| Exam Board | OCR MEI |
|---|---|
| Module | Further Mechanics Major (Further Mechanics Major) |
| Year | 2020 |
| Session | November |
| Marks | 13 |
| Paper | Download PDF ↗ |
| Mark scheme | Download PDF ↗ |
| Topic | Impulse and momentum (advanced) |
| Type | Oblique collision of spheres |
| Difficulty | Challenging +1.2 This is a standard oblique collision problem from Further Mechanics requiring Newton's experimental law and conservation of momentum. Part (a) involves routine application of collision formulas with the smooth surface condition ensuring tangential velocity is unchanged. Parts (c-d) require trigonometric manipulation and optimization, but follow established methods. The multi-part structure and need for careful angle geometry elevate it slightly above average difficulty, but it remains a textbook-style question testing standard techniques rather than requiring novel insight. |
| Spec | 6.03b Conservation of momentum: 1D two particles6.03c Momentum in 2D: vector form6.03k Newton's experimental law: direct impact6.03l Newton's law: oblique impacts |
| Answer | Marks | Guidance |
|---|---|---|
| 11 | (a) | mucosα=mv +mv |
| 1 2 | M1* | 3.3 |
| – correct number of terms | m is the mass of A and |
| Answer | Marks | Guidance |
|---|---|---|
| 3 | M1* | 3.3 |
| Answer | Marks | Guidance |
|---|---|---|
| 3 | A1 | 1.1 |
| Answer | Marks | Guidance |
|---|---|---|
| 1 | M1dep* | 3.4 |
| Answer | Marks | Guidance |
|---|---|---|
| 3 | A1 | 2.2a |
| Answer | Marks | Guidance |
|---|---|---|
| 11 | (b) | The component of the velocity of A perpendicular to the |
| line of centres does not change | B1 | 3.5b |
| Answer | Marks | Guidance |
|---|---|---|
| 11 | (c) | 3tanα−tanα |
| Answer | Marks | Guidance |
|---|---|---|
| 1+(3tanα)(tanα) | M1 | 3.1b |
| Answer | Marks | Guidance |
|---|---|---|
| 1+3tan2α | A1 | 1.1 |
| Answer | Marks | Guidance |
|---|---|---|
| 11 | (d) | M1* |
| Answer | Marks | Guidance |
|---|---|---|
| 1+3tan2α | A1 | 1.1 |
| Answer | Marks | Guidance |
|---|---|---|
| 3 | M1dep* | 1.1 |
| Answer | Marks | Guidance |
|---|---|---|
| 3 | M1 | 1.1 |
| Answer | Marks |
|---|---|
| both previous M marks | 3 |
| Answer | Marks | Guidance |
|---|---|---|
| 6 | A1 | 1.1 |
Question 11:
11 | (a) | mucosα=mv +mv
1 2 | M1* | 3.3 | Use of conservation of linear momentum
– correct number of terms | m is the mass of A and
B, v is the
1
component of the
velocity of A parallel
to the line of centres
after impact and v is
2
the equivalent
component for B
1
v −v =− ucosα
1 2
3 | M1* | 3.3 | Use of Newton’s experimental law –
correct number of terms and consistent
with conservation of linear momentum
1
v = ucosα
1
3 | A1 | 1.1
usinα
tanβ=
v
1 | M1dep* | 3.4 | Use of tan ratio for β with their v
1
usinα
tanβ= ⇒tanβ=3tanα
1
ucosα
3 | A1 | 2.2a | AG – sufficient working must be shown
as answer given
[5]
11 | (b) | The component of the velocity of A perpendicular to the
line of centres does not change | B1 | 3.5b
[1]
11 | (c) | 3tanα−tanα
tanγ=tan(β−α)=
1+(3tanα)(tanα) | M1 | 3.1b | Use of a correct compound-angle formula
tan(β±α)
for and substitute given
result from (a)
2tanα
tanγ=
1+3tan2α | A1 | 1.1
[2]
11 | (d) | M1* | 3.1b | Attempt to differentiate using quotient
rule
dγ
sec2γ =
dα
( )( ) −(2tanα)( )
1+3tan2α 2sec2α 6tanαsec2α
=0
( )
1+3tan2α | A1 | 1.1 | Correct derivative equated to zero
1
1+3tan2α−6tan2α=0⇒tanα=
3 | M1dep* | 1.1 | Find value of tanα or tan2α | π
α=
6
( )
2 3
3
tanγ= ⇒γ=...
2
3
1+3
3 | M1 | 1.1 | Substitute their value for αor tanα into
their expression for tanγ- dependent on
both previous M marks | 3
tanγ=
3
π
γ=
6 | A1 | 1.1
[5]
Two uniform small smooth spheres A and B have equal radii and equal masses. The spheres are on a smooth horizontal surface. Sphere A is moving at an acute angle $\alpha$ to the line of centres, when it collides with B, which is stationary.
After the impact A is moving at an acute angle $\beta$ to the line of centres. The coefficient of restitution between A and B is $\frac{1}{3}$.
\begin{enumerate}[label=(\alph*)]
\item Show that $\tan\beta = 3\tan\alpha$. [5]
\item Explain why the assumption that the contact between the spheres is smooth is needed in answering part (a). [1]
It is given that A is deflected through an angle $\gamma$.
\item Determine, in terms of $\alpha$, an expression for $\tan\gamma$. [2]
\item Determine the maximum value of $\gamma$. You do not need to justify that this value is a maximum. [5]
\end{enumerate}
\hfill \mbox{\textit{OCR MEI Further Mechanics Major 2020 Q11 [13]}}