OCR MEI Further Mechanics Major 2019 June — Question 6 7 marks

Exam BoardOCR MEI
ModuleFurther Mechanics Major (Further Mechanics Major)
Year2019
SessionJune
Marks7
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicMomentum and Collisions 1
TypeDirect collision with direction reversal
DifficultyChallenging +1.2 This is a standard two-stage mechanics problem combining energy conservation with collision theory. While it requires careful bookkeeping through multiple steps (finding P's speed before collision, applying conservation of momentum and restitution formula, then using energy conservation for Q's motion), each individual technique is routine for Further Mechanics students. The 'just reaches the rim' condition provides a clear constraint that makes the problem straightforward to set up and solve algebraically.
Spec6.02i Conservation of energy: mechanical energy principle6.03k Newton's experimental law: direct impact

\includegraphics{figure_6} The rim of a smooth hemispherical bowl is a circle of centre O and radius \(a\). The bowl is fixed with its rim horizontal and uppermost. A particle P of mass \(m\) is released from rest at a point A on the rim as shown in Fig. 6. When P reaches the lowest point of the bowl it collides directly with a stationary particle Q of mass \(\frac{1}{2}m\). After the collision Q just reaches the rim of the bowl. Find the coefficient of restitution between P and Q. [7]

Question 6:
AnswerMarks
61
mga mv2
2
v2 2ga or v 2ga
1
mv mv m 2ga
Q P
2
 
v v e 0 2ga
Q P
11  1
v Q  2gaor 2  2 m  v Q 2  2 mga
 1 2ga 
v  2ga or v  2e
 P 2 P 3  
1  
2ga 2ga e 2ga or
2
2
11 2  1
 m 2ga1e   mga
22 3  2
1
e
AnswerMarks
2M1*
A1
M1*
M1*
B1
M1dep*
A1
AnswerMarks
[7]3.3
1.1
3.3
3.3
3.3
2.1
AnswerMarks
2.2aEquating KE gained for P with the PE
lost
v orv2 of P before impact
Attempt at conservation of momentum
– correct number of terms – must be
using their speed of P before impact in
terms of g and a
Attempt at Newton’s experimental law
– correct number of terms and
consistent with CLM – must be using
their speed of P before impact in terms
of g and a
www where v is the speed of Q after
Q
impact – for reference
v 2 2ga1e
Q 3
Where first v expression comes from
P
1
mv mv m 2gaand v  2ga
2 Q P Q
Setting up an equation involving g, a
and e – dependent on all previous M
marks only and must have found v
P
and/or v from a correct method
AnswerMarks
Qv is the speed of P
before impact
Correct masses for P
and Q – note that v
Q
may already have been
substituted
This mark may be
earned later after v and
Q
v have been found
P
1
Condone mv 2 mga
2 Q
No marks for these
Either substituting into
NEL or considering
energy of Q after
collision
NOTE THAT THERE ARE TWO PAGES FOR THIS QUESTION – PLEASE ENSURE BOTH ARE CHECKED
Question 6:
6 | 1
mga mv2
2
v2 2ga or v 2ga
1
mv mv m 2ga
Q P
2
 
v v e 0 2ga
Q P
11  1
v Q  2gaor 2  2 m  v Q 2  2 mga
 1 2ga 
v  2ga or v  2e
 P 2 P 3  
1  
2ga 2ga e 2ga or
2
2
11 2  1
 m 2ga1e   mga
22 3  2
1
e
2 | M1*
A1
M1*
M1*
B1
M1dep*
A1
[7] | 3.3
1.1
3.3
3.3
3.3
2.1
2.2a | Equating KE gained for P with the PE
lost
v orv2 of P before impact
Attempt at conservation of momentum
– correct number of terms – must be
using their speed of P before impact in
terms of g and a
Attempt at Newton’s experimental law
– correct number of terms and
consistent with CLM – must be using
their speed of P before impact in terms
of g and a
www where v is the speed of Q after
Q
impact – for reference
v 2 2ga1e
Q 3
Where first v expression comes from
P
1
mv mv m 2gaand v  2ga
2 Q P Q
Setting up an equation involving g, a
and e – dependent on all previous M
marks only and must have found v
P
and/or v from a correct method
Q | v is the speed of P
before impact
Correct masses for P
and Q – note that v
Q
may already have been
substituted
This mark may be
earned later after v and
Q
v have been found
P
1
Condone mv 2 mga
2 Q
No marks for these
Either substituting into
NEL or considering
energy of Q after
collision
NOTE THAT THERE ARE TWO PAGES FOR THIS QUESTION – PLEASE ENSURE BOTH ARE CHECKED
\includegraphics{figure_6}

The rim of a smooth hemispherical bowl is a circle of centre O and radius $a$. The bowl is fixed with its rim horizontal and uppermost. A particle P of mass $m$ is released from rest at a point A on the rim as shown in Fig. 6.

When P reaches the lowest point of the bowl it collides directly with a stationary particle Q of mass $\frac{1}{2}m$. After the collision Q just reaches the rim of the bowl.

Find the coefficient of restitution between P and Q. [7]

\hfill \mbox{\textit{OCR MEI Further Mechanics Major 2019 Q6 [7]}}