| Exam Board | OCR MEI |
|---|---|
| Module | Further Mechanics A AS (Further Mechanics A AS) |
| Year | 2018 |
| Session | June |
| Marks | 11 |
| Paper | Download PDF ↗ |
| Mark scheme | Download PDF ↗ |
| Topic | Moments |
| Type | Rod on inclined plane |
| Difficulty | Standard +0.3 This is a standard equilibrium problem requiring moments and resolution of forces. While it involves multiple steps (moments about B, horizontal resolution, vertical resolution), each step follows routine mechanics procedures. The geometry with the 30Β° inclined plane adds mild complexity, but the question guides students through each stage explicitly, making it slightly easier than average for A-level mechanics. |
| Spec | 3.03m Equilibrium: sum of resolved forces = 03.03n Equilibrium in 2D: particle under forces3.04a Calculate moments: about a point3.04b Equilibrium: zero resultant moment and force |
| Answer | Marks | Guidance |
|---|---|---|
| 6 | (i) | R at A perpβr to plane; T along string from B |
| [1] | 1.2 | By eye; arrows needed |
| (ii) | πΓπ = π Γ2πsin60Β° |
| Answer | Marks |
|---|---|
| 3 | M1 |
| Answer | Marks | Guidance |
|---|---|---|
| [2] | 3.3 | |
| 1.1 | Allow sin / cos confusion, sign error | a can be cancelled; ft R from (i) |
| Answer | Marks |
|---|---|
| (iii) | πcosπ = π cos60Β° |
| Answer | Marks |
|---|---|
| 6πcosπ = πβ3 | M1 |
| Answer | Marks |
|---|---|
| [3] | 3.4 |
| Answer | Marks |
|---|---|
| 2.1 | Must have sin/cos in each term; |
| Answer | Marks |
|---|---|
| (iv) | πsinπ+π sin60Β° = π |
| Answer | Marks |
|---|---|
| 3 | M1* |
| Answer | Marks |
|---|---|
| [5] | 3.1b |
| Answer | Marks |
|---|---|
| 1.1 | Resolve vertically for AB; must |
| Answer | Marks |
|---|---|
| Subst for R Must be correct | OR Moments about A |
Question 6:
6 | (i) | R at A perpβr to plane; T along string from B | B1
[1] | 1.2 | By eye; arrows needed
(ii) | πΓπ = π
Γ2πsin60Β°
π
π
= β3
3 | M1
A1
[2] | 3.3
1.1 | Allow sin / cos confusion, sign error | a can be cancelled; ft R from (i)
if R through A (not horiz)
π
Accept
β3
(iii) | πcosπ = π
cos60Β°
π
πcosπ = β3 cos60Β°
3
6πcosπ = πβ3 | M1
M1ft
A1
[3] | 3.4
1.1
2.1 | Must have sin/cos in each term;
allow sin / cos confusion
Using their R from part (ii); allow
sin / cos confusion
AG
(iv) | πsinπ+π
sin60Β° = π
πβ3 π β3
sinπ+ β3Γ = π
6cosπ 3 2
6 β3Γβ3
tanπ = Γ(1β )
β3 3Γ2
π
OR πsinπ+ β3sin60Β° = π
3
π β3
πsinπ = ; Solve with πcosπ = π from
2 6
(iii)
π = 60Β°
π
π = β3
3 | M1*
A1
*M1
(A1)
(M1)
A1
A1
[5] | 3.1b
3.4
1.1
1.1
1.1 | Resolve vertically for AB; must
have T, R and W terms, comps of T
and R; allow sign error
Elim T and subst for R
Attempt to re-arrange to find tan ΞΈ
Subst for R Must be correct | OR Moments about A
ππ = πΓ2πsinπ M1
πΓ2πsinπ ππ
= A1
6πcosπ πβ3
tanπ = β3 M1
PPMMTT
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6 A uniform rod AB has length $2 a$ and weight $W$. The rod is in equilibrium in a horizontal position. The end A rests on a smooth plane which is inclined at an angle of $30 ^ { \circ }$ to the horizontal. The force exerted on AB by the plane is $R$. The end B is attached to a light inextensible string inclined at an angle of $\theta$ to AB as shown in Fig. 6. The rod and string are in the same vertical plane, which also contains the line of greatest slope of the plane on which A lies. The tension in the string is $T$.
\begin{figure}[h]
\begin{center}
\includegraphics[alt={},max width=\textwidth]{fa99d9e6-e174-42dd-ac92-7b7d112c08be-5_474_862_479_616}
\captionsetup{labelformat=empty}
\caption{Fig. 6}
\end{center}
\end{figure}
(i) Add the forces $R$ and $T$ to the copy of Fig. 6 in the Printed Answer Booklet.\\
(ii) By taking moments about B , find an expression for $R$ in terms of $W$.\\
(iii) By resolving horizontally, show that $6 T \cos \theta = W \sqrt { 3 }$.\\
(iv) By finding a second equation connecting $T$ and $\theta$, determine
\begin{itemize}
\item the value of $\theta$,
\item an expression for $T$ in terms of $W$.
\end{itemize}
\hfill \mbox{\textit{OCR MEI Further Mechanics A AS 2018 Q6 [11]}}