| Exam Board | AQA |
|---|---|
| Module | Paper 2 (Paper 2) |
| Session | Specimen |
| Marks | 12 |
| Paper | Download PDF ↗ |
| Mark scheme | Download PDF ↗ |
| Topic | Motion on a slope |
| Type | String at angle to slope |
| Difficulty | Standard +0.3 This is a standard A-level mechanics problem involving resolving forces in equilibrium (part a) and with acceleration (part b). Part (a) requires resolving horizontally and vertically with friction, which is routine. Part (b) adds an incline and acceleration but follows the same systematic approach. The 12 total marks reflect length rather than conceptual difficulty—all techniques are standard for A-level mechanics with no novel insight required. |
| Spec | 3.03c Newton's second law: F=ma one dimension3.03d Newton's second law: 2D vectors3.03e Resolve forces: two dimensions3.03f Weight: W=mg3.03g Gravitational acceleration3.03i Normal reaction force3.03m Equilibrium: sum of resolved forces = 03.03r Friction: concept and vector form3.03s Contact force components: normal and frictional3.03t Coefficient of friction: F <= mu*R model3.03v Motion on rough surface: including inclined planes |
| Answer | Marks |
|---|---|
| 16(a) | Resolves horizontally and |
| Answer | Marks | Guidance |
|---|---|---|
| and cos) | AO3.4 | M1 |
| Answer | Marks | Guidance |
|---|---|---|
| R and F | AO1.1b | A1 |
| Answer | Marks | Guidance |
|---|---|---|
| ‘their’ values for F and R | AO1.2 | B1 |
| Answer | Marks | Guidance |
|---|---|---|
| and contains no slips | AO2.1 | R1 |
| (b)(i) | Draws correct diagram with |
| Answer | Marks | Guidance |
|---|---|---|
| Can use Mg or 8g or 78.4 for W | AO3.3 | B1 |
| Answer | Marks | Guidance |
|---|---|---|
| Q | Marking Instructions | AO |
| Answer | Marks |
|---|---|
| 16(b)(ii) | Resolves perpendicular to the |
| Answer | Marks | Guidance |
|---|---|---|
| directions | AO3.1b | M1 |
| Answer | Marks | Guidance |
|---|---|---|
| vertical equations | AO1.1b | A1 |
| Answer | Marks | Guidance |
|---|---|---|
| Eliminates R to solve for T | AO3.1b | M1 |
| Answer | Marks | Guidance |
|---|---|---|
| without R | AO1.1b | A1 |
| Answer | Marks | Guidance |
|---|---|---|
| Dependent on previous M1 | AO3.1b | dM1 |
| Solves for T | AO1.1b | A1 |
| Answer | Marks | Guidance |
|---|---|---|
| mark have been awarded | AO3.2a | A1F |
| Total | 12 | |
| Q | Marking Instructions | AO |
Question 16:
--- 16(a) ---
16(a) | Resolves horizontally and
vertically to obtain expressions
for F and R
(allow consistent mixing of sin
and cos) | AO3.4 | M1 | Resolving vertically
R = 8 × 9.8 – 50sin 40°
Resolving horizontally
F = 50cos 40°
F R
50cos40(89.850sin40)
50cos40
89.850sin40
μ = 0.8279660445 = 0.83 (2 sf)
AG
Obtains correct expressions for
R and F | AO1.1b | A1
States friction model F = μR with
‘their’ values for F and R | AO1.2 | B1
Completes a rigorous argument
that results with correct μ AG
Only award if they have a
completely correct solution,
which is clear, easy to follow
and contains no slips | AO2.1 | R1
(b)(i) | Draws correct diagram with
exactly four forces showing
arrow heads and labels
Can use Mg or 8g or 78.4 for W | AO3.3 | B1 | T
R
F or μR
W
Q | Marking Instructions | AO | Marks | Typical Solution
--- 16(b)(ii) ---
16(b)(ii) | Resolves perpendicular to the
plane resulting in a three term
equation containing; R, 8gcos 5°
and Tsin 40° (or Tcos 50°)
OR
Resolves horizontally and
vertically to obtain equations of
motion in horizontal and vertical
directions | AO3.1b | M1 | R = 8 9.8cos 5° – Tsin 40°
= 78.1 – Tsin 40°
Tcos 40° – 8 9.8sin 5°– F = 8 3
Tcos 40° – 8 9.8sin 5°
– 0.827…×(8 × 9.8cos 5° –
Tsin 40°) = 24
2489.8sin 5o0.827...89.8cos 5o
T
cos 40o0.827...sin 40o
T = 73.55939193 = 74 (2 sf)
Obtains correct expression for R
OR
Obtains correct horizontal and
vertical equations | AO1.1b | A1
Forms a four term equation of
motion parallel to the plane with
correct terms
(allow sign errors)
OR
Eliminates R to solve for T | AO3.1b | M1
Obtains correct equation of motion
OR
Obtains correct expression(s)
without R | AO1.1b | A1
Uses the friction model in the four
term equation of motion where R is
in the form a – bT and a and b are
positive constants
OR
Uses the friction model in the
horizontal and vertical equations
Dependent on previous M1 | AO3.1b | dM1
Solves for T | AO1.1b | A1
Obtains correct value of T with 2 sf
accuracy.
FT incorrect value found for T
provided both M1 marks and dM1
mark have been awarded | AO3.2a | A1F
Total | 12
Q | Marking Instructions | AO | Marks | Typical Solution
In this question use $g = 9.8$ m s$^{-2}$.
The diagram shows a box, of mass 8.0 kg, being pulled by a string so that the box moves at a constant speed along a rough horizontal wooden board.
The string is at an angle of 40° to the horizontal.
The tension in the string is 50 newtons.
\includegraphics{figure_16a}
The coefficient of friction between the box and the board is $\mu$
Model the box as a particle.
\begin{enumerate}[label=(\alph*)]
\item Show that $\mu = 0.83$
[4 marks]
\item One end of the board is lifted up so that the board is now inclined at an angle of 5° to the horizontal.
The box is pulled up the inclined board.
The string remains at an angle of 40° to the board.
The tension in the string is increased so that the box accelerates up the board at 3 m s$^{-2}$
\includegraphics{figure_16b}
\begin{enumerate}[label=(\roman*)]
\item Draw a diagram to show the forces acting on the box as it moves.
[1 mark]
\item Find the tension in the string as the box accelerates up the slope at 3 m s$^{-2}$.
[7 marks]
\end{enumerate}
\end{enumerate}
\hfill \mbox{\textit{AQA Paper 2 Q16 [12]}}