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Mathematics 9709/42 October/November 2023: question paper and mark scheme

Cambridge AS & A Level Mathematics (9709), Paper 4 Mechanics, October/November 2023. Read both free below, or download them. Done the paper? Get it marked by AI against this mark scheme.

9709_w23_qp_429709_w23_ms_429709/42/O/N/23

Paper
Paper 4 Mechanics
Total marks
50
Time
1 hour 15 minutes
Code on the paper
9709/42/O/N/23
9709_w23_ms_42.pdf

9709/42 mark scheme, question by question

Each question as it's printed, and the mark scheme's points for it, as text. Diagrams, tables and graphs are in the PDFs above.

Question 14 marks

Question

A block of mass 15 kg slides down a line of greatest slope of an inclined plane. The top of the plane is at a vertical height of 1.6 m above the level of the bottom of the plane. The speed of the block at the top of the plane is 2 m s−1 and the speed of the block at the bottom of the plane is 4 m s−1 . Find the work done against the resistance to motion of the block. [4]

Mark scheme

1 1 1 B1 For KE at top or bottom. ± × 15 × 22 [ = ±30] ± × 15 × 42 [ = ±120] Need not be evaluated. 2 2 1 × 15 × ( 4 − 2 ) is B0. 2 2 ±15 g × 1.6 [ = ±240 ] B1 For PE change. Need not be evaluated. 240 + 30 = 120 + W M1 Attempt at work energy equation; 4 relevant terms; dimensionally correct; allow sign errors. 1 × 15 × ( 4 − 2 ) is M0. 2 2 If W = F times a numerical distance seen, then M0. Work done = 150 J A1 1 Alternative method for Q1 1.6 *M1 Attempt to use v 2 = u 2 + 2as with 4 2 = 2 2 + 2a × sin θ 1.6 1.6 s= or but not sin θ cos θ s = 1.6sinθ or 1.6cosθ or 1.6 . If θ is given a value, then M0. Must be using speeds 2 and 4 here. 15g sin θ − R = 15a DM1 3 terms; allow sign errors; allow sin/cos mix but weight must be resolved; dimensionally correct. R = 93.75sinθ A1 R = 93.75cosθ Must be consistent with their s . 1.6 A1 Work done = 93.75sin θ × = 150 J sin θ 4

Question 25 marks

Question

A 30Å R 2N m kg 40Å B The diagram shows a smooth ring R, of mass m kg, threaded on a light inextensible string. A horizontal force of magnitude 2 N acts on R. The ends of the string are attached to fixed points A and B on a vertical wall. The part AR of the string makes an angle of 30Å with the vertical, the part BR makes an angle of 40Å with the vertical and the string is taut. The ring is in equilibrium. Find the tension in the string and find the value of m. [5]

Mark scheme

2 Attempt to resolve in at least one direction to form an equation. *M1 Correct number of terms; allow sign errors; allow sin/cos mix; allow with different T ’s. T sin30 + T sin40 − 2 = 0 A1 If different T ’s then allow M1A1A0 max. T cos30 − T cos 40 − mg = 0 A1 Allow with their T. Attempt to solve for T or m DM1 From equation(s) with correct number of relevant terms. Tension T = 1.75, m = 0.0175 A1 T = 1.7501 m = 0.017497 awrt 1.75 for T www, and awrt 0.0175 for m www. 5

Question 35 marks

Question

120 N 20Å 10 kg 30Å A block of mass 10 kg is at rest on a rough plane inclined at an angle of 30Å to the horizontal. A force of 120 N is applied to the block at an angle of 20Å above a line of greatest slope (see diagram). There is a force resisting the motion of the block and 200 J of work is done against this force when the block has moved a distance of 5 m up the plane from rest. Find the speed of the block when it has moved a distance of 5 m up the plane from rest. [5]

Mark scheme

3 Work done by 120 N force = 120 × 5cos 20 [ = 563.81557.] B1 ( PE change = )10 g × 5sin 30 [ = 250] B1 For PE change. Attempt at work energy equation M1 4 relevant terms; dimensionally correct; allow sign errors; allow sin/cos mix in relevant resolved terms. 1 A1 120 × 5cos 20 − 10 g × 5sin 30 − 200 = × 10 × v 2 2 563.815− 250 − 200 = 5v 2 Speed = 4.77 m s–1 A1 awrt 4.77. 3 Alternative method for Question 3 200 *B1 oe e.g. 5 × RF = 200 . Resistive force = [ = 40] 5 120 cos 20 − RF − 10 g sin30 = 10a *M1 4 relevant terms; dimensionally correct; allow sign errors; allow sin/cos mix; allow with their resistive force or just RF. a = 2.276… A1 Allow arwt 2.3 to 2sf from correct work. v2 = 0 + 2 × ( 2.276) × 5 DM1 Use of v 2 = u 2 + 2as using u = 0 , s = 5 and their positive a which has come from a resistive force using work done. Speed = 4.77 m s–1 A1 awrt 4.77. 5

Question 47 marks

Question

A particle P of mass 0.2 kg lies at rest on a rough horizontal plane. A horizontal force of 1.2 N is applied to P. (a) Given that P is in limiting equilibrium, find the coefficient of friction between P and the plane. [3] (b) Given instead that the coefficient of friction between P and the plane is 0.3, find the distance travelled by P in the third second of its motion. [4]

Mark scheme

4(a) R = 0.2g B1 1.2 = μ × 0.2g M1 Resolve horizontally and using F = µR to get an equation in µ; 2 relevant terms. µ = 0.6 A1 oe 3 4(b) 1.2 − 0.3 × 0.2 g = 0.2a *M1 Resolve horizontally using Newton’s Second Law; 3 relevant terms; allow sign errors; R = 0.2 g only. a=3 A1 0.6 = 0.2a only seen, allow with BOD, but if 0.6 as friction being used as resultant force, this is M0A0. 1 1 DM1 1 s3 = 0 + × 3 × 32 [ = 13.5] s2 = 0 + × 3 × 22 [= 6] For use of s = ut + at 2 (or a 2 2 2 complete method) to find a distance at least once with u = 0 and their positive a and t = 2 or t = 3 . Distance = 13.5 − 6 = 7.5 m A1 www 4

Question 58 marks

Question

A particle A of mass 0.5 kg is projected vertically upwards from horizontal ground with speed 25 m s−1 . (a) Find the speed of A when it reaches a height of 20 m above the ground. [2] When A reaches a height of 20 m, it collides with a particle B of mass 0.3 kg which is moving downwards in the same vertical line as A with speed 32.5 m s−1 . In the collision between the two particles, B is brought to instantaneous rest. (b) Show that the velocity of A immediately after the collision is 4.5 m s−1 downwards. [2] (c) Find the time interval between A and B reaching the ground. You should assume that A does not bounce when it reaches the ground. [4]

Mark scheme

5(a) v2 = 252 + 2 ( − g ) × 20 M1 Use of v 2 = u 2 + 2as with u = 25 , s = 20 and a = ± g. 1 1 OR using change in KE = ± change OR × 0.5 × v 2 = × 0.5 × 252 − 0.5 × g × 20 2 2 in PE. Speed = 15 m s-1 A1 2 5(b) Taking up as positive direction: 0.5 × 15 + 0.3 × ( −32.5 ) = 0.5v + 0 or M1 For use of conservation of momentum, 3 non-zero terms, allow sign errors, using their speed Taking down as positive direction: 0.5 × ( −15 ) + 0.3 × 32.5 = 0.5v + 0 15 m s-1. Must show how ±2.25 is obtained. [Taking up as positive direction: velocity of A = −4.5 m s−1] A1 Any error seen in calculating v is [Taking down as positive direction: velocity of A = 4.5 m s−1] A0. Speed = 4.5 m s–1 direction downwards Must explicitly say 4.5 m s–1 and downwards. 2 5(c) 1 M1 Using constant acceleration Downwards to be positive, for A 20 = 4.5t A + gt A2 and solve for t A formula(e) to get a correct equation 2 1 in t A and solve for t A . Upwards to be positive, for A −20 = −4.5t A − gt A2 and solve for t A If using quadratic formula, must be 2 the correct formula. If factorising, when brackets expanded, 2 terms correct. 1 M1 Using constant acceleration For B 20 = 0 + gtB 2 [t = 2] and solve for t B formula(e) to get a correct equation 2 in t B and solve for t B . t A = 1.6 or t B = 2 A1 Difference = 0.4 s only A1 4

Question 69 marks

Question

A railway engine of mass 120 000 kg is towing a coach of mass 60 000 kg up a straight track inclined at an angle of ! to the horizontal where sin ! = 0.02. There is a light rigid coupling, parallel to the track, connecting the engine and coach. The driving force produced by the engine is 125 000 N and there are constant resistances to motion of 22 000 N on the engine and 13 000 N on the coach. (a) Find the acceleration of the engine and find the tension in the coupling. [5] At an instant when the engine is travelling at 30 m s−1 , it comes to a section of track inclined upwards at an angle " to the horizontal. The power produced by the engine is now 4 500 000 W and, as a result, the engine maintains a constant speed. (b) Assuming that the resistance forces remain unchanged, find the value of ". [4]

Mark scheme

6(a) Engine: 125000 − 120000 g × 0.02 − 22000 − T = 120000a *M1 Attempt at Newton’s second law at 125000 − 120000 g sin (1.145..) − 22000 − T = 120000a least once; correct number of relevant terms; allow sign errors; [125000 − 24000 − 22000 − T = 120000a 79000 − T = 120000a ] allow sin/cos mix; allow g missing; a value for α or sinα must Coach: T − 60000 g × 0.02 − 13000 = 60000a be substituted. T − 60000 g sin (1.145..) − 13000 = 60000 a Allow with α = 1.1 or better [T − 12000 − 13000 = 60000a T − 25000 = 60000a ] [α = 1.145991998]. A1 Any equations correct. System: 125000 − 120000 g × 0.02 − 60000 g × 0.02 − 22000 − 13000 = (120000 + 60000 ) a A1 Two equations correct. 125000 − 120000 gsin (1.145..) − 60000 gsin (1.145..) − 22000 − 13000 = (120000 + 60000 ) a If using separate equations for 125000 − 24000 − 12000 − 22000 − 13000 = (120000 + 60000 ) a 54000 = 180000a engine and coach and different T ’s, then allow M1A1A0 max. Solve for T or a DM1 Using equations with the correct number of relevant terms. If no working seen, must be solutions to their equation(s) to be awarded M1. Acceleration = 0.3 m s–2 A1 Allow 0.299 from use of α = 1.15. and Awrt 43000 to 3sf from correct work. Tension = 43 000 N 5 6(b) 4500000 B1 P Driving force, DF = [ = 150000] Use of F = , 30 v oe e.g. DF × 30 = 4500000 . Attempt to resolve parallel to the track once if using system equation, twice if using equations for M1 Correct number of relevant terms; engine and coach separately allow sign errors; allow sin/cos mix; allow g missing. Must be correct number of equations depending on method. System: 150000 − 120000gsinβ − 60000gsinβ − 22000 − 13000 = 0 A1 Allow DF or their DF. or for Engine: 150000 − 120000 gsinβ − 22000 − T ' = 0 and Coach: T '− 60000 gsinβ − 13000 = 0 Must be using same T ' . Solve to get β = 3.7° A1 3.663058552 awrt 3.7° www. 4

Question 712 marks

Question

A particle X travels in a straight line. The velocity of X at time t s after leaving a fixed point O is denoted by v m s−1 , where v = −0.1t3 + 1.8t2 − 6t + 5.6. The acceleration of X is zero at t = p and t = q, where p < q. (a) Find the value of p and the value of q. [4] It is given that the velocity of X is zero at t = 14. (b) Find the velocities of X at t = p and at t = q, and hence sketch the velocity-time graph for the motion of X for 0 ≤ t ≤ 15. [3] (c) Find the total distance travelled by X between t = 0 and t = 15. [5] Additional Page If you use the following lined page to complete the answer(s) to any question(s), the question number(s) must be clearly shown.

Mark scheme

7(a) Attempt to differentiate v *M1 Decrease power by 1 and a change in coefficient in at least one term (which must be the same term); allow unsimplified; allow p or q for t . v a = is M0. t dv A1 May be unsimplified. a = = 3 × −0.1t 3−1 + 2 × 1.8t 2−1 − 6t1−1 = −0.3t 2 + 3.6t − 6 Allow p or q for t. dt dv DM1 Allow p or q for t. Setting a = = 0 and attempt to solve a 3 term quadratic for t. dt Must get 2 values or numerical dv expressions for t from their three a = dt = 0 3t − 36t + 60 = 0 t − 12t + 20 = 0 2 2 term quadratic. If using quadratic formula, must be the correct formula. If factorising, when brackets expanded, 2 terms correct. p = 2, q = 10 A1 4 7(b) Velocities are 0 m s-1 and 25.6 m s-1 B1 SOI Curve with single minimum turning point followed by single maximum turning point *B1 Ignore placement of graph on axes Not a cusp for the minimum point or maximum point. DB1 All correct in 1st and 4th quadrant. Must go from convex to concave. Need to label 2 and 14 on the t-axis where the curve meets the t-axis. Do not need to show exact velocities at t = 0 or t = 10 or t = 15. Ignore graph outside 0 t 15 . 3 7(c) Attempt to integrate v *M1 Increase power by 1 and a change in coefficient in at least one term (which must be the same term); s = vt is M0. 0.1 3+1 1.8 2+1 6 1+1 A1 May be unsimplified. ( s =) − t + t − t + 5.6t ( +c ) 4 3 2 = −0.025t + 0.6t − 3t + 5.6t [+c] 4 3 2 Attempt distance from t = 0 to t = 14 [= 176.4] DM1 Correct use of limits 0 and 14 for their s, i.e. F (14 ) − F ( 0 ) May see limits 0 to 2 and 2 to 14 used but must be ( F (14) − F ( 2)) + ( F ( 2) − F (0)). Attempt distance from t = 14 to t = 15 [= (-) 8.025] DM1 Correct use of limits 14 and 15 for their s, i.e. ± ( F (15) − F (14) ). 18 For reference F ( 2 ) = = 3.6 , 5 882 F (14 ) = = 176.4 and 5 1347 F (15) = = 168.375. 8 7377 A1 www Total distance =176.4 + 8.025 = 184.425 m = Condone 184 or better. 40 7(c) SC for those who show no integration. Max 3 marks. 14 B1 ( −0.1t + 1.8t − 6t + 5.6) dt = 176.4 3 2 0 15 B1 ( −0.1t + 1.8t − 6t + 5.6) dt = −8.025 3 2 14 15 ( −0.1t + 1.8t − 6t + 5.6 ) dt = 8.025 3 2 OR 14 7377 B1 Condone 184 or better. Total distance =176.4 + 8.025 = 184.425 m = 40 SC for those who show no integration and don’t consider the 2 areas. Max 1 mark. 15 7377 B1 Condone 184 or better. 0 −0.1t 3 + 1.8t 2 − 6t + 5.6 dt = 184.425 m = 40 5

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On this page, free: the mark scheme for AS & A Level Mathematics 9709/42, October/November 2023 (9709_w23_ms_42), and the question paper (9709_w23_qp_42), to read or download, with each question's marking points written out underneath.

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Mathematics 9709/42 for October/November 2023 is out of 50 marks, with 1 hour 15 minutes to answer it.

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