OCR MEI Further Mechanics Major 2020 November — Question 11 13 marks

Exam BoardOCR MEI
ModuleFurther Mechanics Major (Further Mechanics Major)
Year2020
SessionNovember
Marks13
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicImpulse and momentum (advanced)
TypeOblique collision of spheres
DifficultyChallenging +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.
Spec6.03b 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

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 \(\frac{1}{3}\).
  1. Show that \(\tan\beta = 3\tan\alpha\). [5]
  2. 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 \(\gamma\).
  3. Determine, in terms of \(\alpha\), an expression for \(\tan\gamma\). [2]
  4. Determine the maximum value of \(\gamma\). You do not need to justify that this value is a maximum. [5]

Question 11:
AnswerMarks Guidance
11(a) mucosα=mv +mv
1 2M1* 3.3
– correct number of termsm 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
AnswerMarks Guidance
3M1* 3.3
correct number of terms and consistent
with conservation of linear momentum
1
v = ucosα
1
AnswerMarks Guidance
3A1 1.1
usinα
tanβ=
v
AnswerMarks Guidance
1M1dep* 3.4
1
usinα
tanβ= ⇒tanβ=3tanα
1
ucosα
AnswerMarks Guidance
3A1 2.2a
as answer given
[5]
AnswerMarks Guidance
11(b) The component of the velocity of A perpendicular to the
line of centres does not changeB1 3.5b
[1]
AnswerMarks Guidance
11(c) 3tanα−tanα
tanγ=tan(β−α)=
AnswerMarks Guidance
1+(3tanα)(tanα)M1 3.1b
tan(β±α)
for and substitute given
result from (a)
2tanα
tanγ=
AnswerMarks Guidance
1+3tan2αA1 1.1
[2]
AnswerMarks Guidance
11(d) M1*
rule
 dγ 
sec2γ =
 dα 
( )( ) −(2tanα)( )
1+3tan2α 2sec2α 6tanαsec2α
=0
( )
AnswerMarks Guidance
1+3tan2αA1 1.1
1
1+3tan2α−6tan2α=0⇒tanα=
AnswerMarks Guidance
3M1dep* 1.1
α=
6
( )
2 3
3
tanγ= ⇒γ=...
2
 3
1+3 
AnswerMarks Guidance
 3 M1 1.1
their expression for tanγ- dependent on
AnswerMarks
both previous M marks3
tanγ=
3
π
γ=
AnswerMarks Guidance
6A1 1.1
[5]
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]}}