OCR MEI Further Mechanics Minor 2024 June — Question 3 9 marks

Exam BoardOCR MEI
ModuleFurther Mechanics Minor (Further Mechanics Minor)
Year2024
SessionJune
Marks9
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicWork done and energy
TypeMotion on rough inclined plane
DifficultyStandard +0.3 This is a standard A-level mechanics problem involving energy methods on an inclined plane with resistance. Part (a) requires straightforward application of work-energy principles with given resistance per metre. Part (b) adds a simple step of separating friction from total resistance. The problem is well-structured with clear given information and requires only routine application of familiar techniques, making it slightly easier than average.
Spec3.03r Friction: concept and vector form3.03t Coefficient of friction: F <= mu*R model6.02i Conservation of energy: mechanical energy principle

3 The diagram shows the three points A, B and C that lie along a line of greatest slope on a rough plane which is inclined at an angle of \(25 ^ { \circ }\) to the horizontal. \includegraphics[max width=\textwidth, alt={}, center]{0a790ad0-7eda-40f1-9894-f156766ae46f-3_392_1136_383_242} A block of mass 6 kg is placed at B and is projected up the plane towards C with an initial speed of \(u \mathrm {~m} \mathrm {~s} ^ { - 1 }\). The block travels 3.5 m before coming instantaneously to rest at C , before sliding back down the plane. When the block is sliding back down the plane it attains its initial speed at A , which lies \(x \mathrm {~m}\) down the plane from B . It is given that the work done against resistance throughout the motion is 4 joules per metre.
  1. Use an energy method to determine the following.
    1. The value of \(u\)
    2. The value of \(x\) A student claims that half of the energy lost due to resistances is accounted for by friction between the block and the plane, and the other half by air resistance.
  2. Assuming that the student's claim is correct, determine the coefficient of friction between the block and the plane.

Question 3:
AnswerMarks Guidance
3(a) (i)
 u = 5 .8 ( 0 1 5 7 5 )M1
B1
A1
AnswerMarks
[3]3.3
1.1
AnswerMarks
1.1Attempt at WEP; must have 3
terms.
Correct GPE term.
AnswerMarks
(ii)Energy from C to A:
6 g  ( 3 .5 + x ) s i n 2 5  − 4 ( 3 .5 + x ) = 12  6  5 .8 0 1 5 7 5 2
AnswerMarks
 x = 1 .3 ( 4 2 9 2 8 )M1
A1FT
AnswerMarks
A1FT3.3
1.1
AnswerMarks
1.1Attempt at WEP; must have 3
terms.
Correct equation in x FT their value
of u from part (a)
Follow through their value u
Or energy from B to A:
AnswerMarks Guidance
12  6  u 2 + 6 g x s i n 2 5  − 4 ( 7 + x ) = 12  6  u 212  6  u 2 + 6 g x s i n 2 5  − 4 ( 7 + x ) = 12  6  u 2 M1
A1FTM1 3.3
terms.
AnswerMarks Guidance
A1FT1.1 Correct equation in x FT their value
of u from part (a).
AnswerMarks Guidance
 x = 1 .3 ( 4 2 9 2 8 )A1FT 1.1
[3]
If energy methods not used for both (a) (i) and (a) (ii)
award for correct answers.
𝑢 = 5.8(01575…)
AnswerMarks
𝑥 = 1.3(4298…)SC1
SC1
AnswerMarks
[2]cao
cao
AnswerMarks
(b)=2N
Frictional force
R = 6 g c o s 2 5 
So = 2 =0.0375298
AnswerMarks
6gcos25B1
M1
A1
AnswerMarks
[3]3.4
1.1
AnswerMarks
2.2bComponent of the normal contact
force – allow sin/cos mix
Awrt 0.038
AnswerMarks
(a)Let the velocities of A and B after impact be v and v , in
A B
the direction A B .
3  1 = 3 v + 1 v
A B
v − v = e  1
B A
 3 = 3 v + v + e  v = 14 ( 3 − e )
A A A
v = 14 ( 3 − e ) + e = 34 ( 1 + e )
AnswerMarks
BM1
M1
A1
A1
AnswerMarks
[4]3.3
3.3
3.4
AnswerMarks
1.1Attempt at COLM.
Attempt at NEL
AG (note speed requested)
AnswerMarks
(b)12  3   14 ( 3 − e )  2 + 12  1   34 ( 1 + e )  2 = 0 .7 9  12  3  1 2 
 e = 0 .4M1
A1FT
A1
AnswerMarks
[3]3.3
1.1
AnswerMarks
1.1Using the information to set up an equation in e with
their expressions.
Correct equation FT their expressions from part (a).
AnswerMarks Guidance
(c)If they had different radii, the impact could not be direct. B1
[1]3.5b Accept explanations that there cannot be a vertical
impulse/force for motion to continue horizontally
only.
Let the velocities of C and D after impact be v and v , in
C D
the direction C D .
23 ( u + 1 ) = 2 ( v − ( − 1 ) )
D
 v = 13 u − 23
D
( )
1  u − 2  1 = 1  v + 2  13 u − 23
C
v = u − 2 − 23 u + 43 = 13 u − 23 which is the same as v so they
C D
have the same velocity afer impact.
AnswerMarks
OrM1
A1
M1
AnswerMarks
A13.3
1.1
3.3
AnswerMarks
2.2aAttempt at impulse-momentum equation: condone
incorrect signs.
Attempt at COLM: condone incorrect signs.
2
− (𝑢+1) = 𝑣 −𝑢
AnswerMarks Guidance
3 𝐶M1 3.3
incorrect signs.
1 2
⇒ 𝑣 = 𝑢− which is the same as v so they have the
AnswerMarks Guidance
𝐶 3 3 DA1 2.2a
same velocity afer impact.
Or
Let the velocities of C and D after impact be v and v , in
C D
the direction C D .
23 ( u + 1 ) = 2 ( v − ( − 1 ) )
D
𝑢−2 = 𝑣 +2𝑣
AnswerMarks
𝐶 𝐷Let the velocities of C and D after impact be v and v , in
C D3.3
3.3Attempt at impulse-momentum equation: condone
incorrect signs.
Attempt at COLM: condone incorrect signs.
the direction C D .
23 ( u + 1 ) = 2 ( v − ( − 1 ) )
D
M1
𝑢−2 = 𝑣 +2𝑣
AnswerMarks
𝐶 𝐷M1
𝑢 = 𝑣 +2𝑣 +2 Substitute into the Impulse-momentum
𝐶 𝐷
equation
3𝑣 = 𝑣 +2𝑣
AnswerMarks Guidance
𝐷 𝑐 𝐷A1 1.1
𝑣 = 𝑣
AnswerMarks Guidance
𝐶 𝐷A1 2.2a
(e)( ) 2
12  3  13 u − 23
12  1  u 2 + 12  2  1 2
4 4
𝑢2−4𝑢+4 1− +
𝑢 𝑢2
= (= )
3𝑢2+6 6
3+
𝑢2
→ 13 u →  23
AnswerMarks
as so the fraction of energy lost tends to .M1
M1
A1
AnswerMarks
[3]3.1b
1.1
AnswerMarks
2.2aAttempt at formulating an expression in u to
represent the fraction of energy remaining or lost.
Simplifying to a form where the limit can be taken
or is apparent.
cao must follow correct expressions for
𝑉 𝑎𝑛𝑑 𝑉
𝐶 𝐷
3.3
3.3
Attempt at impulse-momentum equation: condone
incorrect signs.
Attempt at COLM: condone incorrect signs.
AnswerMarks
(a)Total area = 12  ( 3 0 + 1 2 0 )  9 0 = 6 7 5 0
 x   2 0   4 5   8 0 
6 7 5 0 = 1 3 5 0 + 2 7 0 0 + 2 7 0 0
y 3 0 4 5 3 0
 x = 5 4
AnswerMarks
and y=36B1
B1
M1
A1
A1
AnswerMarks
[5]1.1
1.2
3.3
1.1
AnswerMarks
1.1Correct centre of mass for
triangle (implied by correct
position vector in either of first
or third term on RHS).
Fully correct equation for
either x or y.
AG: some manipulation
required in order to obtain
answer.
AnswerMarks
(b)If M is the centre of mass, it must lie within BCD, so in the
extreme cases it lies on either BD or CD.
If it lies on BD, then 35 64 −− 0d = 96 00 −− 35 64 (  d = 5 0 )
or in form 𝑦 = 9𝑥−450
If it lies on CD, then 35 64 −− 0d = 93 00 −− 35 64 (  d = 7 0 )
9 315
or in form 𝑦 = − 𝑥+
4 2
AnswerMarks
So 5 0  d  7 0 .M1FT
A1FT
A1FT
AnswerMarks
[3]3.1b
1.1
AnswerMarks
2.2aFollow through incorrect 𝑦̅
Considering gradients or
equations of lines.
One correct equation (implied
by one correct limit).
Range must be clearly stated,
in words if not using
inequalities or set notation.
Take moments about a line parallel to y-axis eg. x = 3 0 :
3 0 R + 3 3 R = 2 4  1 0 0
B D
AnswerMarks
𝑅 = 60 , 𝐷 R B = 1 4 and R C = 2 6M1
A1
AnswerMarks
[4]3.3
2.2a
Question 3:
3 | (a) | (i) | 12  6  u 2 − 4  3 .5 = 6 g  3 .5 s i n 2 5 
 u = 5 .8 ( 0 1 5 7 5 ) | M1
B1
A1
[3] | 3.3
1.1
1.1 | Attempt at WEP; must have 3
terms.
Correct GPE term.
(ii) | Energy from C to A:
6 g  ( 3 .5 + x ) s i n 2 5  − 4 ( 3 .5 + x ) = 12  6  5 .8 0 1 5 7 5 2
 x = 1 .3 ( 4 2 9 2 8 ) | M1
A1FT
A1FT | 3.3
1.1
1.1 | Attempt at WEP; must have 3
terms.
Correct equation in x FT their value
of u from part (a)
Follow through their value u
Or energy from B to A:
12  6  u 2 + 6 g x s i n 2 5  − 4 ( 7 + x ) = 12  6  u 2 | 12  6  u 2 + 6 g x s i n 2 5  − 4 ( 7 + x ) = 12  6  u 2 | M1
A1FT | M1 | 3.3 | Attempt at WEP; must have 4
terms.
A1FT | 1.1 | Correct equation in x FT their value
of u from part (a).
 x = 1 .3 ( 4 2 9 2 8 ) | A1FT | 1.1 | Follow through their value u
[3]
If energy methods not used for both (a) (i) and (a) (ii)
award for correct answers.
𝑢 = 5.8(01575…)
𝑥 = 1.3(4298…) | SC1
SC1
[2] | cao
cao
(b) | =2N
Frictional force
R = 6 g c o s 2 5 
So = 2 =0.0375298
6gcos25 | B1
M1
A1
[3] | 3.4
1.1
2.2b | Component of the normal contact
force – allow sin/cos mix
Awrt 0.038
(a) | Let the velocities of A and B after impact be v and v , in
A B
the direction A B .
3  1 = 3 v + 1 v
A B
v − v = e  1
B A
 3 = 3 v + v + e  v = 14 ( 3 − e )
A A A
v = 14 ( 3 − e ) + e = 34 ( 1 + e )
B | M1
M1
A1
A1
[4] | 3.3
3.3
3.4
1.1 | Attempt at COLM.
Attempt at NEL
AG (note speed requested)
(b) | 12  3   14 ( 3 − e )  2 + 12  1   34 ( 1 + e )  2 = 0 .7 9  12  3  1 2 
 e = 0 .4 | M1
A1FT
A1
[3] | 3.3
1.1
1.1 | Using the information to set up an equation in e with
their expressions.
Correct equation FT their expressions from part (a).
(c) | If they had different radii, the impact could not be direct. | B1
[1] | 3.5b | Accept explanations that there cannot be a vertical
impulse/force for motion to continue horizontally
only.
Let the velocities of C and D after impact be v and v , in
C D
the direction C D .
23 ( u + 1 ) = 2 ( v − ( − 1 ) )
D
 v = 13 u − 23
D
( )
1  u − 2  1 = 1  v + 2  13 u − 23
C
v = u − 2 − 23 u + 43 = 13 u − 23 which is the same as v so they
C D
have the same velocity afer impact.
Or | M1
A1
M1
A1 | 3.3
1.1
3.3
2.2a | Attempt at impulse-momentum equation: condone
incorrect signs.
Attempt at COLM: condone incorrect signs.
2
− (𝑢+1) = 𝑣 −𝑢
3 𝐶 | M1 | 3.3 | Attempt at impulse-momentum equation: condone
incorrect signs.
1 2
⇒ 𝑣 = 𝑢− which is the same as v so they have the
𝐶 3 3 D | A1 | 2.2a
same velocity afer impact.
Or
Let the velocities of C and D after impact be v and v , in
C D
the direction C D .
23 ( u + 1 ) = 2 ( v − ( − 1 ) )
D
𝑢−2 = 𝑣 +2𝑣
𝐶 𝐷 | Let the velocities of C and D after impact be v and v , in
C D | 3.3
3.3 | Attempt at impulse-momentum equation: condone
incorrect signs.
Attempt at COLM: condone incorrect signs.
the direction C D .
23 ( u + 1 ) = 2 ( v − ( − 1 ) )
D
M1
𝑢−2 = 𝑣 +2𝑣
𝐶 𝐷 | M1
𝑢 = 𝑣 +2𝑣 +2 Substitute into the Impulse-momentum
𝐶 𝐷
equation
3𝑣 = 𝑣 +2𝑣
𝐷 𝑐 𝐷 | A1 | 1.1 | For correct equation eliminating u
𝑣 = 𝑣
𝐶 𝐷 | A1 | 2.2a | AG For correct argument leading to equality
(e) | ( ) 2
12  3  13 u − 23
12  1  u 2 + 12  2  1 2
4 4
𝑢2−4𝑢+4 1− +
𝑢 𝑢2
= (= )
3𝑢2+6 6
3+
𝑢2
→ 13 u →  23
as so the fraction of energy lost tends to . | M1
M1
A1
[3] | 3.1b
1.1
2.2a | Attempt at formulating an expression in u to
represent the fraction of energy remaining or lost.
Simplifying to a form where the limit can be taken
or is apparent.
cao must follow correct expressions for
𝑉 𝑎𝑛𝑑 𝑉
𝐶 𝐷
3.3
3.3
Attempt at impulse-momentum equation: condone
incorrect signs.
Attempt at COLM: condone incorrect signs.
(a) | Total area = 12  ( 3 0 + 1 2 0 )  9 0 = 6 7 5 0
 x   2 0   4 5   8 0 
6 7 5 0 = 1 3 5 0 + 2 7 0 0 + 2 7 0 0
y 3 0 4 5 3 0
 x = 5 4
and y=36 | B1
B1
M1
A1
A1
[5] | 1.1
1.2
3.3
1.1
1.1 | Correct centre of mass for
triangle (implied by correct
position vector in either of first
or third term on RHS).
Fully correct equation for
either x or y.
AG: some manipulation
required in order to obtain
answer.
(b) | If M is the centre of mass, it must lie within BCD, so in the
extreme cases it lies on either BD or CD.
If it lies on BD, then 35 64 −− 0d = 96 00 −− 35 64 (  d = 5 0 )
or in form 𝑦 = 9𝑥−450
If it lies on CD, then 35 64 −− 0d = 93 00 −− 35 64 (  d = 7 0 )
9 315
or in form 𝑦 = − 𝑥+
4 2
So 5 0  d  7 0 . | M1FT
A1FT
A1FT
[3] | 3.1b
1.1
2.2a | Follow through incorrect 𝑦̅
Considering gradients or
equations of lines.
One correct equation (implied
by one correct limit).
Range must be clearly stated,
in words if not using
inequalities or set notation.
Take moments about a line parallel to y-axis eg. x = 3 0 :
3 0 R + 3 3 R = 2 4  1 0 0
B D
𝑅 = 60 , 𝐷 R B = 1 4 and R C = 2 6 | M1
A1
[4] | 3.3
2.2a
3 The diagram shows the three points A, B and C that lie along a line of greatest slope on a rough plane which is inclined at an angle of $25 ^ { \circ }$ to the horizontal.\\
\includegraphics[max width=\textwidth, alt={}, center]{0a790ad0-7eda-40f1-9894-f156766ae46f-3_392_1136_383_242}

A block of mass 6 kg is placed at B and is projected up the plane towards C with an initial speed of $u \mathrm {~m} \mathrm {~s} ^ { - 1 }$. The block travels 3.5 m before coming instantaneously to rest at C , before sliding back down the plane. When the block is sliding back down the plane it attains its initial speed at A , which lies $x \mathrm {~m}$ down the plane from B .

It is given that the work done against resistance throughout the motion is 4 joules per metre.
\begin{enumerate}[label=(\alph*)]
\item Use an energy method to determine the following.
\begin{enumerate}[label=(\roman*)]
\item The value of $u$
\item The value of $x$

A student claims that half of the energy lost due to resistances is accounted for by friction between the block and the plane, and the other half by air resistance.
\end{enumerate}\item Assuming that the student's claim is correct, determine the coefficient of friction between the block and the plane.
\end{enumerate}

\hfill \mbox{\textit{OCR MEI Further Mechanics Minor 2024 Q3 [9]}}