| Exam Board | OCR MEI |
|---|---|
| Module | Further Mechanics A AS (Further Mechanics A AS) |
| Year | 2024 |
| Session | June |
| Marks | 13 |
| Paper | Download PDF ↗ |
| Mark scheme | Download PDF ↗ |
| Topic | Moments |
| Type | Ladder against wall |
| Difficulty | Standard +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. |
| Spec | 3.03a 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 |
| Answer | Marks | Guidance |
|---|---|---|
| 3 | (a) | Contact force at A resolved into separate normal and frictional |
| Answer | Marks |
|---|---|
| contact force at C perp. to beam in the correct direction. | B1 |
| Answer | Marks |
|---|---|
| [2] | 3.3 |
| 3.3 | Forces must have arrows and be appropriately labelled |
| Answer | Marks | Guidance |
|---|---|---|
| (b) | (i) | Take the frictional force at A to be F vertically downwards. |
| Answer | Marks |
|---|---|
| F = 2 5 | M1 |
| Answer | Marks |
|---|---|
| [3] | 1.1 |
| Answer | Marks |
|---|---|
| 2.1 | Resolving to obtain an equation involving F, e.g. |
| Answer | Marks | Guidance |
|---|---|---|
| cont | (b) | (ii) |
| Answer | Marks |
|---|---|
| Magnitude is 65.6 (N) | M1* |
| Answer | Marks |
|---|---|
| [3] | 1.1 |
| Answer | Marks |
|---|---|
| 1.1 | Resolving horizontally |
| Answer | Marks |
|---|---|
| (c) | 25 |
| Answer | Marks |
|---|---|
| 22.4(109β¦)Β° below the horizontal. | M1 |
| Answer | Marks |
|---|---|
| [2] | 1.1 |
| 2.5 | Equation for a relevant angle |
| Answer | Marks |
|---|---|
| (d) | FR ο ο³ |
| Answer | Marks |
|---|---|
| 21 | M1 |
| Answer | Marks |
|---|---|
| [2] | 3.4 |
| 1.1 | πΉ = ππ or πΉ β€ ππ seen or implied |
| Answer | Marks | Guidance |
|---|---|---|
| (e) | Both F and R would increase so the magnitude must increase. | |
| A | B1 | |
| [1] | 2.4 | Must acknowledge that both components increase. |
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 ππ
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: π
(2) = 80(3.5sin60Β°)
C
[ π
= 70β3 = 121.24 ]
C
[ 105 = πΉ+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: π
sin60Β° = 80cos60Β°+πΉcos60Β°
A
Perp to AB: π
= 80sin60Β°+πΉsin60Β°+π
cos60Β°
C A
A moments equation, e.g. about
C: π
(2cos60Β°)+πΉ(2sin60Β°) = 80(1.5sin60Β°)
A
G: π
(3.5cos60Β°)+πΉ(3.5sin60Β°) = π
(1.5)
A C
B: π
(7cos60Β°)+πΉ(7sin60Β°)+80(3.5sin60Β°)=π
(5)
A C
No omitted or extra terms. Allow sign errors and sin/cos
confusion. Allow π
in wrong direction (e.g. vertical).
C
In moments about C, note that 2cos60Β° = 1
AG Fully correct working
With F upwards leading to πΉ = β25 they must say βso
the magnitude is 25β or βi.e. 25 downwardsβ to earn A1
3
cont | (b) | (ii) | π
= π
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 π
, not credited in (i)
A
OR Obtaining π
from equation(s) credited in (i),
A
possibly using πΉ = (Β±)25
This M1 can be awarded for work done in (i)
Obtaining a value for π
and using F 2 + R 2
A A
Accept 4 3 0 0
(c) | 25
tanπ =
π
A
22.4(109β¦)Β° below the horizontal. | M1
A1
[2] | 1.1
2.5 | Equation for a relevant angle
π
A 25
e.g. tanπΌ = , sinπ = 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(890β¦)Β° from the downward vertical
Direction must be clear
(d) | FR ο ο³
A
5β3
π β₯ , π β₯ 0.412
21 | M1
A1 FT
[2] | 3.4
1.1 | πΉ = ππ
or πΉ β€ ππ
seen or implied
A A
Must be their forces at A (on diagram) or their values
25
FT is π β₯
their π
A
Allow exact or approximate form. Allow >
Allow inequality stated in words.
Ignore upper limit, e.g. A1 for 0.412 β€ π β€ 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.
βMoment of weight (about C) increases, so the total
contact force must increase to balance itβ
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]}}