Cambridge A Level Mathematics 9709 — 2011 May/June Paper 5 · Variant 3
9709/53/M/J/11 · 7 questions · 50 marks · ≈56 min
The question paper and its mark scheme, free to read here and free to download. This is Cambridge’s own paper, exactly as it was sat.
Question paper4 pages




Mark scheme5 pages
Answers below. Sit the paper first if you are practising.





Questions as text
Q1 · A 60° P 0.2 m A particle P of mass 0.4 kg is attached to a fixed point A by a light…
1 A 60° P 0.2 m A particle P of mass 0.4 kg is attached to a fixed point A by a light inextensible string. The string is inclined at 60◦to the vertical. P moves with constant speed in a horizontal circle of radius 0.2 m. The centre of the circle is vertically below A (see diagram). (i) Show that the tension in the string is 8 N. [2] (ii) Calculate the speed of the particle. [2]
Mark scheme: 1 (i) Tsin30° = 0.4g M1 Resolves vertically T = 8N A1 [2] (ii) Tcos30° = 0.4v 2 / 0.2 ( = 0.4ω 2 × 0.2) M1 Newton’s Second Law radially v = 1.86 ms −1 A1ft ft only on T from part (i) [2] 2 2 2
Q2 · A stone is thrown with speed 15 m s−1 horizontally from the top of a vertical cliff 20 m…
2 A stone is thrown with speed 15 m s−1 horizontally from the top of a vertical cliff 20 m above the sea. Calculate (i) the distance from the foot of the cliff to the point where the stone enters the sea, [3] (ii) the speed of the stone when it enters the sea. [3]
Mark scheme: 2 (i) 20 = gt 2 / 2 (t = 2) M1 y = –gx 2 /(2 × 15 2 ) use of trajectory equation x = 15 × 2 DM1 –20 = –10x 2 / (2 × 15 2 ) x = 30 A1 [3] (ii) v = (g × 2) = 20 B1 v = √(152 + 202) M1 v = 25 A1 [3]
Q3 · F N O 0.4 m 20° A smooth hemispherical shell, with centre O, weight 12 N and radius 0.4…
3 F N O 0.4 m 20° A smooth hemispherical shell, with centre O, weight 12 N and radius 0.4 m, rests on a horizontal plane. A particle of weight W N lies at rest on the inner surface of the hemisphere vertically below O. A force of magnitude F N acting vertically upwards is applied to the highest point of the hemisphere, which is in equilibrium with its axis of symmetry inclined at 20◦to the horizontal (see diagram). (i) Show, by taking moments about O, that F 16.48 correct to 4 significant figures. [3] = (ii) Find the normal contact force exerted by the plane on the hemisphere in terms of W. Hence find the least possible value of W. [3]
Mark scheme: 3 (i) M1 Moments about O F × 0.4sin20° = 12 × (0.4 / 2)cos20° A1 F = 16.48 AG A1 [3] (ii) R = –16.48 + 12 + W B1 Equates forces vertically –16.48 + 12 + W = 0 M1 Works with R = 0 W = 4.48 A1 [3] √ 2 2
Q4 · The ends of a light elastic string of natural length 0.8 m and modulus of elasticity λ N…
4 The ends of a light elastic string of natural length 0.8 m and modulus of elasticity λ N are attached to fixed points A and B which are 1.2 m apart at the same horizontal level. A particle of mass 0.3 kg is attached to the centre of the string, and released from rest at the mid-point of AB. The particle descends 0.32 m vertically before coming to instantaneous rest. (i) Calculate λ. [4] (ii) Calculate the speed of the particle when it is 0.25 m below AB. [4]
Mark scheme: 4 (i) e = √(0.62 + 0.322) – 0.4 ( = 0.28) B1 Extension of half string = 0.28 m 0.3g × 0.32 = 2[λ (0.28 2 – 0.2 2 )] / (2 × 0.4) M1, A1 PE loss = EE gain λ = 10 A1 [4] (ii) e = √(0.62 + 0.252) – 0.4 B1 Extension of half string = 0.25 m 0.3g × 0.25 = 0.3v 2 / 2 + M1 PE loss = KE gain + EE gain 2[10(0.25 2 – 0.2 2 ) / (2 × 0.4)] A1ft N.B. 0.25 is extension of half string v = 1.12 A1 ft on candidates λ only [4]
Q5 · One end of a light elastic string of natural length 0.3 m and modulus of elasticity 6 N…
5 One end of a light elastic string of natural length 0.3 m and modulus of elasticity 6 N is attached to a fixed point O on a smooth horizontal plane. The other end of the string is attached to a particle P of mass 0.2 kg, which moves on the plane in a circular path with centre O. The angular speed of P is ω rad s−1. (i) For the case ω = 5, calculate the extension of the string. [4] (ii) Express the extension of the string in terms of ω, and hence find the set of possible value of ω. [4]
Mark scheme: 5 (i) T = 6e / 0.3 B1 0.2 × 5 2 (0.3 + e) = 6e / 0.3 M1, A1 Newton’s Second Law radially e = 0.1 A1 [4] (ii) 0.2ω 2 (0.3 + e) = 6e / 0.3 M1 Newton’s Second Law radially e = 0.06ω 2/(20 – 0.2ω 2) A1 Other forms acceptable 20 – 0.2ω 2 > 0 M1 Uses denominator > 0 (0 <) ω < 10 A1 Disregard lower limit [4] GCE AS/A LEVEL – May/June 2011 9709 53 2
Q6 · 3 m s–1 P O 0.5 m A O and A are fixed points on a horizontal surface, with OA 0.5 m
6 3 m s–1 P O 0.5 m A O and A are fixed points on a horizontal surface, with OA 0.5 m. A particle P of mass 0.2 kg is = projected horizontally with speed 3 m s−1 from A in the direction OA and moves in a straight line (see diagram). At time t s after projection, the velocity of P is v m s−1 and its displacement from O is x m. 0.4 The coefficient of friction between the surface and P is 0.5, and a force of magnitude N acts on x2 P in the direction PO. (i) Show that, while the particle is in motion, vdv 5 2 . [2] dx = − + x2 (ii) Calculate the distance travelled by P before it comes to rest, and show that P does not subsequently move. [7] [Question 7 is printed on the next page.]
Mark scheme: 6 (i) 0.2a = –0.2g0.5 – 0.4/x 2 M1 Uses Newton’s Second law vdv/dx = –(5 + 2x −)2 AG A1 [2] M1 Separates variables and integrates (ii) ∫vdv = –∫ (5 + 2 x −2 ) d x v 2 /2 = –5x + 2/x ( + c) A1 3 2 /2 = –5 × 0.5 +2/0.5 + c M1 Hence c = 3, or [v 2 / 2] 30 = [–5x + 2/x] 5.0x x = 1 A1 From 0 = –5x + 2/x = 3 Travels ( = 1 – 0.5) = 0.5m A1 F towards O ( 0.4) less than maximum M1, A1 Compares 0.5 × 0.2g and 0.4/1 2 friction ( = 1) [7] 2
Q7 · B a m C a m A 1 m O E D ABCDE is the cross-section through the centre of mass of a…
7 B a m C a m A 1 m O E D ABCDE is the cross-section through the centre of mass of a uniform prism resting in equilibrium with DE on a horizontal surface. The cross-section has the shape of a square OBCD with sides of length a m, from which a quadrant OAE of a circle of radius 1 m has been removed (see diagram). (i) Find the distance of the centre of mass of the prism from O, giving the answer in terms of a, π and √2. [5] (ii) Hence show that 3a2(2 −a) < 32π −2, and verify that this inequality is satisfied by a 1.68 but not by a 1.67. [4] = =
Mark scheme: 7 (i) OG quadrant = 2sin(π /4) / (3π /4) B1 8 / (3 2 π ) a 2 (a 2 /2) = π /4[2sin(π /4) / (3π /4)] M1 –1 each error, min zero +(a 2 – π /4)x A2 There must be 3 moment terms x = 2 2 (3a 3 – 2) / (12a 2 – 3π ) A1 Other forms acceptable [5] (ii) xcos45° > 1 B1 (6a 3 – 4) / (12a 2 – 3π ) > 1 M1 3a 2 (2 – a) < 3π /2 – 2 AG A1 True when a = 1.68, not when a = 1.67 AG B1 RHS = 2.712.. compared with [4] LHS = 2.709.. and 2.76.. respectively
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Cambridge’s own grade thresholds for 2011 May/June, Paper 5 · Variant 3. A higher threshold means an easier paper — the bar moves with how the cohort did.