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

    Mathematics (9709)

    9709/32 May/June 2025 Worked Answers (A-Level Maths 9709 A2)

    17 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 17 questions
    1. Step 1: Multiply both sides by (ex−3)(e^x - 3): ex+2e−x=4ex−12e^x + 2e^{-x} = 4e^x - 12. Step 2: Multiply throughout by exe^x to remove the negative exponent: e2x+2=4e2x−12exe^{2x} + 2 = 4e^{2x} - 12 e^x, hence 3e2x−12ex−2=03e^{2x} - 12e^x - 2 = 0. Step 3: Let u=exu = e^x. Solve 3u2−12u−2=03u^2 - 12u - 2 = 0: u=12±144+246=6±423u = \dfrac{12 \pm \sqrt{144 + 24}}{6} = \dfrac{6 \pm \sqrt{42}}{3}. Step 4: Reject the negative root (since u=ex>0u = e^x > 0). Take u=6+423≈4.1602u = \dfrac{6+\sqrt{42}}{3} \approx 4.1602. Step 5: x=ln⁡u≈ln⁡(4.1602)≈1.426x = \ln u \approx \ln(4.1602) \approx 1.426 (3 d.p.).
      Method:
      Clear the denominator and multiply by exe^x to obtain a quadratic in exe^x, solve it, reject the negative root, and take the natural log.
      Examiner tips
      • Always multiply by exe^x to convert e−xe^{-x} before forming a quadratic
      • Reject negative roots of the quadratic since ex>0e^x > 0
    2. Step 1: Use the binomial series (1+u)n=1+nu+n(n−1)2u2+…(1+u)^n = 1 + nu + \dfrac{n(n-1)}{2}u^2 + \dots with n=−32n = -\dfrac{3}{2}, u=−2xu = -2x. Step 2: Linear term: (−32)(−2x)=3x\left(-\dfrac{3}{2}\right)(-2x) = 3x. Quadratic term: (−3/2)(−5/2)2(−2x)2=15/42⋅4x2=152x2\dfrac{(-3/2)(-5/2)}{2}(-2x)^2 = \dfrac{15/4}{2}\cdot 4x^2 = \dfrac{15}{2}x^2. Step 3: Hence (1−2x)−3/2=1+3x+152x2+…(1-2x)^{-3/2} = 1 + 3x + \dfrac{15}{2}x^2 + \dots. Step 4: Multiply by (6−x)(6-x), keeping terms up to x2x^2: 6 ⁣(1+3x+152x2)−x(1+3x)=6+18x+45x2−x−3x26\!\left(1 + 3x + \dfrac{15}{2}x^2\right) - x(1 + 3x) = 6 + 18x + 45x^2 - x - 3x^2. Step 5: Simplify: 6+17x+42x26 + 17x + 42x^2.
      Method:
      Expand (1−2x)−3/2(1-2x)^{-3/2} to three terms using the rational-index binomial series, then multiply by (6−x)(6-x) keeping only terms up to x2x^2.
      Examiner tips
      • Always expand (1+u)n(1+u)^n first; substitute u=−2xu = -2x at the end
      • Track all x2x^2 contributions, including the cross term from (−x)⋅3x(-x) \cdot 3x
    3. Step 1: The series (1+u)n(1+u)^n for non-integer nn converges if and only if ∣u∣<1|u| < 1. Step 2: Here u=−2xu = -2x, so the requirement is ∣−2x∣<1|-2x| < 1, i.e. ∣x∣<12|x| < \dfrac{1}{2}. Step 3: This is a strict inequality (the series does not converge at ∣u∣=1|u| = 1).
      Method:
      Apply the convergence condition ∣u∣<1|u| < 1 for the binomial series with u=−2xu = -2x.
      Examiner tips
      • The validity condition is always ∣u∣<1|u| < 1 where uu is the bracket inside
      • It is a strict inequality
    4. Step 1: Use the identity cot⁡2x=1−tan⁡2x2tan⁡x\cot 2x = \dfrac{1-\tan^2 x}{2\tan x}. The equation becomes 3tan⁡x−4(1−tan⁡2x)2tan⁡x=3\dfrac{3}{\tan x} - \dfrac{4(1-\tan^2 x)}{2\tan x} = 3, i.e. 3−2(1−tan⁡2x)tan⁡x=3\dfrac{3 - 2(1-\tan^2 x)}{\tan x} = 3. Step 2: Simplify the numerator: 3−2+2tan⁡2x=1+2tan⁡2x3 - 2 + 2\tan^2 x = 1 + 2\tan^2 x, so 1+2tan⁡2xtan⁡x=3\dfrac{1 + 2\tan^2 x}{\tan x} = 3. Step 3: Multiply by tan⁡x\tan x: 2tan⁡2x−3tan⁡x+1=02\tan^2 x - 3\tan x + 1 = 0. Step 4: Factorise: (2tan⁡x−1)(tan⁡x−1)=0(2\tan x - 1)(\tan x - 1) = 0, so tan⁡x=12\tan x = \dfrac{1}{2} or tan⁡x=1\tan x = 1. Step 5: In the interval [0°,180°][0°, 180°]: tan⁡x=1⇒x=45°\tan x = 1 \Rightarrow x = 45°; tan⁡x=12⇒x≈26.6°\tan x = \dfrac{1}{2} \Rightarrow x \approx 26.6°. (The other branches lie outside the interval since tan⁡\tan is negative there.)
      Method:
      Substitute the double-angle identity for cot⁡2x\cot 2x, simplify into a quadratic in tan⁡x\tan x, factorise, and read off the values in [0°,180°][0°, 180°].
      Examiner tips
      • Convert all trig terms to tan⁡x\tan x using a single identity
      • Both roots of the quadratic must be tested in the given interval
    5. Step 1: Let (x+iy)2=−1−45 i(x + iy)^2 = -1 - 4\sqrt{5}\,i. Expanding: x2−y2+2ixy=−1−45 ix^2 - y^2 + 2ixy = -1 - 4\sqrt{5}\,i. Step 2: Equate real and imaginary parts: x2−y2=−1x^2 - y^2 = -1 and 2xy=−452xy = -4\sqrt{5}, hence xy=−25xy = -2\sqrt{5}, so y=−25xy = -\dfrac{2\sqrt{5}}{x}. Step 3: Substitute: x2−20x2=−1x^2 - \dfrac{20}{x^2} = -1. Multiply by x2x^2: x4+x2−20=0x^4 + x^2 - 20 = 0. Step 4: Factorise: (x2−4)(x2+5)=0(x^2 - 4)(x^2 + 5) = 0. Since xx is real, x2=4x^2 = 4, so x=±2x = \pm 2. Step 5: Then y=−25x=∓5y = -\dfrac{2\sqrt{5}}{x} = \mp \sqrt{5}. Hence the two square roots are 2−5 i2 - \sqrt{5}\,i and −2+5 i-2 + \sqrt{5}\,i, i.e. ±(2−5 i)\pm(2 - \sqrt{5}\,i). Verify: (2−5 i)2=4−45 i+5i2=−1−45 i(2 - \sqrt{5}\,i)^2 = 4 - 4\sqrt{5}\,i + 5 i^2 = -1 - 4\sqrt{5}\,i. ✓
      Method:
      Set (x+iy)2(x+iy)^2 equal to the given complex number, equate real and imaginary parts to form a quartic in xx, solve for real xx, then back-substitute to find yy.
      Examiner tips
      • Always verify by squaring the candidate root
      • The two square roots of any non-zero complex number are negatives of each other
    6. Step 1: Define f(x)=∣x−2∣−2sin⁡ ⁣(12x)f(x) = |x - 2| - 2 \sin\!\left(\tfrac{1}{2}x\right). A root of ∣x−2∣=2sin⁡(x/2)|x-2| = 2 \sin(x/2) corresponds to f(x)=0f(x) = 0. Step 2: At x=1x = 1: ∣1−2∣=1|1-2| = 1 and 2sin⁡(0.5)≈2(0.4794)≈0.95892 \sin(0.5) \approx 2(0.4794) \approx 0.9589. So f(1)≈1−0.9589≈0.0411>0f(1) \approx 1 - 0.9589 \approx 0.0411 > 0. Step 3: At x=1.5x = 1.5: ∣1.5−2∣=0.5|1.5-2| = 0.5 and 2sin⁡(0.75)≈2(0.6816)≈1.36332 \sin(0.75) \approx 2(0.6816) \approx 1.3633. So f(1.5)≈0.5−1.3633≈−0.8633<0f(1.5) \approx 0.5 - 1.3633 \approx -0.8633 < 0. Step 4: Since ff is continuous on [1,1.5][1, 1.5] and changes sign, by the Intermediate Value Theorem there is a root in (1,1.5)(1, 1.5).
      Method:
      Form f(x)f(x) as the difference of the two sides, evaluate at x=1x = 1 and x=1.5x = 1.5, observe the sign change, and conclude that a root lies in the interval.
      Examiner tips
      • Set the calculator to radians
      • State the conclusion in words: a sign change indicates a root in the interval
    7. Step 1: With calculator in radians, compute x2=2−2sin⁡(1.03/2)=2−2sin⁡(0.515)≈2−2(0.4926)≈1.0149x_2 = 2 - 2 \sin(1.03/2) = 2 - 2 \sin(0.515) \approx 2 - 2(0.4926) \approx 1.0149. Step 2: x3=2−2sin⁡(1.0149/2)≈2−2(0.4860)≈1.0281x_3 = 2 - 2 \sin(1.0149/2) \approx 2 - 2(0.4860) \approx 1.0281. Step 3: x4≈1.0166x_4 \approx 1.0166, x5≈1.0266x_5 \approx 1.0266, x6≈1.0179x_6 \approx 1.0179, x7≈1.0255x_7 \approx 1.0255, ... Step 4: The iterates oscillate around 1.021.02, with sign change in (1.015,1.025)(1.015, 1.025). Hence the root to 2 d.p. is 1.021.02.
      Method:
      Iterate using a calculator in radians, recording each iterate to 4 d.p., until the sequence has clearly converged to 2 d.p.
      Examiner tips
      • Set calculator to radians
      • Show intermediate iterates to 4 d.p. to justify the 2 d.p. answer
    8. Question 7a

      3 marksR-Formula (Harmonic Form)
      Step 1: Match Rcos⁡(θ−α)=Rcos⁡αcos⁡θ+Rsin⁡αsin⁡θR \cos(\theta - \alpha) = R \cos\alpha \cos\theta + R \sin\alpha \sin\theta with 7sin⁡θ+24cos⁡θ7 \sin\theta + 24 \cos\theta. So Rcos⁡α=24R \cos\alpha = 24 and Rsin⁡α=7R \sin\alpha = 7. Step 2: R=242+72=576+49=625=25R = \sqrt{24^2 + 7^2} = \sqrt{576 + 49} = \sqrt{625} = 25. Step 3: tan⁡α=Rsin⁡αRcos⁡α=724\tan\alpha = \dfrac{R \sin\alpha}{R \cos\alpha} = \dfrac{7}{24}. Step 4: α=tan⁡−1(7/24)≈0.2838\alpha = \tan^{-1}(7/24) \approx 0.2838 radians (4 d.p.).
      Method:
      Expand Rcos⁡(θ−α)R\cos(\theta-\alpha), match coefficients with the original expression, take Pythagorean sum for RR, and take inverse tangent for α\alpha.
      Examiner tips
      • R2R^2 is always the sum of squares of the two coefficients
      • Match terms: for Rcos⁡(θ−α)R\cos(\theta - \alpha), tan⁡α=(coefficient of sin⁡θ)/(coefficient of cos⁡θ)\tan\alpha = (\text{coefficient of }\sin\theta)/(\text{coefficient of }\cos\theta)
    9. Step 1: Substitute θ=x/3\theta = x/3: 7sin⁡(x/3)+24cos⁡(x/3)=25cos⁡(x/3−0.2838)7 \sin(x/3) + 24 \cos(x/3) = 25 \cos(x/3 - 0.2838). The equation becomes 25cos⁡(x/3−0.2838)=24.525 \cos(x/3 - 0.2838) = 24.5, so cos⁡(x/3−0.2838)=0.98\cos(x/3 - 0.2838) = 0.98. Step 2: Take inverse cosine: x/3−0.2838=±cos⁡−1(0.98)≈±0.2003x/3 - 0.2838 = \pm \cos^{-1}(0.98) \approx \pm 0.2003 (principal values). Step 3: Solve: x/3=0.2838+0.2003=0.4841x/3 = 0.2838 + 0.2003 = 0.4841 or x/3=0.2838−0.2003=0.0835x/3 = 0.2838 - 0.2003 = 0.0835. Step 4: Multiply by 3: x≈1.45x \approx 1.45 or x≈0.250x \approx 0.250. Both lie in 0<x<π0 < x < \pi.
      Method:
      Rewrite using the harmonic form, isolate the cosine, take both branches of the inverse cosine, then multiply by 3 and select solutions in the given interval.
      Examiner tips
      • Use both +cos⁡−1+\cos^{-1} and −cos⁡−1-\cos^{-1} to capture all solutions
      • Multiply through by 3 at the end since the inner argument is x/3x/3
    10. Step 1: Separate variables: dx4x+3=cos⁡2θsin⁡2θdθ=cot⁡2θ dθ\dfrac{dx}{4x+3} = \dfrac{\cos 2\theta}{\sin 2\theta} d\theta = \cot 2\theta \, d\theta. Step 2: Integrate: 14ln⁡∣4x+3∣=12ln⁡∣sin⁡2θ∣+c\dfrac{1}{4}\ln|4x+3| = \dfrac{1}{2}\ln|\sin 2\theta| + c. Step 3: Apply initial condition x=0x = 0, θ=π/12\theta = \pi/12 (so 2θ=π/62\theta = \pi/6 and sin⁡2θ=1/2\sin 2\theta = 1/2): 14ln⁡3=12ln⁡(1/2)+c\dfrac{1}{4}\ln 3 = \dfrac{1}{2}\ln(1/2) + c, hence c=14ln⁡3+12ln⁡2c = \dfrac{1}{4}\ln 3 + \dfrac{1}{2}\ln 2. Step 4: Multiply through by 4: ln⁡(4x+3)=2ln⁡∣sin⁡2θ∣+ln⁡3+2ln⁡2=ln⁡(12sin⁡22θ)\ln(4x+3) = 2 \ln|\sin 2\theta| + \ln 3 + 2 \ln 2 = \ln(12 \sin^2 2\theta). Step 5: Exponentiate: 4x+3=12sin⁡22θ4x + 3 = 12 \sin^2 2\theta, so x=12sin⁡22θ−34x = \dfrac{12 \sin^2 2\theta - 3}{4}.
      Method:
      Separate the variables, integrate both sides (using ∫cot⁡2θ=12ln⁡∣sin⁡2θ∣\int \cot 2\theta = \dfrac{1}{2}\ln|\sin 2\theta|), apply the initial condition to find the constant, then exponentiate and solve for xx.
      Examiner tips
      • Multiply your log equation by the LCM (here, 4) before exponentiating to avoid fractional exponents
      • Combine all log constants before exponentiating to avoid algebra slips
    11. Question 9a

      2 marksVector Equation of a Line
      Step 1: A vector line equation uses one point on the line and a direction vector. Step 2: Use AA as the point: position vector (1,−4,2)(1, -4, 2). Step 3: The direction is AB⃗=OB⃗−OA⃗=(−2−1,1−(−4),3−2)=(−3,5,1)\vec{AB} = \vec{OB} - \vec{OA} = (-2-1, 1-(-4), 3-2) = (-3, 5, 1). Step 4: So r=(1,−4,2)+λ(−3,5,1)\mathbf{r} = (1, -4, 2) + \lambda(-3, 5, 1). (Equivalent forms with different point or scaled direction are also valid lines.)
      Method:
      Use point AA and the direction vector AB⃗=OB⃗−OA⃗\vec{AB} = \vec{OB} - \vec{OA} to write the line in the form r=a+λd\mathbf{r} = \mathbf{a} + \lambda \mathbf{d}.
      Examiner tips
      • Always write r=...\mathbf{r} = ..., not λ=...\lambda = ...
      • Direction is the difference of position vectors
    12. Step 1: Compute AB⃗=OB⃗−OA⃗=(−3,5,1)\vec{AB} = \vec{OB} - \vec{OA} = (-3, 5, 1) and AC⃗=OC⃗−OA⃗=(1,7,3)\vec{AC} = \vec{OC} - \vec{OA} = (1, 7, 3). Step 2: Scalar product: AB⃗⋅AC⃗=(−3)(1)+(5)(7)+(1)(3)=−3+35+3=35\vec{AB} \cdot \vec{AC} = (-3)(1) + (5)(7) + (1)(3) = -3 + 35 + 3 = 35. Step 3: Magnitudes: ∣AB⃗∣=9+25+1=35|\vec{AB}| = \sqrt{9+25+1} = \sqrt{35} and ∣AC⃗∣=1+49+9=59|\vec{AC}| = \sqrt{1+49+9} = \sqrt{59}. Step 4: Hence cos⁡BAC=353559=352065=3559=3559\cos BAC = \dfrac{35}{\sqrt{35}\sqrt{59}} = \dfrac{35}{\sqrt{2065}} = \dfrac{\sqrt{35}}{\sqrt{59}} = \sqrt{\dfrac{35}{59}}.
      Method:
      Calculate the scalar product of AB⃗\vec{AB} and AC⃗\vec{AC}, divide by the product of their magnitudes, and simplify the surd.
      Examiner tips
      • cos⁡θ=u⃗⋅v⃗∣u⃗∣∣v⃗∣\cos\theta = \dfrac{\vec{u}\cdot\vec{v}}{|\vec{u}||\vec{v}|} — denominator is the product of moduli, not their squares
      • Simplify 353559=3559\dfrac{35}{\sqrt{35}\sqrt{59}} = \sqrt{\dfrac{35}{59}} for an exact form
    13. Step 1: Area of a triangle using two sides and included angle: Area=12∣AB⃗∣∣AC⃗∣sin⁡BAC\text{Area} = \tfrac{1}{2}|\vec{AB}||\vec{AC}|\sin BAC. Step 2: From cos⁡2BAC=3559\cos^2 BAC = \dfrac{35}{59}: sin⁡2BAC=1−3559=2459\sin^2 BAC = 1 - \dfrac{35}{59} = \dfrac{24}{59}, so sin⁡BAC=2459\sin BAC = \sqrt{\dfrac{24}{59}} (positive in a triangle). Step 3: Substitute: Area=1235⋅59⋅2459=1235⋅24\text{Area} = \tfrac{1}{2} \sqrt{35} \cdot \sqrt{59} \cdot \sqrt{\dfrac{24}{59}} = \tfrac{1}{2} \sqrt{35 \cdot 24} (the 5959 cancels). Step 4: Simplify: 35⋅24=840=4⋅210=2210\sqrt{35 \cdot 24} = \sqrt{840} = \sqrt{4 \cdot 210} = 2\sqrt{210}. Hence Area =12⋅2210=210= \tfrac{1}{2} \cdot 2\sqrt{210} = \sqrt{210}.
      Method:
      Apply Area =12∣AB⃗∣∣AC⃗∣sin⁡BAC= \tfrac{1}{2}|\vec{AB}||\vec{AC}|\sin BAC, find sin⁡\sin from cos⁡\cos via the Pythagorean identity, and simplify the resulting surd.
      Examiner tips
      • Convert cos⁡\cos to sin⁡\sin exactly using sin⁡2+cos⁡2=1\sin^2 + \cos^2 = 1, then simplify the surd
      • Watch out for fortuitous cancellations like the 59\sqrt{59} in this problem
    14. Question 10a

      2 marksPolynomial Division
      Step 1: Write x2=q(1+4x2)+rx^2 = q(1 + 4x^2) + r where qq is constant (the quotient) and rr is constant (the remainder, of degree less than the divisor's leading x2x^2 term). Step 2: Compare x2x^2 coefficients: 1=4q1 = 4q, so q=14q = \dfrac{1}{4}. Step 3: Compare constants: 0=q+r=14+r0 = q + r = \dfrac{1}{4} + r, so r=−14r = -\dfrac{1}{4}. Step 4: Verify: 14(1+4x2)−14=14+x2−14=x2\dfrac{1}{4}(1 + 4x^2) - \dfrac{1}{4} = \dfrac{1}{4} + x^2 - \dfrac{1}{4} = x^2. ✓
      Method:
      Write the division as an identity, compare coefficients of like powers of xx to find both the quotient and remainder.
      Examiner tips
      • When the dividend has the same degree as the divisor, the quotient is a non-zero constant
      • Always verify by multiplying back
    15. Step 1: Apply integration by parts with u=tan⁡−1(2x)u = \tan^{-1}(2x) (du=21+4x2dxdu = \dfrac{2}{1+4x^2}dx) and dv=x dxdv = x\,dx (v=x22v = \dfrac{x^2}{2}): ∫xtan⁡−1(2x) dx=x22tan⁡−1(2x)−∫x21+4x2dx\int x \tan^{-1}(2x)\,dx = \dfrac{x^2}{2}\tan^{-1}(2x) - \int \dfrac{x^2}{1+4x^2}dx. Step 2: Use x21+4x2=14−1/41+4x2\dfrac{x^2}{1+4x^2} = \dfrac{1}{4} - \dfrac{1/4}{1+4x^2} (from polynomial division). Integrate: ∫x21+4x2dx=x4−18tan⁡−1(2x)\int \dfrac{x^2}{1+4x^2}dx = \dfrac{x}{4} - \dfrac{1}{8}\tan^{-1}(2x). Step 3: Combine: antiderivative F(x)=x22tan⁡−1(2x)−x4+18tan⁡−1(2x)F(x) = \dfrac{x^2}{2}\tan^{-1}(2x) - \dfrac{x}{4} + \dfrac{1}{8}\tan^{-1}(2x). Step 4: Evaluate F(0.5)F(0.5): 0.252tan⁡−1(1)−0.54+18tan⁡−1(1)=18⋅π4−18+18⋅π4=π32−18+π32=π16−18\dfrac{0.25}{2}\tan^{-1}(1) - \dfrac{0.5}{4} + \dfrac{1}{8}\tan^{-1}(1) = \dfrac{1}{8} \cdot \dfrac{\pi}{4} - \dfrac{1}{8} + \dfrac{1}{8} \cdot \dfrac{\pi}{4} = \dfrac{\pi}{32} - \dfrac{1}{8} + \dfrac{\pi}{32} = \dfrac{\pi}{16} - \dfrac{1}{8}. Step 5: F(0)=0F(0) = 0. So the definite integral =π16−18= \dfrac{\pi}{16} - \dfrac{1}{8}.
      Method:
      Use integration by parts with u=tan⁡−1(2x)u = \tan^{-1}(2x), then integrate x21+4x2\dfrac{x^2}{1+4x^2} using the quotient/remainder from (a), assemble the antiderivative, and substitute the limits.
      Examiner tips
      • Choosing u=tan⁡−1(2x)u = \tan^{-1}(2x) is essential — letting dv=tan⁡−1(2x)dxdv = \tan^{-1}(2x) dx is much harder
      • Use polynomial division to reduce x21+4x2\dfrac{x^2}{1+4x^2} to a polynomial plus a fraction with a simple antiderivative
    16. Step 1: Use the product rule on y=5sin⁡2x⋅cos⁡2xy = 5 \sin 2x \cdot \cos^2 x with ddx(cos⁡2x)=−2sin⁡xcos⁡x=−sin⁡2x\dfrac{d}{dx}(\cos^2 x) = -2 \sin x \cos x = -\sin 2x: dydx=5(2cos⁡2x)cos⁡2x+5sin⁡2x⋅(−sin⁡2x)⋅...\dfrac{dy}{dx} = 5(2\cos 2x) \cos^2 x + 5 \sin 2x \cdot (-\sin 2x) \cdot .... Better: rewrite y=5(2sin⁡xcos⁡x)cos⁡2x=10sin⁡xcos⁡3xy = 5(2\sin x \cos x)\cos^2 x = 10 \sin x \cos^3 x. Step 2: Differentiate: dydx=10cos⁡x⋅cos⁡3x+10sin⁡x⋅3cos⁡2x(−sin⁡x)=10cos⁡4x−30sin⁡2xcos⁡2x\dfrac{dy}{dx} = 10 \cos x \cdot \cos^3 x + 10 \sin x \cdot 3 \cos^2 x (-\sin x) = 10 \cos^4 x - 30 \sin^2 x \cos^2 x. Step 3: Set dydx=0\dfrac{dy}{dx} = 0: 10cos⁡2x(cos⁡2x−3sin⁡2x)=010 \cos^2 x (\cos^2 x - 3 \sin^2 x) = 0. With 0<x<π/20 < x < \pi/2, cos⁡x≠0\cos x \ne 0, so cos⁡2x=3sin⁡2x\cos^2 x = 3 \sin^2 x. Step 4: Hence sin⁡2xcos⁡2x=13\dfrac{\sin^2 x}{\cos^2 x} = \dfrac{1}{3}, i.e. tan⁡2x=13\tan^2 x = \dfrac{1}{3}, so tan⁡x=13\tan x = \dfrac{1}{\sqrt{3}} (positive in (0,π/2)(0, \pi/2)). Step 5: Therefore x=π6x = \dfrac{\pi}{6}. (Confirm MM by checking it is a maximum, not a minimum.)
      Method:
      Rewrite yy using the double-angle identity, differentiate, set the derivative equal to zero, and reduce to a single trig equation.
      Examiner tips
      • Rewriting 5sin⁡2xcos⁡2x=10sin⁡xcos⁡3x5 \sin 2x \cos^2 x = 10 \sin x \cos^3 x often simplifies the differentiation
      • Always verify the stationary point is a maximum (not minimum or boundary)
    17. Step 1: Rewrite using double-angle: 5sin⁡2xcos⁡2x=5⋅2sin⁡xcos⁡x⋅cos⁡2x=10sin⁡xcos⁡3x5 \sin 2x \cos^2 x = 5 \cdot 2 \sin x \cos x \cdot \cos^2 x = 10 \sin x \cos^3 x. Step 2: Substitute u=cos⁡xu = \cos x, so du=−sin⁡x dxdu = -\sin x \, dx. The integral becomes ∫10sin⁡xcos⁡3x dx=−10∫u3 du\displaystyle\int 10 \sin x \cos^3 x \, dx = -10 \int u^3 \, du. Step 3: Update limits: x=0⇒u=1x = 0 \Rightarrow u = 1 and x=π/4⇒u=cos⁡(π/4)=12x = \pi/4 \Rightarrow u = \cos(\pi/4) = \dfrac{1}{\sqrt{2}}. Step 4: Evaluate: −10[u44]11/2=−10((1/2)44−14)=−10(1/44−14)=−10(116−14)-10 \left[\dfrac{u^4}{4}\right]_{1}^{1/\sqrt{2}} = -10 \left(\dfrac{(1/\sqrt{2})^4}{4} - \dfrac{1}{4}\right) = -10 \left(\dfrac{1/4}{4} - \dfrac{1}{4}\right) = -10 \left(\dfrac{1}{16} - \dfrac{1}{4}\right). Step 5: Simplify: −10⋅(−316)=3016=158-10 \cdot \left(-\dfrac{3}{16}\right) = \dfrac{30}{16} = \dfrac{15}{8}.
      Method:
      Rewrite the integrand using the double-angle identity, substitute u=cos⁡xu = \cos x, change the limits, integrate the polynomial in uu, and evaluate.
      Examiner tips
      • Always change limits when substituting, rather than reverting to xx at the end
      • cos⁡4(π/4)=(1/2)4=1/4\cos^4(\pi/4) = (1/\sqrt{2})^4 = 1/4 — keep this exact

    Sit this paper in the app

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

    Practise in the app