OCR MEI Further Mechanics A AS 2024 June — Question 3 13 marks

Exam BoardOCR MEI
ModuleFurther Mechanics A AS (Further Mechanics A AS)
Year2024
SessionJune
Marks13
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicMoments
TypeLadder against wall
DifficultyStandard +0.3 This is a standard moments equilibrium problem with a beam against a wall. While it requires multiple steps (force diagram, taking moments, resolving forces, finding resultant, and coefficient of friction), all techniques are routine for AS Further Mechanics. The geometry is straightforward with a given angle, and the question guides students through each part systematically. Slightly easier than average due to its structured nature and standard setup.
Spec3.03a Force: vector nature and diagrams3.03m Equilibrium: sum of resolved forces = 03.03n Equilibrium in 2D: particle under forces3.03t Coefficient of friction: F <= mu*R model3.03u Static equilibrium: on rough surfaces3.04a Calculate moments: about a point3.04b Equilibrium: zero resultant moment and force

3 The diagram shows a uniform beam AB , of weight 80 N and length 7 m , resting in equilibrium in a vertical plane. The end A is in contact with a rough vertical wall, and the angle between the beam and the upward vertical is \(60 ^ { \circ }\). The beam is supported by a smooth peg at a point C , where \(\mathrm { AC } = 2 \mathrm {~m}\). \includegraphics[max width=\textwidth, alt={}, center]{a96a0ebe-8f4f-4d79-9d11-9d348ef72314-4_474_709_445_244}
  1. Complete the diagram in the Printed Answer Booklet to show all the forces acting on the beam.
    1. Show that the magnitude of the frictional force exerted on the beam by the wall is 25 N .
    2. Hence determine the magnitude of the total contact force exerted on the beam by the wall.
  2. Determine the direction of the total contact force exerted on the beam by the wall. The coefficient of friction between the beam and the wall is \(\mu\).
  3. Find the range of possible values for \(\mu\).
  4. Explain how your answer to part (b)(ii) would change if the peg were situated closer to A but the angle between the beam and the upward vertical remained at \(60 ^ { \circ }\).

Question 3:
AnswerMarks Guidance
3(a) Contact force at A resolved into separate normal and frictional
components; allow friction either vertically upwards/downwards.
80 N force vertically downward at centre of beam (G) and
AnswerMarks
contact force at C perp. to beam in the correct direction.B1
B1
AnswerMarks
[2]3.3
3.3Forces must have arrows and be appropriately labelled
No extra forces, but condone components shown as well
(Forces at A) Accept contact force as a single force
(neither horizontal nor vertical nor parallel to beam)
B0 for friction labelled πœ‡π‘…
A
(Forces elsewhere) Must be clear right angle or with
right angle marker present.
Max B1 if same label used for two forces
AnswerMarks Guidance
(b)(i) Take the frictional force at A to be F vertically downwards.
Resolving vertically: R s i n 6 0 ο‚° = F + 8 0
C
Moments about A: 𝑅 (2) = 80(3.5sin60Β°)
C
[ 𝑅 = 70√3 = 121.24 ]
C
[ 105 = 𝐹+80 ]
AnswerMarks
F = 2 5M1
M1
A1
AnswerMarks
[3]1.1
1.1
AnswerMarks
2.1Resolving to obtain an equation involving F, e.g.
Parallel to AB: 𝑅 sin60Β° = 80cos60Β°+𝐹cos60Β°
A
Perp to AB: 𝑅 = 80sin60Β°+𝐹sin60Β°+𝑅 cos60Β°
C A
A moments equation, e.g. about
C: 𝑅 (2cos60Β°)+𝐹(2sin60Β°) = 80(1.5sin60Β°)
A
G: 𝑅 (3.5cos60Β°)+𝐹(3.5sin60Β°) = 𝑅 (1.5)
A C
B: 𝑅 (7cos60Β°)+𝐹(7sin60Β°)+80(3.5sin60Β°)=𝑅 (5)
A C
No omitted or extra terms. Allow sign errors and sin/cos
confusion. Allow 𝑅 in wrong direction (e.g. vertical).
C
In moments about C, note that 2cos60Β° = 1
AG Fully correct working
With F upwards leading to 𝐹 = βˆ’25 they must say β€˜so
the magnitude is 25’ or β€˜i.e. 25 downwards’ to earn A1
3
AnswerMarks Guidance
cont(b) (ii)
A C
R =35 3( = 6 0 .6 2 1 7 )
A
( ) 2
Magnitude = 2 5 2 + 3 5 3
AnswerMarks
Magnitude is 65.6 (N)M1*
M1dep*
A1
AnswerMarks
[3]1.1
1.1
AnswerMarks
1.1Resolving horizontally
OR Obtaining another resolving or moments equation,
involving 𝑅 , not credited in (i)
A
OR Obtaining 𝑅 from equation(s) credited in (i),
A
possibly using 𝐹 = (±)25
This M1 can be awarded for work done in (i)
Obtaining a value for 𝑅 and using F 2 + R 2
A A
Accept 4 3 0 0
AnswerMarks
(c)25
tanπœƒ =
𝑅A
AnswerMarks
22.4(109…)Β° below the horizontal.M1
A1
AnswerMarks
[2]1.1
2.5Equation for a relevant angle
𝑅A 25
e.g. tan𝛼 = , sinπœƒ = etc
25 65.6
Provided magnitude in (b)(ii) has been calculated from
perpendicular components, allow M1 for using the same
components to find an angle
Or 67.5(890…)Β° from the downward vertical
Direction must be clear
AnswerMarks
(d)FR  ο‚³
A
5√3
πœ‡ β‰₯ , πœ‡ β‰₯ 0.412
AnswerMarks
21M1
A1 FT
AnswerMarks
[2]3.4
1.1𝐹 = πœ‡π‘… or 𝐹 ≀ πœ‡π‘… seen or implied
A A
Must be their forces at A (on diagram) or their values
25
FT is πœ‡ β‰₯
their 𝑅A
Allow exact or approximate form. Allow >
Allow inequality stated in words.
Ignore upper limit, e.g. A1 for 0.412 ≀ πœ‡ ≀ 1
AnswerMarks Guidance
(e)Both F and R would increase so the magnitude must increase.
AB1
[1]2.4 Must acknowledge that both components increase.
OR Other reasonable explanation, e.g.
β€˜Moment of weight (about C) increases, so the total
contact force must increase to balance it’
Question 3:
3 | (a) | Contact force at A resolved into separate normal and frictional
components; allow friction either vertically upwards/downwards.
80 N force vertically downward at centre of beam (G) and
contact force at C perp. to beam in the correct direction. | B1
B1
[2] | 3.3
3.3 | Forces must have arrows and be appropriately labelled
No extra forces, but condone components shown as well
(Forces at A) Accept contact force as a single force
(neither horizontal nor vertical nor parallel to beam)
B0 for friction labelled πœ‡π‘…
A
(Forces elsewhere) Must be clear right angle or with
right angle marker present.
Max B1 if same label used for two forces
(b) | (i) | Take the frictional force at A to be F vertically downwards.
Resolving vertically: R s i n 6 0 ο‚° = F + 8 0
C
Moments about A: 𝑅 (2) = 80(3.5sin60Β°)
C
[ 𝑅 = 70√3 = 121.24 ]
C
[ 105 = 𝐹+80 ]
F = 2 5 | M1
M1
A1
[3] | 1.1
1.1
2.1 | Resolving to obtain an equation involving F, e.g.
Parallel to AB: 𝑅 sin60Β° = 80cos60Β°+𝐹cos60Β°
A
Perp to AB: 𝑅 = 80sin60Β°+𝐹sin60Β°+𝑅 cos60Β°
C A
A moments equation, e.g. about
C: 𝑅 (2cos60Β°)+𝐹(2sin60Β°) = 80(1.5sin60Β°)
A
G: 𝑅 (3.5cos60Β°)+𝐹(3.5sin60Β°) = 𝑅 (1.5)
A C
B: 𝑅 (7cos60Β°)+𝐹(7sin60Β°)+80(3.5sin60Β°)=𝑅 (5)
A C
No omitted or extra terms. Allow sign errors and sin/cos
confusion. Allow 𝑅 in wrong direction (e.g. vertical).
C
In moments about C, note that 2cos60Β° = 1
AG Fully correct working
With F upwards leading to 𝐹 = βˆ’25 they must say β€˜so
the magnitude is 25’ or β€˜i.e. 25 downwards’ to earn A1
3
cont | (b) | (ii) | 𝑅 = 𝑅 cos60Β°
A C
R =35 3( = 6 0 .6 2 1 7 )
A
( ) 2
Magnitude = 2 5 2 + 3 5 3
Magnitude is 65.6 (N) | M1*
M1dep*
A1
[3] | 1.1
1.1
1.1 | Resolving horizontally
OR Obtaining another resolving or moments equation,
involving 𝑅 , not credited in (i)
A
OR Obtaining 𝑅 from equation(s) credited in (i),
A
possibly using 𝐹 = (±)25
This M1 can be awarded for work done in (i)
Obtaining a value for 𝑅 and using F 2 + R 2
A A
Accept 4 3 0 0
(c) | 25
tanπœƒ =
𝑅A
22.4(109…)Β° below the horizontal. | M1
A1
[2] | 1.1
2.5 | Equation for a relevant angle
𝑅A 25
e.g. tan𝛼 = , sinπœƒ = etc
25 65.6
Provided magnitude in (b)(ii) has been calculated from
perpendicular components, allow M1 for using the same
components to find an angle
Or 67.5(890…)Β° from the downward vertical
Direction must be clear
(d) | FR  ο‚³
A
5√3
πœ‡ β‰₯ , πœ‡ β‰₯ 0.412
21 | M1
A1 FT
[2] | 3.4
1.1 | 𝐹 = πœ‡π‘… or 𝐹 ≀ πœ‡π‘… seen or implied
A A
Must be their forces at A (on diagram) or their values
25
FT is πœ‡ β‰₯
their 𝑅A
Allow exact or approximate form. Allow >
Allow inequality stated in words.
Ignore upper limit, e.g. A1 for 0.412 ≀ πœ‡ ≀ 1
(e) | Both F and R would increase so the magnitude must increase.
A | B1
[1] | 2.4 | Must acknowledge that both components increase.
OR Other reasonable explanation, e.g.
β€˜Moment of weight (about C) increases, so the total
contact force must increase to balance it’
3 The diagram shows a uniform beam AB , of weight 80 N and length 7 m , resting in equilibrium in a vertical plane. The end A is in contact with a rough vertical wall, and the angle between the beam and the upward vertical is $60 ^ { \circ }$. The beam is supported by a smooth peg at a point C , where $\mathrm { AC } = 2 \mathrm {~m}$.\\
\includegraphics[max width=\textwidth, alt={}, center]{a96a0ebe-8f4f-4d79-9d11-9d348ef72314-4_474_709_445_244}
\begin{enumerate}[label=(\alph*)]
\item Complete the diagram in the Printed Answer Booklet to show all the forces acting on the beam.
\item \begin{enumerate}[label=(\roman*)]
\item Show that the magnitude of the frictional force exerted on the beam by the wall is 25 N .
\item Hence determine the magnitude of the total contact force exerted on the beam by the wall.
\end{enumerate}\item Determine the direction of the total contact force exerted on the beam by the wall.

The coefficient of friction between the beam and the wall is $\mu$.
\item Find the range of possible values for $\mu$.
\item Explain how your answer to part (b)(ii) would change if the peg were situated closer to A but the angle between the beam and the upward vertical remained at $60 ^ { \circ }$.
\end{enumerate}

\hfill \mbox{\textit{OCR MEI Further Mechanics A AS 2024 Q3 [13]}}