A Level Further Mathematics 9231 Paper 33, Oct/Nov 2023

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Question paper

9231/33 · Oct/Nov 2023

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1

Two uniform smooth spheres A and B of equal radii have masses m and 2m respectively. The two spheres are moving with equal speeds u on a smooth horizontal surface when they collide. Immediately before the collision, A's direction of motion makes an angle of 60∘ with the line of centres, and B's direction of motion makes an angle θ with the line of centres (see diagram). The coefficient of restitution between the spheres is e. After the collision, the component of the velocity of A along the line of centres is v and B moves perpendicular to the line of centres. Sphere A now has twice as much kinetic energy as sphere B.

Figure 1 of 1 for question 1
a

Show that v=12u(4cos⁡θ−1).

[1]
b

Find the value of cos⁡θ.

[4]
c

Find the value of e.

[2]
2

A ball of mass 2 kg is projected vertically downwards with speed 5 ms−1 through a liquid. At time t s after projection, the velocity of the ball is v ms−1 and its displacement from its starting point is x m. The forces acting on the ball are its weight and a resistive force of magnitude 0.2v2 N.

a

Find an expression for v in terms of t.

[6]
b

Deduce what happens to v for large values of t.

[1]
3

A uniform square lamina of side 2a and weight W is suspended from a light inextensible string attached to the midpoint E of the side AB. The other end of the string is attached to a fixed point P on a rough vertical wall. The vertex B of the lamina is in contact with the wall. The string EP is perpendicular to the side AB and makes an angle θ with the wall (see diagram). The string and the lamina are in a vertical plane perpendicular to the wall. The coefficient of friction between the wall and the lamina is 12. Given that the vertex B is about to slip up the wall, find the value of tan⁡θ.

[8]
Figure 1 of 2 for question 3
Figure 2 of 2 for question 3
4

A light elastic string has natural length 8a and modulus of elasticity 5mg. A particle P of mass m is attached to the midpoint of the string. The ends of the string are attached to points A and B which are a distance 12a apart on a smooth horizontal table. The particle P is held on the table so that AP=BP=L (see diagram). The particle P is released from rest. When P is at the midpoint of AB it has speed 80ag.

a

Find L in terms of a.

[5]
b

Find the initial acceleration of P in terms of g.

[3]
5

A particle P is projected with speed u ms−1 at an angle θ above the horizontal from a point O on a horizontal plane and moves freely under gravity. During its flight P passes through the point which is a horizontal distance 3a from O and a vertical distance 38a above the horizontal plane. It is given that tan⁡θ=13.

a

Show that u2=8ag.

[2]
b

A particle Q is projected with speed V ms−1 at an angle α above the horizontal from O at the instant when P is at its highest point. Particles P and Q both land at the same point on the horizontal plane at the same time. Find V in terms of a and g.

[7]
6

A particle P of mass m is attached to one end of a light inextensible rod of length 3a. An identical particle Q is attached to the other end of the rod. The rod is smoothly pivoted at a point O on the rod, where OQ=x. The system, of rod and particles, rotates about O in a vertical plane. At an instant when the rod is vertical, with P above Q, the particle P is moving horizontally with speed u. When the rod has turned through an angle of 60∘ from the vertical, the speed of P is 2ag, and the tensions in the two parts of the rod, OP and OQ, have equal magnitudes.

a

Show that the speed of Q when the rod has turned through an angle of 60∘ from the vertical is 2x3a−xag.

[2]
b

Find x in terms of a.

[5]
c

Find u in terms of a and g.

[4]

Mark scheme

9231/33 · Oct/Nov 2023

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1a · 1 mark

  • B1

    PCLM: mv=−mucos⁡60∘+2mucos⁡θ v=−12u+2ucos⁡θ⇒v=12u(4cos⁡θ−1)

1b · 4 marks

  • B1

    KE of A=12m(v2+(usin⁡60∘)2)

  • M1

    KE of A=2×KE of B, so 12m(v2+(usin⁡60∘)2)=2×12×2m(usin⁡θ)2

  • M1

    (12u(4cos⁡θ−1))2+34u2=4u2(sin⁡θ)2 8cos⁡2θ−2cos⁡θ−3=0

  • A1

    cos⁡θ=34,−12 but angle is acute, so cos⁡θ=34

1c · 2 marks

  • M1

    NEL: v=e(ucos⁡60∘+ucos⁡θ)

  • A1

    v=u,u=e(12u+34u) e=45

2a · 6 marks

  • B1

    2dvdt=2g−0.2v2

  • M1

    Separate variables and attempt to integrate dv0.1(100−v2)=dt

  • A1

    120ln⁡(10+v10−v)=0.1t+c

  • M1

    t=0,v=5,c=120ln⁡3

  • M1

    2t=ln⁡10+v3(10−v),e2t=10+v3(10−v)

  • A1

    v=30−10e−2t3+e−2t

2b · 1 mark

  • B1

    v→10

3 · 8 marks

  • B1

    Let N be normal reaction at B and F the frictional force acting downwards ↑Tcos⁡θ=F+W

  • B1

    →Tsin⁡θ=N

  • M1

    Moments about B: Ta=Wsin⁡θ×a+Wcos⁡θ×a (method)

  • A1

    Moments about B: Ta=Wsin⁡θ×a+Wcos⁡θ×a (accuracy)

  • M1

    F=12N used

  • M1

    (cos⁡θ+sin⁡θ)(cos⁡θ−12sin⁡θ)=1 oe

  • M1

    12cos⁡θsin⁡θ=32(sin⁡θ)2 sin⁡θ(cos⁡θ−3sin⁡θ)=0

  • A1

    tan⁡θ=13

4a · 5 marks

  • B1

    At least one correct EPE.

  • M1

    Energy equation: gain in KE = loss in EPE (3-term energy equation)

  • A1

    12m×80ag=12×5mg8a((2L−8a)2−(4a)2)

  • M1

    4L2−8aL−20a2=0

  • A1

    L=10a

4b · 3 marks

  • M1

    At P: 2Tcos⁡θ=m×acceleration

  • M1

    Hooke's law: T=5mg8a×12a=152mg

  • A1

    Solve, acceleration = 12g

5a · 2 marks

  • M1

    Use equation of trajectory: y=xtan⁡α−gx22u2sec⁡2α : 38a=3a×13−g×(3a)22u2(1+19)

  • A1

    58a=5gau2,u2=8ga

5b · 7 marks

  • B1

    For P, time of flight T=2usin⁡θg

  • B1

    For P, range =Tucos⁡θ

  • B1

    For Q, time of flight =12T, so range =12TVcos⁡α Equate: Vcos⁡α=2ucos⁡θ (1)

  • M1

    For Q vertically: 0=Vsin⁡α×12T−12gT24, so T=4Vsin⁡αg

  • A1

    Equate with result for P: 4Vsin⁡αg=2usin⁡θg so Vsin⁡α=12usin⁡θ (2)

  • M1

    From (1) and (2): V2=u2(4(cos⁡θ)2+14(sin⁡θ)2)

  • A1

    V2=u2×(4×910+14×110)=14540u2 V=29ag

6a · 2 marks

  • M1

    Angular speeds of P and Q are equal, so vQx=vP3a−x

  • A1

    vQ=2xag3a−x

6b · 5 marks

  • B1

    For P: T+mgcos⁡60∘=m×4ag3a−x

  • B1

    For Q: T−mgcos⁡60∘=mvQ2x

  • M1

    Eliminate T: −mgcos⁡60∘+m⋅4ag3a−x=mgcos⁡60∘+mvQ2x

  • M1

    m×4ag3a−x=1+mx4ag(3a−x)2 4a(3a−x)=(3a−x)2+4ax,x2+2ax−3a2=0

  • A1

    (x−a)(x+3a)=0,x=a

6c · 4 marks

  • B1

    Gain in KE of P: 12m(4ag−u2) Loss in KE of Q: 12m((u2)2−vQ2)

  • B1

    Loss in GPE of P=mg(3a−x)(1−cos⁡60∘)(=mga) Gain in GPE of Q=mgx(1−cos⁡60∘)(=12mga)

  • M1

    12m(4ag−u2)−12m((u2)2−vQ2)=−mgx(1−cos⁡60∘)+mg(3a−x)(1−cos⁡60∘)

  • A1

    Simplify: 4ag−54u2+ag=ag u2=165ag,u=455ag

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