← All A-Level Maths 9709 A2 past papers
    A2
    CAIE | A Level

    Mathematics (9709)

    May/June 2025 Paper 31 Worked Answers (A-Level Maths 9709 A2)

    16 questions · 75 marks · 110 minutes

    Question papers and mark schemes are copyright Cambridge International. We do not reproduce them: the worked answers here are written by The Practice Book. Have the paper open alongside. Get the official paper from Cambridge

    Worked answers for 15 questions
    1. Question 1b

      2 marksModulus Inequalities
      Step 1: Square both sides (valid since both are non-negative): (2x1)2<(x+3)2(2x-1)^2 < (x+3)^2. Step 2: Expand: 4x24x+1<x2+6x+94x^2 - 4x + 1 < x^2 + 6x + 9, giving 3x210x8<03x^2 - 10x - 8 < 0. Step 3: Factorise: (3x+2)(x4)<0(3x + 2)(x - 4) < 0. Critical values are x=23x = -\dfrac{2}{3} and x=4x = 4. Step 4: The quadratic opens upwards, so it is negative between its roots: 23<x<4-\dfrac{2}{3} < x < 4.
      Method:
      Square both sides to eliminate moduli, factorise the resulting quadratic, then read off the interval where it is negative.
      Examiner tips
      • Squaring is valid because a<b    a2<b2|a| < |b| \iff a^2 < b^2
      • For an upward-opening quadratic, (xr1)(xr2)<0(x-r_1)(x-r_2) < 0 on the interval (r1,r2)(r_1, r_2)
    2. Question 2

      3 marksLogarithm Manipulation
      Step 1: Rewrite using log laws: 3lna=lna33 \ln a = \ln a^3 and 12ln(b+4)=lnb+4\dfrac{1}{2}\ln(b+4) = \ln \sqrt{b+4}. Step 2: The equation becomes lna3b+4=2\ln \dfrac{a^3}{\sqrt{b+4}} = 2, so a3b+4=e2\dfrac{a^3}{\sqrt{b+4}} = e^2. Step 3: Rearrange: b+4=a3e2\sqrt{b+4} = \dfrac{a^3}{e^2}. Step 4: Square both sides: b+4=a6e4b + 4 = \dfrac{a^6}{e^4}, hence b=a6e44b = \dfrac{a^6}{e^4} - 4.
      Method:
      Use the power law of logs to rewrite each term, combine into a single log, exponentiate to remove the log, and square to clear the square root.
      Examiner tips
      • Convert all coefficients of logs into powers using klnx=lnxkk \ln x = \ln x^k
      • Remember to square (not just remove the square root) when isolating the variable
    3. Step 1: Multiply numerator and denominator by the conjugate of the denominator (x5)iy(x-5) - iy. The numerator becomes x(x5)+y(y+5)+i[(y+5)(x5)xy]x(x-5) + y(y+5) + i\big[(y+5)(x-5) - xy\big]. Step 2: For the quotient to be real, the imaginary part must vanish: (y+5)(x5)xy=0xy+5x5y25xy=0xy=5(y+5)(x-5) - xy = 0 \Rightarrow xy + 5x - 5y - 25 - xy = 0 \Rightarrow x - y = 5. Step 3: Combine with z2=x2+y2=17|z|^2 = x^2 + y^2 = 17: substitute y=x5y = x - 5 to get x2+(x5)2=17x^2 + (x-5)^2 = 17, i.e. 2x210x+25=172x^2 - 10x + 25 = 17, so x25x+4=0x^2 - 5x + 4 = 0. Step 4: Factorise: (x1)(x4)=0(x-1)(x-4) = 0, giving x=1x = 1 or x=4x = 4. The corresponding values are z=14iz = 1 - 4i or z=4iz = 4 - i.
      Method:
      Substitute z=x+iyz = x + iy, multiply by the conjugate of the denominator, set the imaginary part of the resulting expression to zero, then combine with z2=17|z|^2 = 17 to solve for xx and yy.
      Examiner tips
      • When a quotient must be real, set its imaginary part to zero
      • Always double-check candidate solutions against both conditions
    4. Step 1: At (e,3)(e, 3), since x=etant=ex = e^{\tan t} = e, we have tant=1\tan t = 1 (so t=π/4t = \pi/4). Step 2: Differentiate: dxdt=sec2tetant\dfrac{dx}{dt} = \sec^2 t \cdot e^{\tan t}. At tant=1\tan t = 1: sec2t=1+tan2t=2\sec^2 t = 1 + \tan^2 t = 2, so dxdt=2e=2e\dfrac{dx}{dt} = 2 \cdot e = 2e. Step 3: dydt=6tantsec2t=612=12\dfrac{dy}{dt} = 6 \tan t \cdot \sec^2 t = 6 \cdot 1 \cdot 2 = 12. Step 4: Gradient at the point: dydx=dy/dtdx/dt=122e=6e\dfrac{dy}{dx} = \dfrac{dy/dt}{dx/dt} = \dfrac{12}{2e} = \dfrac{6}{e}. Step 5: Tangent line: y3=6e(xe)y - 3 = \dfrac{6}{e}(x - e), which simplifies to y=6ex6+3=6ex3y = \dfrac{6}{e} x - 6 + 3 = \dfrac{6}{e} x - 3.
      Method:
      Determine tt from the given point, differentiate xx and yy with respect to tt, divide to get dydx\dfrac{dy}{dx}, then write the tangent in point-gradient form.
      Examiner tips
      • Use sec2t=1+tan2t\sec^2 t = 1 + \tan^2 t to evaluate without finding tt explicitly
      • etante^{\tan t} differentiates by chain rule: sec2tetant\sec^2 t \cdot e^{\tan t}
    5. Step 1: Apply the remainder theorem with x=2ax = -2a: f(2a)=3(2a)3+pa(2a)2+7a2(2a)+qa3=24a3+4pa314a3+qa3=(38+4p+q)a3=22a3f(-2a) = 3(-2a)^3 + pa(-2a)^2 + 7a^2(-2a) + qa^3 = -24a^3 + 4pa^3 - 14a^3 + qa^3 = (-38 + 4p + q)a^3 = -22a^3. So 4p+q=164p + q = 16. Step 2: Apply with x=a/3x = a/3: f(a/3)=3(a/3)3+pa(a/3)2+7a2(a/3)+qa3=a39+pa39+7a33+qa3=(1+p9+73+q)a3=a3f(a/3) = 3(a/3)^3 + pa(a/3)^2 + 7a^2(a/3) + qa^3 = \dfrac{a^3}{9} + \dfrac{pa^3}{9} + \dfrac{7a^3}{3} + qa^3 = \left(\dfrac{1+p}{9} + \dfrac{7}{3} + q\right)a^3 = -a^3. Step 3: Multiply through by 99: 1+p+21+9q=91 + p + 21 + 9q = -9, giving p+9q=31p + 9q = -31. Step 4: Solve the system: from 4p+q=164p + q = 16, q=164pq = 16 - 4p. Substitute: p+9(164p)=3135p=175p=5p + 9(16 - 4p) = -31 \Rightarrow -35p = -175 \Rightarrow p = 5, then q=1620=4q = 16 - 20 = -4. So p+q=1p + q = 1.
      Method:
      Apply the remainder theorem at the two roots of the divisors to obtain a pair of linear equations in pp and qq, then solve simultaneously.
      Examiner tips
      • Substitute carefully — keep aa symbolic and divide by a3a^3 at the end
      • Check both equations after solving
    6. Step 1: Multiplication in polar form multiplies moduli and adds arguments: wz=wz=24=8|wz| = |w| \cdot |z| = 2 \cdot 4 = 8. Step 2: arg(wz)=argw+argz=π6+π3=π+2π6=π2\arg(wz) = \arg w + \arg z = \dfrac{\pi}{6} + \dfrac{\pi}{3} = \dfrac{\pi + 2\pi}{6} = \dfrac{\pi}{2}. Step 3: Therefore wz=8eiπ/2wz = 8 e^{i \pi/2}, which is already in the principal range π<θπ-\pi < \theta \le \pi.
      Method:
      Multiply moduli and add arguments to express the product in polar form.
      Examiner tips
      • Always check the result is in the principal range π<θπ-\pi < \theta \le \pi
      • Common identity: eiαeiβ=ei(α+β)e^{i\alpha} \cdot e^{i\beta} = e^{i(\alpha+\beta)}
    7. Step 1: Multiplication by a complex number reiθr e^{i\theta} in the Argand diagram has two geometric effects: enlargement (scale factor rr) and rotation by angle θ\theta (anticlockwise if positive). Step 2: For ω=2eiπ/2\omega = 2 e^{i \pi/2}, the modulus is r=2r = 2 and the argument is θ=π2\theta = \dfrac{\pi}{2}. Step 3: Hence multiplying by ω\omega rotates the point about the origin through π2\dfrac{\pi}{2} anticlockwise and enlarges its distance from the origin by a factor of 22.
      Method:
      Read off the modulus as the enlargement factor and the argument as the (anticlockwise) rotation angle.
      Examiner tips
      • Multiplication by ii alone is rotation by π/2\pi/2 anticlockwise
      • The modulus of the multiplier is the scale factor of the enlargement
    8. Question 7a

      4 marksR-Formula (Harmonic Form)
      Step 1: Expand 5sin(x+π6)=5sinxcosπ6+5cosxsinπ6=532sinx+52cosx5 \sin\left(x + \dfrac{\pi}{6}\right) = 5 \sin x \cos\dfrac{\pi}{6} + 5 \cos x \sin\dfrac{\pi}{6} = \dfrac{5\sqrt{3}}{2} \sin x + \dfrac{5}{2} \cos x. Step 2: Subtracting 4cosx4 \cos x: 532sinx+(524)cosx=532sinx32cosx\dfrac{5\sqrt{3}}{2} \sin x + \left(\dfrac{5}{2} - 4\right) \cos x = \dfrac{5\sqrt{3}}{2} \sin x - \dfrac{3}{2} \cos x. Step 3: Match Rsin(xα)=RcosαsinxRsinαcosxR \sin(x - \alpha) = R \cos\alpha \sin x - R \sin\alpha \cos x. So Rcosα=532R \cos\alpha = \dfrac{5\sqrt{3}}{2} and Rsinα=32R \sin\alpha = \dfrac{3}{2}. Step 4: R2=754+94=844=21R^2 = \dfrac{75}{4} + \dfrac{9}{4} = \dfrac{84}{4} = 21, so R=21R = \sqrt{21}. Step 5: tanα=3/253/2=353=350.3464\tan\alpha = \dfrac{3/2}{5\sqrt{3}/2} = \dfrac{3}{5\sqrt{3}} = \dfrac{\sqrt{3}}{5} \approx 0.3464, so α=tan1(0.3464)0.333\alpha = \tan^{-1}(0.3464) \approx 0.333 radians.
      Method:
      Expand the compound angle, collect sinx\sin x and cosx\cos x terms, equate to RcosαR \cos\alpha and RsinαR \sin\alpha, then compute RR via Pythagoras and α\alpha via tan1\tan^{-1}.
      Examiner tips
      • Always expand the compound angle first before matching coefficients
      • Use tanα=coefficient of cosxcoefficient of sinx\tan\alpha = \dfrac{\text{coefficient of }\cos x}{\text{coefficient of }\sin x} for the form Rsin(xα)R \sin(x - \alpha)
    9. Step 1: Replace xx by 2θ2\theta in the identity to get 21sin(2θ0.333)=7\sqrt{21} \sin(2\theta - 0.333) = \sqrt{7}, so sin(2θ0.333)=721=13\sin(2\theta - 0.333) = \dfrac{\sqrt{7}}{\sqrt{21}} = \dfrac{1}{\sqrt{3}}. Step 2: Let ϕ=2θ0.333\phi = 2\theta - 0.333. The reference angle is sin1(1/3)0.6155\sin^{-1}(1/\sqrt{3}) \approx 0.6155. Step 3: For 0θπ0 \le \theta \le \pi, we need ϕ[0.333,2π0.333]\phi \in [-0.333, 2\pi - 0.333]. Solutions are ϕ=0.6155\phi = 0.6155 and ϕ=π0.6155=2.526\phi = \pi - 0.6155 = 2.526. Step 4: ϕ=0.61552θ=0.948θ=0.47\phi = 0.6155 \Rightarrow 2\theta = 0.948 \Rightarrow \theta = 0.47 (2 d.p.). ϕ=2.5262θ=2.859θ=1.43\phi = 2.526 \Rightarrow 2\theta = 2.859 \Rightarrow \theta = 1.43 (2 d.p.).
      Method:
      Apply the harmonic form to reduce the equation to a single sine, find all solutions for sinϕ=c\sin\phi = c in the appropriate ϕ\phi range, then translate back to θ\theta.
      Examiner tips
      • Don't forget the supplementary angle πϕ\pi - \phi when solving sinϕ=c\sin\phi = c in [0,π][0, \pi]
      • Always check the candidate θ\theta values lie in the given range
    10. Step 1: A line through points with position vectors a\mathbf{a} and b\mathbf{b} has direction vector ba\mathbf{b} - \mathbf{a}. Step 2: Compute AB=ba=(41)i+(12)j+(51)k=3ij+4k\overrightarrow{AB} = \mathbf{b} - \mathbf{a} = (4-1)\mathbf{i} + (1-2)\mathbf{j} + (5-1)\mathbf{k} = 3\mathbf{i} - \mathbf{j} + 4\mathbf{k}. Step 3: A vector equation is r=a+λAB=(i+2j+k)+λ(3ij+4k)\mathbf{r} = \mathbf{a} + \lambda \overrightarrow{AB} = (\mathbf{i} + 2\mathbf{j} + \mathbf{k}) + \lambda(3\mathbf{i} - \mathbf{j} + 4\mathbf{k}).
      Method:
      Subtract position vectors to find the direction, then write the equation in r=a+λd\mathbf{r} = \mathbf{a} + \lambda \mathbf{d} form.
      Examiner tips
      • The position vector in the equation can be either AA or BB — both are valid points on the line
      • Direction vector is unique up to a scalar multiple
    11. Step 1: Compute the scalar product: d1d2=(3)(1)+(1)(2)+(2)(3)=3+2+6=11\mathbf{d}_1 \cdot \mathbf{d}_2 = (3)(1) + (1)(2) + (2)(3) = 3 + 2 + 6 = 11. Step 2: Compute the moduli: d1=9+1+4=14|\mathbf{d}_1| = \sqrt{9 + 1 + 4} = \sqrt{14} and d2=1+4+9=14|\mathbf{d}_2| = \sqrt{1 + 4 + 9} = \sqrt{14}. Step 3: Use cosθ=d1d2d1d2=11140.7857\cos\theta = \dfrac{\mathbf{d}_1 \cdot \mathbf{d}_2}{|\mathbf{d}_1||\mathbf{d}_2|} = \dfrac{11}{14} \approx 0.7857. Step 4: θ=cos1(0.7857)38.2\theta = \cos^{-1}(0.7857) \approx 38.2^\circ. Since this is already acute, no further adjustment is needed.
      Method:
      Compute the scalar product and the moduli, divide and take the inverse cosine; if the angle is obtuse, subtract from 180180^\circ to get the acute angle.
      Examiner tips
      • If the dot product is negative, take its absolute value to get the acute angle
      • a=a12+a22+a32|\mathbf{a}| = \sqrt{a_1^2 + a_2^2 + a_3^2}
    12. Step 1: Compute a1=exp(16(54+3))=exp(16174)=exp(0.7083)2.0306a_1 = \exp\left(\dfrac{1}{6}\left(\dfrac{5}{4} + 3\right)\right) = \exp\left(\dfrac{1}{6} \cdot \dfrac{17}{4}\right) = \exp(0.7083) \approx 2.0306. Step 2: a2=exp(16(52.03062+3))exp(0.7021)2.0180a_2 = \exp\left(\dfrac{1}{6}\left(\dfrac{5}{2.0306^2} + 3\right)\right) \approx \exp(0.7021) \approx 2.0180. Step 3: a32.0231a_3 \approx 2.0231, a42.0210a_4 \approx 2.0210, a52.0218a_5 \approx 2.0218. The sequence stabilises around 2.0212.021, which to 2 d.p. is 2.022.02. Step 4: Verify with a sign-change argument: f(2.015)f(2.015) and f(2.025)f(2.025) have opposite signs in f(x)=xexp((1/6)(5/x2+3))f(x) = x - \exp((1/6)(5/x^2 + 3)), confirming the root is in (2.015,2.025)(2.015, 2.025), i.e. a=2.02a = 2.02 to 2 d.p.
      Method:
      Apply the iteration starting from a0=2a_0 = 2, retaining at least 4 d.p. each step until convergence to 3 d.p., then round to 2 d.p.
      Examiner tips
      • Keep at least 4 d.p. through the iteration to maintain accuracy
      • Stop when two successive values agree to 3 d.p.
    13. Question 10a

      3 marksPolynomial Long Division
      Step 1: Divide x3x^3 by x2x^2 to get xx. Multiply x(x23)=x33xx \cdot (x^2 - 3) = x^3 - 3x and subtract: (x3+5x22x15)(x33x)=5x2+x15(x^3 + 5x^2 - 2x - 15) - (x^3 - 3x) = 5x^2 + x - 15. Step 2: Divide 5x25x^2 by x2x^2 to get 55. Multiply 5(x23)=5x2155 \cdot (x^2 - 3) = 5x^2 - 15 and subtract: (5x2+x15)(5x215)=x(5x^2 + x - 15) - (5x^2 - 15) = x. Step 3: Since deg(x)<deg(x23)\deg(x) < \deg(x^2 - 3), the division stops. Quotient =x+5= x + 5, remainder =x= x. Step 4: Verification: (x+5)(x23)+x=x33x+5x215+x=x3+5x22x15(x + 5)(x^2 - 3) + x = x^3 - 3x + 5x^2 - 15 + x = x^3 + 5x^2 - 2x - 15. ✓
      Method:
      Apply standard polynomial long division, dividing leading terms, multiplying, subtracting, until the remainder has lower degree than the divisor.
      Examiner tips
      • Always verify by reconstructing: dividend = (quotient)(divisor) + remainder
      • Watch the sign of each subtraction step carefully
    14. Step 1: Separate variables: 6ydy=x3+5x22x15x23dx=(x+5+xx23)dx6y \, dy = \dfrac{x^3 + 5x^2 - 2x - 15}{x^2 - 3} dx = \left(x + 5 + \dfrac{x}{x^2 - 3}\right) dx using the given decomposition. Step 2: Integrate both sides: 6ydy=3y2\int 6y \, dy = 3y^2 and (x+5)dx=x22+5x\int (x + 5) dx = \dfrac{x^2}{2} + 5x, xx23dx=12lnx23\int \dfrac{x}{x^2 - 3} dx = \dfrac{1}{2} \ln|x^2 - 3| (recognising f/ff'/f form). Step 3: Combine: 3y2=x22+5x+12lnx23+C3y^2 = \dfrac{x^2}{2} + 5x + \dfrac{1}{2} \ln|x^2 - 3| + C. Step 4: Apply initial condition y=2,x=2y = 2, x = 2: 12=2+10+12ln1+C=12+C12 = 2 + 10 + \dfrac{1}{2}\ln 1 + C = 12 + C, so C=0C = 0. Step 5: Divide by 3: y2=x26+5x3+16lnx23y^2 = \dfrac{x^2}{6} + \dfrac{5x}{3} + \dfrac{1}{6} \ln|x^2 - 3|.
      Method:
      Use the given decomposition to write dydx\dfrac{dy}{dx} as a sum of integrable terms, separate variables, integrate using known forms, and apply the initial condition.
      Examiner tips
      • Recognise f(x)f(x)dx=lnf(x)+C\int \dfrac{f'(x)}{f(x)} dx = \ln|f(x)| + C patterns to avoid lengthier substitution
      • Always check the initial condition gives a sensible value of CC
    15. Step 1: Volume of revolution: V=π0π/2y2dx=π0π/2cos2xsin2xdxV = \pi \int_0^{\pi/2} y^2 \, dx = \pi \int_0^{\pi/2} \cos^2 x \sin 2x \, dx. Step 2: Use sin2x=2sinxcosx\sin 2x = 2 \sin x \cos x: integrand becomes 2cos3xsinx2 \cos^3 x \sin x, so V=2π0π/2cos3xsinxdxV = 2\pi \int_0^{\pi/2} \cos^3 x \sin x \, dx. Step 3: Substitute u=cosxu = \cos x, du=sinxdxdu = -\sin x \, dx. When x=0x = 0, u=1u = 1; when x=π/2x = \pi/2, u=0u = 0. V=2π10u3(du)=2π01u3duV = 2\pi \int_1^0 u^3 (-du) = 2\pi \int_0^1 u^3 \, du. Step 4: Evaluate: V=2π[u44]01=2π14=π2V = 2\pi \left[\dfrac{u^4}{4}\right]_0^1 = 2\pi \cdot \dfrac{1}{4} = \dfrac{\pi}{2}.
      Method:
      Set up V=πy2dxV = \pi \int y^2 \, dx, use sin2x=2sinxcosx\sin 2x = 2 \sin x \cos x, substitute u=cosxu = \cos x, and integrate.
      Examiner tips
      • sin2x\sin 2x inside an integral with cosx\cos x powers usually invites the substitution u=cosxu = \cos x
      • Reverse limits if the substitution flips them, or change the sign of dudu

    Sit this paper in the app

    Timed mock papers, instant marking and worked solutions for every question, free.

    Practise in the app