−3x2+x−1= 3x^3 - 3x^2 + x - 1, remainder =1= 1.
      Method:
      Apply the remainder theorem to find the constant, then long-divide systematically.
      Examiner tips
      • Use f(−1)=f(-1) = remainder as a quick check
      • Treat missing terms with coefficient 00
    3. Step 1: Rearrange: 23x−4⋅5x=32^{3x - 4} \cdot 5^x = 3, so 23x24⋅5x=3\dfrac{2^{3x}}{2^4} \cdot 5^x = 3, giving (23)x⋅5x16=3\dfrac{(2^3)^x \cdot 5^x}{16} = 3, i.e. (23⋅5)x=3⋅16=48(2^3 \cdot 5)^x = 3 \cdot 16 = 48. Step 2: Simplify: 40x=4840^x = 48. Step 3: Take natural logs: xln⁡40=ln⁡48x \ln 40 = \ln 48, so x=ln⁡48ln⁡40x = \dfrac{\ln 48}{\ln 40}.
      Method:
      Combine all base-2 and base-5 terms into 40x40^x, then take logs to express xx as a quotient.
      Examiner tips
      • Combine bases as (23⋅5)x=40x(2^3 \cdot 5)^x = 40^x to simplify
      • log⁡ab=ln⁡bln⁡a\log_a b = \dfrac{\ln b}{\ln a}
    4. Step 1: Substitute the identity: 8sin⁡4x−6sin⁡2x=08 \sin^4 x - 6 \sin^2 x = 0, factor 2sin⁡2x(4sin⁡2x−3)=02 \sin^2 x (4 \sin^2 x - 3) = 0. Step 2: Either sin⁡x=0\sin x = 0 or sin⁡2x=34\sin^2 x = \dfrac{3}{4}, i.e. sin⁡x=±32\sin x = \pm \dfrac{\sqrt{3}}{2}. Step 3: sin⁡x=0\sin x = 0 in [−180∘,180∘][-180^\circ, 180^\circ]: x=−180∘,0∘,180∘x = -180^\circ, 0^\circ, 180^\circ. Step 4: sin⁡x=32\sin x = \dfrac{\sqrt 3}{2}: x=60∘,120∘x = 60^\circ, 120^\circ. sin⁡x=−32\sin x = -\dfrac{\sqrt 3}{2}: x=−60∘,−120∘x = -60^\circ, -120^\circ. Step 5: All seven solutions: ±180∘,±120∘,±60∘,0∘\pm 180^\circ, \pm 120^\circ, \pm 60^\circ, 0^\circ.
      Method:
      Use the identity to reduce, factor out sin⁡2x\sin^2 x, solve both cases, and list all solutions in the interval.
      Examiner tips
      • Never divide by sin⁡2x\sin^2 x — you lose the sin⁡x=0\sin x = 0 solutions
      • Always list ALL solutions in the given range
    5. Step 1: Apply integration by parts with u=x2u = x^2, dv=sin⁡2x dxdv = \sin 2x \, dx: du=2x dxdu = 2x\, dx, v=−12cos⁡2xv = -\dfrac{1}{2} \cos 2x. So ∫x2sin⁡2x dx=−x22cos⁡2x+∫xcos⁡2x dx\int x^2 \sin 2x \, dx = -\dfrac{x^2}{2} \cos 2x + \int x \cos 2x \, dx. Step 2: Apply parts again to ∫xcos⁡2x dx\int x \cos 2x\, dx with u=xu = x, dv=cos⁡2x dxdv = \cos 2x\, dx: du=dxdu = dx, v=12sin⁡2xv = \dfrac{1}{2} \sin 2x. ∫xcos⁡2x dx=x2sin⁡2x−12∫sin⁡2x dx=x2sin⁡2x+14cos⁡2x\int x \cos 2x\, dx = \dfrac{x}{2} \sin 2x - \dfrac{1}{2} \int \sin 2x \, dx = \dfrac{x}{2} \sin 2x + \dfrac{1}{4} \cos 2x. Step 3: Antiderivative: −x22cos⁡2x+x2sin⁡2x+14cos⁡2x-\dfrac{x^2}{2} \cos 2x + \dfrac{x}{2} \sin 2x + \dfrac{1}{4} \cos 2x. Step 4: At x=π/6x = \pi/6: cos⁡(π/3)=1/2\cos(\pi/3) = 1/2, sin⁡(π/3)=3/2\sin(\pi/3) = \sqrt 3 /2. Value: −π2/362⋅12+π/62⋅32+14⋅12=−π2144+π324+18-\dfrac{\pi^2/36}{2} \cdot \dfrac{1}{2} + \dfrac{\pi/6}{2} \cdot \dfrac{\sqrt 3}{2} + \dfrac{1}{4} \cdot \dfrac{1}{2} = -\dfrac{\pi^2}{144} + \dfrac{\pi \sqrt 3}{24} + \dfrac{1}{8}. Step 5: At x=0x = 0: 0+0+140 + 0 + \dfrac{1}{4}. Subtract: −π2144+π324+18−14=−π2144+π324−18-\dfrac{\pi^2}{144} + \dfrac{\pi \sqrt 3}{24} + \dfrac{1}{8} - \dfrac{1}{4} = -\dfrac{\pi^2}{144} + \dfrac{\pi \sqrt 3}{24} - \dfrac{1}{8}.
      Method:
      Apply integration by parts twice to get the antiderivative, then evaluate at the limits using exact values cos⁡π/3=1/2\cos \pi/3 = 1/2 and sin⁡π/3=3/2\sin \pi/3 = \sqrt 3/2.
      Examiner tips
      • Track signs carefully when integrating sin⁡2x\sin 2x (gives −12cos⁡2x-\dfrac{1}{2}\cos 2x)
      • After applying integration by parts twice, evaluate ALL three boundary terms
    6. Step 1: Multiply through by (2−i)(2 - i): 5z−(2−i)(x2+y2)+(20+8i)(2−i)=05z - (2-i)(x^2 + y^2) + (20 + 8i)(2 - i) = 0. Step 2: (20+8i)(2−i)=40−20i+16i−8i2=40+8−4i=48−4i(20+8i)(2-i) = 40 - 20i + 16i - 8i^2 = 40 + 8 - 4i = 48 - 4i. Step 3: Substitute z=x+iyz = x+iy: 5(x+iy)−(2−i)(x2+y2)+48−4i=05(x+iy) - (2-i)(x^2+y^2) + 48 - 4i = 0. Expand (2−i)(x2+y2)=2(x2+y2)−i(x2+y2)(2-i)(x^2+y^2) = 2(x^2+y^2) - i(x^2+y^2). Step 4: Real part: 5x−2(x2+y2)+48=05x - 2(x^2+y^2) + 48 = 0. Imaginary part: 5y+(x2+y2)−4=05y + (x^2+y^2) - 4 = 0. Step 5: From imaginary: x2+y2=4−5yx^2 + y^2 = 4 - 5y. Substitute into real: 5x−2(4−5y)+48=0⇒5x+10y+40=0⇒x+2y+8=05x - 2(4 - 5y) + 48 = 0 \Rightarrow 5x + 10y + 40 = 0 \Rightarrow x + 2y + 8 = 0, so x=−2y−8x = -2y - 8. Step 6: Substitute back: (−2y−8)2+y2=4−5y⇒5y2+37y+60=0⇒(y+5)(5y+12)=0(-2y-8)^2 + y^2 = 4 - 5y \Rightarrow 5y^2 + 37y + 60 = 0 \Rightarrow (y + 5)(5y + 12) = 0, giving y=−5y = -5 or y=−125y = -\dfrac{12}{5}. So z=2−5iz = 2 - 5i or z=−165−125iz = -\dfrac{16}{5} - \dfrac{12}{5} i.
      Method:
      Clear the fraction, expand, equate real and imaginary parts to zero, eliminate ∣z∣2|z|^2 to obtain a linear equation, and solve.
      Examiner tips
      • zz∗z z^* is always real (equals ∣z∣2|z|^2)
      • Eliminating x2+y2x^2 + y^2 between the two equations gives a linear constraint
    7. Step 1: Compute p1=15exp⁡(12)=e0.55≈1.64875≈0.3297p_1 = \dfrac{1}{5} \exp\left(\dfrac{1}{2}\right) = \dfrac{e^{0.5}}{5} \approx \dfrac{1.6487}{5} \approx 0.3297. Step 2: p2=15exp⁡(15⋅0.3297)=15exp⁡(0.6066)≈0.3668p_2 = \dfrac{1}{5} \exp\left(\dfrac{1}{5 \cdot 0.3297}\right) = \dfrac{1}{5} \exp(0.6066) \approx 0.3668. Step 3: p3≈0.3450p_3 \approx 0.3450, p4≈0.3571p_4 \approx 0.3571, p5≈0.3502p_5 \approx 0.3502, p6≈0.3541p_6 \approx 0.3541. Step 4: The sequence oscillates and stabilises around 0.3540.354, which to 2 d.p. is 0.350.35.
      Method:
      Apply the iteration repeatedly, retaining at least 4 d.p., until two successive values agree to 3 d.p.
      Examiner tips
      • Oscillating sequences require more iterations to confirm convergence
      • Keep at least 4 d.p. to check convergence to 2 d.p.
    8. Step 1: l1l_1 has position (3,1,−6)(3, 1, -6) and direction (2,1,4)(2, 1, 4), so r=(3,1,−6)+λ(2,1,4)\mathbf{r} = (3, 1, -6) + \lambda(2, 1, 4). Step 2: For l2l_2, the direction vector has no xx-component: (0,b,c)(0, b, c). It must be perpendicular to (3,−2,1)(3, -2, 1), so (0)(3)+b(−2)+c(1)=−2b+c=0(0)(3) + b(-2) + c(1) = -2b + c = 0, giving c=2bc = 2b. Step 3: Take b=1b = 1, c=2c = 2: direction (0,1,2)(0, 1, 2). So l2:r=(−1,3,−6)+μ(0,1,2)l_2: \mathbf{r} = (-1, 3, -6) + \mu(0, 1, 2).
      Method:
      Write l1l_1 directly, then for l2l_2 set the xx-component to zero and use the scalar-product condition to find the remaining components.
      Examiner tips
      • a⋅b=0  ⟺  a⊥b\mathbf{a} \cdot \mathbf{b} = 0 \iff \mathbf{a} \perp \mathbf{b}
      • Combine constraints sequentially
    9. Step 1: Scalar product: (2)(0)+(1)(1)+(4)(2)=0+1+8=9(2)(0) + (1)(1) + (4)(2) = 0 + 1 + 8 = 9. Step 2: Moduli: ∣d1∣=4+1+16=21|\mathbf{d}_1| = \sqrt{4 + 1 + 16} = \sqrt{21}, ∣d2∣=0+1+4=5|\mathbf{d}_2| = \sqrt{0 + 1 + 4} = \sqrt{5}. Step 3: cos⁡θ=921⋅5=9105≈910.247≈0.8783\cos\theta = \dfrac{9}{\sqrt{21} \cdot \sqrt{5}} = \dfrac{9}{\sqrt{105}} \approx \dfrac{9}{10.247} \approx 0.8783. Step 4: θ=cos⁡−1(0.8783)≈28.6∘\theta = \cos^{-1}(0.8783) \approx 28.6^\circ (or 0.4980.498 rad). This is already acute.
      Method:
      Compute scalar product, moduli, divide, take inverse cosine.
      Examiner tips
      • Take the absolute value of the cosine if it is negative
      • 21⋅5=105\sqrt{21 \cdot 5} = \sqrt{105}
    10. Step 1: Equate xx-components: 3+2λ=−13 + 2\lambda = -1, giving λ=−2\lambda = -2. Step 2: Equate zz-components: −6+4λ=−6+2μ-6 + 4\lambda = -6 + 2\mu, so 4(−2)=2μ4(-2) = 2\mu, giving μ=−4\mu = -4. Step 3: Verify yy: 1+λ=1+(−2)=−11 + \lambda = 1 + (-2) = -1, and 3+μ=3+(−4)=−13 + \mu = 3 + (-4) = -1. ✓ Step 4: Substitute λ=−2\lambda = -2 into l1l_1: (3−4,1−2,−6−8)=(−1,−1,−14)(3 - 4, 1 - 2, -6 - 8) = (-1, -1, -14).
      Method:
      Equate two pairs of components to find λ\lambda and μ\mu, verify the third, and substitute back to get the intersection.
      Examiner tips
      • Always verify the third equation — if it fails, the lines are skew
      • Substitute the parameter back to recover the position vector
    11. Step 1: Factor: 1−9y2=(1−3y)(1+3y)1 - 9y^2 = (1 - 3y)(1 + 3y). Step 2: Set 2(1−3y)(1+3y)=A1+3y+B1−3y\dfrac{2}{(1-3y)(1+3y)} = \dfrac{A}{1+3y} + \dfrac{B}{1-3y}. Step 3: Multiply through: 2=A(1−3y)+B(1+3y)2 = A(1 - 3y) + B(1 + 3y). Step 4: At y=1/3y = 1/3: 2=0+B(1+1)=2B2 = 0 + B(1 + 1) = 2B, so B=1B = 1. At y=−1/3y = -1/3: 2=A(1+1)=2A2 = A(1 + 1) = 2A, so A=1A = 1.
      Method:
      Factor by difference of squares and apply cover-up to find the two constants.
      Examiner tips
      • 1−k2y2=(1−ky)(1+ky)1 - k^2 y^2 = (1 - ky)(1 + ky) — difference of squares
      • Cover-up rule is fastest
    12. Step 1: Separate variables: 2 dy1−9y2=sec⁡23x dx\dfrac{2 \, dy}{1 - 9y^2} = \sec^2 3x \, dx. Step 2: Use partial fractions: 21−9y2=11+3y+11−3y\dfrac{2}{1 - 9y^2} = \dfrac{1}{1 + 3y} + \dfrac{1}{1 - 3y}. Integrate: 13ln⁡∣1+3y∣−13ln⁡∣1−3y∣=13ln⁡∣1+3y1−3y∣\dfrac{1}{3}\ln|1 + 3y| - \dfrac{1}{3}\ln|1 - 3y| = \dfrac{1}{3} \ln\left|\dfrac{1 + 3y}{1 - 3y}\right|. Step 3: Integrate RHS: ∫sec⁡23x dx=13tan⁡3x\int \sec^2 3x \, dx = \dfrac{1}{3} \tan 3x. Step 4: Apply IC y=0,x=π/12y = 0, x = \pi/12: 13ln⁡1=13tan⁡(π/4)+C=13+C\dfrac{1}{3} \ln 1 = \dfrac{1}{3} \tan(\pi/4) + C = \dfrac{1}{3} + C, so C=−13C = -\dfrac{1}{3}. Step 5: ln⁡∣1+3y1−3y∣=tan⁡3x−1\ln\left|\dfrac{1+3y}{1-3y}\right| = \tan 3x - 1. Exponentiate: 1+3y1−3y=etan⁡3x−1\dfrac{1+3y}{1-3y} = e^{\tan 3x - 1}. Step 6: Let k=etan⁡3x−1k = e^{\tan 3x - 1}: 1+3y=k(1−3y)1 + 3y = k(1 - 3y), so 3y(1+k)=k−13y(1 + k) = k - 1, giving y=k−13(k+1)=etan⁡3x−1−13(etan⁡3x−1+1)y = \dfrac{k - 1}{3(k + 1)} = \dfrac{e^{\tan 3x - 1} - 1}{3(e^{\tan 3x - 1} + 1)}.
      Method:
      Separate, decompose using partial fractions, integrate, apply the initial condition, exponentiate, and solve algebraically for yy.
      Examiner tips
      • sec⁡23x=1cos⁡23x\sec^2 3x = \dfrac{1}{\cos^2 3x} — recognise this in the RHS
      • ∫sec⁡2(kx)dx=1ktan⁡(kx)\int \sec^2 (kx) dx = \dfrac{1}{k} \tan(kx)
    13. Question 11b

      6 marksArea by Substitution
      Step 1: Substitute u=3+2tan⁡xu = 3 + 2 \tan x. Then dudx=2sec⁡2x\dfrac{du}{dx} = 2 \sec^2 x, so sec⁡2x dx=du2\sec^2 x \, dx = \dfrac{du}{2}. Step 2: Limits: at x=−π/4x = -\pi/4, tan⁡(−π/4)=−1\tan(-\pi/4) = -1, so u=3−2=1u = 3 - 2 = 1. At x=π/4x = \pi/4, tan⁡(π/4)=1\tan(\pi/4) = 1, so u=3+2=5u = 3 + 2 = 5. Step 3: Area =∫−π/4π/4sec⁡2x3+2tan⁡x dx=∫15u⋅du2=12∫15u1/2 du= \displaystyle \int_{-\pi/4}^{\pi/4} \sec^2 x \sqrt{3 + 2 \tan x} \, dx = \int_1^5 \sqrt u \cdot \dfrac{du}{2} = \dfrac{1}{2} \int_1^5 u^{1/2} \, du. Step 4: ∫u1/2 du=23u3/2\int u^{1/2} \, du = \dfrac{2}{3} u^{3/2}, so Area =12⋅23u3/2∣15=13(53/2−13/2)=55−13= \dfrac{1}{2} \cdot \dfrac{2}{3} u^{3/2} \Big|_1^5 = \dfrac{1}{3} (5^{3/2} - 1^{3/2}) = \dfrac{5\sqrt 5 - 1}{3}.
      Method:
      Use the substitution to convert into ∫u du/2\int \sqrt u \, du/2, change limits, and evaluate.
      Examiner tips
      • Always change limits when substituting (don't substitute back to xx unnecessarily)
      • ∫u1/2du=23u3/2\int u^{1/2} du = \dfrac{2}{3} u^{3/2}

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