| Exam Board | CAIE |
|---|---|
| Module | FP2 (Further Pure Mathematics 2) |
| Year | 2019 |
| Session | June |
| Marks | 10 |
| Paper | Download PDF ↗ |
| Mark scheme | Download PDF ↗ |
| Topic | Momentum and Collisions 1 |
| Type | Three-particle sequential collisions |
| Difficulty | Standard +0.3 This is a standard multi-collision mechanics problem requiring conservation of momentum and Newton's restitution law applied twice, followed by energy calculation. While it involves multiple steps and careful bookkeeping across two collisions, the techniques are routine for Further Maths students and the problem structure is clearly signposted. The algebraic manipulation is straightforward, making it slightly easier than average for FP2. |
| Spec | 6.03b Conservation of momentum: 1D two particles6.03k Newton's experimental law: direct impact |
| Answer | Marks | Guidance |
|---|---|---|
| 3(i) | 2mv + 4mv = 4mu – 4mu [v + 2v = 0] (AEF) | |
| A B A B | M1 | Use conservation of momentum for A and B (m may be omitted) |
| Answer | Marks | Guidance |
|---|---|---|
| B A B A | M1 | Use Newton’s restitution law with consistent LHS signs |
| Answer | Marks | Guidance |
|---|---|---|
| A B | A1 | Combine to find v and v (A0 if directions unclear) |
| Answer | Marks | Guidance |
|---|---|---|
| 3(ii) | [4mv ′] + mv = 4mv – (4/3) mu (AEF) | |
| B C B | M1 | Use conservation of momentum for B & C (m may be omitted) |
| Answer | Marks | Guidance |
|---|---|---|
| C B B | M1 | Use Newton’s restitution law |
| Answer | Marks | Guidance |
|---|---|---|
| B B | M1 | Combine to find quadratic equation for e using v ′ = 0 |
| Answer | Marks | Guidance |
|---|---|---|
| C | A1 | Find value of e, (implicitly) rejecting e = 2 |
| Answer | Marks | Guidance |
|---|---|---|
| Question | Answer | Marks |
| Answer | Marks |
|---|---|
| 3(iii) | For A: Loss = ½ 2m(2u)2 - ½ 2m(4/3u)2 = (20/9) mu2 |
| Answer | Marks | Guidance |
|---|---|---|
| For C: Loss = 0 | M1 | v = – (4/3) u , [v = (2/3) u], v = (4/3) u |
| Answer | Marks |
|---|---|
| M1 | Other two correct |
| Answer | Marks | Guidance |
|---|---|---|
| initial final 1 2 | A1 | Hence find loss in KE |
| Answer | Marks | Guidance |
|---|---|---|
| = 4mu2 + 2mu2 + (8/9) mu2 = (62/9) mu2 | M1 | Find initial KE of 3 particles in terms of m and u |
| Answer | Marks | Guidance |
|---|---|---|
| = (16/9) mu2 + (8/9) mu2 = (24/9) mu2 | M1 | Find final KE of 3 particles in terms of m and u |
| Answer | Marks | Guidance |
|---|---|---|
| initial final 1 2 | A1 | Hence find loss in KE |
| Answer | Marks | Guidance |
|---|---|---|
| = 4mu2 + 2mu2 – (16/9) mu2 – (8/9) mu2 = (30/9) mu2 | M1 | Find losses in KE in both collisions in terms of m and u |
| Answer | Marks |
|---|---|
| = (8/9) mu2 + (8/9) mu2 – (8/9) mu2 = (8/9) mu2 | M1 |
| Answer | Marks | Guidance |
|---|---|---|
| initial final 1 2 | A1 | Hence find loss in KE |
| Answer | Marks | Guidance |
|---|---|---|
| Question | Answer | Marks |
Question 3:
--- 3(i) ---
3(i) | 2mv + 4mv = 4mu – 4mu [v + 2v = 0] (AEF)
A B A B | M1 | Use conservation of momentum for A and B (m may be omitted)
v – v = e (2u + u) [v – v = 3eu]
B A B A | M1 | Use Newton’s restitution law with consistent LHS signs
v = – 2eu and v = eu
A B | A1 | Combine to find v and v (A0 if directions unclear)
A B
3
--- 3(ii) ---
3(ii) | [4mv ′] + mv = 4mv – (4/3) mu (AEF)
B C B | M1 | Use conservation of momentum for B & C (m may be omitted)
v [– v ′] = e (v + 4u/3)
C B B | M1 | Use Newton’s restitution law
4v – (4/3) u = ev + 4eu/3, 4e – 4/3 = e2 + 4e/3
B B | M1 | Combine to find quadratic equation for e using v ′ = 0
B
3e2 – 8e + 4 = 0, e = 2/3 [v = 4u/3]
C | A1 | Find value of e, (implicitly) rejecting e = 2
4
Question | Answer | Marks | Guidance
--- 3(iii) ---
3(iii) | For A: Loss = ½ 2m(2u)2 - ½ 2m(4/3u)2 = (20/9) mu2
For B: Loss = ½ 4m u2 = ½ mu2
For C: Loss = 0 | M1 | v = – (4/3) u , [v = (2/3) u], v = (4/3) u
A B C
One correct
M1 | Other two correct
E – E or L + L = (38/9) mu2
initial final 1 2 | A1 | Hence find loss in KE
Alternative method for question 3(iii)
E = ½ 2m(2u)2 + ½ 4mu2 + ½ m(4u/3)2
initial
= 4mu2 + 2mu2 + (8/9) mu2 = (62/9) mu2 | M1 | Find initial KE of 3 particles in terms of m and u
E = ½ 2mv 2 [+ ½ 4mv ′ 2 ] + ½ mv 2
final A B C
= (16/9) mu2 + (8/9) mu2 = (24/9) mu2 | M1 | Find final KE of 3 particles in terms of m and u
E – E or L + L = (38/9) mu2
initial final 1 2 | A1 | Hence find loss in KE
Alternative method for question 3(iii)
L = ½ 2m(2u)2 + ½ 4mu2 – ½ 2mv 2 – ½ 4mv 2
1 A B
= 4mu2 + 2mu2 – (16/9) mu2 – (8/9) mu2 = (30/9) mu2 | M1 | Find losses in KE in both collisions in terms of m and u
L = ½ 4mv 2 + ½ m(4u/3)2 – [½ 4mv ′ 2 ] – ½ mv 2
2 B B C
= (8/9) mu2 + (8/9) mu2 – (8/9) mu2 = (8/9) mu2 | M1
E – E or L + L = (38/9) mu2
initial final 1 2 | A1 | Hence find loss in KE
3
Question | Answer | Marks | Guidance
Three uniform small spheres $A$, $B$ and $C$ have equal radii and masses $2m$, $4m$ and $m$ respectively. The spheres are moving in a straight line on a smooth horizontal surface, with $B$ between $A$ and $C$. The coefficient of restitution between each pair of spheres is $e$. Spheres $A$ and $B$ are moving towards each other with speeds $2u$ and $u$ respectively. The first collision is between $A$ and $B$.
(i) Find the velocities of $A$ and $B$ after this collision. [3]
Sphere $C$ is moving towards $B$ with speed $\frac{1}{2}u$ and now collides with it. As a result of this collision, $B$ is brought to rest.
(ii) Find the value of $e$. [4]
(iii) Find the total kinetic energy lost by the three spheres as a result of the two collisions. [3]
\hfill \mbox{\textit{CAIE FP2 2019 Q3 [10]}}